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@@ -113,7 +111,7 @@ pre {
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@@ -121,6 +119,8 @@ pre {
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<h1><a name="libFitPofB"></a> libFitPofB </h1>
@@ -169,7 +169,7 @@ Assuming an array of <img alt="N" class="mmpImage" src="../pub/MUSR/LibFitPofB/_
<p style="text-align:center">
<img alt="\frac{\partial^2}{\partial z^2}B&#95;i(z) &#61; \frac{1}{\lambda&#95;i^2}B&#95;i(z)" class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_dfd02951094e1cb98f48e3f6d4562f38.png" title="London-eq" />
</p>
for each layer <img alt="i" class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_c465118a8d86d5f25bba37cc1dcb38a0.png" title="i" /> taking into account the boundary conditions<a name="FootNote1text"></a><span class="FootNoteTextLink" title="F&#46; London&#44; Superfluids&#58; Macroscopic Theory of Superconductivity&#44; Dover &#40;1961&#41;&#44; p&#46; 34"><a href="#FootNote1note" class="foswikiCurrentTopicLink">(1)</a></span>
for each layer <img alt="i" class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_c465118a8d86d5f25bba37cc1dcb38a0.png" title="i" /> taking into account the boundary conditions<a name="FootNote1text"></a><span class="FootNoteTextLink" title="F. London, Superfluids: Macroscopic Theory of Superconductivity, Dover (1961), p. 34"><a href="#FootNote1note" class="foswikiCurrentTopicLink">(1)</a></span>
<p style="text-align:center">
<img alt="B&#95;1(0) &#61; B&#95;N(d) &#61; \mu&#95;0H" class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_432d7664e0756ded77e7423dd256c122.png" title="cond1" />
</p>
@@ -275,11 +275,11 @@ When investigating superconductors in the mixed state by means of conventional &
<img alt="B(\mathbf{r}) &#61; \langle B \rangle \sum\limits&#95;{\mathbf{K}}B&#95;{\mathbf{K}}\exp(-\imath\mathbf{K}\mathbf{r})," class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_c25933e91d56089992506f463d71de8f.png" title="spatialB" />
</p>
where <img alt="\mathbf{r}&#61;(x,y)" class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_e47f33589d28eaa3f9baccb7a80fdbaa.png" title="r" />, <img alt="\mathbf{K}" class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_e6688a12ee4e821abc31b4c1dd511539.png" title="K" /> are the reciprocal lattice vectors of a two-dimensional vortex lattice and the <img alt="B&#95;{\mathbf{K}}" class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_8fa3ac8f18b7bc49eb89163d6528684c.png" title="Bk" /> are the Fourier coefficients depending on the magnetic penetration depth <img alt="\lambda" class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_28f3ed750a4819b4256c2f9be649f594.png" title="lambda" /> and the superconducting coherence length <img alt="\xi" class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_e8414d477977d226317c020980b7d34f.png" title="xi" />. The <img alt="B&#95;{\mathbf{K}}" class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_8fa3ac8f18b7bc49eb89163d6528684c.png" title="Bk" /> for some specific models are as follows: <dl>
