@article{63344,
  abstract     = {{<jats:title>Abstract</jats:title>
          <jats:p>A Neumann-type initial-boundary value problem for <jats:disp-formula>
              <jats:alternatives>
                <jats:tex-math>$$\begin{aligned} \left\{ \begin{array}{l} u_{tt} = \nabla \cdot (\gamma (\Theta ) \nabla u_t) + a \nabla \cdot (\gamma (\Theta ) \nabla u) + \nabla \cdot f(\Theta ), \\ \Theta _t = D\Delta \Theta + \Gamma (\Theta ) |\nabla u_t|^2 + F(\Theta )\cdot \nabla u_t, \end{array} \right. \end{aligned}$$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:mtable>
                      <mml:mtr>
                        <mml:mtd>
                          <mml:mfenced>
                            <mml:mrow>
                              <mml:mtable>
                                <mml:mtr>
                                  <mml:mtd>
                                    <mml:mrow>
                                      <mml:msub>
                                        <mml:mi>u</mml:mi>
                                        <mml:mrow>
                                          <mml:mi>tt</mml:mi>
                                        </mml:mrow>
                                      </mml:msub>
                                      <mml:mo>=</mml:mo>
                                      <mml:mi>∇</mml:mi>
                                      <mml:mo>·</mml:mo>
                                      <mml:mrow>
                                        <mml:mo>(</mml:mo>
                                        <mml:mi>γ</mml:mi>
                                        <mml:mrow>
                                          <mml:mo>(</mml:mo>
                                          <mml:mi>Θ</mml:mi>
                                          <mml:mo>)</mml:mo>
                                        </mml:mrow>
                                        <mml:mi>∇</mml:mi>
                                        <mml:msub>
                                          <mml:mi>u</mml:mi>
                                          <mml:mi>t</mml:mi>
                                        </mml:msub>
                                        <mml:mo>)</mml:mo>
                                      </mml:mrow>
                                      <mml:mo>+</mml:mo>
                                      <mml:mi>a</mml:mi>
                                      <mml:mi>∇</mml:mi>
                                      <mml:mo>·</mml:mo>
                                      <mml:mrow>
                                        <mml:mo>(</mml:mo>
                                        <mml:mi>γ</mml:mi>
                                        <mml:mrow>
                                          <mml:mo>(</mml:mo>
                                          <mml:mi>Θ</mml:mi>
                                          <mml:mo>)</mml:mo>
                                        </mml:mrow>
                                        <mml:mi>∇</mml:mi>
                                        <mml:mi>u</mml:mi>
                                        <mml:mo>)</mml:mo>
                                      </mml:mrow>
                                      <mml:mo>+</mml:mo>
                                      <mml:mi>∇</mml:mi>
                                      <mml:mo>·</mml:mo>
                                      <mml:mi>f</mml:mi>
                                      <mml:mrow>
                                        <mml:mo>(</mml:mo>
                                        <mml:mi>Θ</mml:mi>
                                        <mml:mo>)</mml:mo>
                                      </mml:mrow>
                                      <mml:mo>,</mml:mo>
                                    </mml:mrow>
                                  </mml:mtd>
                                </mml:mtr>
                                <mml:mtr>
                                  <mml:mtd>
                                    <mml:mrow>
                                      <mml:mrow/>
                                      <mml:msub>
                                        <mml:mi>Θ</mml:mi>
                                        <mml:mi>t</mml:mi>
                                      </mml:msub>
                                      <mml:mo>=</mml:mo>
                                      <mml:mi>D</mml:mi>
                                      <mml:mi>Δ</mml:mi>
                                      <mml:mi>Θ</mml:mi>
                                      <mml:mo>+</mml:mo>
                                      <mml:mi>Γ</mml:mi>
                                      <mml:mrow>
                                        <mml:mo>(</mml:mo>
                                        <mml:mi>Θ</mml:mi>
                                        <mml:mo>)</mml:mo>
                                      </mml:mrow>
                                      <mml:msup>
                                        <mml:mrow>
                                          <mml:mo>|</mml:mo>
                                          <mml:mi>∇</mml:mi>
                                          <mml:msub>
                                            <mml:mi>u</mml:mi>
                                            <mml:mi>t</mml:mi>
                                          </mml:msub>
                                          <mml:mo>|</mml:mo>
                                        </mml:mrow>
                                        <mml:mn>2</mml:mn>
                                      </mml:msup>
                                      <mml:mo>+</mml:mo>
                                      <mml:mi>F</mml:mi>
                                      <mml:mrow>
                                        <mml:mo>(</mml:mo>
                                        <mml:mi>Θ</mml:mi>
                                        <mml:mo>)</mml:mo>
                                      </mml:mrow>
                                      <mml:mo>·</mml:mo>
                                      <mml:mi>∇</mml:mi>
                                      <mml:msub>
                                        <mml:mi>u</mml:mi>
                                        <mml:mi>t</mml:mi>
                                      </mml:msub>
                                      <mml:mo>,</mml:mo>
                                    </mml:mrow>
                                  </mml:mtd>
                                </mml:mtr>
                              </mml:mtable>
                            </mml:mrow>
                          </mml:mfenced>
                        </mml:mtd>
                      </mml:mtr>
                    </mml:mtable>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:disp-formula>is considered in a smoothly bounded domain <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$\Omega \subset \mathbb {R}^n$$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:mi>Ω</mml:mi>
