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docs: render equations via math code blocks
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‎lib/node_modules/@stdlib/simulate/iter/bartlett-hann-pulse/README.md‎

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@@ -30,10 +30,14 @@ A Bartlett-Hann pulse waveform is represented by the following equation
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<!-- <equation class="equation" label="eq:bartlett_hann_pulse_waveform" align="center" raw="f(t; T, \tau, A, \varphi) = \begin{cases}A \biggl(0.62 - 0.48\biggl|\frac{t-\varphi}{\tau-1} - \frac{1}{2}\biggr| - 0.38\cos\frac{2\pi (t-\varphi)}{\tau-1}\biggr) & (t-\varphi) \mod T < \tau \\ 0 & \textrm{otherwise} \end{cases}" alt="Equation for a Bartlett-Hann pulse waveform."> -->
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<div class="equation" align="center" data-raw-text="f(t; T, \tau, A, \varphi) = \begin{cases}A \biggl(0.62 - 0.48\biggl|\frac{t-\varphi}{\tau-1} - \frac{1}{2}\biggr| - 0.38\cos\frac{2\pi (t-\varphi)}{\tau-1}\biggr) &amp; (t-\varphi) \mod T < \tau \\ 0 &amp; \textrm{otherwise} \end{cases}" data-equation="eq:bartlett_hann_pulse_waveform">
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```math
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f(t; T, \tau, A, \varphi) = \begin{cases}A \biggl(0.62 - 0.48\biggl|\frac{t-\varphi}{\tau-1} - \frac{1}{2}\biggr| - 0.38\cos\frac{2\pi (t-\varphi)}{\tau-1}\biggr) & (t-\varphi) \mod T < \tau \\ 0 & \textrm{otherwise} \end{cases}
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```
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<!-- <div class="equation" align="center" data-raw-text="f(t; T, \tau, A, \varphi) = \begin{cases}A \biggl(0.62 - 0.48\biggl|\frac{t-\varphi}{\tau-1} - \frac{1}{2}\biggr| - 0.38\cos\frac{2\pi (t-\varphi)}{\tau-1}\biggr) &amp; (t-\varphi) \mod T < \tau \\ 0 &amp; \textrm{otherwise} \end{cases}" data-equation="eq:bartlett_hann_pulse_waveform">
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<img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@76fd234ed3f3558f7a75e86bce3ad928b5fb7e3a/lib/node_modules/@stdlib/simulate/iter/bartlett-hann-pulse/docs/img/equation_bartlett_hann_pulse_waveform.svg" alt="Equation for a Bartlett-Hann pulse waveform.">
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<br>
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</div>
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</div> -->
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<!-- </equation> -->
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‎lib/node_modules/@stdlib/simulate/iter/bartlett-pulse/README.md‎

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<!-- <equation class="equation" label="eq:bartlett_pulse_waveform" align="center" raw="f(t; T, \tau, a, \varphi) = \begin{cases}1 - \biggl|\frac{2(t-\varphi)}{\tau-1} - 1\biggr| & (t-\varphi) \mod T < \tau \\ 0 & \textrm{otherwise} \end{cases}" alt="Equation for a Bartlett pulse waveform."> -->
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<div class="equation" align="center" data-raw-text="f(t; T, \tau, a, \varphi) = \begin{cases}1 - \biggl|\frac{2(t-\varphi)}{\tau-1} - 1\biggr| &amp; (t-\varphi) \mod T < \tau \\ 0 &amp; \textrm{otherwise} \end{cases}" data-equation="eq:bartlett_pulse_waveform">
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```math
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f(t; T, \tau, a, \varphi) = \begin{cases}1 - \biggl|\frac{2(t-\varphi)}{\tau-1} - 1\biggr| & (t-\varphi) \mod T < \tau \\ 0 & \textrm{otherwise} \end{cases}
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```
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<!-- <div class="equation" align="center" data-raw-text="f(t; T, \tau, a, \varphi) = \begin{cases}1 - \biggl|\frac{2(t-\varphi)}{\tau-1} - 1\biggr| &amp; (t-\varphi) \mod T < \tau \\ 0 &amp; \textrm{otherwise} \end{cases}" data-equation="eq:bartlett_pulse_waveform">
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<img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@d8910751300fc12f81545175e5b0dbcbf4a67efa/lib/node_modules/@stdlib/simulate/iter/bartlett-pulse/docs/img/equation_bartlett_pulse_waveform.svg" alt="Equation for a Bartlett pulse waveform.">
