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<div id="jb-print-docs-body" class="onlyprint">
    <h1>The tutorial 8th</h1>
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  <section class="tex2jax_ignore mathjax_ignore" id="the-tutorial-8th">
<h1>The tutorial 8th<a class="headerlink" href="#the-tutorial-8th" title="Link to this heading">#</a></h1>
<p>Describes how PyXplore processes X-ray photoelectron spectroscopy (XPS) data.</p>
<section id="coding">
<h2>coding<a class="headerlink" href="#coding" title="Link to this heading">#</a></h2>
<blockquote>
<div><p><strong>1. Save your XPS data to the root directory and rename the file to <code class="docutils literal notranslate"><span class="pre">int.csv</span></code>.</strong></p>
</div></blockquote>
<div class="cell docutils container">
<div class="cell_input docutils container">
<div class="highlight-ipython3 notranslate"><div class="highlight"><pre><span></span><span class="c1"># import PyXplore package</span>
<span class="kn">from</span> <span class="nn">PyXplore</span> <span class="kn">import</span> <span class="n">WPEM</span>
<span class="kn">import</span> <span class="nn">pandas</span> <span class="k">as</span> <span class="nn">pd</span>
</pre></div>
</div>
</div>
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<div class="output stream highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>β–ˆβ–ˆβ•—    β–ˆβ–ˆβ•—β–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ•— β–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ•—β–ˆβ–ˆβ–ˆβ•—   β–ˆβ–ˆβ–ˆβ•—
β–ˆβ–ˆβ•‘    β–ˆβ–ˆβ•‘β–ˆβ–ˆβ•”β•β•β–ˆβ–ˆβ•—β–ˆβ–ˆβ•”β•β•β•β•β•β–ˆβ–ˆβ–ˆβ–ˆβ•— β–ˆβ–ˆβ–ˆβ–ˆβ•‘
β–ˆβ–ˆβ•‘ β–ˆβ•— β–ˆβ–ˆβ•‘β–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ•”β•β–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ•—  β–ˆβ–ˆβ•”β–ˆβ–ˆβ–ˆβ–ˆβ•”β–ˆβ–ˆβ•‘
β–ˆβ–ˆβ•‘β–ˆβ–ˆβ–ˆβ•—β–ˆβ–ˆβ•‘β–ˆβ–ˆβ•”β•β•β•β• β–ˆβ–ˆβ•”β•β•β•  β–ˆβ–ˆβ•‘β•šβ–ˆβ–ˆβ•”β•β–ˆβ–ˆβ•‘
β•šβ–ˆβ–ˆβ–ˆβ•”β–ˆβ–ˆβ–ˆβ•”β•β–ˆβ–ˆβ•‘     β–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ•—β–ˆβ–ˆβ•‘ β•šβ•β• β–ˆβ–ˆβ•‘
 β•šβ•β•β•β•šβ•β•β• β•šβ•β•     β•šβ•β•β•β•β•β•β•β•šβ•β•     β•šβ•β•                                                  