                    <mml:mo>⊂</mml:mo>
                    <mml:msup>
                      <mml:mrow>
                        <mml:mi>R</mml:mi>
                      </mml:mrow>
                      <mml:mi>n</mml:mi>
                    </mml:msup>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula>, <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$n\ge 1$$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:mi>n</mml:mi>
                    <mml:mo>≥</mml:mo>
                    <mml:mn>1</mml:mn>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula>. In the case when <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$n=1$$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:mi>n</mml:mi>
                    <mml:mo>=</mml:mo>
                    <mml:mn>1</mml:mn>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula>, <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$\gamma \equiv \Gamma $$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:mi>γ</mml:mi>
                    <mml:mo>≡</mml:mo>
                    <mml:mi>Γ</mml:mi>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula> and <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$f\equiv F$$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:mi>f</mml:mi>
                    <mml:mo>≡</mml:mo>
                    <mml:mi>F</mml:mi>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula>, this system coincides with the standard model for heat generation in a viscoelastic material of Kelvin-Voigt type, well-understood in situations in which <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$\gamma =const$$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:mi>γ</mml:mi>
                    <mml:mo>=</mml:mo>
                    <mml:mi>c</mml:mi>
                    <mml:mi>o</mml:mi>
                    <mml:mi>n</mml:mi>
                    <mml:mi>s</mml:mi>
                    <mml:mi>t</mml:mi>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula>. Covering scenarios in which all key ingredients <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$\gamma ,\Gamma ,f$$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:mi>γ</mml:mi>
                    <mml:mo>,</mml:mo>
                    <mml:mi>Γ</mml:mi>
                    <mml:mo>,</mml:mo>
                    <mml:mi>f</mml:mi>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula> and <jats:italic>F</jats:italic> may depend on the temperature <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$\Theta $$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mi>Θ</mml:mi>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula> here, for initial data which merely satisfy <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$u_0\in W^{1,p+2}(\Omega )$$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:msub>
                      <mml:mi>u</mml:mi>
                      <mml:mn>0</mml:mn>
                    </mml:msub>
                    <mml:mo>∈</mml:mo>
                    <mml:msup>
                      <mml:mi>W</mml:mi>
                      <mml:mrow>
                        <mml:mn>1</mml:mn>
                        <mml:mo>,</mml:mo>
                        <mml:mi>p</mml:mi>
                        <mml:mo>+</mml:mo>
                        <mml:mn>2</mml:mn>
                      </mml:mrow>
                    </mml:msup>
                    <mml:mrow>
                      <mml:mo>(</mml:mo>
                      <mml:mi>Ω</mml:mi>
                      <mml:mo>)</mml:mo>
                    </mml:mrow>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula>, <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$u_{0t}\in W^{1,p}(\Omega )$$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:msub>
                      <mml:mi>u</mml:mi>
                      <mml:mrow>
                        <mml:mn>0</mml:mn>
                        <mml:mi>t</mml:mi>
                      </mml:mrow>
                    </mml:msub>
                    <mml:mo>∈</mml:mo>
                    <mml:msup>
                      <mml:mi>W</mml:mi>
                      <mml:mrow>
                        <mml:mn>1</mml:mn>
                        <mml:mo>,</mml:mo>
                        <mml:mi>p</mml:mi>
                      </mml:mrow>
                    </mml:msup>
                    <mml:mrow>
                      <mml:mo>(</mml:mo>
                      <mml:mi>Ω</mml:mi>
                      <mml:mo>)</mml:mo>
                    </mml:mrow>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula> and <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$\Theta _0\in W^{1,p}(\Omega )$$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:msub>
                      <mml:mi>Θ</mml:mi>
                      <mml:mn>0</mml:mn>
                    </mml:msub>
                    <mml:mo>∈</mml:mo>
                    <mml:msup>
                      <mml:mi>W</mml:mi>
                      <mml:mrow>
                        <mml:mn>1</mml:mn>
                        <mml:mo>,</mml:mo>
                        <mml:mi>p</mml:mi>
                      </mml:mrow>
                    </mml:msup>
                    <mml:mrow>
                      <mml:mo>(</mml:mo>
                      <mml:mi>Ω</mml:mi>
                      <mml:mo>)</mml:mo>
                    </mml:mrow>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula> with some <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$p\ge 2$$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:mi>p</mml:mi>
                    <mml:mo>≥</mml:mo>
                    <mml:mn>2</mml:mn>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula> such that <jats:inline-formula>
              <jats:alternatives>
                <jats:tex-math>$$p&gt;n$$</jats:tex-math>
                <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                  <mml:mrow>
                    <mml:mi>p</mml:mi>
                    <mml:mo>&gt;</mml:mo>
                    <mml:mi>n</mml:mi>
                  </mml:mrow>
                </mml:math>
              </jats:alternatives>
            </jats:inline-formula>, a result on local-in-time existence and uniqueness is derived in a natural framework of weak solvability.</jats:p>}},
  author       = {{Winkler, Michael}},
  issn         = {{0095-4616}},
  journal      = {{Applied Mathematics &amp; Optimization}},
  number       = {{2}},
  publisher    = {{Springer Science and Business Media LLC}},
  title        = {{{Rough Data in an Evolution System Generalizing 1D Thermoviscoelasticity with Temperature-Dependent Parameters}}},
  doi          = {{10.1007/s00245-025-10243-9}},
  volume       = {{91}},
  year         = {{2025}},
}