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<br>
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</div> -->
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<!-- </equation> -->
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‎lib/node_modules/@stdlib/simulate/iter/cosine-wave/README.md‎

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<!-- <equation class="equation" label="eq:cosine_waveform" align="center" raw="f(t; \tau, a, \varphi) = a \cos \frac{2\pi(t-\varphi)}{\tau}" alt="Equation for a cosine waveform."> -->
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<div class="equation" align="center" data-raw-text="f(t; \tau, a, \varphi) = a \cos \frac{2\pi(t-\varphi)}{\tau}" data-equation="eq:cosine_waveform">
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```math
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f(t; \tau, a, \varphi) = a \cos \frac{2\pi(t-\varphi)}{\tau}
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```
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<!-- <div class="equation" align="center" data-raw-text="f(t; \tau, a, \varphi) = a \cos \frac{2\pi(t-\varphi)}{\tau}" data-equation="eq:cosine_waveform">
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<img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@5827c258000edcb03496265cdfd372d686b4c656/lib/node_modules/@stdlib/simulate/iter/cosine-wave/docs/img/equation_cosine_waveform.svg" alt="Equation for a cosine waveform.">
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<br>
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</div> -->
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<!-- </equation> -->
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‎lib/node_modules/@stdlib/simulate/iter/dirac-comb/README.md‎

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<!-- <equation class="equation" label="eq:dirac_comb" align="center" raw="f(t; T, \varphi) = \delta((t-\varphi) \bmod T)" alt="Equation for a Dirac comb."> -->
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<div class="equation" align="center" data-raw-text="f(t; T, \varphi) = \delta((t-\varphi) \bmod T)" data-equation="eq:dirac_comb">
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```math
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f(t; T, \varphi) = \delta((t-\varphi) \bmod T)
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```
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<!-- <div class="equation" align="center" data-raw-text="f(t; T, \varphi) = \delta((t-\varphi) \bmod T)" data-equation="eq:dirac_comb">
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<img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@801be3f8c35f2e79fbcf9b6e38568479f6faa5f2/lib/node_modules/@stdlib/simulate/iter/dirac-comb/docs/img/equation_dirac_comb.svg" alt="Equation for a Dirac comb.">
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<br>
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</div> -->
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<!-- </equation> -->
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‎lib/node_modules/@stdlib/simulate/iter/flat-top-pulse/README.md‎

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<!-- <equation class="equation" label="eq:flat_top_pulse_waveform" align="center" raw="f(t; \tau, A, \varphi) = \begin{align*} A\biggl(a_0 &- a_1 \cos\frac{2\pi (t-\varphi)}{\tau-1} + a_2 \cos\frac{2\pi(t-\varphi)}{\tau-1} \\ &- a_3 \cos\frac{2\pi(t-\varphi)}{\tau-1} + a_4 \cos \frac{2\pi (t-\varphi)}{\tau-1} \biggr)\end{align*}" alt="Equation for a flat top pulse waveform."> -->
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<div class="equation" align="center" data-raw-text="f(t; T, \tau, A, \varphi) = \begin{align*} A\biggl(a_0 &amp;- a_1 \cos\frac{2\pi (t-\varphi)}{\tau-1} + a_2 \cos\frac{2\pi(t-\varphi)}{\tau-1} \\ &amp;- a_3 \cos\frac{2\pi(t-\varphi)}{\tau-1} + a_4 \cos \frac{2\pi (t-\varphi)}{\tau-1} \biggr)\end{align*}" data-equation="eq:flat_top_pulse_waveform">
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```math
