Remove indentation from align envs

spatialaudio/nbsphinx#766

doc/source/examples/calculating_quantum_processes.ipynb

@@ -4003,8 +4003,8 @@
     "The decay amplitudes $\\Gamma$ can be calculated from the generalized filter function and are thus amenable to the concatenation property of the control matrices. As the second order of the Magnus expansion involves a double time integral, such a simplification is not possible in the case of the frequency shifts $\\Delta$. However, we can define a filter function for them just the same:\n",
     "\n",
     "\\begin{align}\n",
-    "    \\Gamma_{\\alpha\\beta,kl} &= \\int\\frac{\\mathrm{d}\\omega}{2\\pi}S_{\\alpha\\beta}(\\omega) F_{\\alpha\\beta,kl}^{(\\Gamma)}(\\omega) \\\\\n",
-    "    \\Delta_{\\alpha\\beta,kl} &= \\int\\frac{\\mathrm{d}\\omega}{2\\pi}S_{\\alpha\\beta}(\\omega) F_{\\alpha\\beta,kl}^{(\\Delta)}(\\omega)\n",
+    "\\Gamma_{\\alpha\\beta,kl} &= \\int\\frac{\\mathrm{d}\\omega}{2\\pi}S_{\\alpha\\beta}(\\omega) F_{\\alpha\\beta,kl}^{(\\Gamma)}(\\omega) \\\\\n",
+    "\\Delta_{\\alpha\\beta,kl} &= \\int\\frac{\\mathrm{d}\\omega}{2\\pi}S_{\\alpha\\beta}(\\omega) F_{\\alpha\\beta,kl}^{(\\Delta)}(\\omega)\n",
     "\\end{align}\n",
     "\n",
     "### Performance considerations\n",

doc/source/examples/getting_started.ipynb

@@ -26,9 +26,9 @@
     "The central object of this package is the `PulseSequence` class. It is used to represent the control operation implementing a certain Hamiltonian ${H}_c$ and the sensitivities of the noise afflicting the system. More concisely, the total Hamiltonian of the system is modelled as\n",
     "\n",
     "\\begin{align*}\n",
-    "    {H} &= {H}_c + {H}_n \\\\\n",
-    "    {H}_c &= \\sum_i a_i(t) A_i \\\\\n",
-    "    {H}_n &= \\sum_\\alpha s_\\alpha(t) b_\\alpha(t) B_\\alpha \\\\\n",
+    "{H} &= {H}_c + {H}_n \\\\\n",
+    "{H}_c &= \\sum_i a_i(t) A_i \\\\\n",
+    "{H}_n &= \\sum_\\alpha s_\\alpha(t) b_\\alpha(t) B_\\alpha \\\\\n",
     "\\end{align*}\n",
     "\n",
     "where $A_i$ and $B_\\alpha$ are the control and noise operators, respectively, $a_i(t)$ the control strength of $A_i$ at time $t$, $s_\\alpha(t)$ a deterministic time dependence of the noise operators to model, for instance, non-linear coupling to the noise sources, and $b_\\alpha(t)$ classically fluctuating noise variables. Since the noise is captured in a spectral density function that accounts for different realizations of the random noise, the $b_\\alpha(t)$ are not required at instantiation of a `PulseSequence` instance. Note that we always calculate in units where $\\hbar\\equiv 1$.\n",