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2024Activity reportProject-TeamATLANTIS

RNSR: 202023535Z
  • Research center Inria Centre at Université Côte d'Azur
  • In partnership with:CNRS, Université Côte d'Azur
  • Team name: modeling and numerical methods for computATionaL wave-mAtter iNteracTIons at the nanoScale
  • In collaboration with:Laboratoire Jean-Alexandre Dieudonné (JAD)
  • Domain:Applied Mathematics, Computation and Simulation
  • Theme:Numerical schemes and simulations

Keywords

Computer Science and Digital Science

  • A3.4.5. Bayesian methods
  • A3.4.6. Neural networks
  • A3.4.8. Deep learning
  • A6.1.5. Multiphysics modeling
  • A6.2.1. Numerical analysis of PDE and ODE
  • A6.2.6. Optimization
  • A6.2.7. High performance computing

Other Research Topics and Application Domains

  • B4. Energy
  • B4.3.4. Solar Energy
  • B5.3. Nanotechnology
  • B5.5. Materials
  • B8. Smart Cities and Territories
  • B8.2. Connected city

1 Team members, visitors, external collaborators

Research Scientists

  • Stéphane Lanteri [Team leader, INRIA, Senior Researcher]
  • Mahmoud Elsawy [INRIA, ISFP]

Faculty Members

  • Stéphane Descombes [UNIV COTE D'AZUR, Professor]
  • Claire Scheid [UNIV COTE D'AZUR, Associate Professor]

Post-Doctoral Fellows

  • Ayoub Bellouch [INRIA, Post-Doctoral Fellow]
  • Alemayehu Getahun Kumela [INRIA, Post-Doctoral Fellow, from Nov 2024]

PhD Students

  • Arthur Clini De Souza [SOLNIL, CIFRE]
  • Carlotta Filippin [INRIA, from Nov 2024]
  • Roman Gelly [UNIV COTE D'AZUR, from Sep 2024]
  • Daria Hrebenshchykova [INRIA, from Nov 2024]
  • Enzo Isnard [THALES, CIFRE]
  • Cedric Legrand [INRIA, until Oct 2024]
  • Martin Lepers [STMicroelectronics, CIFRE]
  • Larissa Miguez Da Silva [LNCC-PETROPOLIS, until Mar 2024]
  • Florentin Proust [INRIA]
  • Alexandre Pugin [INRIA, from Oct 2024]

Technical Staff

  • Alexis Gobe [INRIA, Engineer]
  • Arthur Gouinguenet [CNRS, from May 2024, Engineer]
  • Guillaume Leroy [INRIA, Engineer]
  • Alan Youssef [INRIA, Engineer]

Interns and Apprentices

  • Carlotta Filippin [INRIA, Intern, until Mar 2024]
  • Roman Gelly [INRIA, Apprentice, until Sep 2024]
  • Daria Hrebenshchykova [INRIA, Intern, from May 2024 until Oct 2024]
  • Nawfal Maghraoui [INRIA, Intern, from Jun 2024 until Sep 2024]
  • Julien Noel [UNIV COTE D'AZUR, Apprentice, from Oct 2024]
  • Alexandre Pugin [INRIA, Intern, until Feb 2024]

Administrative Assistant

  • Delphine Robache [INRIA]

2 Overall objectives

Nanostructuring of materials has paved the way for manipulating and enhancing wave-matter interactions, thereby opening the door for the full control of these interactions at the nanoscale. In particular, the interaction of light waves (or more general optical waves) with matter is a subject of rapidly increasing scientific importance and technological relevance. Indeed, the corresponding science, referred to as nanophotonics43, aims at using nanoscale light-matter interactions to achieve an unprecedented level of control on light. Nanophotonics encompasses a wide variety of topics, including metamaterials, plasmonics, high resolution imaging, quantum nanophotonics and functional photonic materials. Previously viewed as a largely academic field, nanophotonics is now entering the mainstream, and will play a major role in the development of exciting new products, ranging from high efficiency solar cells, to personalized health monitoring devices able to detect the chemical composition of molecules at ultralow concentrations. Plasmonics 46 is a field closely related to nanophotonics. Metallic nanostructures whose optical scattering is dominated by the response of the conduction electrons are considered as plasmonic media. If the metallic structure presents an interface with a positive dielectric permittivity, collective oscillations of surface electrons create waves (called surface plasmons) that are guided along the interface, with the unique characteristic of subwavelength-scale confinement. Nanofabricated systems that exploit these plasmon waves offer fascinating opportunities for crafting and controlling the propagation of light in matter. In particular, it can be used to channel light efficiently into nanometer-scale volumes. As light is squeezed down into nanoscale volumes, field enhancement effects occur resulting in new optical phenomena that can be exploited to challenge existing technological limits and deliver superior photonic devices. The resulting enhanced sensitivity of light to external parameters (for example, an applied electric field or the dielectric constant of an adsorbed molecular layer) shows also great promises for applications in sensing and switching.

In ATLANTIS, our research activities aim at studying and impacting some scientific and technological challenges raised by physical problems involving optical waves in interaction with nanostructured matter. A crucial component in the implementation of this scientific endeavor lies in a close networking with physicists who bring the experimental counterpart of the proposed research. Driven by a number of nanophotonics-related physical drivers, our overall objectives are to design and develop innovative numerical methodologies for the simulation of nanoscale light-matter interactions and to demonstrate their capabilities by studying challenging applications in close collaboration with our physicist partners. On the methodological side, the Discontinous Galerkin (DG) family of methods is a cornerstone of our contributions. In particular, we study various variants of DG methods that can deal with complex material models and coupled PDE systems that are relevant to the study of nanoscale light-matter interactions. Moreover, mathematical modeling is a central activity of the team, in particular for shaping initial and boundary value problems in view of devising accurate, efficient and robust numerical methods in the presence of multiple space and time scales or/and geometrical singularities. Additional methodological topics that are considered in close collaboration with colleagues from other Inria teams or external applied mathematics research groups are model order reduction, inverse design. Novel methodological contributions on these topics in the context of the physical problems studied in ATLANTIS are eventually implemented in the DIOGENeS software suite, which is a unique software plaform dedicated to computational nanophotonics.

3 Research program

3.1 Driving physical fields

Our research activities eventually materialize as innovative computational techniques for studying concrete questions and applications that are tightly linked to specific physical fields (driving physical fields) related to nanophotonics and plasmonics. In most cases, these scientific topics and applications are addressed in close collaboration with physicists.

Quantum plasmonics. The physical phenomena involved in the deep confinement of light when interacting with matter opens a major route for novel nanoscale devices design. Indeed, the recent progress of fabrication at the nanoscale makes it possible to conceive metallic structures with increasingly large size mismatch, in which microscale devices can be characterized by sub-nanometer features 38. These advances have also allowed to achieve spatial separation between metallic elements of only few nanometers 36. At such sizes quantum effects become non-negligible, producing huge variations in the macroscopic optical response. Following this evolution, the quantum plasmonics field has emerged, and with it the possibility of building quantum-controled devices, such as single photon sources, transistors and ultra-compact circuitry at the nanoscale. In ATLANTIS, we study novel numerical modeling methods for solving some semi-classical models of quantum plasmonic effects such as in the context of the PhD work of Nikolkai Schmitt 53-18.

Planar optics. Nanostructuring of matter can be tailored to shape, control wavefront and achieve unusual device operations. Recent years have seen tremendous advances in the fabrication and understanding of two-dimensional (2D) materials, giving rise to the field of planar optics. In particular, the concept of quasi-2D metasurfaces has started to develop into an exciting research area, where nanostructured surfaces are designed for novel functionalities 44-37-39. Metasurfaces are planar metamaterials with subwavelength thickness, consisting of single-layer or few-layer stacks of nanostructures. They can be readily fabricated using lithography and nanoprinting methods, and the ultrathin thickness in the wave propagation direction can greatly suppress the undesirable losses. Metasurfaces enable a spatially varying optical response (e.g. scattering amplitude, phase, and polarization). They mold optical wavefronts into shapes that can be designed at will, and facilitate the integration of functional materials to accomplish active control and greatly enhanced nonlinear response. Our first contributions on this topic have been obtained in the context of the ANR OPERA project (completed in September 2022) and are concerned with numerical modeling methods for the inverge design of metasurfaces 5-3 and metalenses 4.

Thermoplasmonics. Plasmonic resonances can be exploited for many applications 46. In particular, the strong local field enhancement associated with the plasmonic resonances of a metallic nanostructure, together with the absorption properties of the metal, induce a photo-thermal energy conversion. Thus, in the vicinity of the nanostructure, the temperature increases. These effects, viewed as ohmic losses, have been for a long time considered as a severe drawback for the realization of efficient devices. However, the possibility to control this temperature rise with the illumination wavelength or polarization has gathered strong interest in the nano-optics community, establishing the basis of thermoplasmonics 34. By increasing temperature in their surroundings, metal nanostructures can be used as integrated heat nanosources. Decisive advances are foreseen in nanomedicine with applications in photothermal cancer therapy, nano-surgery, drug delivery, photothermal imaging, protein tracking, photoacoustic imaging, but also in nano-chemistry, optofluidics, solar and thermal energy harvesting (thermophotovoltaics).

Optoelectronics and nanoelectronics. Semiconductors also play a major role in leveraging nanoscale light-matter interactions. Emission or absorption of light by a semiconductor is at the heart of optoelectronics, which is concerned with devices that source, detect or control light. Photodiodes, solar cells, light emitting diodes (LEDs), optical fibers and semiconductor lasers are some typical examples of optoelectronic devices. The attractive properties of these devices is based on their efficiency in converting light into electrical signals (or vice versa). Using a structuration with low dimensional materials and carrier-photons interaction, optoelectronics aims at improving the quality of these systems. A closeby field is nanoelectronics 47, i.e., the physical field that, while incorporating manufacturing constraints, tries to describe and understand the influence of the nanostructuration of electronic devices on their electronic properties. This area has quickly evolved with the increasing fabrication capabilities. One striking motivating example is the drastic increase of the number of transistors (of a few nanometer size) per chip on integrated circuits. At the achieved nanostructuration scales, inter-atomic forces, tunneling or quantum mechanical properties have a non-negligible impact. A full understanding of these effects is mandatory for exploiting them in the design of electronic components, thereby improving their characteristics.

3.2 Research agenda

The processes that underly the above-described physical fields raise a number of modeling challenges that motivate our research agenda:

  • They exhibit multiple space and time scales;
  • They are highly sensitive to exquisite geometrical features of nanostructures and matter nanostructuring;
  • They impose dealing with unconventional material models;
  • They may require to leave the comfortable setting of linear differential models;
  • Some of them are inherently multiphysics processes.

3.2.1 Core research topics

Our research activities are organized around core theoretical and methodological topics to address the above-listed modeling challenges.

High order DG methods. Designing numerical schemes that are high order accurate on general meshes, i.e., unstructured or hybrid structured/unstructured meshes, is a major objective of our core research activities in ATLANTIS. We focus on the family of Discontinuous Galerkin (DG) methods that has been extensively developed for wave propagation problems during the last 15 years. We investigate several variants, namely nodal DGTD for time-domain problems, and HDG (Hybridized DG) for frequency-domain problems, with the general goal of devising, analyzing and developing extensions of these methods in order to deal with the above-mentioned physical drivers: nonlinear features, in particular in relation with generation of higher order harmonics in electromagnetic wave interaction with nonlinear materials, and nonlinear models of electronic response in metallic and semiconductor materials; multiphysic couplings such as for instance when considering PDE models relevant to thermoplasmonics, optoelectronics and nanoelectronics. There are to date very few works promoting DG-type methods for these situations. Our methodological contributions of these methods eventually materialize in the DIOGENeS software suite.

Time integration for multiscale problems. Multiscale physical problems with complex geometries or heterogeneous media are extremely challenging for conventional numerical simulations. Adaptive mesh refinement is an attractive technique for treating such problems and will be developed in our research activities in ATLANTIS. Local mesh refinement imposes a severe stability condition on explicit time integration since the allowed maximal time step size is constrained by the smallest element in the mesh. We consider different ways to overcome this stability condition, especially by using implicit-explicit (IMEX) methods where a time implicit scheme is used only for the refined part of the mesh, and a time explicit scheme is used for the other part.

Reduced-order and surrogate modeling. Reduced-order modeling aims at reducing the computational requirements of costly high-fidelity solution methods while maintaining an acceptable level of accuracy. One of the most studied methods for establishing the reduced-order model is the Proper Orthogonal Decomposition (POD), also known as Karhunen-Loéve decomposition, principal component analysis, or singular value decomposition, which uses the solutions of high fidelity numerical simulations or experiments at certain time instants, typically called snapshots, to compute a set of POD basis vectors spanning a low-dimensional space. POD is very popular in the computational fluid dynamics field. However, the development of POD for electromagnetics has been more scarce. We study POD-based reduced-order modeling strategies in the context of a long term collaboration that has started in 2018 with researchers at the School of Mathematical Sciences of the University of Electronic Science and Technology of China and Southwest University of Finance & Economics, which are both located in Chengdu. In the context of this collabortaion, we have proposed and developed several reduced-order modeling techniques, from intrusive to fully data-driven and non-intrusive methods, for time-domain electromagnetics. Alternatively, several works in the recent years have promoted highly efficient surrogate modeling approaches based on Deep Neural Networks (DNNs) to achieve non-linear reduced-order modeling. This is also a novel direction of investigation that we have started to consider in 2023 in the team.