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f(t; \tau, A, \varphi) = \begin{align*} A\biggl(a_0 &- a_1 \cos\frac{2\pi (t-\varphi)}{\tau-1} + a_2 \cos\frac{2\pi(t-\varphi)}{\tau-1} \\ &- a_3 \cos\frac{2\pi(t-\varphi)}{\tau-1} + a_4 \cos \frac{2\pi (t-\varphi)}{\tau-1} \biggr)\end{align*}
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```
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<!-- <div class="equation" align="center" data-raw-text="f(t; T, \tau, A, \varphi) = \begin{align*} A\biggl(a_0 &amp;- a_1 \cos\frac{2\pi (t-\varphi)}{\tau-1} + a_2 \cos\frac{2\pi(t-\varphi)}{\tau-1} \\ &amp;- a_3 \cos\frac{2\pi(t-\varphi)}{\tau-1} + a_4 \cos \frac{2\pi (t-\varphi)}{\tau-1} \biggr)\end{align*}" data-equation="eq:flat_top_pulse_waveform">
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<img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@157025f95b239be39ac0c70158f96243f1be978e/lib/node_modules/@stdlib/simulate/iter/flat-top-pulse/docs/img/equation_flat_top_pulse_waveform.svg" alt="Equation for a flat top pulse waveform.">
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<!-- </equation> -->
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‎lib/node_modules/@stdlib/simulate/iter/hann-pulse/README.md‎

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<!-- <equation class="equation" label="eq:hann_pulse_waveform" align="center" raw="f(t; T, \tau, a, \varphi) = \begin{cases} \frac{a}{2}\biggl(1-\cos \frac{2\pi (t-\varphi)}{\tau-1}\biggr) & (t-\varphi) \mod T < \tau \\ 0 & \textrm{otherwise} \end{cases}" alt="Equation for a Hann pulse waveform."> -->
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<div class="equation" align="center" data-raw-text="f(t; T, \tau, a, \varphi) = \begin{cases} \frac{a}{2}\biggl(1-\cos \frac{2\pi (t-\varphi)}{\tau-1}\biggr) &amp; (t-\varphi) \mod T < \tau \\ 0 &amp; \textrm{otherwise} \end{cases}" data-equation="eq:hann_pulse_waveform">
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```math
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f(t; T, \tau, a, \varphi) = \begin{cases} \frac{a}{2}\biggl(1-\cos \frac{2\pi (t-\varphi)}{\tau-1}\biggr) & (t-\varphi) \mod T < \tau \\ 0 & \textrm{otherwise} \end{cases}
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```
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<!-- <div class="equation" align="center" data-raw-text="f(t; T, \tau, a, \varphi) = \begin{cases} \frac{a}{2}\biggl(1-\cos \frac{2\pi (t-\varphi)}{\tau-1}\biggr) &amp; (t-\varphi) \mod T < \tau \\ 0 &amp; \textrm{otherwise} \end{cases}" data-equation="eq:hann_pulse_waveform">
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<img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@08cee6de617d64ec3324479142e1cdf0036898d8/lib/node_modules/@stdlib/simulate/iter/hann-pulse/docs/img/equation_hann_pulse_waveform.svg" alt="Equation for a Hann pulse waveform.">
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<!-- </equation> -->
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‎lib/node_modules/@stdlib/simulate/iter/lanczos-pulse/README.md‎

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<!-- <equation class="equation" label="eq:lanczos_pulse_waveform" align="center" raw="f(t; T, \tau, a, \varphi) = \begin{cases}\operatorname{sinc}\biggl( \frac{2(t-\varphi)}{\tau-1} - 1\biggr) & (t-\varphi) \mod T < \tau \\ 0 & \textrm{otherwise} \end{cases}" alt="Equation for a Lanczos pulse waveform."> -->
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<div class="equation" align="center" data-raw-text="f(t; T, \tau, a, \varphi) = \begin{cases}\operatorname{sinc}\biggl( \frac{2(t-\varphi)}{\tau-1} - 1\biggr) &amp; (t-\varphi) \mod T < \tau \\ 0 &amp; \textrm{otherwise} \end{cases}" data-equation="eq:lanczos_pulse_waveform">
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```math
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f(t; T, \tau, a, \varphi) = \begin{cases}\operatorname{sinc}\biggl( \frac{2(t-\varphi)}{\tau-1} - 1\biggr) & (t-\varphi) \mod T < \tau \\ 0 & \textrm{otherwise} \end{cases}
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```
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<!-- <div class="equation" align="center" data-raw-text="f(t; T, \tau, a, \varphi) = \begin{cases}\operatorname{sinc}\biggl( \frac{2(t-\varphi)}{\tau-1} - 1\biggr) &amp; (t-\varphi) \mod T < \tau \\ 0 &amp; \textrm{otherwise} \end{cases}" data-equation="eq:lanczos_pulse_waveform">