A Diffraction Refinement Software : WPEM
Bin Cao, Advanced Materials Thrust, Hong Kong University of Science and Technology (Guangzhou)
URL : https://github.com/Bin-Cao/WPEM
Executed on : 2025-07-22 11:02:07  | Have a great day.
====================================================================================================
</pre></div>
</div>
</div>
</div>
<blockquote>
<div><p><strong>2. Parse your diffraction data (<code class="docutils literal notranslate"><span class="pre">bing</span> <span class="pre">energy</span></code>, intensity) and perform background processing.</strong></p>
</div></blockquote>
<div class="cell docutils container">
<div class="cell_input docutils container">
<div class="highlight-ipython3 notranslate"><div class="highlight"><pre><span></span><span class="n">intensity_csv</span> <span class="o">=</span> <span class="n">pd</span><span class="o">.</span><span class="n">read_csv</span><span class="p">(</span><span class="sa">r</span><span class="s1">&#39;int.csv&#39;</span><span class="p">,</span><span class="n">header</span><span class="o">=</span><span class="kc">None</span> <span class="p">)</span>
<span class="n">var</span> <span class="o">=</span> <span class="n">WPEM</span><span class="o">.</span><span class="n">BackgroundFit</span><span class="p">(</span><span class="n">intensity_csv</span><span class="p">,</span><span class="n">segement</span><span class="o">=</span><span class="p">[[</span><span class="mi">910</span><span class="p">,</span><span class="mi">931</span><span class="p">],[</span><span class="mi">948</span><span class="p">,</span><span class="mi">952</span><span class="p">],[</span><span class="mi">958</span><span class="p">,</span><span class="mi">959</span><span class="p">],[</span><span class="mi">966</span><span class="p">,</span><span class="mi">970</span><span class="p">]],</span><span class="n">bac_num</span><span class="o">=</span><span class="mi">120</span><span class="p">,</span><span class="n">Model</span><span class="o">=</span><span class="s1">&#39;XPS&#39;</span><span class="p">,</span><span class="n">noise</span> <span class="o">=</span> <span class="mf">0.05</span><span class="p">,</span><span class="n">bac_var_type</span><span class="o">=</span><span class="s1">&#39;multivariate gaussian&#39;</span><span class="p">)</span>
</pre></div>
</div>
</div>
<div class="cell_output docutils container">
<img alt="../../_images/9a72e2a8dccbcf64abfeb8a2eab9fa988629866dce60f476adac1acee635b9c7.png" src="../../_images/9a72e2a8dccbcf64abfeb8a2eab9fa988629866dce60f476adac1acee635b9c7.png" />
<img alt="../../_images/a7d040a67d12e14e2a70047ab928c73da14f75827fb366f931965173a18ff060.png" src="../../_images/a7d040a67d12e14e2a70047ab928c73da14f75827fb366f931965173a18ff060.png" />
<img alt="../../_images/d787df8081dcd8cf12cefc99637d7a8d3e1b3204bf8edf07912ac1c716a7771d.png" src="../../_images/d787df8081dcd8cf12cefc99637d7a8d3e1b3204bf8edf07912ac1c716a7771d.png" />
<img alt="../../_images/60c6db4eaa2cab53d24386ec1b18c1a9bea706b82bb6b2710ff4247625087ac7.png" src="../../_images/60c6db4eaa2cab53d24386ec1b18c1a9bea706b82bb6b2710ff4247625087ac7.png" />
<div class="output stream highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>================================
</pre></div>
</div>
<div class="output text_plain highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>&lt;Figure size 640x480 with 0 Axes&gt;
</pre></div>
</div>
</div>
</div>
<blockquote>
<div><p><strong>3. After running the code, a new folder named <code class="docutils literal notranslate"><span class="pre">ConvertedDocuments</span></code> will be created in the root directory. This folder contains the background information.</strong></p>
</div></blockquote>
<blockquote>
<div><p><strong>Copy the two important files β€” <code class="docutils literal notranslate"><span class="pre">bac.csv</span></code> and <code class="docutils literal notranslate"><span class="pre">no_bac_intensity.csv</span></code> β€” from <code class="docutils literal notranslate"><span class="pre">ConvertedDocuments</span></code> into the root directory, as they are required for the next steps.</strong></p>
</div></blockquote>
<div class="admonition seealso">
<p class="admonition-title">See also</p>
<p>A key difference with XPS is that the initial binding energy needs to be queried and input using two parameters: <code class="docutils literal notranslate"><span class="pre">AtomIdentifier</span></code> and <code class="docutils literal notranslate"><span class="pre">satellitePeaks</span></code>.**</p>
</div>
<div class="cell docutils container">
<div class="cell_input docutils container">
<div class="highlight-ipython3 notranslate"><div class="highlight"><pre><span></span><span class="n">AtomIdentifier</span> <span class="o">=</span> <span class="p">[[</span><span class="s1">&#39;CuII&#39;</span><span class="p">,</span><span class="s1">&#39;2p3/2&#39;</span><span class="p">,</span><span class="mf">933.7</span><span class="p">,],[</span><span class="s1">&#39;CuII&#39;</span><span class="p">,</span><span class="s1">&#39;2p1/2&#39;</span><span class="p">,</span><span class="mi">954</span><span class="p">,],]</span>
<span class="n">satellitePeaks</span> <span class="o">=</span> <span class="p">[[</span><span class="s1">&#39;CuII&#39;</span><span class="p">,</span> <span class="s1">&#39;2p3/2&#39;</span><span class="p">,</span><span class="mf">941.6</span><span class="p">,],[</span><span class="s1">&#39;CuII&#39;</span><span class="p">,</span><span class="s1">&#39;2p3/2&#39;</span><span class="p">,</span><span class="mf">943.4</span><span class="p">],[</span><span class="s1">&#39;CuII&#39;</span><span class="p">,</span><span class="s1">&#39;2p1/2&#39;</span><span class="p">,</span><span class="mf">962.5</span><span class="p">,],]</span>
<span class="c1"># The file name of non-background data </span>
<span class="n">no_bac_intensity_file</span> <span class="o">=</span> <span class="s2">&quot;no_bac_intensity.csv&quot;</span> 
<span class="c1"># The file name of raw/original data </span>
<span class="n">original_file</span> <span class="o">=</span> <span class="s2">&quot;int.csv&quot;</span>  
<span class="c1"># The file name of background data </span>
<span class="n">bacground_file</span> <span class="o">=</span> <span class="s2">&quot;bac.csv&quot;</span>  