Scientific Machine Learning. Scientific Machine Learning (SciML) is a relatively new research field based on both machine learning (ML) and scientific computing tools. Its aim is the development of new methods to solve several kinds of problems, which can be forward solution of multidimensional partial differential equations, identification of parameters, or inverse problems. The methods that are investigated in this context must be robust, reliable and interpretable. These new SciML tools should also allow the natural inclusion of data in the numerical simulation in order to generate new results. We initiated in 2022 a new research direction on a particular family of DNNs referred as Physics-Informed Neural Networks (PINNs) 51 that we plan to investigate for PDE models that are relevant to nanophotonics with the goal of designing non-intrusive surrogate modeling approaches that require a minimal amount of training data.

Dealing with complex materials. Physically relevant simulations deal with increasing levels of complexity in the geometrical and/or physical characteristics of nanostructures, as well as their interaction with light. Standard simulation methods may fail to reproduce the underlying physical phenomena, therefore motivating the search for more sophisticated light-matter interaction numerical modeling strategies. A first direction consists in refining classical linear dispersion models and we put a special focus on deriving a complete hierarchy of models, that will encompass standard linear models to more complex and nonlinear ones (such as Kerr-type materials, nonlinear quantum hydrodynamic theory models, etc.). One possible approach relies on an accurate description of the Hamiltonian dynamics with intricate kinetic and exchange correlation energies, for different modeling purposes. A second direction is motivated by the study of 2D materials. A major concern is centered around the choice of the modeling approach between a full costly 3D modeling and the use of equivalent boundary conditions, that could in all generality be nonlinear. Assessing these two directions requires efficient dedicated numerical algorithms that are able to tackle several types of nonlinearities and scales.

Dealing with coupled models. Several of our target physical fields are multiphysics in essence and require going beyond the sole description of the electromagnetic response. In thermoplasmonics, the various phenomena (heat transfer through light concentration, bubbles formation and dynamics) call for different kinds of governing PDEs (Maxwell, conduction, fluid dynamics). Since, in addition, these phenomena can occur in significatively different space and time scales, drawing a quite complete picture of the underlying physics is a challenging task, both in terms of modeling and numerical treatment. In the nanoelectronics field, an accurate description of the electronic properties involves including quantum effects. A coupling between Maxwell’s and Schrödinger's equations (again at significantly different time and space scales) is a possible relevant scenario. In the optoelectronics field, the accurate prediction of semiconductors optical properties is a major concern. A possible strategy may require to solve both the electromagnetic and the drift-diffusion equations. In all these aforementioned examples, difficulties mainly arise both from the differences in physical nature as well as in the time/space scales at which each physical phenomenon occurs. Accurately modeling/solving their coupled interactions remains a formidable challenge.

High performance computing (HPC). HPC is transversal to almost all the other research topics considered in the team, and is concerned with both numerical algorithm design and software development. We work toward taking advantage of fine grain massively parallel processing offered by GPUs in modern exascale architectures, by revisiting the algorithmic structure of the computationally intensive numerical kernels of the high order DG-based solvers that we develop in the framework of the DIOGENeS software suite.

3.2.2 Complementary topics

Beside the above-discussed core research topics, we have also identified additional topics that are important or compulsory in view of maximizing the impact in nanophotonics or nanophononics of our core activities and methodological contributions.

Numerical optimization. Inverse design has emerged rather recently in nanophotonics, and is currently the subject of intense research as witnessed by several reviews 48. Artificial Intelligence (AI) techniques are also increasingly investigated within this context 54. In ATLANTIS, we will extend the modeling capabilities of the DIOGENeS software suite by using statistical learning techniques for the inverse design of nanophotonic devices. When it is linked to the simulation of a realistic 3D problem making use of one of the high order DG and HDG solvers we develop, the evaluation of a figure of merit is a costly process. Since a sufficiently large input data set of candidate designs, as required by using Deep Learning (DL), is generally not available, global optimization strategies relying on Gaussian Process (GP) models are considered in the first place. This activity will be conducted in close collaboration with researchers of the ACUMES project-team. In particular, we investigate GP-based inverse design strategies that were initially developed for optimization studies in relation with fluid flow problems 40-41 and fluid-structure interaction problems 52.

Uncertainty analysis and quantification. The automatic inverse design of nanophotonic devices enables scientists and engineers to explore a wide design space and to maximize a device performance. However, due to the large uncertainty in the nanofabrication process, one may not be able to obtain a deterministic value of the objective, and the objective may vary dramatically with respect to a small variation in uncertain parameters. Therefore, one has to take into account the uncertainty in simulations and adopt a robust design model 45. We study this topic in close collaboration with researchers of the ACUMES project-team one on hand, and researchers at TU Braunschweig in Germany.

Numerical linear algebra. Sparse linear systems routinely appear when discretizing frequency-domain wave-matter interaction PDE problems. In the past, we have considered direct methods, as well as domain decomposition preconditioning coupled with iterative algorithms to solve such linear systems 15. In the future, we would like to further enhance the efficiency of our solvers by considering state-of-the-art linear algebra techniques such as block Krylov subspace methods 33, or low-rank compression techniques 50. We will also focus on multi-incidence problems in periodic structures, that are relevant to metagrating or metasurface design. Indeed, such problems lead to the resolution of several sparse linear systems that slightly differ from one another and could benefit from dedicated solution algorithms. We will collaborate with researchers of the CONCACE (Inria center at Université de Bordeaux) industrial project-team to develop efficient and scalable solution strategies for such questions.

4 Application domains

Nanoscale wave-matter interactions find many applications of industrial and societal relevance. The applications discussed in this section are those that we address in the first place in the short- to medium-term. Our general goal is to impact scientific discovery and technological development in these application topics by leveraging our methodological contributions for the numerical modeling of nanoscale wave-matter interactions, and working in close collaboration with external partners either from the academic or the industrial world. Each of these applications is linked to one or more of the driving physical fields described in section 3.1 except nanoelectronics that we consider as a more prospective, hence long-term application.

4.1 Nanostructures for sunlight harvesting

Photovoltaics (PV) converts photon energy from the sun into electric energy. One of the major challenges of the PV sector is to achieve high conversion efficiencies at low cost. Indeed, the ultimate success of PV cell technology requires substantial progress in both cost reduction and efficiency improvement. An actively studied approach to simultaneously achieve both objectives is to exploit light trapping schemes. Light trapping enables solar cells absorption using an active material layer much thinner than the material intrinsic absorption length. This then reduces the amount of materials used in PV cells, cuts cell cost, facilitates mass production of these cells that are based on less abundant material and moreover can improve cell efficiency (due to better collection of photogenerated charge carriers). Enhancing the light absorption in ultrathin film silicon solar cells is thus of paramount importance for improving efficiency and reducing costs. Our activities in relation with this application field aim at precisely studying light absorption in nanostructured solar cell structures (see Fig. 1). We consider both the accurate simulation of light trapping for a given texturing of material layers, and the goal-oriented inverse design of the geometrical characteristics of nanostructuring. This application domain is studied in collaboration with physicists from C2N (Centre for Nanosciences and Nanotechnology) in Campus Paris-Saclay), from LAAS (Laboratoire d'Analyse et d'Architecture des Systèmes) in Toulouse and from the Fraunhofer-Institut für Solare Energiesysteme ISE in Freiburg, Germany.

Figure 1

Example of a PV cell with nanocone gratings. Field map of the module of the electric field.

Figure 1: Example of a PV cell with nanocone gratings. Field map of the module of the electric field.

4.2 Metasurfaces for light front shaping

In the last decade metasurfaces have revolutionized the field of optics with the promise to replace bulky and difficult-to-align optical components with ultrathin and flat devices like metagratings, metalenses and metaholograms, which can also implement new functionalities in terms of aberrations correction and arbitrary wavefront shaping. Metasurfaces produce abrupt changes over the scale of the free-space wavelength in the phase, amplitude and/or polarization of a light beam. Metasurfaces are generally created by assembling arrays of miniature, anisotropic light scatterers, e.g., resonators such as optical antennas. The spacing between antennas and their dimensions are much smaller than the wavelength. As a result the metasurfaces, on account of Huygens principle, are able to mould optical wavefronts into arbitrary shapes with subwavelength resolution by introducing spatial variations in the optical response of the light scatterers (see Fig. 2). Designing metasurfaces for realistic applications such as metalenses is a challenging inverse problem. In this context, an important line of research of the team during the last years has been dedicated to improve the capabilities of these numerical tools to produce novel inverse design methodologies for optical metasurfaces. This application domain is studied in collaboration with several groups of physicists in France and abroad, in particular from CRHEA (Centre de Recherche sur l'Hétéro-Epitaxie et ses Applications) in Sophia Antipolis, MPQ (Matériaux et Phénomènes Quantiques) at Université Paris Cité and EPFL in Lausanne, Switzerland.

Figure 2

Different light front shaping schemes with a metasurface.

Figure 2: Different light front shaping schemes with a metasurface.

4.3 Nanostructuring for THz wave generation

Recent research on the interaction of short optical pulses with semiconductors has stimulated the development of low power terahertz (THz) radiation transmitters. The THz spectral range of electromagnetic waves (0.1 to 10 THz) is of great interest. In particular, it includes the excitation frequencies of semiconductors and dielectrics, as well as rotational and vibrational resonances of complex molecules. As a result, THz waves have many applications in areas ranging from the detection of dangerous or illicit substances and biological sensing to diagnosis and diseases treatment in medicine. The most common mecanism of THz generation is based on the use of THz photoconductive antennas (PCA), consisting of two electrodes spaced by a given gap and placed onto a semiconductor surface. The excitation of the gap by a femtosecond optical pulse induces a sharp increase of the concentration of charge carriers for a short period of time, and a THz pulse is generated. Computer simulation plays a central role in understanding and mastering these phenomena in order to improve the design of PCA devices. The numerical modeling of a general 3D PCA configuration is a challenging task. Indeed, it requires the simultaneous solution of charge transport in the semiconductor substrate and the electromagnetic wave radiation from the antenna in fullwave context. The recently-introduced concept of hybrid photoconductive antennas leveraging plasmonic effects is even more challenging since it requires to include plasmonic nanostructures in the modeling setting. So far, existing simulation approaches are based on the Finite Difference Time-Domain (FDTD) method, and are only able to deal with classical PCAs. In relation with the design of photonic devices for THz waves generation and manipulation, we intend to develop a multiscale numerical modeling strategy for solving the system of Maxwell equations coupled to various models of charge carrier dynamics in semiconductors. Our first achievements on this topic have been obtained in the context of the PhD thesis of Massimiliano Montone defended in June 2023 (see Fig. 3).

Left: unstructured mesh of a model of a plasmon-enhanced antenna. Right: concurrent snapshots of photo-generation and electron concentration at relevant times in the illuminated region of a plasmon-enhanced antenna. Times are marked in ps, in ascending order, from the top to the bottom.

Figure 3: Left: unstructured mesh of a model of a plasmon-enhanced antenna. Right: concurrent snapshots of photo-generation and electron concentration at relevant times in the illuminated region of a plasmon-enhanced antenna. Times are marked in ps, in ascending order, from the top to the bottom.

4.4 Plasmonic nanostructures for nanoscale sensing

The propagation of light in a slit between metals is known to give rise to guided modes. When the slit is of nanometric size, plasmonic effects must be taken into account, since most of the mode propagates inside the metal. Indeed, light experiences an important slowing-down in the slit, the resulting mode being called gap plasmon. Hence, a metallic structure presenting a nanometric slit can act as a light trap, i.e. light will accumulate in a reduced space and lead to very intense, localized fields. Nanocubes are extensively studied in this context and have been shown to support such gap plasmon modes (see Fig. 4). At visible frequencies, the lossy behavior of metals will cause the progressive absorption of the trapped electromagnetic field, turning the metallic nanocubes into efficient absorbers. The frequencies at which this absorption occurs can be tuned by adjusting the dimensions of the nanocube and the spacer. Such metallic nanocubes can be used for a broad range of applications including plasmonic sensing, surface enhanced Raman scattering (SERS), metamaterials, catalysis, and bionanotechnology. We aim at devising a numerical methodology for characterizing the impact of geometrical parameters such as the dimensions of the cube, the rounding of nanocube corners or the size of the slit separating the cube and the substrate, on the overall performance of these absorbers. In practice, this leads us to address two main modeling issues. First, as the size of the slit is decreased, spatial dispersion effects have to be taken into account when dealing with plasmonic structures. For this purpose, we consider a fluid model in the form of a nonlocal hydrodynamic Drude model, which materializes as a system of PDEs coupled to Maxwell's equations. The second issue is concerned with the assessment of geometrical uncertainties and their role in the development of spatial dispersion effects. This application domain is currently studied in collaboration with physicists from the Pascal Institute at Université Clermont Auvergne in Clermont-Ferrand.

Figure 4

Left: scanning electronic microscopy image of silver nanocubes. Right: nanocube setup consisting of an infinite gold ground layer, a dielectric spacer and the cube surrounded by vacuum.

Figure 4: Left: scanning electronic microscopy image of silver nanocubes. Right: nanocube setup consisting of an infinite gold ground layer, a dielectric spacer and the cube surrounded by vacuum.