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<img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@4fa8f0c0d831199775879b44805649a741cf37ce/lib/node_modules/@stdlib/simulate/iter/lanczos-pulse/docs/img/equation_lanczos_pulse_waveform.svg" alt="Equation for a Lanczos pulse waveform.">
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<!-- </equation> -->
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‎lib/node_modules/@stdlib/simulate/iter/periodic-sinc/README.md‎

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<!-- <equation class="equation" label="eq:periodic_sinc" align="center" raw="D_N(x; A) = \begin{cases}\frac{A\sin(Nx/2)} {N\sin(x/2)} & x \neq 2\pi k\ \textrm{for}\ k = 0, \pm 1, \pm 2, \ldots \\ A (-1)^{k(N-1)} & x = 2\pi k\ \textrm{for}\ k = 0, \pm 1, \pm 2, \ldots \end{cases}" alt="Periodic sinc function."> -->
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<div class="equation" align="center" data-raw-text="D_N(x; A) = \begin{cases}\frac{A\sin(Nx/2)} {N\sin(x/2)} &amp; x \neq 2\pi k\ \textrm{for}\ k = 0, \pm 1, \pm 2, \ldots \\ A (-1)^{k(N-1)} &amp; x = 2\pi k\ \textrm{for}\ k = 0, \pm 1, \pm 2, \ldots \end{cases}" data-equation="eq:periodic_sinc">
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```math
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D_N(x; A) = \begin{cases}\frac{A\sin(Nx/2)} {N\sin(x/2)} & x \neq 2\pi k\ \textrm{for}\ k = 0, \pm 1, \pm 2, \ldots \\ A (-1)^{k(N-1)} & x = 2\pi k\ \textrm{for}\ k = 0, \pm 1, \pm 2, \ldots \end{cases}
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```
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<!-- <div class="equation" align="center" data-raw-text="D_N(x; A) = \begin{cases}\frac{A\sin(Nx/2)} {N\sin(x/2)} &amp; x \neq 2\pi k\ \textrm{for}\ k = 0, \pm 1, \pm 2, \ldots \\ A (-1)^{k(N-1)} &amp; x = 2\pi k\ \textrm{for}\ k = 0, \pm 1, \pm 2, \ldots \end{cases}" data-equation="eq:periodic_sinc">
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<img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@d985bb501380970d8c79ffba20ce15965a7acfa9/lib/node_modules/@stdlib/simulate/iter/periodic-sinc/docs/img/equation_periodic_sinc.svg" alt="Periodic sinc function.">
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<!-- </equation> -->
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<!-- <equation class="equation" label="eq:periodic_sinc_substitution_odd" align="center" raw="x = \frac{2\pi (t-\varphi)}{\tau}" alt="Periodic sinc function substitution for odd N."> -->
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<div class="equation" align="center" data-raw-text="x = \frac{2\pi (t-\varphi)}{\tau}" data-equation="eq:periodic_sinc_substitution_odd">
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```math
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x = \frac{2\pi (t-\varphi)}{\tau}
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```
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<!-- <div class="equation" align="center" data-raw-text="x = \frac{2\pi (t-\varphi)}{\tau}" data-equation="eq:periodic_sinc_substitution_odd">
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<img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@d985bb501380970d8c79ffba20ce15965a7acfa9/lib/node_modules/@stdlib/simulate/iter/periodic-sinc/docs/img/equation_periodic_sinc_substitution_odd.svg" alt="Periodic sinc function substitution for odd N.">
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<br>
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</div> -->
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<!-- </equation> -->
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and, for even `N`, let
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<!-- <equation class="equation" label="eq:periodic_sinc_substitution_even" align="center" raw="x = \frac{4\pi (t-\varphi)}{\tau}" alt="Periodic sinc function substitution for even N."> -->
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<div class="equation" align="center" data-raw-text="x = \frac{4\pi (t-\varphi)}{\tau}" data-equation="eq:periodic_sinc_substitution_even">