<span class="c1"># Execute the model</span>
<span class="n">WPEM</span><span class="o">.</span><span class="n">XPSfit</span><span class="p">(</span>
        <span class="n">var</span><span class="p">,</span> <span class="n">AtomIdentifier</span><span class="p">,</span> <span class="n">satellitePeaks</span><span class="p">,</span><span class="n">no_bac_intensity_file</span><span class="p">,</span> <span class="n">original_file</span><span class="p">,</span> <span class="n">bacground_file</span><span class="p">,</span> 
    <span class="n">bta</span> <span class="o">=</span> <span class="mf">0.80</span><span class="p">,</span><span class="n">iter_max</span> <span class="o">=</span> <span class="mi">50</span><span class="p">,</span>
<span class="p">)</span>
</pre></div>
</div>
</div>
<div class="cell_output docutils container">
<div class="output stream highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>Started at Tue Jul 22 11:02:12 2025 

Initialization
--------------------------------------------------------------------------------


β€”β€”β€”β€”β€”β€”β€”β€”β€”β€” Initilize the parameters by WPEM β€”β€”β€”β€”β€”β€”β€”β€”β€”β€”
Parameters of XPS are initialized has been completed 
</pre></div>
</div>
<div class="output stderr highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>  0%|                                                    | 0/50 [00:00&lt;?, ?it/s]
</pre></div>
</div>
<div class="output stderr highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span> 10%|β–ˆβ–ˆβ–ˆβ–ˆβ–                                       | 5/50 [00:00&lt;00:01, 41.72it/s]
</pre></div>
</div>
<div class="output stream highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>WPEM 0-th iteration
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.7, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 954, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.6], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.4], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.5]]]
Rp:45.523 | Rwp:51.131 | Rsquare:287.228


WPEM 1-th iteration
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.7, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 954, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.6], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.4], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.5]]]
Rp:45.938 | Rwp:51.811 | Rsquare:294.326


WPEM 2-th iteration
Under the central field approximation, the effective charge of CuII is: 25.799
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5567944942568406
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.882, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.956, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.462], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.371], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.385]]]
Rp:46.259 | Rwp:52.489 | Rsquare:301.292