4.5 Plasmonic nanostructures for photothermal effects

Plasmonic resonances can be exploited for many applications. In particular, the strong local field enhancement associated with the plasmonic resonances of a metallic nanostructure or a dimer of metallic nanostructures (see Fig. 5), together with the absorption properties of the metal, induce a photothermal energy conversion. Thus, in the vicinity of the nanostructure, the temperature increases. These effects, viewed as ohmic losses, have been for a long time considered as a severe drawback for the realization of efficient devices. However, the possibility to control this temperature rise with the illumination wavelength or polarization has gathered strong interest in the nano-optics community, establishing the basis of thermoplasmonics. By increasing temperature in their surroundings, metal nanostructures can be used as integrated heat nanosources. Decisive advances are foreseen in nanomedicine with applications in photothermal cancer therapy, nano-surgery, drug delivery, photothermal imaging, protein tracking, photoacoustic imaging, but also in nano-chemistry, optofluidics, solar and thermal energy harvesting (thermophotovoltaics). Modeling realistic thermoplasmonics effects is a highly multiscale and challenging task. Indeed, the irradiation of a metallic nanoparticle embedded in water with ultrashort laser pulses rapidly excite plasmons that, in return, excite the particle's phonons, which then act as hot carriers and heat the surrounding of the particle through conduction at the metal interface. This process takes place in 10-100 fs1. Furthermore, the concentration of the electromagnetic field in a small volume near the particle can lead to the excitation of a nanoscale plasma in 100 fs – 5 ps. The plasma energy is then transferred to the water molecules in a few picoseconds, leading to high stress and thermal confinement. The resulting extreme temperature and pressure induce cavitation in 1 ns, leading to the formation, growth and collapse of 0.1–10 μm diameter bubbles, with lifetimes ranging from 100 ps up to 100 ns. As of today, the computational methods that have been developed do not enable, as such, efficient prototyping for applications. Our ambition on this topic is to propose innovative numerical methods that are able to deal accurately and efficiently with all the peculiarities of thermoplasmonics phenomena.

Figure 5

Plamonic sphere dimer demonstrating field enhancement in the gap between two glod nanospheres.

Figure 5: Plamonic sphere dimer demonstrating field enhancement in the gap between two glod nanospheres.

4.6 Light management by disordered nanostructures

With recent advances in nanophotonics and nanofabrication, disordered nanostructures are studied for the design of different optical systems with unique features that otherwise cannot be realised by their periodic counterpart, including generation of colors, broadband transmission enhancement, perfect focusing, broadband light trapping and broadband energy harvesting. The disparity of involved length scales, with features on a nanoscale and device characteristics possibly on a millimeter or centimeter scale, renders the quantitative description of the emerging phenomena extremely challenging. Our works on this topic aim at producing fast and accurate optical modeling methods enabling the rigorous calculation of the scattering by a large ensemble of cylindrical scattering centers embedded in a thin film or a bulk medium depending on the target application.

5 Social and environmental responsibility

5.1 Impact of research results

The parts of our research activities that are addressing the design of nanostructures for sunlight harvesting on one hand, and of nanostructures for photothermal effects on the other hand, target applications concerned with production of renewable energy and biomedical engineering (ranging from light controlled drug-release to the battle against Covid-19 in the context of the ANR SWAG-P project).

6 Highlights of the year

6.1 Awards

Ayoub Bellouch (postdoctoral fellow in the team) has been awarded the special prize "Antennas & Propagation" at the JNM 2024 (Journées Nationales Microondes, June 4-7, 2024, in Antibes Juan-Les-Pins) for his work on optimization of subwavelength reflectors for a 2D-Beam steering antenna in Ka-Band 25.

7 New software, platforms, open data

7.1 New software

7.1.1 DIOGENeS

  • Name:
    DIscOntinuous GalErkin Nanoscale Solvers
  • Keywords:
    High-Performance Computing, Computational electromagnetics, Discontinuous Galerkin, Computational nanophotonics
  • Functional Description:
    The DIOGENeS software suite provides several tools and solvers for the numerical resolution of light-matter interactions at nanometer scales. A choice can be made between time-domain (DGTD solver) and frequency-domain (HDGFD solver) depending on the problem. The available sources, material laws and observables are very well suited to nano-optics and nano-plasmonics (interaction with metals). A parallel implementation allows to consider large problems on dedicated cluster-like architectures.
  • URL:
  • Contact:
    Stéphane Lanteri

8 New results

8.1 High order methods for complex problems

In this section, we present ongoing studies aiming at designing, analyzing and developing high order numerical methods for solving PDE systems modeling nanoscale light-matter interactions in relation with the physical seetings and applications presented in section 3. We focus on the family of Discontinuous Galerkin (DG) methods. In the time-domain setting, the starting point of these works is the DGTD (Discontinuous Galerkin Time-Domain) method introduced in 9. In the frequency-domain setting, the HDGFD (Hybridized Discontinuous Galerkin Frequency-Domain) method 1 is considered as the basis of our works.

8.1.1 Time-domain numerical modeling of gain media

Participants: Stéphane Descombes, Stéphane Lanteri, Cédric Legrand, Gian Luca Lippi [INPHYNI laboratory, Sophia Antipolis].

In laser physics, gain or amplification is a process where the medium transfers part of its energy to an incident electromagnetic radiation, resulting in an increase in optical power. This is the basic principle of all lasers. Quantitatively, gain is a measure of the ability of a laser medium to increase optical power. Modeling optical gain requires to study the interaction of the atomic structure of the medium with the incident electromagnetic wave. Indeed, electrons and their interactions with electromagnetic fields are important in our understanding of chemistry and physics. In the classical view, the energy of an electron orbiting an atomic nucleus is larger for orbits further from the nucleus of an atom. However, quantum mechanical effects force electrons to take on discrete positions in orbitals. Thus, electrons are found in specific energy levels of an atom. In a semiclassical setting, such transitions between atomic energy levels are generally described by the so-called rate equations. These rate equations model the behavior of a gain material, and they need to be solved self-consistently with the system of Maxwell equations. So far, the resulting coupled system of Maxwell-rate equations has mostly been considered in a time-domain setting using the FDTD method for which several extensions have been proposed. In the context of the PhD of Cédric Legrand, we study an alternative numerical modeling approach based on a high order DGTD method. This year, we have proposed a first variant that extends the DGTD method introduced in 42. This novel DGTD method has been formulated and analyzed in the three-dimensional case. A fully discrete stability analysis has been conducted and a computer implementation has been finalized. Numerical validations are underway before proceeding to a concrete application in the field of random lasing in collaboration with Gian Luca Lippi at INPHYNI laboratory.

8.1.2 Time-domain numerical modeling of semiconductor devices

Participants: Eric Guichard [Silvaco Inc., Santa Clars, CA, USA], Stéphane Lanteri, Massimiliano Montone, Claire Scheid.

In the field of semiconductor physics modeling, charge carrier transport is the starring phenomenon that needs to be predicted in order to build a mathematical model, based on higher-level quantities (e.g. electric current and voltage), that can be practically used for device simulation. Charge carrier transport is generally described by a drift-diffusion model. This yields a system of coupled partial differential equations which can be solved at two levels: (1) quasistatic approximation: the external force applied to the crystal is electrostatic, and drift-diffusion equations are coupled to a Poisson equation for the electrostatic potential. The goal is to determine the spatial distribution of carrier concentrations and the electric field (deduced from the potential); (2) fullwave model: the crystal is subject to an applied electromagnetic field, and Maxwell equations are coupled with transport equations for carrier dynamics. The goal is to determine the space-time evolution of carrier concentrations and the electromagnetic field. The quasistatic approximation is rigorous when the steady state of the semiconductor has to be calculated. For example, this could be a preliminary step to the fullwave simulation of a device that is biased prior to responding to a (time-varying) electromagnetic excitation. The fullwave model is particularly relevant to electro-optics, i.e. when light-matter interaction is investigated. Indeed, such study is essential to understanding and accurately modeling the operation of photonic devices for light generation, modulation, absorption. In the context of the PhD of Massimiliano Montone (defended in March 2023), we have a designed a DGTD method for solving the coupled system of Maxwell equations and drift-diffusion equations in the fullwave setting. The method has been formulated in the general three-dimensional case, and a computer implementation has been realized in a one dimensional and two-dimensional setting. Furthermore a 1D theoretical stability study has been completed. A preprint gathering the first academical results has been submitted 32. Another paper is in preparation containing more applied results.

8.1.3 Time-domain numerical modeling of plasmonic-based nanoscale heating

Participants: Yves D'Angelo [LJAD, Université Côte d'Azur], Thibault Laufroy, Claire Scheid.

Due to the various scales and phenomena that come into play in realistic thermoplasmonics problems, accurate numerical modeling is challenging. Laser illumination first excites a plasmon oscillation (reaction of the electrons of the metal) that relaxes to a thermal equilibrium and in turn excites the metal lattice (phonons). The latter is then responsible for heating the surroundings. A relevant modeling approach thus consists in describing the electron-phonon coupling through the evolution of their respective temperature. Maxwell's equations are then coupled to a set of coupled nonlinear hyperbolic (or parabolic) equations for the temperatures of respectively electrons, phonons and environment. The nonlinearities and the different time scales at which each thermalization occurs make the numerical approximation of these equations quite challenging. In the context of the PhD of Thibault Laufroy, which has started in October 2020, we propose to develop a suitable numerical framework for studying thermoplasmonics. As a first step, we have reviewed the models used in thermoplasmonics that are most often based on strong or weak (nonlinear) couplings of Maxwell's equations with nonlinear equations modeling heat transfer (hyperbolic or parabolic). We first especially targeted the hyperbolic version of the model and proposed an implementation in 2D, based on a Discontinuous Galerkin approximation in space. We used specific strategies for time integration to account for the multiple time scales of the problem. This has been validated on academical test cases, but also on more concrete cases. A theoretical stability study has also been achieved. A preprint with these first results will soon be submitted for publication. Finally, in view of studying more concrete situations, we have initiated discussions with Stefan Dilhaire (professor at University of Bordeaux and Laboratoire Ondes et matières d'Aquitaine) on one side, and Leonidas Agiotis (postdoctoral researcher, Polytechnique Montréal) on the other side.

8.1.4 Time-domain numerical modeling of liquid crystal materials

Participants: Mahmoud Elsawy, Stéphane Descombes, Stéphane Lanteri, Claire Scheid.

Liquid crystal (LC)-based reconfigurable metasurfaces offer significant potential for advancing active metasurface technologies. This potential stems from their cost-efficiency, ease of fabrication, and ability to operate across a wide frequency spectrum. Among the various types of LCs, nematic liquid crystals are particularly prominent due to their favorable properties for such applications. Traditional LC modeling typically focuses on simulating the static response of the anisotropic permittivity tensor, often assuming that the permittivity simply transitions between two distinct states. However, this static approach neglects the dynamic time-dependent behavior of LCs, a critical factor that is overlooked in the majority of existing studies. Such neglect can lead to inaccuracies in predicting modulation times. Moreover, when LCs are integrated into highly resonant structures, the strong optical confinement within these structures can further influence the LC response time, necessitating more sophisticated modeling. To address these challenges, we have initiated in 2024 a study to develop a comprehensive dynamic model of LC behavior. By coupling the differential equations governing LC orientation under time-varying applied voltages with Maxwell's equations, the proposed model provides an accurate representation of the time-dependent transitions in LC orientation. This approach should surpass conventional odelin approaches by capturing the intricate dynamics of LC responses under varying excitation conditions. Consequently, the proposed model enables precise temporal control of unit cell responses, making it particularly well-suited for the design of reflective and transmissive multiresonant metasurfaces in advanced technological applications. As a next step, we will devise an appropriate discretization of this dynamic model of LC behavior.

8.1.5 Numerical modeling of time-modulated metasurfaces

Participants: Mahmoud Elsawy, Roman Gelly, Stéphane Lanteri.

Active metasurfaces represent a transformative platform for the dynamic modulation of electromagnetic wavefronts, achieved through precise spatial control of the phase and amplitude of scattered light by leveraging arrays of subwavelength scatterers under external stimuli. This spatial modulation imparts tailored momentum to the outgoing light, enabling advanced functionalities such as beam steering, focusing, and holography. Yet, the periodic temporal modulation of these metasurfaces offers the ability to manipulate the frequency content of the scattered light, adding a new dimension of control and unlocking novel possibilities in optical signal processing and frequency-domain applications. However, the accurate numerical modeling of time-modulated metasurfaces poses significant challenges. Temporal modulation introduces dynamic variations in the electromagnetic properties of the metasurface, specifically in the permittivity, which must be seamlessly integrated into Maxwell's equations to account for the interplay between spatial and temporal effects. Such modeling is crucial to predict and optimize the metasurface performance, particularly for applications involving complex temporal waveforms or high-speed modulation. In our work we rely on the Discontinuous Galerkin Time-Domain (DGTD)to address these challenges. In this context, the DGTD approach allows for the discretization of Maxwell's equations in both space and time, enabling accurate modeling of the temporal modulation effects while maintaining the spatial fidelity required to capture subwavelength features. By exploiting DGTD, it is possible to capture the full dynamics of time-modulated metasurfaces, including the generation of frequency sidebands and their spatial diffraction. This capability is essential for designing metasurfaces that integrate both spatial and temporal modulation, enabling functionalities such as frequency mixing, harmonic beam steering, and the controlled breaking of Lorentz reciprocity. Furthermore, the DGTD approach is well-equipped to handle the computational demands of large-scale metasurfaces operating at high frequencies, ensuring accurate predictions and facilitating experimental validation. We have started by the 2D implemntation and we are currently preparing the compariosn with state-of-the art results. The next step is to integrate our 2D code with advanced optimization algorithm to design realistic time-modulated metasurface that can be fabricated and characerized experimentally. This work is carried out in the context of the PhD thesis of Roman Gelly.

8.1.6 Efficient approximation of high-frequency Helmholtz problems

Participants: Théophile Chaumont-Frelet, Victorita Dolean [TU Eindhoven, The Netherlands], Maxime Ingremeau [LJAD, Université Côte d'Azur], Florentin Proust.