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```math
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x = \frac{4\pi (t-\varphi)}{\tau}
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```
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<!-- <div class="equation" align="center" data-raw-text="x = \frac{4\pi (t-\varphi)}{\tau}" data-equation="eq:periodic_sinc_substitution_even">
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<img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@d985bb501380970d8c79ffba20ce15965a7acfa9/lib/node_modules/@stdlib/simulate/iter/periodic-sinc/docs/img/equation_periodic_sinc_substitution_even.svg" alt="Periodic sinc function substitution for even N.">
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</div> -->
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<!-- </equation> -->
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where `τ` is the period (i.e., the number of iterations until a waveform repeats) and `φ` is the phase (iteration) offset. For odd `N`, we can thus substitute and express the periodic [sinc][@stdlib/math/base/special/sinc] function as
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<!-- <equation class="equation" label="eq:periodic_sinc_in_terms_of_period" align="center" raw="D_N(t; A, \tau, \varphi) = \begin{cases}\frac{A\sin(N\pi(t-\varphi)/\tau)} {N\sin(\pi (t-\varphi)/\tau)} & t-\varphi \neq \tau k\ \textrm{for}\ k = 0, \pm 1, \pm 2, \ldots \\ A (-1)^{k(N-1)} & t-\varphi = \tau k\ \textrm{for}\ k = 0, \pm 1, \pm 2, \ldots \end{cases}" alt="Periodic sinc function as a function of the waveform period."> -->
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<div class="equation" align="center" data-raw-text="D_N(t; A, \tau, \varphi) = \begin{cases}\frac{A\sin(N\pi(t-\varphi)/\tau)} {N\sin(\pi (t-\varphi)/\tau)} &amp; t-\varphi \neq \tau k\ \textrm{for}\ k = 0, \pm 1, \pm 2, \ldots \\ A (-1)^{k(N-1)} &amp; t-\varphi = \tau k\ \textrm{for}\ k = 0, \pm 1, \pm 2, \ldots \end{cases}" data-equation="eq:periodic_sinc_in_terms_of_period">
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```math
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D_N(t; A, \tau, \varphi) = \begin{cases}\frac{A\sin(N\pi(t-\varphi)/\tau)} {N\sin(\pi (t-\varphi)/\tau)} & t-\varphi \neq \tau k\ \textrm{for}\ k = 0, \pm 1, \pm 2, \ldots \\ A (-1)^{k(N-1)} & t-\varphi = \tau k\ \textrm{for}\ k = 0, \pm 1, \pm 2, \ldots \end{cases}
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```
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<!-- <div class="equation" align="center" data-raw-text="D_N(t; A, \tau, \varphi) = \begin{cases}\frac{A\sin(N\pi(t-\varphi)/\tau)} {N\sin(\pi (t-\varphi)/\tau)} &amp; t-\varphi \neq \tau k\ \textrm{for}\ k = 0, \pm 1, \pm 2, \ldots \\ A (-1)^{k(N-1)} &amp; t-\varphi = \tau k\ \textrm{for}\ k = 0, \pm 1, \pm 2, \ldots \end{cases}" data-equation="eq:periodic_sinc_in_terms_of_period">
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<img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@d985bb501380970d8c79ffba20ce15965a7acfa9/lib/node_modules/@stdlib/simulate/iter/periodic-sinc/docs/img/equation_periodic_sinc_in_terms_of_period.svg" alt="Periodic sinc function as a function of the waveform period.">
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<!-- </equation> -->
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<!-- <equation class="equation" label="eq:periodic_sinc_in_terms_of_sinc_function" align="center" raw="D_N(\pi x; N, A) = A \cdot \frac{\operatorname{sinc}(Nx/2)} {\operatorname{sinc}(x/2)}" alt="Periodic sinc function in terms of the sinc function."> -->
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<div class="equation" align="center" data-raw-text="D_N(\pi x; N, A) = A \cdot \frac{\operatorname{sinc}(Nx/2)} {\operatorname{sinc}(x/2)}" data-equation="eq:periodic_sinc_in_terms_of_sinc_function">
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```math
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D_N(\pi x; N, A) = A \cdot \frac{\operatorname{sinc}(Nx/2)} {\operatorname{sinc}(x/2)}
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```