WPEM 3-th iteration
Under the central field approximation, the effective charge of CuII is: 25.795
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5493864287697079
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.89, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.951, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.494], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.403], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.384]]]
Rp:46.344 | Rwp:52.587 | Rsquare:302.297


WPEM 4-th iteration
Under the central field approximation, the effective charge of CuII is: 25.793
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5472711772701394
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.895, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.95, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.493], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.427], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.382]]]
Rp:46.408 | Rwp:52.650 | Rsquare:303.038


WPEM 5-th iteration
Under the central field approximation, the effective charge of CuII is: 25.792
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.546155096073957
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.898, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.95, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.491], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.444], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.38]]]
Rp:46.461 | Rwp:52.699 | Rsquare:303.633


WPEM 6-th iteration
Under the central field approximation, the effective charge of CuII is: 25.79
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5454956959926958
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.904, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.949, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.488], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.456], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.377]]]
Rp:46.505 | Rwp:52.739 | Rsquare:304.134


WPEM 7-th iteration
Under the central field approximation, the effective charge of CuII is: 25.789
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5451827544054262
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.907, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.95, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.484], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.465], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.375]]]
Rp:46.544 | Rwp:52.777 | Rsquare:304.591


WPEM 8-th iteration
Under the central field approximation, the effective charge of CuII is: 25.788
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5451634921635551
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.911, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.95, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.481], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.471], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.372]]]
Rp:46.580 | Rwp:52.811 | Rsquare:305.005


WPEM 9-th iteration
</pre></div>
</div>
<div class="output stream highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>Under the central field approximation, the effective charge of CuII is:
</pre></div>
</div>
<div class="output stderr highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span> 20%|β–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–Œ                                  | 10/50 [00:00&lt;00:00, 42.08it/s]
</pre></div>
</div>
<div class="output stderr highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span> 30%|β–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–‰                              | 15/50 [00:00&lt;00:00, 42.40it/s]
</pre></div>
</div>
<div class="output stream highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span> 25.788
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5453921338017769
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.913, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.952, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.478], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.475], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.369]]]
Rp:46.613 | Rwp:52.844 | Rsquare:305.400


WPEM 10-th iteration
Under the central field approximation, the effective charge of CuII is: 25.787
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5458271150863314
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.916, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.953, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.475], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.478], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.366]]]
Rp:46.642 | Rwp:52.873 | Rsquare:305.753


WPEM 11-th iteration
Under the central field approximation, the effective charge of CuII is: 25.786
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5464314126562455
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.92, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.953, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.472], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.481], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.363]]]
Rp:46.669 | Rwp:52.900 | Rsquare:306.083


WPEM 12-th iteration
Under the central field approximation, the effective charge of CuII is: 25.785
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5471734006441921
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.923, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.953, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.469], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.482], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.36]]]
Rp:46.694 | Rwp:52.926 | Rsquare:306.393


WPEM 13-th iteration
Under the central field approximation, the effective charge of CuII is: 25.785
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5480263287264948
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.925, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.955, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.467], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.484], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.358]]]
Rp:46.719 | Rwp:52.951 | Rsquare:306.698


WPEM 14-th iteration
Under the central field approximation, the effective charge of CuII is: 25.784
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5489679638914116
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.929, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.956, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.465], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.484], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.355]]]
Rp:46.742 | Rwp:52.974 | Rsquare:306.972


WPEM 15-th iteration
Under the central field approximation, the effective charge of CuII is: 25.784
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5499791639996481
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.93, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.958, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.463], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.485], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.352]]]
Rp:46.765 | Rwp:52.997 | Rsquare:307.245


WPEM 16-th iteration
Under the central field approximation, the effective charge of CuII is: 25.783
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5510444226206037
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.934, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.958, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.461], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.486], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.349]]]
Rp:46.786 | Rwp:53.017 | Rsquare:307.489