Helmholtz problems describe the time-harmonic solutions of the wave equation (possibly in a heterogeneous medium, in a bounded medium, with boundary conditions, etc.). In general, there is no explicit solution to such an equation, and an approximate solution of the equation must be computed numerically. All the existing methods (finite elements, finite differences, etc.) have in common that they are more and more expensive when the frequency of the waves increases. In 35, we study new finite-dimensional spaces specifically designed to approximate the solutions to high-frequency Helmholtz problems with smooth variable coefficients. These discretization spaces are spanned by Gaussian coherent states, that have the key property to be localized in phase space. We carefully select the Gaussian coherent states spanning the approximation space by exploiting the (known) micro-localization properties of the solution. This work is conducted in the context of the Inria POPEG Exploratory Research Action and the topic is also at the heart of the PhD thesis of Florentin Proust.

In the beginning of this thesis, such a method had been implemented for a simple one-dimensional problem. Even in this very simple case, it became clear that Gaussian coherent states could not be used in practice because they were strongly ill-conditioned. However, if the discretization spaces are now spanned by some particular linear combinations of Gaussian coherent states forming a so-called Wilson basis, then this problem disappears. In 35, it had been mathematically proved that using Gaussian coherent states to solve high-frequency Helmholtz problems had some advantages. In 2023, we had started to prove similar - and even broader - results about Wilson basis. In 2024, we continued to work on these theoretical aspects. We also developed a Python code to solve one-dimensional Helmholtz problems with Gaussian coherent states or with a Wilson basis. More precisely, we first focused on a one-dimensional equation with constant coefficients, and then we started to generalize to one-dimensional equations with variable coefficients. This one-dimensional code should be finished by the end of next February. Afterwards, we plan to come back to the theoretical part of the PhD. Finally, in June 2024, Florentin Proust went to the ECCOMAS conference, in Lisbon. He gave a talk in which he introduced the topic of his PhD 26.

8.2 Data-driven reduced-order modeling

In short, reduced order modeling (ROM) allows to construct simplifications of high fidelity, complex models. The resulting lower fidelity (also referred as surrogate) models capture the salient features of the source models so that one can quickly study a system's dominant effects using minimal computational resources.

8.2.1 POD-based ROM methods for parameterized electromagnetic problems

Participants: Xiao-Feng He [UESTC, Chengdu, China], Stéphane Lanteri, Kun Li [SUFEC, Chengdu, China], Liang Li [UESTC, Chengdu, China], Yixin Li [UESTC, Chengdu, China], Ying Zhao [UESTC, Chengdu, China].

In collaboration with researchers at the University of Electronic Science and Technology of China (UESTC) and the Southwestern University of Finance (SUFEC) and Economics, which are both located in Chengdu, we study ROM for time-domain electromagnetics and nanophotonics. More precisely, we have considered the applicability of the proper orthogonal decomposition (POD) technique for the system of time-domain Maxwell equations, possibly coupled to a Drude dispersion model, which is employed to describe the interaction of light with nanometer scale metallic structures. Our first contributions are described in 10-12 where we have proposed POD approach for building a reduced subspace with a significantly smaller dimension given a set of space-time snapshots that are extracted from simulations with a high order DGTD method. Then, a POD-based ROM is established by projecting (Galerkin projection) the global semi-discrete DG scheme onto the low-dimensional space spanned by the POD basis functions.

Subsequently, we have designed several fully data-driven non-intrusive POD-based ROM approaches. In 11, we have proposed the POD-CSI method in the context of parameterized time-domain electromagnetic scattering problems. The considered parameters are the dielectric electric permittivity and the temporal variable. The snapshot vectors are produced by a high order DGTD method formulated on an unstructured simplicial mesh. Because the second dimension of the snapshots matrix is large, a two-step or nested POD method is employed to extract time- and parameter-independent POD basis functions. By using the singular value decomposition (SVD) method, the principal components of the projection coefficient matrices (also referred to as the reduced coefficient matrices) of full-order solutions onto the reduced-basis (RB) subspace are extracted. A cubic spline interpolation-based (CSI) approach is proposed to approximate the dominating time- and parameter-modes of the reduced coefficient matrices without resorting to Galerkin projection. The generation of snapshot vectors, the construction of POD basis functions and the approximation of reduced coefficient matrices based on the CSI method are completed during the offline stage. The RB solutions for new time and parameter values can be rapidly recovered via outputs from the interpolation models in the online stage. In particular, the offline and online stages of the proposed POD-CSI method are completely decoupled, which ensures the computational validity of the method. Moreover, a surrogate error model is constructed as an efficient error estimator for the POD-CSI method. Then in 7-16 we have designed improved versions of the POD-CSI method respectively refererred as POD-CSI-CAE and POD-DMD-RBF.

8.2.2 Nonlinear ROM with Graph Convolutional Autoencoder

Participants: Carlotta Filippin, Stéphane Lanteri, Federico Pichi [EPFL, Switzerland], Maria Strazzullo [Politecnico di Torino, Italy].

Although this POD-CSI method introduced in 11 provides encouraging results, it is not as efficient and robust as one would expect from a ROM perspective. Indeed, the hyperbolic nature of the underlying PDE system, i.e., the system of time-domain Maxwell equations, is known to represent a challenging issue for linear reduction methods such as POD. In practice, a large number of modes is required therefore hampering the obtention of an efficient ROM strategy. One possible path to address this problem, which is currently investigated by several groups worldwide, relies on nonlinear reduction techniques. We initiated this year a study on nonlinear ROM for the time-domain Maxwell equations. More precisely, we study the approach recently proposed in 49, which proposes a nonlinear model order reduction based on a Graph Convolutional Autoencoder (GCA-ROM). This preliminary study aims at realizing a first adaptation and evaluation of the GCA-ROM in the modeling context of time-domain electromagnetics. This study is at the heart of the Master thesis of Carlotta Filippin, and it is conducted in collaboration with Federico Pichi (EPFL, Switzerland) and Maria Strazzullo (Politecnico di Torino, Italy).

8.3 Numerical optimization and inverse design approaches

Participants: Ayoub Bellouch, Mickaël Binois [ACUMES project-team, Centre Inria d'Université Côte d'Azur], Régis Duvigneau [ACUMES project-team, Centre Inria d'Université Côte d'Azur], Mahmoud Elsawy, Stéphane Lanteri.

Developing inverse design approaches for discovering non-intuitive nanostructures or material nanostructuring for harvesting and tailoring the interaction of light with matter on the nanoscale is an important methdological objective of the team.

For this, one has typically to deal with two numerical ingredients: on the one hand, a numerical method for characterizing the optical performance of a given design of the photonic device at hand, which is generally referred to as the forward problem; on the other hand, the so-called inverse problem calls for a numerical optimization algorithm 6, which has to be compatible with the required number of design parameters and the computational cost of the evaluation of a single design with the numerical characterization method. For what concern the former taks, mathematical modeling is generally based on the system of three-dimensional (3D) Maxwell equations formulated in the time-domain or frequency-domain, which is coupled to an appropriate model of frequency-dependent material response. In the recent years, we have developed a computational framework that combines high order Discontinuous Galerkin (DG) methods for solving the system of time-domain 9 or frequency-domain 1 Maxwell equations in 3D with an efficient global optimization technique that belongs to the class of Bayesian optimization.

In our works, we use one of the most advanced optimization techniques based on a statistical learning-based approach, which is known as Efficient Global Optimization (EGO). The EGO algorithm is a global optimization algorithm that substitutes the complex and costly iterative electromagnetic evaluation process with a simpler and cheaper metamodel. EGO is related to the class of Bayesian optimization. Contrary to the traditional common global optimization strategies like genetic algorithms, EGO is not based on adaptive sampling but on a surrogate model, which is constructed on the basis of available objective function evaluations. This surrogate model utilizes a statistical learning criterion related to the optimization target (usually called merit function) in order to identify which design (set of parameters) should be tested in the next iteration that would provide better results close to the predefined goal.

In general, the EGO is based on two phases. The first one is the Design Of Experiment (DOE), in which an initial database is generated. In essence, a uniform sampling strategy (e.g. Latin Hypercube Sampling) is deployed in order to generate different designs in which the cost function is evaluated using an electromagnetic solver. In the second phase, using the data obtained from the DOE, a Gaussian Process (GP) model, is constructed to fit these data. This GP model allows us to predict the values of the cost function in the parameter space without the need to perform additional electromagnetic simulations. Once this GP model is determined, one can estimate at any point of the design space, the objective function (mean of the GP model) and an uncertainty value (variance of the GP model).The mean and the variance are used together to determine a statistical merit function. In our case, we rely on the expected improvement, which is a function whose maximum defines the next design parameters set to be evaluated. That is to say, in the search parameter space where this function is maximized, we extract the corresponding parameter values, and the corresponding design will be simulated using our electromagnetic solver. Then the database is updated accounting for this new observation (construction of a new GP model based on the updated database). We repeat this process until a predefined convergence criterion is reached, or when the expected improvement is sufficiently small.

In the recent past, in close collaboration with researchers from the ACUMES project-team, we have developed inverse design approaches for single-objective optimization of phase gradient metasurfaces operating at visible wavelengths 5. Then, in 4, we presented for the first time to the metasurface community a multiobjective inverse design approach leveraging the EGO method. Finally, in 3, we addressed the optimization of metasurface designs taking into account uncertainties due to fabrication errors still in the framework of the EGO method. All these achievements clearly demonstrate the versatility of the EGO method for inverse design of nanoscale photonic devices.

This year, we have initiated a novel research direction on multifidelity optimization, still in the framework of the EGO algorithm. The overarching goal is to substantially reduce the computational cost of a complex numerical optimization scenario by wisely exploiting different levels of fidelity, i.e., accuracy in our context, in the numerical characterization (forward step) of a device design. For this, we can rely on the flexibility of our DG-based fullwave solvers by playing with the mesh resolution level or/and the degree of the polynomial interpolation method used to approximate the electromagnetic field components cell-wise. Aletrnatively, we can also leverage reduced-order models (see Section 8.2).

8.4 Deep Learning methods

We initiated in 2022 a prospective research direction on alternative numerical modeling methods based on Neural Networks (NN). We investigate both data-driven and model-driven approaches for dealing with the system of Maxwell equations possibly coupled with various material models of interest to nanophotonics. One first question that we want to address is whether DL methods can yield highly efficient surrogate models of 3D time-domain electromagnetic wave propagation problems. Beside, we are also interested in devising DL-based methods for dealing with problems which are more difficult to handle with traditional numerical methods such as electromagnetic wave interaction with space-time adaptive materials or nonlinear media. For this purpose, we study the formulation and application of Physics-Informed Neural Networks (PINNs) that can accurately and efficiently deal with the modeling characteristics of these problems.

8.4.1 PINNs for the parametric Maxwell equations

Participants: Stéphane Lanteri, Nawfal Maghraoui, Alexandre Pugin, Mathieu Riou [Thales Research & Technology, Palaiseau, France].

Numerical simulations of electromagnetic wave propagation problems primarily rely on discretization of the system of time-domain Maxwell equations using finite difference or finite element type methods. For complex and realistic three-dimensional situations, such a process can be computationally prohibitive, especially in view of many-query analyses (e.g., optimization design and uncertainty quantification). Therefore, developing cost-effective surrogate models is of great practical significance. Among the different possible approaches for building a surrogate model of a given PDE system in a non-intrusive way (i.e., with minimal modifications to an existing discretization-based simulation methodology), approaches based on neural networks and Deep Learning (DL) has recently shown new promises due to their capability of handling nonlinear or/and high dimensional problems. In the present study, we propose to focus on the particular case of Physics-Informed Neural Networks (PINNs) introduced in 51. PINNs are neural networks trained to solve supervised learning tasks while respecting any given laws of physics described by a general (possibly nonlinear) PDE system. They seamlessly integrate the information from both the measurements and partial differential equations (PDEs) by embedding the PDEs into the loss function of a neural network using automatic differentiation. In 2022, we have initiated a study dedicated to the applicability of PINNs for building efficient surrogate models of the parametric Maxwell equations. We have progressed on this obejctive this year in the context of the Master internships of Nawfal Maghraoui (frequency-domain Maxwell equations) and Alexandre Pugin (time-domain Maxwell equations). Both settings are now at the heart of the PhD project of Alexandre Pugin, which has started on October 2024.

8.4.2 Multilevel and distributed PINNs for the Helmholtz equation

Participants: Victorita Dolean [TU Eindhoven, The Netherlands], Daria Hrebenshchykova, Stéphane Lanteri, Victor Michel-Dansac [MACARON project-team, Centre Inria de l'Université de Lorraine].

In the context of the Master intersnhip of Daria Hrebenshchykova 31, we investigate recently proposed extensions of PINNs, namely Finite Basis PINNs (FBPINNs) and Multilevel Finite Basis PINNs (MFBPINNs), for solving the Helmholtz equation in one and two dimensions. Through numerical simulations, we compare the efficiency, accuracy, and scalability of these methods. While FBPINNs exhibit good performance for low-frequency problems, the multilevel method outperforms the FBPIN method for high-frequency problems. This work also introduces neural network architectures and training schemes, including architectures based on single and multiple optimizers, integrated into the ScimBa library developed by the MACARON project-team of Centre Inria de l'Université de Lorraine. The results demonstrate the advantages of the multilevel approach for solving complex frequency-domain acoustic and electromagnetic wave propagation problems, which will be the objective of the PhD project of Daria Hrebenshchykova that has started on November 2024.