@article{63242,
  abstract     = {{<jats:title>Abstract</jats:title>
                  <jats:p>
                    For
                    <jats:inline-formula>
                      <jats:alternatives>
                        <jats:tex-math>$$p&gt;2$$</jats:tex-math>
                        <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                          <mml:mrow>
                            <mml:mi>p</mml:mi>
                            <mml:mo>&gt;</mml:mo>
                            <mml:mn>2</mml:mn>
                          </mml:mrow>
                        </mml:math>
                      </jats:alternatives>
                    </jats:inline-formula>
                    , the equation
                    <jats:disp-formula>
                      <jats:alternatives>
                        <jats:tex-math>$$\begin{aligned} u_t = u^p u_{xx}, \qquad x\in \mathbb {R}, \ t\in \mathbb {R}, \end{aligned}$$</jats:tex-math>
                        <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                          <mml:mrow>
                            <mml:mtable>
                              <mml:mtr>
                                <mml:mtd>
                                  <mml:mrow>
                                    <mml:msub>
                                      <mml:mi>u</mml:mi>
                                      <mml:mi>t</mml:mi>
                                    </mml:msub>
                                    <mml:mo>=</mml:mo>
                                    <mml:msup>
                                      <mml:mi>u</mml:mi>
                                      <mml:mi>p</mml:mi>
                                    </mml:msup>
                                    <mml:msub>
                                      <mml:mi>u</mml:mi>
                                      <mml:mrow>
                                        <mml:mi>xx</mml:mi>
                                      </mml:mrow>
                                    </mml:msub>
                                    <mml:mo>,</mml:mo>
                                    <mml:mspace/>
                                    <mml:mi>x</mml:mi>
                                    <mml:mo>∈</mml:mo>
                                    <mml:mi>R</mml:mi>
                                    <mml:mo>,</mml:mo>
                                    <mml:mspace/>
                                    <mml:mi>t</mml:mi>
                                    <mml:mo>∈</mml:mo>
                                    <mml:mi>R</mml:mi>
                                    <mml:mo>,</mml:mo>
                                  </mml:mrow>
                                </mml:mtd>
                              </mml:mtr>
                            </mml:mtable>
                          </mml:mrow>
                        </mml:math>
                      </jats:alternatives>
                    </jats:disp-formula>
                    is shown to admit positive and spatially increasing smooth solutions on all of
                    <jats:inline-formula>
                      <jats:alternatives>
                        <jats:tex-math>$$\mathbb {R}\times \mathbb {R}$$</jats:tex-math>
                        <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                          <mml:mrow>
                            <mml:mi>R</mml:mi>
                            <mml:mo>×</mml:mo>
                            <mml:mi>R</mml:mi>
                          </mml:mrow>
                        </mml:math>
                      </jats:alternatives>
                    </jats:inline-formula>
                    which are precisely of the form of an accelerating wave for
                    <jats:inline-formula>
                      <jats:alternatives>
                        <jats:tex-math>$$t&lt;0$$</jats:tex-math>
                        <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                          <mml:mrow>
                            <mml:mi>t</mml:mi>
                            <mml:mo>&lt;</mml:mo>
                            <mml:mn>0</mml:mn>
                          </mml:mrow>
                        </mml:math>
                      </jats:alternatives>
                    </jats:inline-formula>
                    , and of a wave slowing down for
                    <jats:inline-formula>
                      <jats:alternatives>
                        <jats:tex-math>$$t&gt;0$$</jats:tex-math>
                        <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                          <mml:mrow>
                            <mml:mi>t</mml:mi>
                            <mml:mo>&gt;</mml:mo>
                            <mml:mn>0</mml:mn>
                          </mml:mrow>
                        </mml:math>
                      </jats:alternatives>
                    </jats:inline-formula>
                    . These solutions satisfy
                    <jats:inline-formula>
                      <jats:alternatives>
                        <jats:tex-math>$$u(\cdot ,t)\rightarrow 0$$</jats:tex-math>
                        <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                          <mml:mrow>
                            <mml:mi>u</mml:mi>
                            <mml:mo>(</mml:mo>
                            <mml:mo>·</mml:mo>
                            <mml:mo>,</mml:mo>
                            <mml:mi>t</mml:mi>
                            <mml:mo>)</mml:mo>
                            <mml:mo>→</mml:mo>
                            <mml:mn>0</mml:mn>
                          </mml:mrow>
                        </mml:math>
                      </jats:alternatives>
                    </jats:inline-formula>
                    in
                    <jats:inline-formula>
                      <jats:alternatives>
                        <jats:tex-math>$$L^\infty _{loc}(\mathbb {R})$$</jats:tex-math>
                        <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                          <mml:mrow>
                            <mml:msubsup>
                              <mml:mi>L</mml:mi>
                              <mml:mrow>
                                <mml:mi>loc</mml:mi>
                              </mml:mrow>
                              <mml:mi>∞</mml:mi>
                            </mml:msubsup>
                            <mml:mrow>
                              <mml:mo>(</mml:mo>
                              <mml:mi>R</mml:mi>
                              <mml:mo>)</mml:mo>
                            </mml:mrow>
                          </mml:mrow>
                        </mml:math>
                      </jats:alternatives>
                    </jats:inline-formula>
                    as
                    <jats:inline-formula>
                      <jats:alternatives>
                        <jats:tex-math>$$t\rightarrow + \infty $$</jats:tex-math>
                        <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                          <mml:mrow>
                            <mml:mi>t</mml:mi>
                            <mml:mo>→</mml:mo>
                            <mml:mo>+</mml:mo>
                            <mml:mi>∞</mml:mi>
                          </mml:mrow>
                        </mml:math>
                      </jats:alternatives>
                    </jats:inline-formula>
                    and as
                    <jats:inline-formula>
                      <jats:alternatives>
                        <jats:tex-math>$$t\rightarrow -\infty $$</jats:tex-math>
                        <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                          <mml:mrow>
                            <mml:mi>t</mml:mi>
                            <mml:mo>→</mml:mo>
                            <mml:mo>-</mml:mo>
                            <mml:mi>∞</mml:mi>
                          </mml:mrow>
                        </mml:math>
                      </jats:alternatives>
                    </jats:inline-formula>
                    , and exhibit a yet apparently undiscovered phenomenon of transient rapid spatial growth, in the sense that
                    <jats:disp-formula>
                      <jats:alternatives>
                        <jats:tex-math>$$\begin{aligned} \lim _{x\rightarrow +\infty } x^{-1} u(x,t) \quad \text{ exists } \text{ for } \text{ all } t&lt;0, \end{aligned}$$</jats:tex-math>
                        <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                          <mml:mrow>
                            <mml:mtable>
                              <mml:mtr>
                                <mml:mtd>
                                  <mml:mrow>
                                    <mml:munder>
                                      <mml:mo>lim</mml:mo>
                                      <mml:mrow>
                                        <mml:mi>x</mml:mi>
                                        <mml:mo>→</mml:mo>
                                        <mml:mo>+</mml:mo>
                                        <mml:mi>∞</mml:mi>
                                      </mml:mrow>