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<!-- <div class="equation" align="center" data-raw-text="D_N(\pi x; N, A) = A \cdot \frac{\operatorname{sinc}(Nx/2)} {\operatorname{sinc}(x/2)}" data-equation="eq:periodic_sinc_in_terms_of_sinc_function">
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<img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@d985bb501380970d8c79ffba20ce15965a7acfa9/lib/node_modules/@stdlib/simulate/iter/periodic-sinc/docs/img/equation_periodic_sinc_in_terms_of_sinc_function.svg" alt="Periodic sinc function in terms of the sinc function.">
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<!-- </equation> -->
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‎lib/node_modules/@stdlib/simulate/iter/pulse/README.md‎

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<!-- <equation class="equation" label="eq:pulse_waveform" align="center" raw="f(t; T, \tau, a_{\textrm{min}}, a_{\textrm{max}}, \varphi) = \begin{cases} a_{\textrm{max}} & (t-\varphi) \mod T < \tau \\ a_{\textrm{min}} & \textrm{otherwise} \end{cases}" alt="Equation for a pulse wave."> -->
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<div class="equation" align="center" data-raw-text="f(t; T, \tau, a_{\textrm{min}}, a_{\textrm{max}}, \varphi) = \begin{cases} a_{\textrm{max}} &amp; (t-\varphi) \mod T < \tau \\ a_{\textrm{min}} &amp; \textrm{otherwise} \end{cases}" data-equation="eq:pulse_waveform">
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```math
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f(t; T, \tau, a_{\textrm{min}}, a_{\textrm{max}}, \varphi) = \begin{cases} a_{\textrm{max}} & (t-\varphi) \mod T < \tau \\ a_{\textrm{min}} & \textrm{otherwise} \end{cases}
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```
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<!-- <div class="equation" align="center" data-raw-text="f(t; T, \tau, a_{\textrm{min}}, a_{\textrm{max}}, \varphi) = \begin{cases} a_{\textrm{max}} &amp; (t-\varphi) \mod T < \tau \\ a_{\textrm{min}} &amp; \textrm{otherwise} \end{cases}" data-equation="eq:pulse_waveform">
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<img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@36d0ed92c4707f9bb44e4a6fde78f19f6f28762e/lib/node_modules/@stdlib/simulate/iter/pulse/docs/img/equation_pulse_waveform.svg" alt="Equation for a pulse wave.">
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<br>
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</div>
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</div> -->
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<!-- </equation> -->
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‎lib/node_modules/@stdlib/simulate/iter/sawtooth-wave/README.md‎

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<!-- <equation class="equation" label="eq:sawtooth_waveform" align="center" raw="f(t; \tau, a, \varphi) = \frac{2a}{\pi} \operatorname{arctan} \tan \frac{\pi(t-\varphi)}{\tau}" alt="Equation for a sawtooth waveform."> -->
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<div class="equation" align="center" data-raw-text="f(t; \tau, a, \varphi) = \frac{2a}{\pi} \operatorname{arctan} \tan \frac{\pi(t-\varphi)}{\tau}" data-equation="eq:sawtooth_waveform">
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```math
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f(t; \tau, a, \varphi) = \frac{2a}{\pi} \operatorname{arctan} \tan \frac{\pi(t-\varphi)}{\tau}
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```
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<!-- <div class="equation" align="center" data-raw-text="f(t; \tau, a, \varphi) = \frac{2a}{\pi} \operatorname{arctan} \tan \frac{\pi(t-\varphi)}{\tau}" data-equation="eq:sawtooth_waveform">
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<img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@5827c258000edcb03496265cdfd372d686b4c656/lib/node_modules/@stdlib/simulate/iter/sawtooth-wave/docs/img/equation_sawtooth_waveform.svg" alt="Equation for a sawtooth waveform.">
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<br>
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<!-- </equation> -->
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