WPEM 17-th iteration
Under the central field approximation, the effective charge of CuII is: 25.783
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5521503490396586
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.936, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.96, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.459], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.486], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.346]]]
Rp:46.807 | Rwp:53.037 | Rsquare:307.734


WPEM 18-th iteration
Under the central field approximation, the effective charge of CuII is: 25.782
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5532863008297899
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.939, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.96, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.458], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.486], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.343]]]
Rp:46.825 | Rwp:53.055 | Rsquare:307.952


WPEM 19-th iteration
</pre></div>
</div>
<div class="output stream highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>Under the central field approximation, the effective charge of CuII is:
</pre></div>
</div>
<div class="output stderr highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span> 40%|β–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–                         | 20/50 [00:00&lt;00:00, 42.56it/s]
</pre></div>
</div>
<div class="output stderr highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span> 50%|β–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–Œ                     | 25/50 [00:00&lt;00:00, 42.52it/s]
</pre></div>
</div>
<div class="output stream highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span> 25.782
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5544429415618155
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.941, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.962, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.457], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.486], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.341]]]
Rp:46.844 | Rwp:53.072 | Rsquare:308.171


WPEM 20-th iteration
Under the central field approximation, the effective charge of CuII is: 25.781
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.555613074431947
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.944, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.962, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.456], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.486], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.338]]]
Rp:46.860 | Rwp:53.088 | Rsquare:308.365


WPEM 21-th iteration
Under the central field approximation, the effective charge of CuII is: 25.781
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5567901839116616
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.946, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.964, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.455], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.485], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.336]]]
Rp:46.877 | Rwp:53.104 | Rsquare:308.561


WPEM 22-th iteration
Under the central field approximation, the effective charge of CuII is: 25.781
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.557969499145315
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.948, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.966, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.454], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.485], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.333]]]
Rp:46.893 | Rwp:53.119 | Rsquare:308.747


WPEM 23-th iteration
Under the central field approximation, the effective charge of CuII is: 25.78
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5591467458468962
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.951, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.966, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.453], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.485], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.331]]]
Rp:46.907 | Rwp:53.131 | Rsquare:308.908


WPEM 24-th iteration
Under the central field approximation, the effective charge of CuII is: 25.78
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5603181176256709
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.953, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.967, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.452], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.484], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.328]]]
Rp:46.921 | Rwp:53.144 | Rsquare:309.075


WPEM 25-th iteration
Under the central field approximation, the effective charge of CuII is: 25.78
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5614811413142897
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.954, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.969, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.451], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.484], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.326]]]
Rp:46.935 | Rwp:53.156 | Rsquare:309.232


WPEM 26-th iteration
Under the central field approximation, the effective charge of CuII is: 25.779
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.562633440628492
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.957, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.969, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.451], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.483], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.324]]]
Rp:46.946 | Rwp:53.167 | Rsquare:309.365


WPEM 27-th iteration
Under the central field approximation, the effective charge of CuII is: 25.779
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5637727599829994
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.959, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.971, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.45], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.482], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.322]]]
Rp:46.959 | Rwp:53.177 | Rsquare:309.506


WPEM 28-th iteration
Under the central field approximation, the effective charge of CuII is: 25.779
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5648979422231769
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.96, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.972, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.45], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.482], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.32]]]
Rp:46.970 | Rwp:53.188 | Rsquare:309.638


WPEM 29-th iteration
</pre></div>
</div>
<div class="output stream highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>Under the central field approximation, the effective charge of CuII is:
</pre></div>
</div>
<div class="output stderr highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span> 60%|β–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–Š                 | 30/50 [00:00&lt;00:00, 42.60it/s]
</pre></div>
</div>
<div class="output stderr highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span> 70%|β–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆ             | 35/50 [00:00&lt;00:00, 42.74it/s]
</pre></div>
</div>
<div class="output stream highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span> 25.778
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5660076798457581
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.963, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.972, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.449], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.481], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.318]]]
Rp:46.980 | Rwp:53.196 | Rsquare:309.749


