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<head>
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<title>User manual — musrfit 1.5.0 documentation</title>
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<title>User manual — musrfit 1.5.1 documentation</title>
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<li class="right" >
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<a href="tutorial.html" title="Tutorial for musrfit"
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accesskey="P">previous</a> |</li>
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<li><a href="index.html">musrfit 1.5.0 documentation</a> »</li>
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<li><a href="index.html">musrfit 1.5.1 documentation</a> »</li>
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</dl>
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<span id="index-20"></span><dl class="docutils" id="msr-alpha-beta">
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<dt><strong>alpha, beta</strong> (fit type 2, 3, 5)</dt>
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<dd><p class="first">These parameters are used to correct the asymmetry for different detector efficiencies, solid angles and initial asymmetries. They are defined as <span class="math">\(\alpha = N_{0,b}/N_{0,f}\)</span> and <span class="math">\(\beta = A_{0,b}/A_{0,f}\)</span>. If the parameters are not specified in the <a class="reference internal" href="#msr-run-block"><em>RUN block</em></a>, for each one the value of 1 is assumed (for fittype 5 alpha is estimated from the ration of sum of Bp+Bm and Fp+Fm). Example for alpha with fit parameter number 1:</p>
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<dd><p class="first">These parameters are used to correct the asymmetry for different detector efficiencies, solid angles and initial asymmetries. They are defined as <span class="math">\(\alpha = N_{0,b}/N_{0,f}\)</span> and <span class="math">\(\beta = A_{0,b}/A_{0,f}\)</span>. If the parameters are not specified in the <a class="reference internal" href="#msr-run-block"><em>RUN block</em></a>, for each one the value of 1 is assumed (for fittype 5, alpha is estimated from the ratio of <span class="math">\(\sum_i \left( N_{\mathrm{bp}}(i)+N_{\mathrm{bm}}(i) \right)\)</span> and <span class="math">\(\sum_i \left( N_{\mathrm{fp}}(i)+N_{\mathrm{fm}}(i) \right)\)</span>). Example for alpha with fit parameter number 1:</p>
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<div class="last highlight-python"><div class="highlight"><pre><span></span>alpha 1
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</pre></div>
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</div>
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</div>
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<div class="section" id="beta-nmr-asymmetry-fit-fit-type-5">
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<span id="bnmr-asymmetry-fit"></span><span id="index-69"></span><h3>beta-NMR Asymmetry Fit (fit type 5)<a class="headerlink" href="#beta-nmr-asymmetry-fit-fit-type-5" title="Permalink to this headline">¶</a></h3>
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<p>For a beta-NMR asymmetry fit (fit type 5) four histograms are needed, two for positive and two for negative helicities. These are given by the <a class="reference internal" href="#msr-forward-backward"><em>forward</em></a> and <a class="reference internal" href="#msr-forward-backward"><em>backward</em></a> keywords
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<p>Four histograms are needed for a beta-NMR asymmetry fit (fit type 5), two for positive helecity and two for negative. These are given by the <a class="reference internal" href="#msr-forward-backward"><em>forward</em></a> and <a class="reference internal" href="#msr-forward-backward"><em>backward</em></a> keywords
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in the <a class="reference internal" href="#msr-run-block"><em>RUN block</em></a>. Additionally, the parameters <a class="reference internal" href="#msr-alpha-beta"><em>alpha</em></a> and <a class="reference internal" href="#msr-alpha-beta"><em>beta</em></a> which relate the detector
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efficiencies, solid angles and initial asymmetries of the two detectors can be supplied. The constant background for the two histograms is either given by
