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        <h2>Section: 
      Overall Objectives</h2>
        <h3 class="titre3">Presentation</h3>
        <p>In applications involving complex physics, such as plasmas and nanotechnologies,
numerical simulations serve as a prediction tool supplementing real experiments and are largely endorsed by engineers or researchers. Their performances rely
not only on computational power, but also on the efficiency of the underlying numerical method and the complexity of the underlying models. The contribution of applied mathematics is then required, on the one hand for
a better understanding of qualitative properties and a better identification of the different regimes present in the model, and on the other hand, for a more sounded construction of new models based on asymptotic analysis. This mathematical analysis is expected to greatly impact the design of <i>multiscale</i> numerical schemes.</p>
        <p>The proposed research group <span class="smallcap">MINGuS </span> will be dedicated
to the mathematical and numerical analysis of (possibly stochastic) partial differential equations (PDEs),
originating from plasma physics and nanotechnologies,
with emphasis on
<i>multiscale</i> phenomena either of <b>highly-oscillatory</b>, of <b>dissipative</b> or <b>stochastic</b> types.
These equations can be also encountered in applications to rarefied gas dynamics, radiative transfer,
population dynamics or laser propagation, for which the
multiscale character is modelled by a scale physical parameter <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mi>ε</mi></math></span>.</p>
        <p>Producing accurate solutions of multiscale equations is extremely challenging owing to severe restrictions to the numerical methods imposed by fast (or stiff) dynamics.
<i>Ad-hoc</i> numerical methods should aim at capturing the slow dynamics solely, instead of resolving finely the stiff dynamics at a formidable computational cost. At the other end of the spectrum, the separation of scales -as required for numerical efficiency- is envisaged in asymptotic techniques, whose purpose is to describe the model in the limit where the small parameter <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mi>ε</mi></math></span> tends to zero.
<span class="smallcap">MINGuS </span> aspires to accommodate sophisticated tools of mathematical analysis and heuristic numerical methods in order to produce simultaneously rich asymptotic models and efficient numerical methods.</p>
        <p class="notaparagraph">To be more specific, <span class="smallcap">MINGuS </span> aims at finding, implementing and analysing
new multiscale numerical schemes for the following physically relevant multiscale problems:</p>
        <p><b>Highly-oscillatory Schrödinger equation for nanoscale physics:</b>
In quantum mechanics, the Schrödinger equation describes
how the quantum state of some physical system changes with time.
Its mathematical and numerical study is of paramount
importance to fundamental and applied physics in general.
We wish to specifically contribute to the mathematical modeling
and the numerical simulation of confined quantum
mechanical systems (in one or more space dimensions) possibly involving stochastic terms.
Such systems are involved in quantum
semi-conductors or atom-chips, as well as in cold atom physics (Bose-Einstein condensates)
or laser propagation in optical fibers.</p>
        <p>The prototypical equation is written</p>
        <div align="center" class="mathdisplay">
          <a name="uid4"/>
          <table width="100%">
            <tr valign="middle">
              <td align="center">
                <math xmlns="http://www.w3.org/1998/Math/MathML">
                  <mtable frame="solid">
                    <mtr>
                      <mtd>
                        <mi>i</mi>
                        <mi>ε</mi>
                        <msub>
                          <mi>∂</mi>
                          <mi>t</mi>
                        </msub>
                        <msup>
                          <mi>ψ</mi>
                          <mi>ε</mi>
                        </msup>
                        <mo>=</mo>
                        <mfrac>
                          <msup>
                            <mi>ε</mi>
                            <mn>2</mn>
                          </msup>
                          <mi>β</mi>
                        </mfrac>
                        <mi>Δ</mi>
                        <msup>
                          <mi>ψ</mi>
                          <mi>ε</mi>
                        </msup>
                        <mo>+</mo>
                        <msup>
                          <mrow>
                            <mo>|</mo>
                            <msup>
                              <mi>ψ</mi>
                              <mi>ε</mi>
                            </msup>
                            <mo>|</mo>
                          </mrow>
                          <mn>2</mn>
                        </msup>
                        <msup>
