@article{53319,
  abstract     = {{<jats:title>Abstract</jats:title>
               <jats:p>The Neumann problem for (0.1)$$ \begin{align}&amp; V_t = \Delta V-aV+f(x,t) \end{align}$$is considered in bounded domains $\Omega \subset {\mathbb {R}}^n$ with smooth boundary, where $n\ge 1$ and $a\in {\mathbb {R}}$. By means of a variational approach, a statement on boundedness of the quantities $$ \begin{eqnarray*} \sup_{t\in (0,T)} \int_\Omega \big|\nabla V(\cdot,t)\big|^p L^{\frac{n+p}{n+2}} \Big( \big|\nabla V(\cdot,t)\big| \Big) \end{eqnarray*}$$in dependence on the expressions (0.2)$$ \begin{align}&amp; \sup_{t\in (0,T-\tau)} \int_t^{t+\tau} \int_\Omega |f|^{\frac{(n+2)p}{n+p}} L\big( |f|\big) \end{align}$$is derived for $p\ge 2$, $\tau&amp;gt;0$, and $T\ge 2\tau $, provided that $L\in C^0([0,\infty ))$ is positive, strictly increasing, unbounded, and slowly growing in the sense that $\limsup _{s\to \infty } \frac {L(s^{\lambda _0})}{L(s)} &amp;lt;\infty $ for some $\lambda _0&amp;gt;1$. In the particular case when $p=n\ge 2$, an additional condition on growth of $L$, particularly satisfied by $L(\xi ):=\ln ^\alpha (\xi +b)$ whenever $b&amp;gt;0$ and $\alpha&amp;gt;\frac {(n+2)(n-1)}{2n}$, is identified as sufficient to ensure that as a consequence of the above, bounds for theintegrals in (0.2) even imply estimates for the spatio-temporal modulus of continuity of solutions to (0.1). A subsequent application to the Keller–Segel system $$ \begin{eqnarray*} \left\{ \begin{array}{l} u_t = \nabla \cdot \big( D(v)\nabla u\big) - \nabla \cdot \big( uS(v)\nabla v\big) + ru - \mu u^2, \\[1mm] v_t = \Delta v-v+u, \end{array} \right. \end{eqnarray*}$$shows that when $n=2$, $r\in {\mathbb {R}}$, $0&amp;lt;D\in C^2([0,\infty ))$, and $S\in C^2([0,\infty )) \cap W^{1,\infty }((0,\infty ))$ and thus especially in the presence of arbitrarily strong diffusion degeneracies implied by rapid decay of $D$, any choice of $\mu&amp;gt;0$ excludes blowup in the sense that for all suitably regular nonnegative initial data, an associated initial-boundary value problem admits a global bounded classical solution.</jats:p>}},
  author       = {{Winkler, Michael}},
  issn         = {{1073-7928}},
  journal      = {{International Mathematics Research Notices}},
  keywords     = {{General Mathematics}},
  number       = {{19}},
  pages        = {{16336--16393}},
  publisher    = {{Oxford University Press (OUP)}},
  title        = {{{A Result on Parabolic Gradient Regularity in Orlicz Spaces and Application to Absorption-Induced Blow-Up Prevention in a Keller–Segel-Type Cross-Diffusion System}}},
  doi          = {{10.1093/imrn/rnac286}},
  volume       = {{2023}},
  year         = {{2022}},
}

@article{53321,
  abstract     = {{<jats:p> The chemotaxis system [Formula: see text] is considered in a ball [Formula: see text], [Formula: see text], where the positive function [Formula: see text] reflects suitably weak diffusion by satisfying [Formula: see text] for some [Formula: see text]. It is shown that whenever [Formula: see text] is positive and satisfies [Formula: see text] as [Formula: see text], one can find a suitably regular nonlinearity [Formula: see text] with the property that at each sufficiently large mass level [Formula: see text] there exists a globally defined radially symmetric classical solution to a Neumann-type boundary value problem for (⋆) which satisfies [Formula: see text] </jats:p>}},
  author       = {{Winkler, Michael}},
  issn         = {{0219-1997}},
  journal      = {{Communications in Contemporary Mathematics}},
  keywords     = {{Applied Mathematics, General Mathematics}},
  number       = {{10}},
  publisher    = {{World Scientific Pub Co Pte Ltd}},
  title        = {{{Arbitrarily fast grow-up rates in quasilinear Keller–Segel systems}}},
  doi          = {{10.1142/s0219199722500626}},
  volume       = {{25}},
  year         = {{2022}},
}