8.4.3 Efficient deep learning methodology for large-scale metalens

Participants: Marco Abbarchi [Solnil, Marseille, France], Arthur Clini de Souza, Mahmoud Elsawy, Hugo Enrique Hernandez-Figueroa [University of Campinas (Unicamp), Campinas, Sao Paulo, Brazil], Badre Kerzabi [Solnil, Marseille, France], Stéphane Lanteri, Plaoma Pellegrini [University of Campinas (Unicamp), Campinas, Sao Paulo, Brazil].

Metasurfaces are the 2D equivalent of metamaterials, having wavelength-sized elements that leverage various physical phenomena to control the wavefront of the transmitted and reflected beams. Building on our recent advancements in deep learning (DL) 2, we develop an efficient deep learning strategy for designing large-scale metalenses in reflection 21-24. Our strategy is based on optimizing several beam deflectors for a wide range of diffracted angles. This eliminates the need for individual optimization for each angle, similar to our earlier work on color filter designs in 2. The proposed structure consists of supercells with two distinct ridges made of TiO2 (see Fig. 6). The widths, height and spacing between these ridges are optimized parameters, ensuring enhanced performance of the diffracted beams. We simulated 10 000 different unit cells configurations to build a dataset. Afterwards, we trained a deep neural network surrogate model, which defines two functions. Firstly, it can be exploited as a fast solver to replace costly fullwave simulations. Secondly, it represents a differentiable solver, enabling efficient gradient optimization. The next step is training a Multi-Valued Artificial Neural Network (MVANN) to predict the possible designs responsible for generating a target response. The last step is using a network, hereby called the condenser, to filter out the spurious solutions of the MVANN and post-process the geometrical parameters, such as uniforming the height across all solutions and applying hard constraints. This approach allowed precise selection of the period and corresponding deflection angles. Several metalenses with different diameters have been optimized ranging from 50 µm to 1 mm demonstrating scalability of our approach. Our academic partner in Brazil is in the process of fabricating the optimized metalens structures. The results of this study are expected to be published in early 2025.

(a) shows the representation of the considered structure with the optimization parameters. (b) presents the gathering technique to form highly perfroamnce metalens in reflection. (c): numerical simulation of a metalens with numerical aperture in the range of 0.5 with a diameter of 50 μm.

Figure 6: Panel (a) shows the representation of the considered structure with the optimization parameters. Panel (b) presents the gathering technique to form highly performance metalens in reflection. Panel (c) displays numerical simulation of a metalens with numerical aperture in the range of 0.5 with a diameter of 50 μm.

8.5 Discovering novel nanoscale structures

At the creation of the team in February 2020, our collaborations with physicists from the nanophotonics domain aimed at leveraging our developed numerical modeling methodologies in order to study specific topics in relation with concrete applications (see Section 8.7 for more details). An evolution that started in 2022 was our will to adapt and exploit these numerical methodologies to discover nanostructure organizations exhibiting behaviors and performances opening the road to new application perspectives.

8.5.1 Trimer metasurfaces for highly sensitive biomedical sensors

Participants: Haogang Cai [Department of Biomedical Engineering, New York University, USA], Mahmoud Elsawy, Stéphane Lanteri, Hao Wang [Department of Biomedical Engineering, New York University, USA].

In this work, we design a highly sensitive metasurface for biomedical sensing relying on toroidal dipoles. Through numerical simulations (see Fig. 7) and experimental validation, we unveil that these metasurfaces offer remarkable sensitivity, especially across the visible spectrum. This high sensitivity enables the detection of refractive index variations with high precision, which would have great value in many biomedical applications. The fabrication and the experimental characterization have been done and showed a very good agreement with our numerical simulations. We are preparing a paper to be submitted in early 2025.

Figure 7

(a) shows the transmission response of the trimer metasurface. (b) presents the sensitivity analysis of the three main modes together the field profile of the toridal mode.

Figure 7: Panel (a) shows the transmission response of the trimer metasurface. Panel (b) presents the sensitivity analysis of the three main modes together the field profile of the toridal mode.

8.6 Software developments in DIOGENeS

Participants: Alexis Gobé, Arthur Gouinguenet, Guillaume Leroy, Stéphane Lanteri, Alan Youssef.

In order to maximize the impact of our research activities described in section 3, a modern software platform is necessary. For that purpose, the team develops the DIOGENeS (DIscOntinuous GalErkin Nanoscale Solvers) software suite, which is dedicated to the numerical modeling of nanoscale wave-matter interactions in the 3D case. The initial (and current) version of this software concentrates on light-matter interactions with nanometer scale structures, for applications to nanophotonics and nanoplasmonics. DIOGENeS is a unique numerical framework leveraging the capabilities of discontinuous Galerkin methods for the simulation of multiscale problems relevant to nanophotonics and nanoplasmonics. DIOGENeS is a major asset in our strategy to demonstrate that the methodological contributions that we produce can be successfully applied to problems addressed by physicists and engineers trying to exploit specific features of nanoscale wave-matter interactions for scientific and technological applications.

This suite is organized around the following components:

  • A core library containing all the basic building blocks for the construction of high order discontinuous Galerkin methods formulated on tetrahedral, orthogonal hexahedral and hybrid tetrahedral-hexahedral meshes;
  • Fullwave solvers implementing high order discontinuous Galerkin methods for the discretization of time domain (DGTD - Discontinuous Galerkin Time-Domain) and in frequency domain (HDGFD - Hybridized Discontinuous Galerkin Frequency-Domain) coupled to a generalized model of physical dispersion in metallic or semiconductor materials;
  • A library of geometric modeling modules for the definition of simulation configurations involving nanostructures or nanostructured materials. This library exploits the Python API of the GMSH solver;
  • A bridge component between fullwave solvers, geometric modeling modules and numerical optimization algorithms for the inverse design of nanostructures. This component integrates shape parameterization modules, but also scripts defining optimization workflows driving the use of statistical learning-based global optimization algorithms from the Trieste toolbox, which is built on TensorFlow and is dedicated to Bayesian optimization;
  • A library of core modules for allowing users to define their own physical observables, e.g., total transmittance, volumic absorptance, scattering parameters, etc., from results of fullwave simulations.

The core library and the fullwave solvers are based on an object-oriented architecture implemented in Fortran 2008. The DGTD and HDGFD solvers are adapted to high performance computing platforms. Two levels of parallelization are currently exploited: a coarse-grained parallelization in distributed memory (between shared-memory processing nodes) combining a partitioning of the computation mesh and a parallel programming based on the message exchange model using the MPI standard.

This year, several novel features have been developed that are concerned with the GFactory and Observer components (see Fig. 8). In addition, we have initiated the development of the Surrogates component, which integrates our contributions on fully data-driven ROM methods. Moreover, a GPU accelerated version of the DGTD fullwave solver has been developed, thus drastically enhancing the high performance computing capabilities of this simulation tool.

Architecture of the DIOGENeS software suite. DGTD and HDGFD are the high order DG-based fullwave solvers for time-domain and frequency-domain modeling settings. GFactory is the geometrical modeling component that exploits the Python API of the GMSH mesh generation tool. Observer is the base component for developing post-processing scripts of simulation results. Optim is the base component for developing inverse design workflows in Python by using statistical learning global optimization algorithms from external frameworks such as Trieste.

Figure 8: Architecture of the DIOGENeS software suite. DGTD and HDGFD are the high order DG-based fullwave solvers for time-domain and frequency-domain modeling settings. GFactory is the geometrical modeling component that exploits the Python API of the GMSH mesh generation tool. Observer is the base component for developing post-processing scripts of simulation results. Optim is the base component for developing inverse design workflows in Python by using statistical learning global optimization algorithms from external frameworks such as Trieste.

8.7 Applications

8.7.1 Modeling of centimeter-scale metasurfaces in imaging systems

Participants: Mahmoud Elsawy, Sébastien Héron [Thales Research & Technology, Palaiseau, France], Enzo Isnard, Stéphane Lanteri.

Metasurfaces are 2D optical components structured at sub-wavelength scale that locally control the properties of incident light. They can perform various functions such as beam steering, polarization control and focusing. However, metasurfaces are still difficult to incorporate into imaging systems due to the difficulty of modeling their behavior together with other components. For a traditional optical system composed of mirrors or refractive lenses, ray-tracing tools are used to predict the imaging performances. For metasurfaces, one cannot use these tools, as geometrical optics is no longer valid for describing the interactions of light with sub-wavelength elements. To accurately simulate them, Maxwell's equations have to be solved using finite difference or finite element methods. These methods are computionally expensive and are only adapted for components of size around ten wavelengths. Thus, they are of no practical use to simulate metasurfaces inside imaging optical systems (see Fig. 9), which are in the centimeter scale for industrial applications in imaging. Beyond this size limitation, one may need to integrate a metasurface neither at the entrance nor at the output of the system. This positionning often leads to smaller incident angle and/or to decrease of the component area because of its relative position with respect to the system stop and pupils. Besides, this also leads to modeling issues: a) the incidents fields are not plane waves anymore, and b) computed electromagnetic fields after the metasurface need to be recast as rays. To address these issues, we develop a novel numerical methodology to couple a fullwave solver with a ray tracing tool in order to simulate a whole system containing mesurfaces and refractive components 22. The main objective is to fully simulate and optimize the whole system including the metasurface to achieve various functionality. This work is implemented in the frame of the PhD of Enzo Isnard. We are preparing a manuscript to be submitted soon to Optics Express journal in early 2025.

Figure 9

Example of an imaging system containing a metasurface. To simulate the whole system, we need to convert rays into electromagnetic fields and vice versa. As the metasurface lies in the middle of the system, the incident wavefront is not necessarily planar.

Figure 9: Example of an imaging system containing a metasurface. To simulate the whole system, we need to convert rays into electromagnetic fields and vice versa. As the metasurface lies in the middle of the system, the incident wavefront is not necessarily planar.

8.7.2 Advanced modeling of nanostructured CMOS imagers based on DG methods

Participants: Stéphane Lanteri, Denis Rideau [STMicroelectronics, Crolles].

The exploitation of nanostructuring to improve the performance of CMOS (Complementary Metal-Oxide-Semiconductor) imagers based on microlens grids is a very promising avenue. In this perspective, numerical modeling is a key component to accurately characterize the absorption properties of these complex imaging structures, which are intrinsically multiscale (from the micrometer scale of the lenses to the nanometric characteristics of the nanostructured material layers). The FDTD (Finite Difference Time-Domain) method is the solution adopted in the first instance for the simulation of the interaction of light with this type of structure. However, because FDTD is based on a Cartesian mesh, this method shows limitations when it comes to accurately account for complex geometric features such as the curvature of microlenses or the texturing of material layer surfaces. In this context of the PhD of Jérémy Grebot, our main objectives are (1) to leverage locally refined meshes with a high order DGTD method for modeling the propagation of light in a nanostructured CMOS imager and, (2) to study and optimize the impact of nanostructuring for improving light absorption. In particular, with respect to the second objective, an inverse design methodology combining a high order DGTD method with a statistical learning-based global optimization algorithm is developed for studying various nanostructuring patterns of the surface of the absorbing semiconductor material such as one- and two-dimensional gratings.

8.7.3 Nanoimprint color filter metasurface for imaging devices

Participants: David Grosso [Institut Matériaux Microélectronique Nanosciences de Provence (IM2NP) Aix-Marseille Université and Solnil], Marco Abbarchi [Institut Matériaux Microélectronique Nanosciences de Provence (IM2NP) Aix-Marseille Université and Solnil], Badre Kerzabi [Solnil], Mahmoud Elsawy, Alexis Gobé, Stéphane Lanteri.

Due to the rapid growth of metasurface applications, several manufacturing techniques have been developed in the past few years. Among them, NanoImprint Lithography (NIL) has been considered as a promising fabrication possibility for metasurface. NIL can achieve features below 100 nm without the need for complex and expensive optics and light sources needed to achieve similar resolutions in advanced photolithography. Yet, despite the advantages of this fabrication procedure, it has some limitations related to the dimensions of the single nanoresonators. In other words, the fabrication constraints related to the aspect ratio (ratio between height and width) is important. Typically, a maximum aspect ratio of 2 can be considered in such a technique. In this work, together with our collaborators from IM2NP, Aix-Marseille Université and the Solnil startup who are specialists in nanoimprint technology, we aim at optimizing a low cost color filtering metasurface for imaging applications taking into account all the fabrication constraints. The main goal of this study is to rely on inverse design strategies to unveil the geometrical characteristics and topological arrangement of meta-atoms to maximize the efficiency of several metasurface configurations. Various shapes with different physical mechanisms have been investigated. It is worth mentioning that, in this study, various shapes have been optimized and studied numerically, yet, as a starting point for the fabrication, the cylindrical pillars will be considered as a first illustration for the nanoimprint fabrication.

8.7.4 Optimization of light trapping in nanostructured solar cells

Participants: Stéphane Collin [Sunlit team, C2N-CNRS, Paris-Saclay, France], Alexis Gobé, Henning Helmers [Fraunhofer-Institut für Solare Energiesysteme ISE, Freiburg, Germany], Oliver Höhn [Fraunhofer-Institut für Solare Energiesysteme ISE, Freiburg, Germany], Stéphane Lanteri, Guillaume Leroy, Ines Revol [LAAS, Toulouse, France].