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<a class="reference internal" href="#msr-background-asymmetry"><em>background-determined intervals</em></a> or specified through <a class="reference internal" href="#msr-backgr-fix"><em>backgr.fix</em></a> in the <a class="reference internal" href="#msr-run-block"><em>RUN-block</em></a>.</p>
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<p>The experimental asymmetry <span class="math">\(a(k)\)</span> then is calculated from the four histograms:</p>
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<p>The experimental asymmetry <span class="math">\(a(k)\)</span> is then calculated from the four histograms:</p>
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<div class="math">
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\[a(k)=\frac{\left[N_{\mathrm{fp}}(k)-B_{\mathrm{fp}}\right]-\left[N_{\mathrm{bp}}(k)-B_{\mathrm{bp}}\right]}{\left[N_{\mathrm{fp}}(k)-B_{\mathrm{fp}}\right]+\left[N_{\mathrm{bp}}(k)-B_{\mathrm{bp}}\right]}
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- \frac{\left[N_{\mathrm{fm}}(k)-B_{\mathrm{fm}}\right]-\left[N_{\mathrm{bm}}(k)-B_{\mathrm{bm}}\right]}{\left[N_{\mathrm{fm}}(k)-B_{\mathrm{fm}}\right]+\left[N_{\mathrm{bm}}(k)-B_{\mathrm{bm}}\right]},\]</div>
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@@ -1893,12 +1893,12 @@ efficiencies, solid angles and initial asymmetries of the two detectors can be s
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<div><ul class="simple">
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<li><span class="math">\(N_{\mathrm{fp}}(k)\)</span>: counts in the <strong>forward</strong> histogram channel with positive helicity <span class="math">\(k\)</span></li>
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<li><span class="math">\(N_{\mathrm{bp}}(k)\)</span>: counts in the <strong>backward</strong> histogram channel with positive helicity <span class="math">\(k\)</span></li>
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<li>:math:` B_{mathrm{fp}}`: constant background in the <strong>forward</strong> histogram with positive helicity (RUN block: <a class="reference internal" href="#msr-backgr-fix"><em>backgr.fix</em></a> or <a class="reference internal" href="#msr-background-asymmetry"><em>background</em></a>)</li>
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<li>:math:` B_{mathrm{bp}}`: constant background in the <strong>backward</strong> histogram with positive helicity (RUN block: <a class="reference internal" href="#msr-backgr-fix"><em>backgr.fix</em></a> or <a class="reference internal" href="#msr-background-asymmetry"><em>background</em></a>)</li>
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<li><span class="math">\(B_{\mathrm{fp}}\)</span>: constant background in the <strong>forward</strong> histogram with positive helicity (RUN block: <a class="reference internal" href="#msr-backgr-fix"><em>backgr.fix</em></a> or <a class="reference internal" href="#msr-background-asymmetry"><em>background</em></a>)</li>
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<li><span class="math">\(B_{\mathrm{bp}}\)</span>: constant background in the <strong>backward</strong> histogram with positive helicity (RUN block: <a class="reference internal" href="#msr-backgr-fix"><em>backgr.fix</em></a> or <a class="reference internal" href="#msr-background-asymmetry"><em>background</em></a>)</li>
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<li><span class="math">\(N_{\mathrm{fm}}(k)\)</span>: counts in the <strong>forward</strong> histogram channel with negative helicity <span class="math">\(k\)</span></li>
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<li><span class="math">\(N_{\mathrm{bm}}(k)\)</span>: counts in the <strong>backward</strong> histogram channel with negative helicity <span class="math">\(k\)</span></li>
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<li>:math:` B_{mathrm{fm}}`: constant background in the <strong>forward</strong> histogram with negative helicity (RUN block: <a class="reference internal" href="#msr-backgr-fix"><em>backgr.fix</em></a> or <a class="reference internal" href="#msr-background-asymmetry"><em>background</em></a>)</li>
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<li>:math:` B_{mathrm{bm}}`: constant background in the <strong>backward</strong> histogram with negative helicity (RUN block: <a class="reference internal" href="#msr-backgr-fix"><em>backgr.fix</em></a> or <a class="reference internal" href="#msr-background-asymmetry"><em>background</em></a>)</li>