<dt> London model with Gaussian cutoff<a name="FootNote2text"></a><span class="FootNoteTextLink" title="E&#46;H&#46; Brandt&#44; &#91;&#91;http&#58;&#47;&#47;dx&#46;doi&#46;org&#47;10&#46;1007&#47;BF00683568&#93;&#91;J&#46; Low Temp&#46; Phys&#46; &#42;73&#42;&#44; 355 &#40;1988&#41;&#93;&#93;&#46;"><a href="#FootNote2note" class="foswikiCurrentTopicLink">(2)</a></span> </dt><dd> <p style="text-align:center"><img alt="B&#95;{\mathbf{K}} &#61; \frac{\exp\left({-K^2\xi^2/2}\right)}{1 + K^2\lambda^2}" class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_469d5d1b83125e4915e2f073d8150b12.png" title="BkLondon" /></p>
</dd> <dt> Modified London model<a name="FootNote3text"></a><span class="FootNoteTextLink" title="T&#46;M&#46; Riseman _et al&#46;_&#44; &#91;&#91;http&#58;&#47;&#47;dx&#46;doi&#46;org&#47;10&#46;1103&#47;PhysRevB&#46;52&#46;10569&#93;&#91;Phys&#46; Rev&#46; B &#42;52&#42;&#44; 10569 &#40;1995&#41;&#93;&#93;&#46;"><a href="#FootNote3note" class="foswikiCurrentTopicLink">(3)</a></span> </dt><dd> <p style="text-align:center"><img alt="B&#95;{\mathbf{K}} &#61; \frac{\exp\left({-K^2\xi^2/2(1-b)}\right)}{1 + K^2\lambda^2/(1-b)}," class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_b6719fad8e30208538b34bc94040b7a5.png" title="BkML" /></p> where <img alt="b &#61; \langle B \rangle/\mu&#95;0H&#95;{\mathrm{c}2}." class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_039b3b38df7c6f284089c14f1efdf643.png" title="b" />
</dd> <dt> Analytical Ginzburg-Landau model<a name="FootNote4text"></a><span class="FootNoteTextLink" title="A&#46; Yaouanc&#44; P&#46; Dalmas de R&#38;eacute&#59;otier and E&#46;H&#46; Brandt&#44; &#91;&#91;http&#58;&#47;&#47;dx&#46;doi&#46;org&#47;10&#46;1103&#47;PhysRevB&#46;55&#46;11107&#93;&#91;Phys&#46; Rev&#46; B &#42;55&#42;&#44; 11107 &#40;1997&#41;&#93;&#93;&#46;"><a href="#FootNote4note" class="foswikiCurrentTopicLink">(4)</a></span> </dt><dd> <p style="text-align:center"><img alt="B&#95;{\mathbf{K}} &#61; \frac{f&#95;{\infty}K&#95;1\left(\frac{\xi&#95;v}{\lambda}\sqrt{f&#95;{\infty}^2+\lambda^2K^2}\right)}{K&#95;1\left(\frac{\xi&#95;v}{\lambda}f&#95;{\infty}\right)\sqrt{f&#95;{\infty}^2+\lambda^2K^2}}," class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_3146cb17887e3a20cc2078f103605af5.png" title="BkAGL" /></p> where <img alt="f&#95;{\infty} &#61; 1 - b^4,~\xi&#95;v &#61; \xi\left(\sqrt{2}-{3\xi}/\left({4\lambda}\right)\right)\sqrt{(1+b^4)(1-2b(1-b)^2)}" class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_e0b0e98f9a3974249b42b6910523c8a4.png" title="f_inf_and_xi_v" /> and <img alt="K&#95;1" class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_3cee3cc69dbe918398ec39a72a465014.png" title="K1" /> is a modified Bessel function.