There is significant recent interest in designing ultrathin crystalline silicon solar cells with active layer thickness of a few micrometers. Efficient light absorption in such thin films requires both broadband antireflection coatings and effective light trapping techniques, which often have different design considerations. In collaboration with physicists from the Sunlit team at C2N-CNRS, we exploit statistical learning methods for the inverse design of material nanostructuring with the goal of optimizing light trapping properties of ultraphin solar cells. This objective is challenging because the underlying electromagnetic wave problems exhibit multiple resonances, while the geometrical settings are non-trivial. Such multi-resonant solar cell structures are attractive for maximizing light absorption for the full solar light spectrum as illustrated in Fig. 10. We exploit statistical learning methods for the inverse design of material nanostructuring with the goal of optimizing light trapping properties of ultraphin solar cells. This study is conducted in collaboration with physicists from C2N (Centre for Nanosciences and Nanotechnology) in Campus Paris-Saclay), LAAS (Laboratoire d'Analyse et d'Architecture des Systèmes) in Toulouse and the Fraunhofer-Institut für Solare Energiesysteme ISE in Freiburg, Germany.

Optimization of light absorption in a solar cell based on a pyramidal grating. Top figures: geometrical model. Bottom: absorption spectra.

Figure 10: Optimization of light absorption in a solar cell based on a pyramidal grating. Top figures: geometrical model. Bottom: absorption spectra.

8.7.5 Plasmonic sensing with nanocubes

Participants: Antoine Moreau [Institut Pascal, Clermont-Ferrand, France], Stéphane Lanteri, Guillaume Leroy, Claire Scheid.

The propagation of light in a slit between metals is known to give rise to guided modes. When the slit is of nanometric size, plasmonic effects must be taken into account, since most of the mode propagates inside the metal. Indeed, light experiences an important slowing-down in the slit, the resulting mode being called gap-plasmon. Hence, a metallic structure presenting a nanometric slit can act as a light trap, i.e. light will accumulate in a reduced space and lead to very intense, localized fields. We study the generation of gap plasmons by various configurations of silver nanocubes separated from a gold substrate by a dielectric layer, thus forming a narrow slit under the cube. When excited from above, this configuration is able to support gap-plasmon modes which, once trapped, will keep bouncing back and forth inside the cavity. We exploit statistical learning methods for the goal-oriented inverse design of cube size, dielectric and gold layer thickness, as well as gap size between cubes in a dimer configuration (see Fig. 11). This study is conducted in collaboration with Antoine Moreau at Institut Pascal (CNRS). Starting in January 2024, we will continue this study in the context of the ANR SWAG-P project, which is coordinated by Antoine Moreau from Institut Pascal, Clermont-Ferrand, France.

Optimization of a plasmonic nanocube dimer setting for the generation of Fano resonances.

Figure 11: Optimization of a plasmonic nanocube dimer setting for the generation of Fano resonances.

8.7.6 Multiple scattering in random media

Participants: Stéphane Descombes, Stéphane Lanteri, Guillaume Leroy, Cédric Legrand, Gian Luca Lippi [INPHYNI laboratory, Nice].

Fluorescence signals emitted by probes, used to characterize the expression of biological markers in tissues or cells, can be very hard to detect due to a small amount of molecules of interest (proteins, nucleic sequences), to specific genes expressed at the cellular level, or to the limited number of cells expressing these markers in an organ or a tissue. Access to information coming from weaker emitters can only come from strengthening the signal, since electronic post-amplification raises the noise floor as well. Molecule-specific biochemical processes are being developed for this purpose, and a new mechanism based on the simultaneous action of stimulated emission and multiple scattering induced by nanoparticles suspended in the sample has been recently demonstrated to effectively amplify weak fluorescence signals. A precise assessment of the signal fluorescence amplification that can be achieved by such a scattering medium requires an electromagnetic wave propagation modeling approach capable of accurately and efficiently coping with multiple space and time scales, as well as with non-trivial geometrical features (shape and topological organization of scatterers in the medium). In the context of a collaboration with physicists from the Institut de Physique de Nice INPHYNI (Gian Luca Lippi from the complex photonic systems and materials group), we initiated this year a study on the simultaneous action of stimulated emission and multiple scattering by randomly distributed nanospheres in a bulk medium (see Fig. 12). From the numerical modeling point of view, our short term goal is to develop a time-domain numerical methodology for the simulation of random lasing in a gain medium.

Multiple scattering by randomly distributed nanospheres in a bulk medium.

Figure 12: Multiple scattering by randomly distributed nanospheres in a bulk medium.

8.7.7 Nonlinear wavefront shaping with optical metasurfaces

Participants: Giuseppe Leo [CNRS-MPQ, Université Paris Cité, France], Jean-Michel Gerard [PHELIQS, CEA and Université Grenoble Alpes, France], Mahmoud Elsawy, Stéphane Lanteri.

In recent years, the control of sub-wavelength light-matter interactions has enabled the observation of new linear optical phenomena, further establishing a new class of ultra-thin devices for real-world applications. To extend metasurface functionality and implement nonlinear manipulations, the scientific community has considered optical metasurfaces for harmonic emission field control. However, the performance of nonlinear metasurfaces is still modest. Flat optics have also shown their potential in the nonlinear optics with wavefront shaping in far-harmonic fields. There is currently a related effort by the nonlinear nanophotonics community to seek higher conversion efficiencies across narrow resonances of the quasi-bound states of the continuum (qBIC) associated with strong near-field coupling and nonlocal resonance modes. However, the overall performance is relatively weak as most of the current studies ignore the strong near-field coupling between neighboring cells. In this collaboration, we exploit the specific advantages of 'thin' resonators that behave like phased-array antennas, unlike photonic crystals with strong localized energies, to develop highly efficient nonlinear metasurfaces for nonlinear wavefront shaping. Within this strategy, we improve the performance of nonlinear wavefront shaping by inverse design optimization of both meta-atoms and meta-molecules. In addition, we consider long-term design options for nonlinear metasurfaces based on perfect nonlocal responses and long-range near-field coupling, and rigorous computational methods to address nonlinearities in terms of nonlocal configurations. Our preliminary results (see Fig. 13) show the ability to improve the second harmonic generation signal by almost a factor of seven. Fabrication and characterization of the structure is currently underway, and the results will be published in a prominent journal. Since October 2024, we continue this study in the context of the ANR NO-RESTRAIN project, which is coordinated by Giuseppe Leo from the MPQ (Matériaux et Phénomènes Quantiques) at Université Paris Cité, France.

Figure 13

Optimized second-harmonic generation (SHG) from an asymmetric nanochair (inset). The left column represent the comparison of SHG response as a function of the pump wavelength for three different designs (classical denote the design without optimization). The right column refers to the field profiles at the two frequencies 2ω and ω for the optimal design.

Figure 13: Optimized second-harmonic generation (SHG) from an asymmetric nanochair (inset). The left column represent the comparison of SHG response as a function of the pump wavelength for three different designs (classical denote the design without optimization). The right column refers to the field profiles at the two frequencies 2ω and ω for the optimal design.

9 Bilateral contracts and grants with industry

9.1 Bilateral contracts with industry

Nom: Simulation of photonic pigments

Participants: Alexis Gobé, Stéphane Lanteri.

  • Duration: Oct 2024 - Mar 2026
  • Local coordinator: Stéphane Lanteri
  • Participants: Valérie Alard [LVMH], Nicolas Benoot [LVMH]
  • To manufacture a colored material, one normally use a dye or pigment. But another approach to producing color is to fabricate a nanostructure that reflects or scatters light so that waves of certain frequencies can interfere constructively. These nanostructured materials are said to have structural colors. Unlike traditional colors, which comes from light-absorbing dyes or pigments that absorb light, structural colors can be made resistant to fading. In this context, it is desirable to obtain a structural color that is independent of angle, i.e., the color is the same regardless of the orientation of the material, and whatever the angle between the light source and the eyes. There are many structurally colored materials that, like an opal stone, are iridescent, which means that the color changes depending on viewing angle and orientation. The reason for this is that the nanostructure of these materials is well-ordered (or crystalline), as in photonic crystals. To manufacture materials whose color is independent of angle, we need to create disordered nanostructures. These materials are called photonic glasses. The aim is to study how the optical properties of these glasses are linked to their structure and the particles. This type of study is primarily based on experiment. In this project, we relied on numerical modeling to study the optical properties of photonic pigments.

Nom: Metasurfaces for the visible, mid-infrared and long infrared

Participants: Mahmoud Elsawy, Arthur Gouinguenet, Stéphane Lanteri.

  • Duration: Sep 2024 - Dec 2025
  • Local coordinator: Stéphane Lanteri
  • Participants: Michel Jegouzo [Safran E&D], Pascal Junique [Safran E&D], Emmanuel Kling [Safran E&D]
  • We initiated this year a novel collaboration with Safran Electronics & Defense in Eragny for the design of several variants of metasurfaces or the visible, mid-infrared and long infrared spectra. In this context, we explore various shapes of meta-atoms for the definition of metadeflectors and metalenses driven by precise operational performances.

10 Partnerships and cooperations

10.1 International initiatives

10.1.1 Associate Teams in the framework of an Inria International Lab or in the framework of an Inria International Program

DNN4Photonics
  • Title:
    Deep Neural Networks for the design of photonic devices
  • Duration:
    2024 ->
  • Coordinators:
    Stéphane Lanteri and Hugo Enrique Hernandez Figueroa (LEMAC laboratory)
  • Partners:
    • Laboratory of Applied and Computational Electromagnetics (LEMAC), Universidade Estadual de Campinas, Brazil
  • Inria contact:
    Stéphane Lanteri
  • Summary:
    In the context of this partnership with researchers form the LEMAC laboratory at Universidade Estadual de Campinas, we aim at studying and developing disruptive approaches based on Deep Neural Networks for modeling and shaping the interactions of optical waves (or light waves) with matter when the latter is structured at the subwavelength scale. Electronic devices that exploit these interactions in their design are called photonic devices. We propose to investigate data-driven Deep Learning methodologies for two main objectives: (1) devising fast and reliable surrogates of light wave propagation in the general case of three-dimentional spatial domains with complex scattering objects and, (2) devising inverse design strategies of photonic devices with unprecedented properties.

10.1.2 STIC/MATH/CLIMAT AmSud projects

  • Claire Scheid is member of the MatAmSud (between Chile, Uruguay, Argentina and France) project entitled NoLoCE (Nonlocal and Local Coupled Equations: Analysis, Computation, and Probability), PI: Juan Pablo Borthagaray (Associate Professor at the Instituto de Matemática y Estadística, Facultad de Ingeniería, Universidad de la República, Uruguay).

10.2 National initiatives

10.2.1 ANR projects

SWEET (Sub-WavelEngth Electro-optic sysTems)

Participants: Henri Camon [CNRS-LAAS], Jean-Yves Duboz [CNRS-CRHEA], Mahmoud Elsawy, Olivier Gauthier-Lafaye [CNRS-LAAS], Samira Khadir [CNRS-CRHEA], Stéphane Lanteri, Daniel Turover [NAPA Technologies].

  • Type: ANR
  • Duration: Jan 2023 to Dec 2026
  • Coordinator: CNRS-LAAS (Toulouse)
  • Partner: Inria (ATLANTIS project-team), CNRS-CRHEA (Sophia Atipolis), NAPA Technologies (Archamps)
  • Inria contact: Stéphane Lanteri
  • Beam steering is a key enabling photonic technology that would improve the performance of light detection and ranging modules (LiDAR). A typical LiDAR component consists of a light source for illumination, a light modulating device to scan the scene and finally a fast detection system to recover the optical information received from the scene. The operation principle of conventional LiDARs relies on the Time-of-Flight (ToF) measurement, where a pulsed laser directed toward a distant reflective object measures the propagation round-trip time (ToF) of light pulses propagating from the laser to the scene and back to the detection module. The LiDAR sector is currently ongoing important research and development efforts to enable real-time sensing of the distance of fast-moving objects, with applications in robotics, autonomous vehicles and future augmented reality devices. Dynamic beam steering with competitive performances requires the deflection of a light beam along any arbitrary direction to spatially scan a large angular field-of-view (FoV) with high speed and high efficiency. SWEET addresses several drawbacks of current LiDAR technologies by proposing innovative ultrafast beam steering systems, their combinations and integration into demonstrator. We propose to realize an ultrafast 2D beam steering system using innovative transparent tunable MS using LC and III-nitride materials. Our motivation is to develop a generic technology to meet the market needs of LiDAR applications in terms of operation speed, FoV, angular resolution, manufacturability. As indicators, we consider the most stringent requirements for LiDAR integration in the automotive industry. In this context, the general objective of our contribution to the SWEET project is to design active metasurface components for dynamic beam steering.
SWAG-P (Sensing With A Gap-Plasmon)

Participants: David Duche [CNRS-IM2NP], Frederic Dumur [CNRS-ICR], Stéphane Lanteri, Olivie Margeat [CNRS-IM2NP], Antoine Moreau [CNRS-Institut Pascal], Carmen Ruiz-Herrero [CNRS-IM2NP], Claire Scheid, Beniamino Sciacca [CNRS-CINaM].