@article{53323,
  abstract     = {{<jats:title>Abstract</jats:title><jats:p>In a ball <jats:inline-formula><jats:alternatives><jats:tex-math>$$\Omega =B_R(0)\subset \mathbb {R}^n$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
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              </mml:math></jats:alternatives></jats:inline-formula>, <jats:inline-formula><jats:alternatives><jats:tex-math>$$n\ge 2$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
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              </mml:math></jats:alternatives></jats:inline-formula>, the chemotaxis system <jats:disp-formula><jats:alternatives><jats:tex-math>$$\begin{aligned} \left\{ \begin{array}{l}u_t = \nabla \cdot \big ( D(u) \nabla u \big ) - \nabla \cdot \big ( uS(u)\nabla v\big ), \\ 0 = \Delta v - \mu + u, \qquad \mu =\frac{1}{|\Omega |} \int _\Omega u, \end{array} \right. \qquad \qquad (\star ) \end{aligned}$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
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              </mml:math></jats:alternatives></jats:disp-formula>is considered under no-flux boundary conditions, with a focus on nonlinearities <jats:inline-formula><jats:alternatives><jats:tex-math>$$S\in C^2([0,\infty ))$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
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              </mml:math></jats:alternatives></jats:inline-formula> which exhibit super-algebraically fast decay in the sense that with some <jats:inline-formula><jats:alternatives><jats:tex-math>$$K_S&gt;0, \beta \in [0,1)$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
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              </mml:math></jats:alternatives></jats:inline-formula> and <jats:inline-formula><jats:alternatives><jats:tex-math>$$\xi _0&gt;0$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
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                </mml:mrow>
              </mml:math></jats:alternatives></jats:inline-formula>, <jats:disp-formula><jats:alternatives><jats:tex-math>$$\begin{aligned} S(\xi )&gt;0 \quad \text{ and } \quad S'(\xi ) \le -K_S\xi ^{-\beta } S(\xi ) \qquad \text{ for } \text{ all } \xi \ge \xi _0. \end{aligned}$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                <mml:mrow>
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                          <mml:mo>&gt;</mml:mo>
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              </mml:math></jats:alternatives></jats:disp-formula>It is, inter alia, shown that if furthermore <jats:inline-formula><jats:alternatives><jats:tex-math>$$D\in C^2((0,\infty ))$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                <mml:mrow>
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                      <mml:mi>∞</mml:mi>
                      <mml:mo>)</mml:mo>
                    </mml:mrow>
                    <mml:mo>)</mml:mo>
                  </mml:mrow>
                </mml:mrow>
              </mml:math></jats:alternatives></jats:inline-formula> is positive and suitably small in relation to <jats:italic>S</jats:italic> by satisfying <jats:disp-formula><jats:alternatives><jats:tex-math>$$\begin{aligned} \frac{\xi S(\xi )}{D(\xi )} \ge K_{SD}\xi ^\lambda \qquad \text{ for } \text{ all } \xi \ge \xi _0 \end{aligned}$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
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                </mml:mrow>
              </mml:math></jats:alternatives></jats:disp-formula>with some <jats:inline-formula><jats:alternatives><jats:tex-math>$$K_{SD}&gt;0$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                <mml:mrow>
                  <mml:msub>
                    <mml:mi>K</mml:mi>
                    <mml:mrow>
                      <mml:mi>SD</mml:mi>
                    </mml:mrow>
                  </mml:msub>
                  <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>$$\lambda &gt;\frac{2}{n}$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                <mml:mrow>
                  <mml:mi>λ</mml:mi>
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                  </mml:mfrac>
                </mml:mrow>
              </mml:math></jats:alternatives></jats:inline-formula>, then throughout a considerably large set of initial data, (<jats:inline-formula><jats:alternatives><jats:tex-math>$$\star $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                <mml:mo>⋆</mml:mo>
              </mml:math></jats:alternatives></jats:inline-formula>) admits global classical solutions (<jats:italic>u</jats:italic>, <jats:italic>v</jats:italic>) fulfilling <jats:disp-formula><jats:alternatives><jats:tex-math>$$\begin{aligned} \frac{z(t)}{C} \le \Vert u(\cdot ,t)\Vert _{L^\infty (\Omega )} \le Cz(t) \qquad \text{ for } \text{ all } t&gt;0, \end{aligned}$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                <mml:mrow>