                                    </mml:munder>
                                    <mml:msup>
                                      <mml:mi>x</mml:mi>
                                      <mml:mrow>
                                        <mml:mo>-</mml:mo>
                                        <mml:mn>1</mml:mn>
                                      </mml:mrow>
                                    </mml:msup>
                                    <mml:mi>u</mml:mi>
                                    <mml:mrow>
                                      <mml:mo>(</mml:mo>
                                      <mml:mi>x</mml:mi>
                                      <mml:mo>,</mml:mo>
                                      <mml:mi>t</mml:mi>
                                      <mml:mo>)</mml:mo>
                                    </mml:mrow>
                                    <mml:mspace/>
                                    <mml:mspace/>
                                    <mml:mtext>exists</mml:mtext>
                                    <mml:mspace/>
                                    <mml:mspace/>
                                    <mml:mtext>for</mml:mtext>
                                    <mml:mspace/>
                                    <mml:mspace/>
                                    <mml:mtext>all</mml:mtext>
                                    <mml:mspace/>
                                    <mml:mi>t</mml:mi>
                                    <mml:mo>&lt;</mml:mo>
                                    <mml:mn>0</mml:mn>
                                    <mml:mo>,</mml:mo>
                                  </mml:mrow>
                                </mml:mtd>
                              </mml:mtr>
                            </mml:mtable>
                          </mml:mrow>
                        </mml:math>
                      </jats:alternatives>
                    </jats:disp-formula>
                    that
                    <jats:disp-formula>
                      <jats:alternatives>
                        <jats:tex-math>$$\begin{aligned} \lim _{x\rightarrow +\infty } x^{-\frac{2}{p}} u(x,t) \quad \text{ exists } \text{ for } \text{ all } t&gt;0, \end{aligned}$$</jats:tex-math>
                        <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                          <mml:mrow>
                            <mml:mtable>
                              <mml:mtr>
                                <mml:mtd>
                                  <mml:mrow>
                                    <mml:munder>
                                      <mml:mo>lim</mml:mo>
                                      <mml:mrow>
                                        <mml:mi>x</mml:mi>
                                        <mml:mo>→</mml:mo>
                                        <mml:mo>+</mml:mo>
                                        <mml:mi>∞</mml:mi>
                                      </mml:mrow>
                                    </mml:munder>
                                    <mml:msup>
                                      <mml:mi>x</mml:mi>
                                      <mml:mrow>
                                        <mml:mo>-</mml:mo>
                                        <mml:mfrac>
                                          <mml:mn>2</mml:mn>
                                          <mml:mi>p</mml:mi>
                                        </mml:mfrac>
                                      </mml:mrow>
                                    </mml:msup>
                                    <mml:mi>u</mml:mi>
                                    <mml:mrow>
                                      <mml:mo>(</mml:mo>
                                      <mml:mi>x</mml:mi>
                                      <mml:mo>,</mml:mo>
                                      <mml:mi>t</mml:mi>
                                      <mml:mo>)</mml:mo>
                                    </mml:mrow>
                                    <mml:mspace/>
                                    <mml:mspace/>
                                    <mml:mtext>exists</mml:mtext>
                                    <mml:mspace/>
                                    <mml:mspace/>
                                    <mml:mtext>for</mml:mtext>
                                    <mml:mspace/>
                                    <mml:mspace/>
                                    <mml:mtext>all</mml:mtext>
                                    <mml:mspace/>
                                    <mml:mi>t</mml:mi>
                                    <mml:mo>&gt;</mml:mo>
                                    <mml:mn>0</mml:mn>
                                    <mml:mo>,</mml:mo>
                                  </mml:mrow>
                                </mml:mtd>
                              </mml:mtr>
                            </mml:mtable>
                          </mml:mrow>
                        </mml:math>
                      </jats:alternatives>
                    </jats:disp-formula>
                    but that
                    <jats:disp-formula>
                      <jats:alternatives>
                        <jats:tex-math>$$\begin{aligned} u(x,0)=K e^{\alpha x} \qquad \text{ for } \text{ all } x\in \mathbb {R}\end{aligned}$$</jats:tex-math>
                        <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                          <mml:mrow>
                            <mml:mtable>
                              <mml:mtr>
                                <mml:mtd>
                                  <mml:mrow>
                                    <mml:mi>u</mml:mi>
                                    <mml:mrow>
                                      <mml:mo>(</mml:mo>
                                      <mml:mi>x</mml:mi>
                                      <mml:mo>,</mml:mo>
                                      <mml:mn>0</mml:mn>
                                      <mml:mo>)</mml:mo>
                                    </mml:mrow>
                                    <mml:mo>=</mml:mo>
                                    <mml:mi>K</mml:mi>
                                    <mml:msup>
                                      <mml:mi>e</mml:mi>
                                      <mml:mrow>
                                        <mml:mi>α</mml:mi>
                                        <mml:mi>x</mml:mi>
                                      </mml:mrow>
                                    </mml:msup>
                                    <mml:mspace/>
                                    <mml:mspace/>
                                    <mml:mtext>for</mml:mtext>
                                    <mml:mspace/>
                                    <mml:mspace/>
                                    <mml:mtext>all</mml:mtext>
                                    <mml:mspace/>
                                    <mml:mi>x</mml:mi>
                                    <mml:mo>∈</mml:mo>
                                    <mml:mi>R</mml:mi>
                                  </mml:mrow>
                                </mml:mtd>
                              </mml:mtr>
                            </mml:mtable>
                          </mml:mrow>
                        </mml:math>
                      </jats:alternatives>
                    </jats:disp-formula>
                    with some
                    <jats:inline-formula>
                      <jats:alternatives>
                        <jats:tex-math>$$K&gt;0$$</jats:tex-math>
                        <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                          <mml:mrow>
                            <mml:mi>K</mml:mi>
                            <mml:mo>&gt;</mml:mo>
                            <mml:mn>0</mml:mn>
                          </mml:mrow>
                        </mml:math>
                      </jats:alternatives>
                    </jats:inline-formula>
                    and
                    <jats:inline-formula>
                      <jats:alternatives>
                        <jats:tex-math>$$\alpha &gt;0$$</jats:tex-math>
                        <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                          <mml:mrow>
                            <mml:mi>α</mml:mi>
                            <mml:mo>&gt;</mml:mo>
                            <mml:mn>0</mml:mn>
                          </mml:mrow>
                        </mml:math>
                      </jats:alternatives>
                    </jats:inline-formula>
                    .
                  </jats:p>}},
  author       = {{Hanfland, Celina and Winkler, Michael}},
  issn         = {{2296-9020}},
  journal      = {{Journal of Elliptic and Parabolic Equations}},
  number       = {{3}},
  pages        = {{2041--2063}},
  publisher    = {{Springer Science and Business Media LLC}},
  title        = {{{Exactly wave-type homoclinic orbits and emergence of transient exponential growth in a super-fast diffusion equation}}},
  doi          = {{10.1007/s41808-025-00316-9}},
  volume       = {{11}},
  year         = {{2025}},
}