  • Type: ANR
  • Duration: Jan 2024 to Dec 2027
  • Coordinator: CNRS-Institut Pascal (Clermont-Ferrand)
  • Partner: Inria (ATLANTIS project-team), CNRS-IM2NP (Marseille), CNRS-CINaM (Marseille), CNRS-ICR (Marseille)
  • Inria contact: Claire Scheid
  • Point of Care (POC) tests are expected to continue to be increasingly relied on in the coming years. They have been central to the strategy for combating the COVID-19 pandemic and are expected to play an increasingly important role in the future for fighting other epidemics, particularly in developing countries such as India or China. The World Health Organization (WHO) has defined the ideal POC test, emphasizing the importance of Affordable, Sensitive, Specific, User- friendly, Rapid/Robust, Equipment-free, and Deliverable (ASSURED) diagnostic methods. Among all the techniques used to design biosensors, optical techniques are booming, thanks to numerous innovations in nanophotonics and plasmonics. However, not so many innovations meet the ASSURED criteria. To be deliverable, a device has to be stable for months. It is important to use as little materials as possible, because sensors have to be disposed of after use. Miniaturization is attractive in this perspective, especially since it is associated with lower detection limits. Plasmonic resonators have an edge here because of their large interaction cross-section: their response is thus easier to measure. Regarding all the ASSURED criteria, plasmonic sensors at the end of a fiber offer very interesting characteristics. The goal of the SWAG-P project is to explore the potential of a new class of plasmonic resonators with unique properties, called gap-plasmon resonators, for the detection of biological molecules of interest. These resonators are optical “patch antennas” that can be fabricated simply by depositing metal nanocubes of a few tens of nanometers on a dielectric film, deposited on a very thin layer of functionalizable gold. We want to fabricate a biosensor based on an optical fiber to interrogate gap-plasmon resonators through the thin metallic film, from within the fiber. Such a biosensor that can potentially meet all the criteria of the ASSURED framework.
NO-RESTRAIN (NOnlinear metasuRfacE on Silicon photodiode foR infrAred detectIoN)

Participants: Jean-Michel Gerard [PHELIQS, CEA and Université Grenoble Alpes, France], Mahmoud Elsawy, Giuseppe Leo [CNRS-MPQ, Université Paris Cité, France], Stéphane Lanteri.

  • Type: ANR
  • Duration: Oct 2024 to Sep 2027
  • Coordinator: CNRS-MPQ(Grenoble)
  • Partner: Inria (ATLANTIS project-team), CNRS-MPQ, Université Paris Cité (Paris), PHELIQS, CEA and Université Grenoble (Grenoble) Alpes
  • Inria contact: Mahmoud Elsawy
  • In the last years, metasurfaces have revolutionized the field of optics, with the promise of replacing bulky optical systems and providing new functionalities by nanostructured thin films. Flat optics also showed its potential in the nonlinear regime, mostly in III-V semiconductors, and in the NOMOS project MPQ and PHELIQS recently achieved second harmonic generation with phase-front control in a nonlinear metasurface (NLMS). Today the NO-RESTRAIN project aims to harness the full potential of NLMSs by tackling an old problem of nonlinear optics: the upconversion of infrared radiation into the silicon absorption band via sum frequency generation (SFG). By heterogeneous integration of a high-efficiency NLMS, a linear metalens and a single photon avalanche photodiode (SPAD), the project will demonstrate a miniature device allowing for ultrafast detection of infrared signals with wavelength beyond the fast-detection limit of InGaAs APDs. To this end, we will address a triple challenge in design, forefront nanofabrication, and ultrafast characterization. Based on the complementary competences of partners INRIA , MPQ and PHELIQS in design, nanofabrication and nanophotonic measurements, we will both push forward fundamental research and go beyond purely academic interest. The NO-RESTRAIN device will provide the breakthrough of ultrafast detection of infrared radiation at 300 K, spurring the transition of the young NLMS research field from fundamental research into a set of high-impact applied technologies.

10.2.2 DGA/AID RAPID project

AEROCOM (Ultra-flat and low-cost antennas)

Participants: Ayoub Bellouch, Guillaume Bouchet [NANOE], Guillaume de Calan [NANOE], Mahmoud Elsawy, Van Hoang [Thales Research & Technology], Guillaume Leroy, Stéphane Lanteri, Julien Sourice [NANOE], Erika Vandelle [Thales Research & Technology].

  • Type: RAPID
  • Duration: Jan 2023 to Sep 2025
  • Coordinator: NANOE (Palaiseau)
  • Partner: Inria (ATLANTIS project-team), Thales Research & Technology (Palaiseau)
  • Inria contact: Stéphane Lanteri
  • The development of agile, ultra-flat and low-cost Ka-band antennas is a major challenge to enable Internet accessibility in mobility, in particular on board of public land and air transport (trains, buses, airliners), and to secure communication servers (for combat aircraft, military vehicles, etc.). A possible antenna architecture to address this challenge is composed of a radiating source and a deflection system consisting of two deflectors. The compactness and the moderate cost of the de-pointing system could be obtained thanks to the sub-wavelength structuring technique, and to the shaping by additive manufacturing. Indeed, the sub-wavelength patterning technique has recently shown the possibility to realize antenna components much thinner than a homogeneous bulk material, with equivalent or even better radio frequency performance. In this context, the general objective of our contribution to the AEROCOM project is to develop an advanced numerical methodology for the virtual design of subwavelength structured deflectors and their cascading to achieve an ultra-flat Ka-band antenna system consisting of two such metadeflectors.

11 Dissemination

Participants: Stéphane Descombes, Mahmoud Elsawy, Stéphane Lanteri, Claire Scheid.

11.1 Promoting scientific activities

11.1.1 Scientific events: organisation

Member of the organizing committees
  • Claire Scheid has been mentor for the workshop "Empowering a diverse computational mathematics research community", ICERM, Brown University, and coleader of the workgroup "Compatible discretization for nonlinear optical phenomenon" with Camille Carvalho (INSA Lyon, France) and Vrushali A. Bokil (Oregon State University, USA). This mentoring activity is continuing on a regular basis oustside the workshop itself.
  • Stéphane Lanteri is a member of the organization comittee of the "ICON - Nonlinear cell photonics" thematic semester of Université Côte d'Azur. The overarching ICON project aims to consolidate ongoing research initiatives at Université Côte d'Azur, encompassing various aspects of photonics and life sciences, from experimental and applied methods to numerical modeling. Additionally, the project seeks to enrich these endeavors by integrating external insights and expertise, fostering collaborations with researchers from France and beyond.

11.1.2 Journal

  • Stéphane Lanteri is the Lead Editor of a feature issue of Journal of the Optical Society of America B dedicated to recent research results on inverse design in photonics 27.

11.1.3 Invited talks

  • Mahmoud Elsawy, September 26, 2024, INSP - Sorbonne Université, Paris.
  • Mahmoud Elsawy, November 8, 2024, Laboratory of Applied and Computational Electromagnetics (LEMAC), Universidade Estadual de Campinas, Brazil.
  • Claire Scheid, Oberwolfach workshop on "Nonlinear Optics: Physics, Analysis, and Numerics", March 11-15, 2024, MFO center, Germany.
  • Stéphane Lanteri was a plenary speaker at the 16th International Conference on Mathematical and Numerical Aspects of Wave Propagation - Waves 202423, June 30-Jyly 5, 2025, Berlin, Germany.
  • Stéphane Lanteri, April 30, 2024, CEA SPEC - IRAMIS, Gif-sur-Yvette, France.
  • Stéphane Lanteri, October 10, 2024, Thales Research & Technology, Palaiseau, France.
  • Stéphane Lanteri, November 8, 2024, Laboratory of Applied and Computational Electromagnetics (LEMAC), Universidade Estadual de Campinas Campinas, Brazil.
  • Stéphane Lanteri, December 5, 2024, Barcelona Supercomputing Center, Spain.

11.1.4 Leadership within the scientific community

  • Since July 2023, Claire Scheid is member of the Scientific Committee of the "Maison de la simulation et des interactions" of Université Côte d'Azur.
  • Since October 2024, Claire Scheid is an elected CNU (Comité National des Universités) member of the 26th section (applied mathematics).
  • Since June 2024, Stéphane Lanteri is a member of the Scientific Council of the 3iA Côte d'Azur.

11.1.5 Research administration

  • Stéphane Lanteri is a member of the Project-team Committee's Bureau of the Inria research center at Université Côte d'Azur.
  • Stéphane Lanteri is the Deputy Head of Science of Inria Research Center at Université Côte d'Azur (since September 2022).
  • Stéphane Lanteri is a member of Evaluation Committee of Inria (since September 2022).
  • Since September 2024, Claire Scheid is responsible (maths side) of the Mathematics-Physics double degree program (for the 3 years) at Université Côte d'Azur.

11.2 Teaching - Supervision - Juries

11.2.1 Teaching

  • Mahmoud Elsawy, Resolution of linear and nonlinear systems, 24h TP, L3, Université Côte d'Azur.
  • Claire Scheid, Optimisation et éléments finis. Lecture, practical works, M1 MPA and IM, 72h eq.TD, Université Côte d'Azur.
  • Claire Scheid, Option modélisation. Lectures and practical works, M2 Agrégation, 45h eq.TD, Université Côte d'Azur.
  • Claire Scheid, Approximation Numérique des fonctions, intégrales et équations différentielles. Lecture, L3, 56h, Université Côte d'Azur.
  • Stéphane Descombes, Scientific Machine Learning, 15 h, MAM5, Polytech Nice Sophia - Université Côte d'Azur.
  • Stéphane Descombes, Approximation Numérique des fonctions, intégrales et équations différentielles, practical works, L3, 28h, Université Côte d'Azur.
  • Stéphane Descombes, Introduction aux équations aux dérivées partielles, M1, 30h, Université Côte d'Azur.
  • Stéphane Descombes, Calcul scientifique, M1, 30h, Université Côte d'Azur
  • Stéphane Lanteri, Scientific Machine Learning, 24 h, MAM5, Polytech Nice Sophia - Université Côte d'Azur.

11.2.2 Supervision

  • PhD in progress: Arthur Clini De Souza. (Cifre PhD grant with Solnil, Marseille), Deep neural networks for the design of large-scale photonic devices for active beam steering, co-supervised by Mahmoud Elsawy and Stéphane Lanteri.
  • PhD in progress: Daria Hrebenshchykova (PEPR NumPEx PhD fellowship), Building physics-based multilevel substitution models from neural networks. Application to electromagnetic wave propagation, co-supervised by Victor Michel-Dansac (MACARON project-team, Centre Inria de l'Université de Lorraine), Victorita Dolean (Eindhoven University of Technology, The Netherlands) and Stéphane Lanteri.
  • PhD in progress: Enzo Isnard (Cifre PhD grant with Thales Research & Technology, Palaiseau), Modeling and optimization of freeform optical metasurfaces integrated into an imaging system, co-supervised by Mahmoud Elsawy and Stéphane Lanteri.
  • PhD in progress: Carlotta Filippin (ANR SWAG-P PhD fellowship), Reduced-order modeling and global optimization for the robust design of Gap Plasmon Resonators, co-supervised by Claire Scheid, Antoine Moreau (Institut Pascal, Universi†é Clermont-Auvergene) and Stéphane Lanteri.
  • PhD in progress: Roman Gelly (PhD fellowship from Université Côte d'Azur), Advanced numerical modeling of time-modulated metasurfaces, co-supervised by Mahmoud Elsawy and Stéphane Lanteri.
  • PhD defended: Jérémy Grebot (Cifre PhD grant with STMicroelectronics), Advanced modeling of nanostructured CMOS imagers28, Université Côte d'Azur, May 2024, co-supervised by Stéphane Lanteri and Claire Scheid.
  • PhD in progress: Thibault Laufroy (PhD fellowship from Université Côte d'Azur), High order finite element type solvers for thermoplamonics, co-supervised by Yves d'Angelo and Claire Scheid.
  • PhD in progress: Cédric Legrand (DGA-Inria PhD fellowship), High order finite element type solvers for modeling gain media, co-supervised by Stéphane Descombes and Stéphane Lanteri.
  • PhD in progress: Florentin Proust, Novel finite element methods for dealing with high frequency wave propagation problems, co-supervised by Maxime Ingremeau (Université Côte d'Azur, LJAD) and Théophile Chaumont-Frelet.
  • PhD in progress: Alexandre Pugin (DGA-Inria PhD fellowship), Physically informed neural networks for building surrogate models in numerical electromagnetics, co-supervised by Stéphane Descombes and Stéphane Lanteri.
  • Apprenticeship in progress: Julien Noël (MAM5, Polytech Nice Sophia - Université Côte d'Azur), Numerical study of Maxwell-Schrödinger equations, co-supervised by Stéphane Descombes and Claire Scheid.
  • Postdoc in progress: Ayoub Bellouch (AEROCOM RAPID project), Advanced computational design of cascaded metadeflectors for an ultra-flat antenna system Lanteri Stéphane, co-supervised by Mahmoud Elsawy and Stéphane Lanteri.
  • Postdoc in progress: Alemayehu Getahun Kumela (Inria Exploratory Action META4PIQ), Metasurfaces for quantum information processing, supervised by Mahmoud Elsawy.

11.2.3 Juries

  • Mahmoud Elsawy was an examiner for the PhD of Lucas Grosjean, entitled "Nanophotonique en niobate de lithium pour l'intelligence artificielle", Université Bourgogne Franche-Comté, France, December 16, 2024.
  • Mahmoud Elsawy was an examiner for the PhD of Xingyu Yang entitled "Manipulating the inverse Faraday effect at the nanoscale", Sorbonne Université, France, September 27, 2024.
  • Claire Scheid was an examiner for the PhD of Étienne Peillon entitled "Simulation and analysis of sign-changing Maxwell’s equations in cold plasma", ENSTA, Institut Polytechnique de Paris, France, April 4, 2024.
  • Stéphane Lanteri was a reviever for the HDR (accreditation to supervise research) of Juliette Chabassier entitled "Modélisation physique et simulation numérique d’instruments de musique", Université de Pau et des Pays de l'Adour, France, June 26, 2024.
  • Stéphane Lanteri was an examiner for the PhD of Francisco Orlandini entitled "A waveguide port boundary condition for the finite element analysis of optical devices", Universidade Estadual de Campinas Campinas, Brazil, October 7, 2024.
  • Stéphane Lanteri was an examiner for the PhD of Valentin Ritzenthaler entitled "Stratégies de couplage des méthodes Compatible Discrete Operators appliquées aux équations de Maxwell dans le domaine temporel", ISAE-SUPAERO, Toulouse, France, December 10, 2024.