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              </mml:math></jats:alternatives></jats:disp-formula>with some <jats:inline-formula><jats:alternatives><jats:tex-math>$$C=C^{(u,v)}\ge 1$$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
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                      <mml:mi>u</mml:mi>
                      <mml:mo>,</mml:mo>
                      <mml:mi>v</mml:mi>
                      <mml:mo>)</mml:mo>
                    </mml:mrow>
                  </mml:msup>
                  <mml:mo>≥</mml:mo>
                  <mml:mn>1</mml:mn>
                </mml:mrow>
              </mml:math></jats:alternatives></jats:inline-formula>, where <jats:italic>z</jats:italic> denotes the solution of <jats:disp-formula><jats:alternatives><jats:tex-math>$$\begin{aligned} \left\{ \begin{array}{l}z'(t) = z^2(t) \cdot S\big ( z(t)\big ), \qquad t&gt;0, \\ z(0)=\xi _0, \end{array} \right. \end{aligned}$$</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:msup>
                                      <mml:mi>z</mml:mi>
                                      <mml:mo>′</mml:mo>
                                    </mml:msup>
                                    <mml:mrow>
                                      <mml:mo>(</mml:mo>
                                      <mml:mi>t</mml:mi>
                                      <mml:mo>)</mml:mo>
                                    </mml:mrow>
                                    <mml:mo>=</mml:mo>
                                    <mml:msup>
                                      <mml:mi>z</mml:mi>
                                      <mml:mn>2</mml:mn>
                                    </mml:msup>
                                    <mml:mrow>
                                      <mml:mo>(</mml:mo>
                                      <mml:mi>t</mml:mi>
                                      <mml:mo>)</mml:mo>
                                    </mml:mrow>
                                    <mml:mo>·</mml:mo>
                                    <mml:mi>S</mml:mi>
                                    <mml:mrow>
                                      <mml:mo>(</mml:mo>
                                    </mml:mrow>
                                    <mml:mi>z</mml:mi>
                                    <mml:mrow>
                                      <mml:mo>(</mml:mo>
                                      <mml:mi>t</mml:mi>
                                      <mml:mo>)</mml:mo>
                                    </mml:mrow>
                                    <mml:mrow>
                                      <mml:mo>)</mml:mo>
                                    </mml:mrow>
                                    <mml:mo>,</mml:mo>
                                    <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:mtr>
                                <mml:mtd>
                                  <mml:mrow>
                                    <mml:mrow />
                                    <mml:mi>z</mml:mi>
                                    <mml:mrow>
                                      <mml:mo>(</mml:mo>
                                      <mml:mn>0</mml:mn>
                                      <mml:mo>)</mml:mo>
                                    </mml:mrow>
                                    <mml:mo>=</mml:mo>
                                    <mml:msub>
                                      <mml:mi>ξ</mml:mi>
                                      <mml:mn>0</mml:mn>
                                    </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>which is seen to exist globally, and to satisfy <jats:inline-formula><jats:alternatives><jats:tex-math>$$z(t)\rightarrow +\infty $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                <mml:mrow>
                  <mml:mi>z</mml:mi>
                  <mml:mo>(</mml:mo>
                  <mml:mi>t</mml:mi>
                  <mml:mo>)</mml:mo>
                  <mml:mo>→</mml:mo>
                  <mml:mo>+</mml:mo>
                  <mml:mi>∞</mml:mi>
                </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:mi>∞</mml:mi>
                </mml:mrow>
              </mml:math></jats:alternatives></jats:inline-formula>. As particular examples, exponentially and doubly exponentially decaying <jats:italic>S</jats:italic> are found to imply corresponding infinite-time blow-up properties in (<jats:inline-formula><jats:alternatives><jats:tex-math>$$\star $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">
                <mml:mo>⋆</mml:mo>
              </mml:math></jats:alternatives></jats:inline-formula>) at logarithmic and doubly logarithmic rates, respectively.</jats:p>}},
  author       = {{Winkler, Michael}},
  issn         = {{1040-7294}},
  journal      = {{Journal of Dynamics and Differential Equations}},
  keywords     = {{Analysis}},
  publisher    = {{Springer Science and Business Media LLC}},
  title        = {{{Slow Grow-up in a Quasilinear Keller–Segel System}}},
  doi          = {{10.1007/s10884-022-10167-w}},
  year         = {{2022}},
}