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<li><span class="math">\(B_{\mathrm{fm}}\)</span>: constant background in the <strong>forward</strong> histogram with negative helicity (RUN block: <a class="reference internal" href="#msr-backgr-fix"><em>backgr.fix</em></a> or <a class="reference internal" href="#msr-background-asymmetry"><em>background</em></a>)</li>
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<li><span class="math">\(B_{\mathrm{bm}}\)</span>: constant background in the <strong>backward</strong> histogram with negative helicity (RUN block: <a class="reference internal" href="#msr-backgr-fix"><em>backgr.fix</em></a> or <a class="reference internal" href="#msr-background-asymmetry"><em>background</em></a>)</li>
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</ul>
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</div></blockquote>
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<p>This theoretical asymmetry <span class="math">\(a(t)\)</span> is used to fit the function</p>
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@@ -1914,7 +1914,8 @@ efficiencies, solid angles and initial asymmetries of the two detectors can be s
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</div></blockquote>
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<p>For the graphical representation in plot type 5 the equation above is rearranged to get <span class="math">\(A(t)\)</span>:</p>
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<div class="math">
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\[A(t)=\frac{(\alpha -1)+(\alpha +1)a(t)}{(\alpha\beta +1)+(\alpha\beta -1)a(t)}-\frac{(\alpha +1)a(t)-(\alpha -1)}{(\alpha\beta +1)+(1-\alpha\beta)a(t)}=\frac{\alpha\left[N_{\mathrm{fp}}(t)-B_{\mathrm{fp}}\right]-\left[N_{\mathrm{bp}}(t)-B_{\mathrm{bp}}\right]}{\alpha\beta\left[N_{\mathrm{fp}}(t)-B_{\mathrm{fp}}\right]+\left[N_{\mathrm{bp}}(t)-B_{\mathrm{bp}}\right]} -\frac{\alpha\left[N_{\mathrm{fm}}(t)-B_{\mathrm{fm}}\right]-\left[N_{\mathrm{bm}}(t)-B_{\mathrm{bm}}\right]}{\alpha\beta\left[N_{\mathrm{fm}}(t)-B_{\mathrm{fm}}\right]+\left[N_{\mathrm{bm}}(t)-B_{\mathrm{bm}}\right]}\]</div>
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\[\begin{split}A(t) &= \frac{(\alpha -1)+(\alpha +1)a(t)}{(\alpha\beta+1)+(\alpha\beta -1)a(t)}-\frac{(\alpha +1)a(t)-(\alpha-1)}{(\alpha\beta +1)+(1-\alpha\beta)a(t)} \\
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&= \frac{\alpha\left[N_{\mathrm{fp}}(t)-B_{\mathrm{fp}}\right]-\left[N_{\mathrm{bp}}(t)-B_{\mathrm{bp}}\right]}{\alpha\beta\left[N_{\mathrm{fp}}(t)-B_{\mathrm{fp}}\right]+\left[N_{\mathrm{bp}}(t)-B_{\mathrm{bp}}\right]} -\frac{\alpha\left[N_{\mathrm{fm}}(t)-B_{\mathrm{fm}}\right]-\left[N_{\mathrm{bm}}(t)-B_{\mathrm{bm}}\right]}{\alpha\beta\left[N_{\mathrm{fm}}(t)-B_{\mathrm{fm}}\right]+\left[N_{\mathrm{bm}}(t)-B_{\mathrm{bm}}\right]}\end{split}\]</div>
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<p>and plotted together with the function given in the THEORY block.</p>
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</div>
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<div class="section" id="non-mgrsr-fit-fit-type-8">
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@@ -2288,12 +2289,12 @@ In case this cannot be ensured, the parallelization can be disabled by <em>̵
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<li class="right" >
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<a href="tutorial.html" title="Tutorial for musrfit"
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>previous</a> |</li>
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<li><a href="index.html">musrfit 1.5.0 documentation</a> »</li>
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<li><a href="index.html">musrfit 1.5.1 documentation</a> »</li>
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</ul>
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</div>
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<div class="footer">
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© Copyright 2019, Andreas Suter.
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Last updated on May 15, 2019.
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Last updated on Jul 24, 2019.
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Created using <a href="http://sphinx-doc.org/">Sphinx</a> 1.2.3.
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