Little Modifications in the documentation webpage

fobos123deimos · Dec 17, 2024 · 71d1ce6 · 71d1ce6
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diff --git a/docs/fast_wave.html b/docs/fast_wave.html
@@ -439,7 +439,7 @@ <h2 id="contact">📬 Contact</h2>
 </span><span id="L-103"><a href="#L-103"><span class="linenos">103</span></a>
 </span><span id="L-104"><a href="#L-104"><span class="linenos">104</span></a><span class="sd">    &lt;br&gt;</span>
 </span><span id="L-105"><a href="#L-105"><span class="linenos">105</span></a>
-</span><span id="L-106"><a href="#L-106"><span class="linenos">106</span></a><span class="sd">    The energy eigenfunction for an energy state $\mathbf{n}$ is the wavefunction for an energy state $\mathbf{n}$ of a Quantum Harmonic Oscillator. From this definition, we can then represent the wave function $\Psi(x,t)$ as a series expansion of its family of energy eigenfunctions $\{\psi_{n}(x)\}$ [[5](#references)]:</span>
+</span><span id="L-106"><a href="#L-106"><span class="linenos">106</span></a><span class="sd">    The energy eigenfunction for an energy state $\mathbf{n}$ is the wavefunction for an energy state $\mathbf{n}$ of a Quantum Harmonic Oscillator. From this definition, we can then represent the wave function $\Psi(x,t)$ as a series expansion of its family of energy eigenfunctions $\\{\psi_{n}(x)\\}$ [[5](#references)]:</span>
 </span><span id="L-107"><a href="#L-107"><span class="linenos">107</span></a>
 </span><span id="L-108"><a href="#L-108"><span class="linenos">108</span></a><span class="sd">    $$</span>
 </span><span id="L-109"><a href="#L-109"><span class="linenos">109</span></a><span class="sd">    \Psi(y,t) = \sum_{n=0}^{\infty} c_{n} \, \psi_{n}(y) \, e^{-\mathbf{i}E_{n}t/\hbar} \quad \mathbf{(6)}</span>

diff --git a/src/fast_wave/__init__.py b/src/fast_wave/__init__.py
@@ -104,7 +104,7 @@
 
     <br>
 
-    The energy eigenfunction for an energy state $\mathbf{n}$ is the wavefunction for an energy state $\mathbf{n}$ of a Quantum Harmonic Oscillator. From this definition, we can then represent the wave function $\Psi(x,t)$ as a series expansion of its family of energy eigenfunctions $\{\psi_{n}(x)\}$ [[5](#references)]:
+    The energy eigenfunction for an energy state $\mathbf{n}$ is the wavefunction for an energy state $\mathbf{n}$ of a Quantum Harmonic Oscillator. From this definition, we can then represent the wave function $\Psi(x,t)$ as a series expansion of its family of energy eigenfunctions $\\{\psi_{n}(x)\\}$ [[5](#references)]:
 
     $$
     \Psi(y,t) = \sum_{n=0}^{\infty} c_{n} \, \psi_{n}(y) \, e^{-\mathbf{i}E_{n}t/\hbar} \quad \mathbf{(6)}
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@@ Expand Up / @@ -104,7 +104,7 @@ @@
         <br>
-        The energy eigenfunction for an energy state $\mathbf{n}$ is the wavefunction for an energy state $\mathbf{n}$ of a Quantum Harmonic Oscillator. From this definition, we can then represent the wave function $\Psi(x,t)$ as a series expansion of its family of energy eigenfunctions $\{\psi_{n}(x)\}$ [[5](#references)]:
+        The energy eigenfunction for an energy state $\mathbf{n}$ is the wavefunction for an energy state $\mathbf{n}$ of a Quantum Harmonic Oscillator. From this definition, we can then represent the wave function $\Psi(x,t)$ as a series expansion of its family of energy eigenfunctions $\\{\psi_{n}(x)\\}$ [[5](#references)]:
         $$
         \Psi(y,t) = \sum_{n=0}^{\infty} c_{n} \, \psi_{n}(y) \, e^{-\mathbf{i}E_{n}t/\hbar} \quad \mathbf{(6)}
@@ Expand Down @@