@article{53327,
  author       = {{Tao, Youshan and Winkler, Michael}},
  issn         = {{0022-0396}},
  journal      = {{Journal of Differential Equations}},
  keywords     = {{Analysis, Applied Mathematics}},
  pages        = {{390--418}},
  publisher    = {{Elsevier BV}},
  title        = {{{Global solutions to a Keller-Segel-consumption system involving singularly signal-dependent motilities in domains of arbitrary dimension}}},
  doi          = {{10.1016/j.jde.2022.10.022}},
  volume       = {{343}},
  year         = {{2022}},
}

@article{53325,
  author       = {{Desvillettes, Laurent and Laurençot, Philippe and Trescases, Ariane and Winkler, Michael}},
  issn         = {{0362-546X}},
  journal      = {{Nonlinear Analysis}},
  keywords     = {{Applied Mathematics, Analysis}},
  publisher    = {{Elsevier BV}},
  title        = {{{Weak solutions to triangular cross diffusion systems modeling chemotaxis with local sensing}}},
  doi          = {{10.1016/j.na.2022.113153}},
  volume       = {{226}},
  year         = {{2022}},
}

@article{53331,
  abstract     = {{<jats:p>In a ball <jats:inline-formula><jats:alternatives><jats:tex-math>$\Omega \subset \mathbb {R}^{n}$</jats:tex-math><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="png" xlink:href="S0308210522000397_inline1.png" /></jats:alternatives></jats:inline-formula> with <jats:inline-formula><jats:alternatives><jats:tex-math>$n\ge 2$</jats:tex-math><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="png" xlink:href="S0308210522000397_inline2.png" /></jats:alternatives></jats:inline-formula>, the chemotaxis system
<jats:disp-formula><jats:alternatives><jats:tex-math>\[ \left\{ \begin{array}{@{}l} u_t = \nabla \cdot \big( D(u)\nabla u\big) + \nabla\cdot \big(\dfrac{u}{v} \nabla v\big), \\ 0=\Delta v - uv \end{array} \right. \]</jats:tex-math><jats:graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="png" mimetype="image" position="float" xlink:href="S0308210522000397_eqnU1.png" /></jats:alternatives></jats:disp-formula>is considered along with no-flux boundary conditions for <jats:inline-formula><jats:alternatives><jats:tex-math>$u$</jats:tex-math><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="png" xlink:href="S0308210522000397_inline3.png" /></jats:alternatives></jats:inline-formula> and with prescribed constant positive Dirichlet boundary data for <jats:inline-formula><jats:alternatives><jats:tex-math>$v$</jats:tex-math><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="png" xlink:href="S0308210522000397_inline4.png" /></jats:alternatives></jats:inline-formula>. It is shown that if <jats:inline-formula><jats:alternatives><jats:tex-math>$D\in C^{3}([0,\infty ))$</jats:tex-math><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="png" xlink:href="S0308210522000397_inline5.png" /></jats:alternatives></jats:inline-formula> is such that <jats:inline-formula><jats:alternatives><jats:tex-math>$0&lt; D(\xi ) \le {K_D} (\xi +1)^{-\alpha }$</jats:tex-math><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="png" xlink:href="S0308210522000397_inline6.png" /></jats:alternatives></jats:inline-formula> for all <jats:inline-formula><jats:alternatives><jats:tex-math>$\xi &gt;0$</jats:tex-math><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="png" xlink:href="S0308210522000397_inline7.png" /></jats:alternatives></jats:inline-formula> with some <jats:inline-formula><jats:alternatives><jats:tex-math>${K_D}&gt;0$</jats:tex-math><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="png" xlink:href="S0308210522000397_inline8.png" /></jats:alternatives></jats:inline-formula> and <jats:inline-formula><jats:alternatives><jats:tex-math>$\alpha &gt;0$</jats:tex-math><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="png" xlink:href="S0308210522000397_inline9.png" /></jats:alternatives></jats:inline-formula>, then for all initial data from a considerably large set of radial functions on <jats:inline-formula><jats:alternatives><jats:tex-math>$\Omega$</jats:tex-math><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" mime-subtype="png" xlink:href="S0308210522000397_inline10.png" /></jats:alternatives></jats:inline-formula>, the corresponding initial-boundary value problem admits a solution blowing up in finite time.</jats:p>}},
  author       = {{Wang, Yulan and Winkler, Michael}},
  issn         = {{0308-2105}},
  journal      = {{Proceedings of the Royal Society of Edinburgh: Section A Mathematics}},
  keywords     = {{General Mathematics}},
  number       = {{4}},
  pages        = {{1150--1166}},
  publisher    = {{Cambridge University Press (CUP)}},
  title        = {{{Finite-time blow-up in a repulsive chemotaxis-consumption system}}},
  doi          = {{10.1017/prm.2022.39}},
  volume       = {{153}},
  year         = {{2022}},
}

@article{53344,
  abstract     = {{<jats:p> A no-flux initial-boundary value problem for the cross-diffusion system [Formula: see text] is considered in smoothly bounded domains [Formula: see text] with [Formula: see text]. It is shown that whenever [Formula: see text] is positive on [Formula: see text] and such that [Formula: see text] for some [Formula: see text], for all suitably regular positive initial data a global very weak solution, particularly preserving mass in its first component, can be constructed. This extends previous results which either concentrate on non-degenerate analogs, or are restricted to the special case [Formula: see text]. </jats:p><jats:p> To appropriately cope with the considerably stronger cross-degeneracies thus allowed through [Formula: see text] when [Formula: see text] is large, in its core part the analysis relies on the use of the Moser–Trudinger inequality in controlling the respective diffusion rates [Formula: see text] from below. </jats:p>}},
  author       = {{Winkler, Michael}},
  issn         = {{1664-3607}},
  journal      = {{Bulletin of Mathematical Sciences}},
  keywords     = {{General Mathematics}},
  number       = {{02}},
  publisher    = {{World Scientific Pub Co Pte Ltd}},
  title        = {{{Application of the Moser–Trudinger inequality in the construction of global solutions to a strongly degenerate migration model}}},
  doi          = {{10.1142/s1664360722500126}},
  volume       = {{13}},
  year         = {{2022}},
}

@techreport{35788,
  author       = {{Fochmann, Martin and Heinemann-Heile, Vanessa and Huber, Hans-Peter and Maiterth, Ralf and Sureth-Sloane, Caren}},
  issn         = {{1556-5068}},
  keywords     = {{General Earth and Planetary Sciences, General Environmental Science}},
  title        = {{{Zusatzkosten der Besteuerung – Eine Analyse des steuerlichen Verwaltungsaufwands und der subjektiv wahrgenommenen Steuerbelastung (An Empirical Analysis of Firms’ Hidden Cost of Taxation)}}},
  doi          = {{10.2139/ssrn.4210460}},
  volume       = {{100}},
  year         = {{2022}},
}