12 Scientific production

12.1 Major publications

  • 1 articleE.Emmanuel Agullo, L.Luc Giraud, A.Alexis Gobé, M.Matthieu Kuhn, S.Stephane Lanteri and L.Ludovic Moya. High order HDG method and domain decomposition solvers for frequency‐domain electromagnetics.International Journal of Numerical Modelling: Electronic Networks, Devices and FieldsOctober 2019HALDOIback to textback to text
  • 2 articleA.Arthur Clini de Souza, S.Stéphane Lanteri, H. E.Hugo Enirique Hernández-Figueroa, M.Marco Abbarchi, D.David Grosso, B.Badre Kerzabi and M.Mahmoud Elsawy. Back-propagation optimization and multi-valued artificial neural networks for highly vivid structural color filter metasurfaces.Scientific Reports131December 2023, 21352HALDOIback to textback to text
  • 3 articleM.Mahmoud Elsawy, M.Mickael Binois, R.Régis Duvigneau, S.Stéphane Lanteri and P.Patrice Genevet. Optimization of metasurfaces under geometrical uncertainty using statistical learning.Optics Express29192021, 29887HALDOIback to textback to text
  • 4 articleM. M.Mahmoud M R Elsawy, A.Anthony Gourdin, M.Mickael Binois, R.Régis Duvigneau, D.Didier Felbacq, S.Samira Khadir, P.Patrice Genevet and S.Stéphane Lanteri. Multiobjective statistical learning optimization of RGB metalens.ACS photonics88July 2021, 2498–2508HALDOIback to textback to text
  • 5 articleM. M.Mahmoud M R Elsawy, S.Stéphane Lanteri, R.Régis Duvigneau, G.Gauthier Brière, M. S.Mohamed Sabry Mohamed and P.Patrice Genevet. Global optimization of metasurface designs using statistical learning methods.Scientific Reports91November 2019HALDOIback to textback to text
  • 6 articleM.Mahmoud Elsawy, S.Stéphane Lanteri, R.Régis Duvigneau, J.Jonathan Fan and P.Patrice Genevet. Numerical optimization methods for metasurfaces.Laser and Photonics Reviews1410October 2020, 1900445HALDOIback to text
  • 7 articleX.-F.Xiao-Feng He, L.Liang Li, S.Stéphane Lanteri and K.Kun Li. Model order reduction for parameterized electromagnetic problems using matrix decomposition and deep neural networks.Journal of Computational and Applied Mathematics431October 2023, 115271HALDOIback to text
  • 8 articleX.-F.Xiao-Feng He, L.Liang Li, S.Stéphane Lanteri and K.Kun Li. Reduced Order Modeling for Parameterized Electromagnetic Simulation Based on Tensor Decomposition.IEEE Journal of Multiscale and Multiphysics Computational Techniques8August 2023, 296-305HALDOI
  • 9 articleS.Stephane Lanteri, C.Claire Scheid and J.Jonathan Viquerat. Analysis of a Generalized Dispersive Model Coupled to a DGTD Method with Application to Nanophotonics.SIAM Journal on Scientific Computing393January 2017, A831 - A859HALDOIback to textback to text
  • 10 articleK.Kun Li, T.-Z.Ting-Zhu Huang, L.Liang Li and S.Stéphane Lanteri. A reduced-order discontinuous Galerkin method based on a Krylov subspace technique in nanophotonics.Applied Mathematics and Computation358October 2019, 128-145HALDOIback to text
  • 11 articleK.Kun Li, T.-Z.Ting-Zhu Huang, L.Liang Li and S.Stéphane Lanteri. Non-intrusive reduced-order modeling of parameterized electromagnetic scattering problems using cubic spline interpolation.Journal of Scientific Computing872May 2021HALDOIback to textback to text
  • 12 articleK.Kun Li, T.-Z.Ting-Zhu Huang, L.Liang Li and S.Stéphane Lanteri. POD-based model order reduction with an adaptive snapshot selection for a discontinuous Galerkin approximation of the time-domain Maxwell's equations.Journal of Computational Physics396November 2019, 106-128HALDOIback to text
  • 13 articleK.Kun Li, T.Ting‐zhu Huang, L.Liang Li and S.Stéphane Lanteri. Simulation of the interaction of light with 3‐D metallic nanostructures using a proper orthogonal decomposition‐Galerkin reduced‐order discontinuous Galerkin time‐domain method.Numerical Methods for Partial Differential EquationsSeptember 2022HALDOI
  • 14 articleK.Kun Li, T.-Z.Ting-Zhu Huang, L.Liang Li, Y.Ying Zhao and S.Stéphane Lanteri. A non-intrusive model order reduction approach for parameterized time-domain Maxwell's equations.Discrete and Continuous Dynamical Systems - Series B281March 2022, 449-473HALDOI
  • 15 articleL.Liang Li, S.Stéphane Lanteri and R.Ronan Perrussel. A hybridizable discontinuous Galerkin method combined to a Schwarz algorithm for the solution of 3d time-harmonic Maxwell's equations.Journal of Computational Physics256January 2014, 563-581HALDOIback to text
  • 16 articleK.Kun Li, Y.Yixin Li, L.Liang Li and S.Stéphane Lanteri. Surrogate modeling of time-domain electromagnetic wave propagation via dynamic mode decomposition and radial basis function.Journal of Computational Physics491October 2023, 112354HALDOIback to text
  • 17 articleN.Nikolai Schmitt, C.Claire Scheid, S.Stéphane Lanteri, A.Antoine Moreau and J.Jonathan Viquerat. A DGTD method for the numerical modeling of the interaction of light with nanometer scale metallic structures taking into account non-local dispersion effects.Journal of Computational Physics316July 2016HALDOI
  • 18 articleN.Nikolai Schmitt, C.Claire Scheid, J.Jonathan Viquerat and S.Stéphane Lanteri. Simulation of three-dimensional nanoscale light interaction with spatially dispersive metals using a high order curvilinear DGTD method.Journal of Computational Physics373November 2018, 210-229HALback to text

12.2 Publications of the year

International journals

International peer-reviewed conferences

  • 21 inproceedingsA.Arthur Clini de Souza, S.Stéphane Lanteri, H. E.Hugo Enrique Hernandez-Figueroa, M.Marco Abbarchi, D.David Grosso, B.Badre Kerzabi and M.Mahmoud Elsawy. Inverse design of bright, dielectric metasurfaces color filters based on back-propagation and multi-valued artificial neural networks.SPIE digital libraryMachine Learning in Photonics13017Proceedings Volume 13017, Machine Learning in Photonics; 130170E (2024)Strasbourg, FranceSPIEJune 2024, 24HALDOIback to text
  • 22 inproceedingsE.Enzo Isnard, S.Sébastien Héron, M.Mahmoud Elsawy and S.Stéphane Lanteri. Modeling of centimeter-scale metasurfaces in imaging systems.SPIE digital libraryComputational Optics 202413023Proceedings volume 13023 SPIE optical systems design: Computational Optics 2024Strasbourg, FranceSPIEApril 2024, 15HALDOIback to text
  • 23 inproceedingsS.Stéphane Lanteri, T.-Z.Ting-Zhu Huang, K.Kun Li, L.Liang Li and A.Alan Youssef. Reduced-order modeling for time-domain electromagnetics.Waves 2024 - The 16th International Conference on Mathematical and Numerical Aspects of Wave PropagationBerlin, GermanyL. GizonJune 2024, 25-30HALDOIback to text
  • 24 inproceedingsA. C.Arthur Clini de Souza, P. E.Paloma Elias da Silva Pellegrini, S. V.Silvia Vaz Guerra Nista, S.Stéphane Lanteri, H. E.Hugo Enrique Hernandez-Figueroa, M.Marco Abbarchi, B.Badre Kerzabi and M.Mahmoud Elsawy. Cost-efficient deep learning method for mass inverse design of photonic devices.IEEE Xplore2024 SBFoton International Optics and Photonics Conference (SBFoton IOPC)Salvador, BrazilIEEEDecember 2024, 3HALDOIback to text

Conferences without proceedings

Edition (books, proceedings, special issue of a journal)

  • 27 periodicalInverse design in photonics.Journal of the Optical Society of America B41Inverse design in photonics2January 2024, IDP1HALDOIback to text

Doctoral dissertations and habilitation theses

Reports & preprints

12.3 Cited publications

  • 33 articleE.E. Agullo, L.L. Giraud and Y.Y.F. Jing. Block GMRES method with ineact breackdowns and deflated restarting.SIAM J. Matrix Anal. Appl.3542014, 1625--1261back to text
  • 34 bookG.G. Baffou. Thermoplasmonics.Cambridge University Press2017back to text
  • 35 articleT.T. Chaumont-Frelet, V.V. Dolean and M.M. Ingremeau. Efficient approximation of high-frequency Helmholtz solutions by Gaussian coherent states.Numer. Math.1562024, 1385–1426back to textback to text
  • 36 articleX.X. Chen, H.H.R. Park, M.M. Pelton, X.X. Piao, N.N.C. Lindquist, H.H. Im, Y.Y.. Kim, J.J.S. Ahn, K.K.J. Ahn, N.N. Park, D.D.S. Kim and S.S.H. Oh. Atomic layer lithography of wafer-scale nanogap arrays for extreme confinement of electromagnetic waves.Nature Comm.42013, 2361back to text
  • 37 articleH.H.T. Chen, A.A.J. Taylor and N.N. Yu. A review of metasurfaces: physics and applications.Rep. Progr. Phys.7972016, 076401back to text
  • 38 articleC.C. Cirac\`i, R.R.T. Hill, J.J.J Mock, Y.Y. Urzhumov, A.A.I. Fernández-Domínguez, S.S.A. Maier, J.J.B. Pendry, A.A. Chilkoti and D.D.R. Smith. Probing the ultimate limits of plasmonic enhancement.Science33760982012, 1072--1074back to text
  • 39 articleF.F. Ding, A.A. Pors and S.S.I. Bozhevolnyi. Gradient metasurfaces: a review of fundamentals and applications.Rep. Progr. Phys.8122018, 026401back to text
  • 40 articleR.R. Duvigneau and P.P. Chandrashekar. Kriging-based optimization applied to flow control.Int. J. Num. Fluids692012, 1701--1714back to text
  • 41 articleR.R. Duvigneau, J.J. Labroquère and E.E. Guilmineau. Comparison of turbulence closures for optimized active control.Comput. Fluids1242016, 67--77back to text
  • 42 articleL.L. Fezoui, S.S. Lanteri, S.S. Lohrengel and S.S. Piperno. Convergence and stability of a discontinuous Galerkin time-domain method for the 3D heterogeneous Maxwell equations on unstructured meshes.ESAIM: Math. Model. Num. Anal.3962005, 1149--1176back to text
  • 43 bookS.S.V. Gaponenko. Introduction to nanophotonics.Cambridge University Press2010back to text
  • 44 articleP.P. Genevet and F.F. Capasso. Holographic optical metasurfaces: a review of current progress.Rep. Progr. Phys.7822015, 024401back to text
  • 45 articleY.Y. He, M.M. Razi, C.C. Forestiere, L. D.L. Dal Negro and R.R.M. Kirby. Uncertainty quantification guided robust design for nanoparticles morphology.Comp. Meth. Appl. Mech. Engrg.893362018, 578--593back to text
  • 46 bookS.S.A. Maier. Plasmonics - Fundamentals and applications.Springer2007back to textback to text
  • 47 bookV.V.V. Mitin, V.V.A. Kochelap and M.M.A. Stroscio. Introduction to nanoelectronics.Cambridge University Press2012back to text
  • 48 articleS.S. Molesky, Z.Z. Lin, A.A.Y. Piggott, W.W. Jin, J.J. Vuckovic and A.A.W. Rodriguez. Inverse design in nanophotonics.Nat. Phot.122018, 659--670back to text
  • 49 articleF.F. Pichi, B.B. Moya and J. H.J.S. Hesthaven a. A graph convolutional autoencoder approach to model order reduction for parametrized PDEs.J. Comput. Phys.5012024, 112762back to text
  • 50 articleG.G. Pichon, E.E. Darve, M.M. Faverge, P.P. Ramet and J.J. Roman. Sparse supernodal solver using block low-rank compression: design performance and analysis.J. Comp. Sci.272018, 255--270back to text
  • 51 articleM.M. Raissi, P.P. Perdikaris and G.G.E. Karniadakis. Physics-informed neural networks: a deep learning framework for solving forward and inverse problems involving nonlinear partial differential equations.J. Comput. Phys.3782019, 686--707back to textback to text
  • 52 articleM.M. Sacher, F.F. Hauville, R.R. Duvigneau, O. L.O. Le Mâitre, N.N. Aubib and M.M. Durand. Efficient optimization procedure in non-linear fluid-structure interaction problem: application to mainsail trimming in upwind conditions.J. Fluids and Struct.692017, 209--231back to text
  • 53 phdthesisN.N. Schmitt. High order simulation and calibration strategies for spatial dispersion models in nanophotonics.University of Nice-Sophia Antipolis2018back to text
  • 54 articleK.K. Yao, R.R. Unni and Y.Y. Zheng. Intelligent nanophotonics: merging photonics and artificial intelligence at the nanoscale.Nanophot.832019, Open AccessURL: https://doi.org/10.1515/nanoph-2018-0183back to text
  1. 11 fs = 1 femtosecond= 10-15 s; 1 ps = 1 picosecond = 10-12 s; 1 ns = 1 nanosecond = 10-9 s.