                          <mi>ψ</mi>
                          <mi>ε</mi>
                        </msup>
                        <mo>+</mo>
                        <msup>
                          <mi>ψ</mi>
                          <mi>ε</mi>
                        </msup>
                        <mi>ξ</mi>
                      </mtd>
                    </mtr>
                  </mtable>
                </math>
              </td>
              <td class="eqno" width="10" align="right">(1)</td>
            </tr>
          </table>
        </div>
        <p class="notaparagraph">where the function <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msup><mi>ψ</mi><mi>ε</mi></msup><mo>=</mo><msup><mi>ψ</mi><mi>ε</mi></msup><mrow><mo>(</mo><mi>t</mi><mo>,</mo><mi>x</mi><mo>)</mo></mrow><mo>∈</mo><mi>ℂ</mi></mrow></math></span> depends on time
<span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mo>≥</mo><mn>0</mn></mrow></math></span> and position <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>x</mi><mo>∈</mo><msup><mi>ℝ</mi><mn>3</mn></msup></mrow></math></span>, <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>ξ</mi><mo>=</mo><mi>ξ</mi><mo>(</mo><mi>x</mi><mo>,</mo><mi>t</mi><mo>)</mo></mrow></math></span> is a white noise and where
the small parameter <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mi>ε</mi></math></span> is the Planck's constant
describing the microscopic/macroscopic ratio. The limit <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>ε</mi><mo>→</mo><mn>0</mn></mrow></math></span> is referred to as the semi-classical limit. The regime <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>ε</mi><mo>=</mo><mn>1</mn></mrow></math></span> and <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>β</mi><mo>→</mo><mn>0</mn></mrow></math></span> (this can be for instance the relative length of the optical fiber) is highly-oscillatory.
The noise <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mi>ξ</mi></math></span> acts as a potential, it may represent several external perturbations. For instance temperature effects in Bose-Einstein condensation or amplification in optical fibers. The highly oscillatory regime combined with noise introduces new challenges in the design of efficient schemes.</p>
        <p><b>Highly-oscillatory or highly-dissipative kinetic equations:</b>
Plasma is sometimes considered as the fourth state of matter,
obtained for example by bringing a gas to a very high temperature.
A globally neutral gas of neutral and charged particles, called plasma, is then obtained and is described by
a kinetic equation as soon as collective effects dominate
as compared to binary collisions. A situation of major importance is magnetic fusion in which collisions are not predominant.
In order to confine such a plasma in devices like tokamaks (ITER project) or stellarators, a large magnetic field is used to endow the charged particles with a cyclotronic motion around field lines. Note that kinetic models are also widely used for modeling plasmas in earth
magnetosphere or in rarefied gas dynamics.</p>
        <p>Denoting <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msup><mi>f</mi><mi>ε</mi></msup><mo>=</mo><msup><mi>f</mi><mi>ε</mi></msup><mrow><mo>(</mo><mi>t</mi><mo>,</mo><mi>x</mi><mo>,</mo><mi>v</mi><mo>)</mo></mrow><mo>∈</mo><msup><mi>ℝ</mi><mo>+</mo></msup></mrow></math></span> the distribution
function of charged particles at time <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mo>≥</mo><mn>0</mn></mrow></math></span>, position <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>x</mi><mo>∈</mo><msup><mi>ℝ</mi><mn>3</mn></msup></mrow></math></span> and velocity <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>v</mi><mo>∈</mo><msup><mi>ℝ</mi><mn>3</mn></msup></mrow></math></span>, a typical kinetic equation for <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>f</mi><mi>ε</mi></msup></math></span> reads</p>
        <div align="center" class="mathdisplay">
          <a name="uid5"/>
          <table width="100%">
            <tr valign="middle">
              <td align="center">
                <math xmlns="http://www.w3.org/1998/Math/MathML">
                  <mtable frame="solid">
                    <mtr>
                      <mtd>
                        <msub>
                          <mi>∂</mi>
                          <mi>t</mi>
                        </msub>
                        <msup>
                          <mi>f</mi>
                          <mi>ε</mi>
                        </msup>
                        <mo>+</mo>
                        <mi>v</mi>
                        <mo>·</mo>
                        <msub>
                          <mi>∇</mi>
                          <mi>x</mi>
                        </msub>
                        <msup>
                          <mi>f</mi>
                          <mi>ε</mi>
                        </msup>
                        <mo>+</mo>
                        <mfenced separators="" open="(" close=")">
                          <mi>E</mi>