@techreport{35795,
  author       = {{Greil, Stefan and Overesch, Michael and Rohlfing-Bastian, Anna and Schreiber, Ulrich and Sureth-Sloane, Caren}},
  issn         = {{1556-5068}},
  title        = {{{Towards an Amended Arm's Length Principle - Tackling complexity and implementing destination rules in transfer pricing}}},
  doi          = {{10.2139/ssrn.4166972}},
  volume       = {{89}},
  year         = {{2022}},
}

@inproceedings{52574,
  author       = {{Werth, Gerda}},
  booktitle    = {{Beiträge zum Mathematikunterricht}},
  location     = {{Frankfurt am. Main}},
  publisher    = {{WTM}},
  title        = {{{Neue Wege im mathematischen Unterricht - Auf den Spuren Mathilde Vaertings}}},
  doi          = {{https://doi.org/10.37626/GA9783959872089.0}},
  year         = {{2022}},
}

@article{35749,
  author       = {{Arbeitskreis Verrechnungspreise der Schmalenbach-Gesellschaft für Betriebswirtschaftslehre e.V., . and lead authors: Kreuzer, A and Maier, H and Martini, J. T. and Niemann, Rainer and Schachtebeck, Maite and Simons, Dirk and Stoltenberg, J and Sureth-Sloane, Caren}},
  journal      = {{Internationales Steuerrecht}},
  number       = {{22}},
  pages        = {{824--829}},
  title        = {{{Chancen und Risiken eines Cooperative Compliance-Ansatzes für die deutsche Besteuerungspraxis von multinationalen Unternehmen – Erfahrungen verschiedener Länder und Eindrücke deutscher Unternehmensvertreter}}},
  volume       = {{31}},
  year         = {{2022}},
}

@unpublished{53421,
  abstract     = {{We define invariants $\operatorname{inv}_1,\dots,\operatorname{inv}_m$ of
Galois extensions of number fields with a fixed Galois group. Then, we propose
a heuristic in the spirit of Malle's conjecture which asymptotically predicts
the number of extensions that satisfy $\operatorname{inv}_i\leq X_i$ for all
$X_i$. The resulting conjecture is proved for abelian Galois groups. We also
describe refined Artin conductors that carry essentially the same information
as the invariants $\operatorname{inv}_1,\dots,\operatorname{inv}_m$.}},
  author       = {{Gundlach, Fabian}},
  booktitle    = {{arXiv:2211.16698}},
  title        = {{{Malle's conjecture with multiple invariants}}},
  year         = {{2022}},
}

@inproceedings{49825,
  author       = {{Lehmann, Isabell and Acar, Evrim and Hasija, Tanuj and Akhonda, M.A.B.S. and Calhoun, Vince D. and Schreier, Peter and Adali, Tulay}},
  booktitle    = {{ICASSP 2022 - 2022 IEEE International Conference on Acoustics, Speech and Signal Processing (ICASSP)}},
  publisher    = {{IEEE}},
  title        = {{{Multi-Task fMRI Data Fusion Using IVA and PARAFAC2}}},
  doi          = {{10.1109/icassp43922.2022.9747662}},
  year         = {{2022}},
}

@article{53238,
  author       = {{Tavana, Madjid and Khalili Nasr, Arash and Mina, Hassan and Michnik, Jerzy}},
  issn         = {{0038-0121}},
  journal      = {{Socio-Economic Planning Sciences}},
  keywords     = {{Management Science and Operations Research, Statistics, Probability and Uncertainty, Strategy and Management, Economics and Econometrics, Geography, Planning and Development}},
  publisher    = {{Elsevier BV}},
  title        = {{{A private sustainable partner selection model for green public-private partnerships and regional economic development}}},
  doi          = {{10.1016/j.seps.2021.101189}},
  volume       = {{83}},
  year         = {{2022}},
}