@unpublished{63384,
  abstract     = {{Two fundamental ways to represent a group are as permutations and as matrices. In this paper, we study linear representations of groups that intertwine with a permutation representation. Recently, D'Alconzo and Di Scala investigated how small the matrices in such a linear representation can be. The minimal dimension of such a representation is the \emph{linear dimension of the group action} and this has applications in cryptography and cryptosystems.

We develop the idea of linear dimension from an algebraic point of view by using the theory of permutation modules. We give structural results about representations of minimal dimension and investigate the implications of faithfulness, transitivity and primitivity on the linear dimension. Furthermore, we compute the linear dimension of several classes of finite primitive permutation groups. We also study wreath products, allowing us to determine the linear dimension of imprimitive group actions. Finally, we give the linear dimension of almost simple finite $2$-transitive groups, some of which may be used for further applications in cryptography. Our results also open up many new questions about linear representations of group actions.}},
  author       = {{Devillers, Alice and Giudici, Michael and Hawtin, Daniel R. and Klawuhn, Lukas-André Dominik and Morgan, Luke}},
  title        = {{{Linear dimension of group actions}}},
  year         = {{2025}},
}

@inbook{63390,
  author       = {{Buhl, Heike M. and Hilkenmeier, Johanna}},
  booktitle    = {{Handbuch Entwicklungs- und Erziehungspsychologie}},
  editor       = {{Kracke, Bärbel and Noack, Peter}},
  publisher    = {{Springer}},
  title        = {{{Bildung und Lesesozialisation im Elternhaus}}},
  doi          = {{10.1007/978-3-642-54061-5_10-2}},
  year         = {{2025}},
}

@article{63405,
  author       = {{Eremin, Oxana and Richter, Susanne and Letzner, Celina}},
  journal      = {{blog interdisziplinäre geschlechterforschung}},
  publisher    = {{www.gender-blog.de/beitrag/zeit-fuer-gender-podcasts/ }},
  title        = {{{„Zeit für Gender“ – Podcasts aus der Fachcommunity 2}}},
  doi          = {{DOI: https://doi.org/10.17185/gender/20251217}},
  year         = {{2025}},
}

@article{63505,
  abstract     = {{<jats:title>Abstract</jats:title>
               <jats:p>The main goal of this work is to study the $L^{p}$-asymptotic behavior of solutions to the heat equation on arbitrary rank Riemannian symmetric spaces of non-compact-type $G/K$ for non-bi-$K$ invariant initial data. For initial data $u_{0}$ compactly supported or in a weighted $L^{1}(G/K)$ space with a weight depending on $p\in [1, \infty ]$, we introduce a mass function $M_{p}(u_{0})(\cdot )$, and prove that if $h_{t}$ is the heat kernel on $G/K$, then $$ \begin{align*} &amp;\|h_t\|_p^{-1}\,\|u_0\ast h_t \, - \,M_p(u_0)(\cdot)\,h_t\|_p \rightarrow 0 \quad \textrm{as} \quad t\rightarrow \infty.\end{align*} $$ Interestingly, the $L^{p}$ heat concentration leads to completely different expressions of the mass function for $1\leq p &amp;lt;2$ and $2\leq p\leq \infty $. If we further assume that the initial data are bi-$K$-invariant, then our mass function boils down to the constant $\int _{G/K}u_{0}$ in the case $p=1$, and more generally to $\mathcal{H}{u_{0}}(i\rho (2/p-1))$ if $1\leq p&amp;lt;2$, and to $\mathcal{H}{u_{0}}(0)$ if $2\leq p \leq \infty $. Thus, we improve upon results by Vázquez, Anker et al., and Naik et al., clarifying the nature of the problem.</jats:p>}},
  author       = {{Papageorgiou, Effie}},
  issn         = {{1073-7928}},
  journal      = {{International Mathematics Research Notices}},
  number       = {{7}},
  publisher    = {{Oxford University Press (OUP)}},
  title        = {{{<i>L</i>
          p Asymptotics for the Heat Equation on Symmetric Spaces for Non-symmetric Solutions}}},
  doi          = {{10.1093/imrn/rnaf074}},
  volume       = {{2025}},
  year         = {{2025}},
}

@article{63503,
  author       = {{Bruno, Tommaso and Papageorgiou, Effie}},
  issn         = {{0021-7670}},
  journal      = {{Journal d'Analyse Mathématique}},
  number       = {{2}},
  pages        = {{733--767}},
  publisher    = {{Springer Science and Business Media LLC}},
  title        = {{{Pointwise convergence to initial data for some evolution equations on symmetric spaces}}},
  doi          = {{10.1007/s11854-025-0403-2}},
  volume       = {{157}},
  year         = {{2025}},
}

@inproceedings{62924,
  author       = {{Wittkopp, Laura and Pollmeier, Pascal and Fechner, Sabine}},
  booktitle    = {{Jahrestagung der Gesellschaft für Didaktik der Chemie und Physik e.V. (GDCP)}},
  location     = {{Frankfurt am Main}},
  title        = {{{Effekte nachhaltigkeitsbezogener Kontexte beim Chemielernen}}},
  year         = {{2025}},
}

