Update equation src URLs

Author: kgryte

lib/node_modules/@stdlib/constants/float64/apery/README.md

@@ -29,7 +29,7 @@ limitations under the License.
 <!-- <equation class="equation" label="eq:apery_constant" align="center" raw="\zeta(3) = \sum_{n=1}^\infty \frac{1}{n^3} = \lim_{n\to\infty} \biggl(\frac{1}{1^3} + \frac{1}{2^3} + \cdots + \frac{1}{n^3}\biggr)" alt="Apéry's constant"> -->
 
 <div class="equation" align="center" data-raw-text="\zeta(3) = \sum_{n=1}^\infty \frac{1}{n^3} = \lim_{n\to\infty} \biggl(\frac{1}{1^3} + \frac{1}{2^3} + \cdots + \frac{1}{n^3}\biggr)" data-equation="eq:apery_constant">
-    <img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@7e0a95722efd9c771b129597380c63dc6715508b/lib/node_modules/@stdlib/constants/float64/apery/docs/img/equation_apery_constant.svg" alt="Apéry's constant">
+    <img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@5d87cc7cb2c58aeb732872f89562d2c89571cc8a/lib/node_modules/@stdlib/constants/float64/apery/docs/img/equation_apery_constant.svg" alt="Apéry's constant">
     <br>
 </div>
 

lib/node_modules/@stdlib/constants/float64/phi/README.md

@@ -29,7 +29,7 @@ The [golden ratio][phi] can be defined algebraically as
 <!-- <equation class="equation" label="eq:golden_ratio" align="center" raw="\phi = \frac{1 + \sqrt{5}}{2}" alt="Golden ratio"> -->
 
 <div class="equation" align="center" data-raw-text="\phi = \frac{1 + \sqrt{5}}{2}" data-equation="eq:golden_ratio">
-    <img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@7e0a95722efd9c771b129597380c63dc6715508b/lib/node_modules/@stdlib/constants/float64/phi/docs/img/equation_golden_ratio.svg" alt="Golden ratio">
+    <img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@5d87cc7cb2c58aeb732872f89562d2c89571cc8a/lib/node_modules/@stdlib/constants/float64/phi/docs/img/equation_golden_ratio.svg" alt="Golden ratio">
     <br>
 </div>
 

lib/node_modules/@stdlib/simulate/iter/dirac-comb/README.md

@@ -31,7 +31,7 @@ A Dirac comb is represented by the following equation
 <!-- <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."> -->
 
 <div class="equation" align="center" data-raw-text="f(t; T, \varphi) = \delta((t-\varphi) \bmod T)" data-equation="eq:dirac_comb">
-    <img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@5827c258000edcb03496265cdfd372d686b4c656/lib/node_modules/@stdlib/simulate/iter/dirac-comb/docs/img/equation_dirac_comb.svg" alt="Equation for a Dirac comb.">
+    <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.">
     <br>
 </div>
 

lib/node_modules/@stdlib/simulate/iter/periodic-sinc/README.md

@@ -31,7 +31,7 @@ The periodic [sinc][@stdlib/math/base/special/sinc] function, also known as the
 <!-- <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."> -->
 
 <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">
-    <img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@5827c258000edcb03496265cdfd372d686b4c656/lib/node_modules/@stdlib/simulate/iter/periodic-sinc/docs/img/equation_periodic_sinc.svg" alt="Periodic sinc function.">
+    <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.">
     <br>
 </div>
 
@@ -44,7 +44,7 @@ To express the periodic [sinc][@stdlib/math/base/special/sinc] function as a fun
 <!-- <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."> -->
 
 <div class="equation" align="center" data-raw-text="x = \frac{2\pi (t-\varphi)}{\tau}" data-equation="eq:periodic_sinc_substitution_odd">
-    <img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@5827c258000edcb03496265cdfd372d686b4c656/lib/node_modules/@stdlib/simulate/iter/periodic-sinc/docs/img/equation_periodic_sinc_substitution_odd.svg" alt="Periodic sinc function substitution for odd N.">
+    <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.">
     <br>
 </div>
 
@@ -55,7 +55,7 @@ and, for even `N`, let
 <!-- <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."> -->
 
 <div class="equation" align="center" data-raw-text="x = \frac{4\pi (t-\varphi)}{\tau}" data-equation="eq:periodic_sinc_substitution_even">
-    <img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@5827c258000edcb03496265cdfd372d686b4c656/lib/node_modules/@stdlib/simulate/iter/periodic-sinc/docs/img/equation_periodic_sinc_substitution_even.svg" alt="Periodic sinc function substitution for even N.">
+    <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.">
     <br>
 </div>
 
@@ -66,7 +66,7 @@ where `τ` is the period (i.e., the number of iterations until a waveform repeat
 <!-- <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."> -->
 
 <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">
-    <img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@5827c258000edcb03496265cdfd372d686b4c656/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.">
+    <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.">
     <br>
 </div>
 
@@ -79,7 +79,7 @@ Note that the periodic [sinc][@stdlib/math/base/special/sinc] can be equivalentl
 <!-- <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."> -->
 
 <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">
-    <img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@5827c258000edcb03496265cdfd372d686b4c656/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.">
+    <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.">
     <br>
 </div>
 

lib/node_modules/@stdlib/simulate/iter/pulse/README.md

@@ -31,7 +31,7 @@ A pulse waveform is represented by the following equation
 <!-- <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."> -->
 
 <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">
-    <img src="https://cdn.jsdelivr.net/gh/stdlib-js/stdlib@5827c258000edcb03496265cdfd372d686b4c656/lib/node_modules/@stdlib/simulate/iter/pulse-wave/docs/img/equation_pulse_waveform.svg" alt="Equation for a pulse wave.">
+    <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.">
     <br>
 </div>