WPEM 30-th iteration
Under the central field approximation, the effective charge of CuII is: 25.778
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5671005785860104
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.965, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.973, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.449], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.48], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.316]]]
Rp:46.991 | Rwp:53.205 | Rsquare:309.867


WPEM 31-th iteration
Under the central field approximation, the effective charge of CuII is: 25.778
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5681762572904128
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.966, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.975, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.448], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.479], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.315]]]
Rp:47.001 | Rwp:53.213 | Rsquare:309.979


WPEM 32-th iteration
Under the central field approximation, the effective charge of CuII is: 25.778
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5692340206264659
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.968, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.976, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.448], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.478], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.313]]]
Rp:47.010 | Rwp:53.221 | Rsquare:310.086


WPEM 33-th iteration
Under the central field approximation, the effective charge of CuII is: 25.777
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5702732984093672
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.971, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.976, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.447], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.478], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.312]]]
Rp:47.018 | Rwp:53.227 | Rsquare:310.171


WPEM 34-th iteration
Under the central field approximation, the effective charge of CuII is: 25.777
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5712933580372739
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.972, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.977, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.447], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.477], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.31]]]
Rp:47.026 | Rwp:53.234 | Rsquare:310.266


WPEM 35-th iteration
Under the central field approximation, the effective charge of CuII is: 25.777
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.572294379994188
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.973, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.978, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.447], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.476], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.309]]]
Rp:47.035 | Rwp:53.240 | Rsquare:310.356


WPEM 36-th iteration
Under the central field approximation, the effective charge of CuII is: 25.777
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5732761313904181
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.974, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.98, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.446], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.475], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.307]]]
Rp:47.042 | Rwp:53.247 | Rsquare:310.442


WPEM 37-th iteration
Under the central field approximation, the effective charge of CuII is: 25.776
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5742384328292118
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.977, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.979, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.446], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.474], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.306]]]
Rp:47.048 | Rwp:53.251 | Rsquare:310.507


WPEM 38-th iteration
Under the central field approximation, the effective charge of CuII is: 25.776
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5751808651457964
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.978, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.98, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.446], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.473], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.305]]]
Rp:47.055 | Rwp:53.256 | Rsquare:310.584


WPEM 39-th iteration
</pre></div>
</div>
<div class="output stderr highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span> 80%|β–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–        | 40/50 [00:00&lt;00:00, 41.60it/s]
</pre></div>
</div>
<div class="output stderr highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span> 90%|β–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–‹    | 45/50 [00:01&lt;00:00, 41.77it/s]
</pre></div>
</div>
<div class="output stream highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>Under the central field approximation, the effective charge of CuII is: 25.776
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5761039142795297
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.979, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.981, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.446], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.472], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.304]]]
Rp:47.063 | Rwp:53.262 | Rsquare:310.657


WPEM 40-th iteration
Under the central field approximation, the effective charge of CuII is: 25.776
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.577007586734658
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.98, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.982, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.446], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.472], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.303]]]
Rp:47.070 | Rwp:53.266 | Rsquare:310.726


WPEM 41-th iteration
Under the central field approximation, the effective charge of CuII is: 25.775
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5778919101049942
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.983, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.982, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.445], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.471], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.302]]]
Rp:47.075 | Rwp:53.269 | Rsquare:310.775


WPEM 42-th iteration
Under the central field approximation, the effective charge of CuII is: 25.775
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5787566161284525
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.984, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.983, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.445], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.47], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.301]]]
Rp:47.082 | Rwp:53.274 | Rsquare:310.838


WPEM 43-th iteration
Under the central field approximation, the effective charge of CuII is: 25.775
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5796023832221879
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.985, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.984, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.445], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.469], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.3]]]
Rp:47.088 | Rwp:53.278 | Rsquare:310.897


WPEM 44-th iteration
Under the central field approximation, the effective charge of CuII is: 25.775
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.580429346649011
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.986, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.985, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.445], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.468], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.299]]]
Rp:47.094 | Rwp:53.282 | Rsquare:310.953