@article{63091,
  abstract     = {{We present the design and characterization of a guided-wave, bright, and highly frequency non-degenerate parametric down-conversion (PDC) source in thin-film lithium niobate. The source generates photon pairs with wavelengths of 815 nm and 1550 nm, linking the visible wavelength regime with telecommunication wavelengths. We confirm the high quality of the generated single photons by determining a value for the heralded second-order correlation function as low as g_h^(2)=(6.7+/-1.1)*10^8-3). Furthermore, we achieve a high spectral brightness of 0.44·10pairs/(smWGHz) which is two orders of magnitude higher than sources based on weakly guiding waveguides. The shape of the PDC spectrum and the strong agreement between the effective and nominal bandwidth highlight our high fabrication quality of periodically poled waveguides. The good agreement between the measured and simulated spectral characteristics of our source demonstrates our excellent understanding of the PDC process. Our result is a valuable step towards practical and scalable quantum communication networks as well as photonic quantum computing.}},
  author       = {{Babel, Silia and Bollmers, Laura and Roeder, Franz and Ridder, Werner and Golla, Christian and Köthemann, Ronja and Reineke, Bernhard and Herrmann, Harald and Brecht, Benjamin and Eigner, Christof and Padberg, Laura and Silberhorn, Christine}},
  issn         = {{1094-4087}},
  journal      = {{Optics Express}},
  number       = {{25}},
  publisher    = {{Optica Publishing Group}},
  title        = {{{Ultrabright, two-color photon pair source based on thin-film lithium niobate for bridging visible and telecom wavelengths}}},
  doi          = {{10.1364/oe.571605}},
  volume       = {{33}},
  year         = {{2025}},
}

@article{62652,
  abstract     = {{<jats:p>Driven by the urgent need for a green, safe, and cost‐effective approach to producing H<jats:sub>2</jats:sub> and H<jats:sub>2</jats:sub>O<jats:sub>2</jats:sub>—both highly valuable in green energy and environmental protection fields—piezocatalysis, which converts mechanical energy into valuable chemicals, has emerged as a promising solution. However, current catalyst systems face challenges due to the need for materials with both a strong piezoelectric effect and favorable catalytic activity. Herein, the construction of an oxidized carbon nitride (<jats:italic>g</jats:italic>‐C<jats:sub>3</jats:sub>N<jats:sub>4</jats:sub>) matrix anchored with TiO<jats:sub>2</jats:sub> nanoparticles via alkaline hydrothermal treatment is reported. Under ultrasonication, the <jats:italic>g</jats:italic>‐C<jats:sub>3</jats:sub>N<jats:sub>4</jats:sub>/TiO<jats:sub>2</jats:sub> composite exhibits optimal performance under carefully controlled alkaline hydrothermal conditions. With a low concentration of Ba(OH)<jats:sub>2</jats:sub> during hydrothermal treatment, Ba(OH)<jats:sub>2</jats:sub> provides an alkaline medium, oxidizing the <jats:italic>g</jats:italic>‐C<jats:sub>3</jats:sub>N<jats:sub>4</jats:sub> species and introducing structural defects into the <jats:italic>g</jats:italic>‐C<jats:sub>3</jats:sub>N<jats:sub>4</jats:sub> framework. The disruption of the <jats:italic>g</jats:italic>‐C<jats:sub>3</jats:sub>N<jats:sub>4</jats:sub> matrix, along with its interaction with TiO<jats:sub>2</jats:sub> nanoparticles, enhances the piezoelectric effect. Consequently, the oxidized <jats:italic>g</jats:italic>‐C<jats:sub>3</jats:sub>N<jats:sub>4</jats:sub>/TiO<jats:sub>2</jats:sub> composite achieves a remarkable H<jats:sub>2</jats:sub> production rate of 4427.2 μmol g<jats:sup>−1</jats:sup> and an H<jats:sub>2</jats:sub>O<jats:sub>2</jats:sub> production rate of 809.3 μmol g<jats:sup>−1</jats:sup> within 1 h without the addition of any sacrificial agents or cocatalysts. This work presents an effective strategy for the structural optimization of <jats:italic>g</jats:italic>‐C<jats:sub>3</jats:sub>N<jats:sub>4</jats:sub>‐based materials and may inspire new approaches for designing advanced piezocatalysts.</jats:p>}},
  author       = {{Pan, Ying and Liao, Luocheng and Zhang, Xinwen and Liu, Yunya and Su, Ran and Lopez Salas, Nieves}},
  issn         = {{1864-5631}},
  journal      = {{ChemSusChem}},
  number       = {{19}},
  publisher    = {{Wiley}},
  title        = {{{Oxidation‐Enhanced Piezocatalytic Activity in Carbon Nitride‐Based Catalysts for Hydrogen and Hydrogen Peroxide Production}}},
  doi          = {{10.1002/cssc.202500980}},
  volume       = {{18}},
  year         = {{2025}},
}

@article{62651,
  abstract     = {{<jats:p>
                    Aqueous zinc (Zn)‐ion capacitors (AZICs) have addressed considerable attention due to their high energy density, low toxicity, and rich abundance of Zn metal. However, the development of ultra‐long cycle life and high energy density AZICs is often hindered by the lack of adequately optimized active carbon (AC) electrodes and compatible electrolytes. Herein, high‐performance, free‐standing AC electrodes for AZICs are derived from sustainable precursors—adenine and D‐ribose—using magnesium chloride hexahydrate as an activation agent via a eutectic template strategy. Furthermore, an aqueous hybrid electrolyte tailored to the designed AC electrodes is developed, significantly enhancing the stability and cycle life of AZICs. The resulting AZIC achieves a high specific capacity of 164.39 F g
                    <jats:sup>−1</jats:sup>
                    at 0.1 A g
                    <jats:sup>−1</jats:sup>
                    and a magnificently long cell life of over 50 000 cycles with nearly 94.5% capacitance retention at 10 000
                    <jats:sup>th</jats:sup>
                    cycles, and 76.3% at 50 000
                    <jats:sup>th</jats:sup>
                    cycle. The pouch cell assembly also demonstrates comparable specific capacitance and energy density to the coin cell, underscoring the potential of large‐scale applications of AZICs.
                  </jats:p>}},
  author       = {{Tao, Li and Li, Chun and Lu, Xuejun and Mir, Rameez Ahmad and Lopez Salas, Nieves and Liu, Jian}},
  issn         = {{2566-6223}},
  journal      = {{Batteries &amp; Supercaps}},
  number       = {{11}},
  publisher    = {{Wiley}},
  title        = {{{Adenine and D‐Ribose Coderived Activated Carbon with N‐Methyl‐2‐Pyrrolidone‐Modified Aqueous Electrolyte for Long‐Life Zinc‐Ion Capacitors}}},
  doi          = {{10.1002/batt.202500161}},
  volume       = {{8}},
  year         = {{2025}},
}