                          <mo>+</mo>
                          <mfrac>
                            <mn>1</mn>
                            <mi>ε</mi>
                          </mfrac>
                          <mrow>
                            <mo>(</mo>
                            <mi>v</mi>
                            <mo>×</mo>
                            <mi>B</mi>
                            <mo>)</mo>
                          </mrow>
                        </mfenced>
                        <mo>·</mo>
                        <msub>
                          <mi>∇</mi>
                          <mi>v</mi>
                        </msub>
                        <msup>
                          <mi>f</mi>
                          <mi>ε</mi>
                        </msup>
                        <mo>=</mo>
                        <mfrac>
                          <mn>1</mn>
                          <mi>β</mi>
                        </mfrac>
                        <mi>Q</mi>
                        <mrow>
                          <mo>(</mo>
                          <msup>
                            <mi>f</mi>
                            <mi>ε</mi>
                          </msup>
                          <mo>)</mo>
                        </mrow>
                        <mo>+</mo>
                        <msup>
                          <mi>f</mi>
                          <mi>ε</mi>
                        </msup>
                        <msup>
                          <mi>m</mi>
                          <mi>ε</mi>
                        </msup>
                      </mtd>
                    </mtr>
                  </mtable>
                </math>
              </td>
              <td class="eqno" width="10" align="right">(2)</td>
            </tr>
          </table>
        </div>
        <p class="notaparagraph">where <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo>(</mo><mi>E</mi><mo>,</mo><mi>B</mi><mo>)</mo></mrow></math></span> is the electro-magnetic field
(which may itself depend on <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mi>f</mi></math></span> through Maxwell's equations), <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mi>ε</mi></msup></math></span> is a random process
(which may describe absorption or creation of particles) and <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mi>Q</mi></math></span> is a collision operator.
The dimensionless parameters <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>ε</mi><mo>,</mo><mi>β</mi></mrow></math></span> are related to the cyclotronic frequency
and the mean free path.
Limits <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>ε</mi><mo>→</mo><mn>0</mn></mrow></math></span> and <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>β</mi><mo>→</mo><mn>0</mn></mrow></math></span> do not share the same character
(the former is oscillatory and the latter is dissipative) and lead respectively to gyrokinetic and hydrodynamic models. The noise term <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mi>ε</mi></msup></math></span> is correlated in space and time. At the limit <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>ε</mi><mo>→</mo><mn>0</mn></mrow></math></span>, it converges formally to a white noise and stochastic PDEs are obtained.</p>
        <p><span class="smallcap">MINGuS </span> project is the follow-up of <span class="smallcap">IPSO </span>, ending in december in 2017. <span class="smallcap">IPSO </span> original aim was to extend the analysis of geometric schemes from ODEs to PDEs. During the last evaluation period, IPSO also considered the numerical analysis of geometric schemes for (S)PDEs, possibly including multiscale phenomena.
Breakthrough results <a href="./bibliography.html#mingus-2018-bid0">[36]</a>, <a href="./bibliography.html#mingus-2018-bid1">[38]</a>, <a href="./bibliography.html#mingus-2018-bid2">[39]</a>, <a href="./bibliography.html#mingus-2018-bid3">[42]</a>
have been recently obtained which deserve to be deepened and extended. It thus appears quite natural to build the <span class="smallcap">MINGuS </span> team upon these foundations.</p>
        <p>The objective of
<span class="smallcap">MINGuS </span> is twofold: the construction and the analysis of numerical schemes (such as “Uniformly Accurate numerical schemes", introduced by members of the <span class="smallcap">IPSO </span> project)
for multiscale (S)PDEs originating from physics. In turn, this requires <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo>(</mo><mi>i</mi><mo>)</mo></mrow></math></span> a deep mathematical
understanding of the (S)PDEs under consideration and <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo>(</mo><mi>i</mi><mi>i</mi><mo>)</mo></mrow></math></span> a strong involvement into increasingly realistic problems,
possibly resorting to parallel computing. For this aspect, we intend to benefit from the Inria Selalib software
library which turns out to be the ideal complement of our activities.</p>
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