@article{53240,
  author       = {{Tavana, Madjid and Azadmanesh, Abdolreza and Nasr, Arash Khalili and Mina, Hassan}},
  issn         = {{1368-3500}},
  journal      = {{Current Issues in Tourism}},
  keywords     = {{Tourism, Leisure and Hospitality Management, Geography, Planning and Development}},
  number       = {{22}},
  pages        = {{3709--3734}},
  publisher    = {{Informa UK Limited}},
  title        = {{{A multicriteria-optimization model for cultural heritage renovation projects and public-private partnerships in the hospitality industry}}},
  doi          = {{10.1080/13683500.2021.2015299}},
  volume       = {{25}},
  year         = {{2022}},
}

@article{53241,
  author       = {{Khalili-Damghani, Kaveh and Tavana, Madjid and Ghasemi, Peiman}},
  issn         = {{0254-5330}},
  journal      = {{Annals of Operations Research}},
  keywords     = {{Management Science and Operations Research, General Decision Sciences}},
  number       = {{1}},
  pages        = {{103--141}},
  publisher    = {{Springer Science and Business Media LLC}},
  title        = {{{A stochastic bi-objective simulation–optimization model for cascade disaster location-allocation-distribution problems}}},
  doi          = {{10.1007/s10479-021-04191-0}},
  volume       = {{309}},
  year         = {{2022}},
}

@article{53236,
  author       = {{Tavana, Madjid and Shaabani, Akram and Di Caprio, Debora and Bonyani, Abbas}},
  issn         = {{0957-4174}},
  journal      = {{Expert Systems with Applications}},
  keywords     = {{Artificial Intelligence, Computer Science Applications, General Engineering}},
  publisher    = {{Elsevier BV}},
  title        = {{{A novel Interval Type-2 Fuzzy best-worst method and combined compromise solution for evaluating eco-friendly packaging alternatives}}},
  doi          = {{10.1016/j.eswa.2022.117188}},
  volume       = {{200}},
  year         = {{2022}},
}

@article{53237,
  author       = {{Tavana, Madjid and Kian, Hadi and Nasr, Arash Khalili and Govindan, Kannan and Mina, Hassan}},
  issn         = {{0959-6526}},
  journal      = {{Journal of Cleaner Production}},
  keywords     = {{Industrial and Manufacturing Engineering, Strategy and Management, General Environmental Science, Renewable Energy, Sustainability and the Environment}},
  publisher    = {{Elsevier BV}},
  title        = {{{A comprehensive framework for sustainable closed-loop supply chain network design}}},
  doi          = {{10.1016/j.jclepro.2021.129777}},
  volume       = {{332}},
  year         = {{2022}},
}

@article{53239,
  author       = {{Tavana, Madjid and Ghasrikhouzani, Mohsen and Abtahi, Amir-Reza}},
  issn         = {{0953-7325}},
  journal      = {{Technology Analysis & Strategic Management}},
  keywords     = {{Management Science and Operations Research, Strategy and Management}},
  number       = {{8}},
  pages        = {{859--875}},
  publisher    = {{Informa UK Limited}},
  title        = {{{A technology development framework for scenario planning and futures studies using causal modeling}}},
  doi          = {{10.1080/09537325.2021.1931672}},
  volume       = {{34}},
  year         = {{2022}},
}

@article{53242,
  author       = {{Ebadi Torkayesh, Ali and Tavana, Madjid and Santos-Arteaga, Francisco J.}},
  issn         = {{0959-6526}},
  journal      = {{Journal of Cleaner Production}},
  keywords     = {{Industrial and Manufacturing Engineering, Strategy and Management, General Environmental Science, Renewable Energy, Sustainability and the Environment, Building and Construction}},
  publisher    = {{Elsevier BV}},
  title        = {{{A multi-distance interval-valued neutrosophic approach for social failure detection in sustainable municipal waste management}}},
  doi          = {{10.1016/j.jclepro.2022.130409}},
  volume       = {{336}},
  year         = {{2022}},
}