@article{62653,
  abstract     = {{<jats:p>Enhanced bifunctional electrocatalysis <jats:italic>via</jats:italic> CuSe<jats:sub>2</jats:sub>/FeSe<jats:sub>2</jats:sub> heterojunctions for efficient water splitting was achieved.</jats:p>}},
  author       = {{Kumari, Sandhyawasini and Pahra, Swapna and Tripathy, Amrita and Sumanth, N. and Lopez Salas, Nieves and Tiwari, Santosh K. and Khan, Afaq Ahmad and Devi, Pooja and Santosh, M. S.}},
  issn         = {{2040-3364}},
  journal      = {{Nanoscale}},
  number       = {{33}},
  pages        = {{19253--19265}},
  publisher    = {{Royal Society of Chemistry (RSC)}},
  title        = {{{Interfacial engineering of CuSe<sub>2</sub>/FeSe<sub>2</sub> heterojunctions for water splitting: a pathway to high-performance hydrogen and oxygen evolution reactions}}},
  doi          = {{10.1039/d5nr01393c}},
  volume       = {{17}},
  year         = {{2025}},
}

@article{62656,
  author       = {{Hu, Jiajun and Goberna-Ferrón, Sara and Simonelli, Laura and Lopez Salas, Nieves and García, Hermenegildo and Albero, Josep}},
  issn         = {{2574-0962}},
  journal      = {{ACS Applied Energy Materials}},
  number       = {{2}},
  pages        = {{1179--1188}},
  publisher    = {{American Chemical Society (ACS)}},
  title        = {{{Fe and Sn Single-Site-Based Electrodes for High-Current CO<sub>2</sub> Reduction in Acid Media and Stable Zn–CO<sub>2</sub> Batteries}}},
  doi          = {{10.1021/acsaem.4c02704}},
  volume       = {{8}},
  year         = {{2025}},
}

@article{62659,
  abstract     = {{<jats:p>The growing rise in agricultural activities has resulted in an increase in unutilized waste which is a significant contributor to greenhouse gas emissions. This has led to a need for sustainable methods to add value to such waste. This work focused on the transformation of agricultural waste into usable products through alkaline treatment to obtain lignin and cellulose, and the evaluation of the derived lignin as a viable carbon precursor in energy storage applications. Laser scribing was used as a fast and simple strategy in producing laser-induced graphene (LIG) electrodes. Lignin was isolated from wheat straw using sodium hydroxide treatment. The pulp from the treatment was subjected to bleaching with sodium chlorite followed by acid hydrolysis to extract microcrystalline cellulose. Fourier-transform infrared spectroscopy (FTIR), Transmission electron microscopy, and Xray diffraction were used for characterization of the materials produced. The fabricated supercapacitor could achieve an areal capacitance (C<jats:sub>A</jats:sub>) of 5.12 mF/cm<jats:sup>2</jats:sup> (0.02 mA/cm<jats:sup>2</jats:sup>). This study illustrated the successful valorization of wheat straw residue into microcrystalline cellulose and the use of extracted lignin in producing graphitic carbon electrodes for supercapacitors.</jats:p>}},
  author       = {{Katwesigye, Samuel and El-Khouly, Mohamed E. and Lopez Salas, Nieves and Khalil, Ahmed S.G.}},
  issn         = {{1662-9752}},
  journal      = {{Materials Science Forum}},
  pages        = {{115--120}},
  publisher    = {{Trans Tech Publications, Ltd.}},
  title        = {{{Sustainable Development of Graphene Electrodes for Supercapacitors through Laser Scribing of Agrowaste Derived Lignin}}},
  doi          = {{10.4028/p-fgw0gq}},
  volume       = {{1152}},
  year         = {{2025}},
}

@article{53414,
  abstract     = {{By constructing a non-empty domain of discontinuity in a suitable homogeneous
space, we prove that every torsion-free projective Anosov subgroup is the
monodromy group of a locally homogeneous contact Axiom A dynamical system with
a unique basic hyperbolic set on which the flow is conjugate to the refraction
flow of Sambarino. Under the assumption of irreducibility, we utilize the work
of Stoyanov to establish spectral estimates for the associated complex Ruelle
transfer operators, and by way of corollary: exponential mixing, exponentially
decaying error term in the prime orbit theorem, and a spectral gap for the
Ruelle zeta function. With no irreducibility assumption, results of
Dyatlov-Guillarmou imply the global meromorphic continuation of zeta functions
with smooth weights, as well as the existence of a discrete spectrum of
Ruelle-Pollicott resonances and (co)-resonant states. We apply our results to
space-like geodesic flows for the convex cocompact pseudo-Riemannian manifolds
of Danciger-Gu\'eritaud-Kassel, and the Benoist-Hilbert geodesic flow for
strictly convex real projective manifolds.}},
  author       = {{Delarue, Benjamin and Monclair, Daniel and Sanders, Andrew}},
  journal      = {{Geometric and Functional Analysis (GAFA)}},
  pages        = {{673–735}},
  title        = {{{Locally homogeneous Axiom A flows I: projective Anosov subgroups and exponential mixing}}},
  doi          = {{10.1007/s00039-025-00712-2}},
  volume       = {{35}},
  year         = {{2025}},
}