WPEM 45-th iteration
Under the central field approximation, the effective charge of CuII is: 25.775
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5812376463631543
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.986, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.986, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.445], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.468], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.298]]]
Rp:47.100 | Rwp:53.286 | Rsquare:311.006


WPEM 46-th iteration
Under the central field approximation, the effective charge of CuII is: 25.774
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5820274758618512
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.989, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.985, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.445], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.467], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.298]]]
Rp:47.104 | Rwp:53.287 | Rsquare:311.041


WPEM 47-th iteration
Under the central field approximation, the effective charge of CuII is: 25.774
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5827986841757195
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.99, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.986, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.445], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.466], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.297]]]
Rp:47.110 | Rwp:53.291 | Rsquare:311.089


WPEM 48-th iteration
Under the central field approximation, the effective charge of CuII is: 25.774
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5835520752315267
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.99, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.987, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.445], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.465], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.296]]]
</pre></div>
</div>
<div class="output stderr highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>100%|β–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆ| 50/50 [00:01&lt;00:00, 42.14it/s]
</pre></div>
</div>
<div class="output stderr highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>100%|β–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆβ–ˆ| 50/50 [00:01&lt;00:00, 42.20it/s]
</pre></div>
</div>
<div class="output stderr highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>
</pre></div>
</div>
<div class="output stream highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>Rp:47.115 | Rwp:53.294 | Rsquare:311.135


WPEM 49-th iteration
Under the central field approximation, the effective charge of CuII is: 25.774
The Integrated Energy ratio for satellite peak of [(&#39;CuII&#39;, &#39;2p3/2&#39;), (&#39;CuII&#39;, &#39;2p1/2&#39;)] is 0.5842878717303636
The energies of electrons are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 933.991, [2, 1, 1.5]], [&#39;CuII&#39;, &#39;2p1/2&#39;, 953.987, [2, 1, 0.5]]]]
The energies of satellite peak are:
[[[&#39;CuII&#39;, &#39;2p3/2&#39;, 941.444], [&#39;CuII&#39;, &#39;2p3/2&#39;, 943.465], [&#39;CuII&#39;, &#39;2p1/2&#39;, 962.296]]]
Rp:47.120 | Rwp:53.297 | Rsquare:311.179


After update the background :   Rp = 47.075 | Rwp = 53.216 | Rsquare = 310.640
</pre></div>
</div>
<img alt="../../_images/e771332a0c9b055fc96971b62ad709146904438581e58c52ce40bb694f5637b4.png" src="../../_images/e771332a0c9b055fc96971b62ad709146904438581e58c52ce40bb694f5637b4.png" />
<img alt="../../_images/1790b28cbec61f61dc4307fca2564753bcf459a701a8345baefcbb07126d19b1.png" src="../../_images/1790b28cbec61f61dc4307fca2564753bcf459a701a8345baefcbb07126d19b1.png" />
<img alt="../../_images/2af622ccdec2bd40c06a663dbcef632af0718e6e48228cffd81521607078c23a.png" src="../../_images/2af622ccdec2bd40c06a663dbcef632af0718e6e48228cffd81521607078c23a.png" />
<div class="output stream highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>50-th iterations, reach the maximum number of iteration steps.
 Rp: 47.075
Rwp: 53.216 


WPEM-XPS program running time :  0 hours 0 minute  5 second  
</pre></div>
</div>
<div class="output text_plain highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>&#39;0 hours 0 minute  5 second  &#39;
</pre></div>
</div>
<div class="output text_plain highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>&lt;Figure size 640x480 with 0 Axes&gt;
</pre></div>
</div>
</div>
</div>
<blockquote>
<div><p><strong>The results are saved in the <code class="docutils literal notranslate"><span class="pre">XPSFittingProfile</span></code> folder.</strong></p>
</div></blockquote>
</section>
</section>

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