<dt> London model with Gaussian cutoff<a name="FootNote2text"></a><span class="FootNoteTextLink" title="E.H. Brandt, <a href="http://dx.doi.org/10.1007/BF00683568" target="_top">J. Low Temp. Phys. <strong>73</strong>, 355 (1988)</a>."><a href="#FootNote2note" class="foswikiCurrentTopicLink">(2)</a></span> </dt><dd> <p style="text-align:center"><img alt="B&#95;{\mathbf{K}} &#61; \frac{\exp\left({-K^2\xi^2/2}\right)}{1 + K^2\lambda^2}" class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_469d5d1b83125e4915e2f073d8150b12.png" title="BkLondon" /></p>
</dd> <dt> Modified London model<a name="FootNote3text"></a><span class="FootNoteTextLink" title="T.M. Riseman <em>et al.</em>, <a href="http://dx.doi.org/10.1103/PhysRevB.52.10569" target="_top">Phys. Rev. B <strong>52</strong>, 10569 (1995)</a>."><a href="#FootNote3note" class="foswikiCurrentTopicLink">(3)</a></span> </dt><dd> <p style="text-align:center"><img alt="B&#95;{\mathbf{K}} &#61; \frac{\exp\left({-K^2\xi^2/2(1-b)}\right)}{1 + K^2\lambda^2/(1-b)}," class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_b6719fad8e30208538b34bc94040b7a5.png" title="BkML" /></p> where <img alt="b &#61; \langle B \rangle/\mu&#95;0H&#95;{\mathrm{c}2}." class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_039b3b38df7c6f284089c14f1efdf643.png" title="b" />
</dd> <dt> Analytical Ginzburg-Landau model<a name="FootNote4text"></a><span class="FootNoteTextLink" title="A. Yaouanc, P. Dalmas de R&eacute;otier and E.H. Brandt, <a href="http://dx.doi.org/10.1103/PhysRevB.55.11107" target="_top">Phys. Rev. B <strong>55</strong>, 11107 (1997)</a>."><a href="#FootNote4note" class="foswikiCurrentTopicLink">(4)</a></span> </dt><dd> <p style="text-align:center"><img alt="B&#95;{\mathbf{K}} &#61; \frac{f&#95;{\infty}K&#95;1\left(\frac{\xi&#95;v}{\lambda}\sqrt{f&#95;{\infty}^2+\lambda^2K^2}\right)}{K&#95;1\left(\frac{\xi&#95;v}{\lambda}f&#95;{\infty}\right)\sqrt{f&#95;{\infty}^2+\lambda^2K^2}}," class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_3146cb17887e3a20cc2078f103605af5.png" title="BkAGL" /></p> where <img alt="f&#95;{\infty} &#61; 1 - b^4,~\xi&#95;v &#61; \xi\left(\sqrt{2}-{3\xi}/\left({4\lambda}\right)\right)\sqrt{(1+b^4)(1-2b(1-b)^2)}" class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_e0b0e98f9a3974249b42b6910523c8a4.png" title="f_inf_and_xi_v" /> and <img alt="K&#95;1" class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_3cee3cc69dbe918398ec39a72a465014.png" title="K1" /> is a modified Bessel function.
</dd></dl>
Apart from the mentioned analytical models the <strong>numerical Ginzburg-Landau model</strong> <a name="FootNote5text"></a><span class="FootNoteTextLink" title="E&#46;H&#46; Brandt&#44; &#91;&#91;http&#58;&#47;&#47;dx&#46;doi&#46;org&#47;10&#46;1103&#47;PhysRevB&#46;68&#46;054506&#93;&#91;Phys&#46; Rev&#46; B &#42;68&#42;&#44; 054506 &#40;2003&#41;&#93;&#93;&#46;"><a href="#FootNote5note" class="foswikiCurrentTopicLink">(5)</a></span> is available. In this case <img alt="B(\mathbf{r})" class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_373e9bf1fc97e2c6aacf93bcc090402c.png" title="BofR" /> is obtained by an iterative minimization of the free energy of the vortex lattice.
Apart from the mentioned analytical models the <strong>numerical Ginzburg-Landau model</strong> <a name="FootNote5text"></a><span class="FootNoteTextLink" title="E.H. Brandt, <a href="http://dx.doi.org/10.1103/PhysRevB.68.054506" target="_top">Phys. Rev. B <strong>68</strong>, 054506 (2003)</a>."><a href="#FootNote5note" class="foswikiCurrentTopicLink">(5)</a></span> is available. In this case <img alt="B(\mathbf{r})" class="mmpImage" src="../pub/MUSR/LibFitPofB/_MathModePlugin_373e9bf1fc97e2c6aacf93bcc090402c.png" title="BofR" /> is obtained by an iterative minimization of the free energy of the vortex lattice.
<p></p>
<font color="#ff0000">Concerning the applicability (e.g. field regions) of each of the mentioned models please refer to the original publications!</font>
<p></p>
@@ -414,7 +414,7 @@ An example XML file looks as follows:
</div>
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@@ -445,17 +445,15 @@ An example XML file looks as follows:
</tr>
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