@article{64884,
  abstract     = {{To address the challenges associated with poor drug solubility and uncontrolled drug release in conventional dosage forms, a combination of polymer design and advanced drug delivery approaches has been employed. The development of pH-responsive nanoparticles for controlled and selective drug release represents a notable advance in adaptive nanomedicine. This study explores the design of a pH-responsive polymer, poly(1,4-phenyleneacetone dimethylene ketal) (PPADK). Additionally, the incorporation of light-responsive ortho-nitrobenzyl groups (o-NB-PPADK) enhanced the degradation upon exposure to light. Based on the polymer, nanoparticles were prepared using the solvent displacement method. The fluorescence dye Lumogen® Red was incorporated as a model substance. The nanoparticles were characterized by dynamic light scattering to determine their hydrodynamic diameter and size distribution, and the surface charge was analyzed. Atomic force microscopy was used to visualize the surface morphology. The nanoparticles remained stable under physiological pH conditions while exhibiting accelerated degradation and substance release in acidic environment, a property potentially exploitable for tumor targeting. Further enhanced degradation and correspondingly increased release was achieved by incorporating light-responsive elements in the polymer structure.
The cytotoxicity of these newly designed nanoparticles was evaluated in cell culture using a breast cancer cell line. These results support the potential of o-NB-PPADK nanoparticles as a possible candidate for selective and effective cancer therapy, combining stimuli-responsive degradation mechanisms for improved therapeutic outcomes.}},
  author       = {{Kramer, Maurice and van der Linde, Matthias and Hönscheid, Lisa and Horky, Corinna and Völlmecke, Katharina and Mulac, Dennis and Herrmann, Fabian and Kuckling, Dirk and Langer, Klaus}},
  issn         = {{0378-5173}},
  journal      = {{International Journal of Pharmaceutics}},
  keywords     = {{Nanoparticles, Drug delivery, Controlled release, Stimuli-responsiveTumor targeting}},
  publisher    = {{Elsevier BV}},
  title        = {{{Enlightening release strategies: Accelerated nanoparticle degradation and substance release utilizing light- and pH-responsive polymers}}},
  doi          = {{10.1016/j.ijpharm.2025.126127}},
  volume       = {{684}},
  year         = {{2025}},
}

@article{64885,
  abstract     = {{The tribological behavior of thermo‐responsive poly(N‐isopropylacrylamide) (PNIPAAm)‐based microgels is investigated for use as water‐dispersible lubricant additives. Two types of microgels are synthesized using a surfactant‐free emulsion polymerization method: MG0, consisting of pure PNIPAAm with a volume phase transition temperature (VPTT) of ≈33 °C, and MG16, consisting of PNIPAAm copolymerized with hydrophobic tert‐butyl acrylamide, exhibiting a lower VPTT of around 23 °C. Swelling and lubrication performance are evaluated at 20 and 40 °C. Both microgels significantly reduce friction and wear compared to water alone. At 20 °C, MG0 remains fully swollen and provides effective wear protection through hydrated microgel lubrication. MG16, being near its VPTT, exhibits partial collapse and slightly higher wear. At 40 °C, MG16 demonstrates improved wear resistance, attributed to enhanced film compaction in the collapsed state. Raman spectroscopy and scanning electron microscopy–energy‐dispersive X‐ray spectroscopy confirm that carbon‐rich tribofilms are formed via tribochemical reactions. MG0 produces more graphitic films, while MG16 generates amorphous carbon structures. These findings highlight the tunability of microgel composition for designing adaptive, water‐based lubricants for temperature‐sensitive applications.}},
  author       = {{Syed, Junaid and Dyck, Florian and Herberg, Artjom and Kuckling, Dirk and Gosvami, Nitya Nand}},
  issn         = {{1438-1656}},
  journal      = {{Advanced Engineering Materials}},
  number       = {{1}},
  publisher    = {{Wiley}},
  title        = {{{Microgel Additives for Aqueous Lubrication: Tailoring Friction and Wear via Composition and Thermal Responsiveness}}},
  doi          = {{10.1002/adem.202501673}},
  volume       = {{28}},
  year         = {{2025}},
}

@misc{64894,
  abstract     = {{This dataset contains experimental measurements of the radial dynamic and quasi-static characteristics of four different types of Rubber-Metal Bushings (RMBs) used in the suspension system of a passenger car under harmonic displacement excitation. For each bushing type, 2–3 individual specimens were tested.
 
Quasi-static measurements were performed at a constant excitation frequency of 0.05 Hz with varying displacement amplitudes. Dynamic measurements were conducted with displacement amplitudes ranging from 0.04 mm to 0.3 mm and excitation frequencies of 2, 5, 10, ..., up to 100 Hz.

The data is structured by bushing type, measurement mode, amplitude, and frequency, and is provided in *.csv  and *.hrm format. It is intended to support further research in modeling rubber-metal bushings and parameter identification techniques.}},
  author       = {{Schütte, Jan}},
  keywords     = {{bushing, experimental data, rubber-metal-bushing, Dataset suspension}},
  publisher    = {{LibreCat University}},
  title        = {{{Experimental Dataset: Force and Displacement Measurements of Four Rubber-Metal Bushing Types from a Passenger Car under Harmonic Displacement Excitation}}},
  doi          = {{10.5281/ZENODO.14851317}},
  year         = {{2025}},
}

@article{63513,
  author       = {{Grimminger-Seidensticker, Elke and Treder, Alexandra and Niederhaus, Constanze}},
  journal      = {{Zeitschrift für Sportpädagogische Forschung}},
  number       = {{2}},
  pages        = {{189--212}},
  publisher    = {{Nomos}},
  title        = {{{Sprachbezogene Kompetenzerwartungen im Sportunterricht – Eine systematische Lehrplananalyse}}},
  doi          = {{10.5771/2196-58218-2025-2-186}},
  volume       = {{13}},
  year         = {{2025}},
}

@inbook{57545,
  author       = {{Flath, Beate and Jacke, Christoph and Schroeter-Wittke, Harald}},
  booktitle    = {{Transdisziplinäre Räume in den Kulturwissenschaften}},
  editor       = {{Kornbach, Alina  and Lammer, Christina  and Magdeburg, Lena}},
  isbn         = {{978-3-534-64164-2}},
  pages        = {{211--254}},
  title        = {{{Den Schein werfen/wahren. Transdiziplinaritäten und Popkulturforschungen. Ein Übersetzungsraum als Partitur }}},
  volume       = {{3}},
  year         = {{2025}},
}

