Notation Update (#15)

* Changed DTFT notation: (\mathrm{e}^{\mathrm{j}\Omega}) to (\Omega)

* also updated for stft and fir filter

filter_design/fir_filter.ipynb

@@ -391,18 +391,18 @@
     "An FIR filter $h[k]$ is used for convolution (i.e. filtering process)\n",
     "\n",
     "\\begin{align}\n",
-    "x[k] \\ast h[k] \\circ-\\bullet X(\\mathrm{e}^{\\mathrm{j}\\Omega}) \\cdot H(\\mathrm{e}^{\\mathrm{j}\\Omega}),\n",
+    "x[k] \\ast h[k] \\circ-\\bullet X(\\Omega) \\cdot H(\\Omega),\n",
     "\\end{align}\n",
     "\n",
     "whereas the DFT windowing process involves a multiplication with a window $w[k]$\n",
     "\n",
     "\\begin{align}\n",
-    "x[k] \\cdot w[k] \\circ-\\bullet \\frac{1}{2\\pi} X(\\mathrm{e}^{\\mathrm{j}\\Omega}) \\circledast_{2\\pi} W(\\mathrm{e}^{\\mathrm{j}\\Omega}).\n",
+    "x[k] \\cdot w[k] \\circ-\\bullet \\frac{1}{2\\pi} X(\\Omega) \\circledast_{2\\pi} W(\\Omega).\n",
     "\\end{align}\n",
     "\n",
     "In the DTFT domain this results in multiplication and circular convolution, respectively.\n",
     "\n",
-    "So, for the finite-length sequences $h[k]$ and $w[k]$ the same design fundamentals hold: we must put zeros at suitable locations in the z-plane to realize a certain desired DTFT spectrum, either $H(\\mathrm{e}^{\\mathrm{j}\\Omega})$ or $W(\\mathrm{e}^{\\mathrm{j}\\Omega})$. Depending on the application, filtering or windowing, the DTFT design criteria might be very different, since the DTFT spectrum acts as multiplication or convolution onto the input signal's DTFT spectrum. However, the design concepts and algorithms itself are basically the same, this is sometimes not so obvious in textbooks. "
+    "So, for the finite-length sequences $h[k]$ and $w[k]$ the same design fundamentals hold: we must put zeros at suitable locations in the z-plane to realize a certain desired DTFT spectrum, either $H(\\Omega)$ or $W(\\Omega)$. Depending on the application, filtering or windowing, the DTFT design criteria might be very different, since the DTFT spectrum acts as multiplication or convolution onto the input signal's DTFT spectrum. However, the design concepts and algorithms itself are basically the same, this is sometimes not so obvious in textbooks. "
    ]
   },
   {
@@ -435,13 +435,13 @@
     "The squared magnitude response can be given analytically as (try yourself, make use of $\\mathrm{e}^{-\\mathrm{j}\\Omega}=\\cos(\\Omega)-\\mathrm{j}\\sin(\\Omega)$ ) \n",
     "\n",
     "\\begin{equation}\n",
-    "|H(\\mathrm{e}^{\\mathrm{j}\\Omega})|^2 = |1 + \\mathrm{e}^{-\\mathrm{j}\\Omega}|^2 = 2 \\cos(\\Omega) + 2 = 4 \\cos^2(\\frac{\\Omega}{2}).\n",
+    "|H(\\Omega)|^2 = |1 + \\mathrm{e}^{-\\mathrm{j}\\Omega}|^2 = 2 \\cos(\\Omega) + 2 = 4 \\cos^2(\\frac{\\Omega}{2}).\n",
     "\\end{equation}\n",
     "\n",
     "Thus the magnitude response is \n",
     "\n",
     "\\begin{equation}\n",
-    "|H(\\mathrm{e}^{\\mathrm{j}\\Omega})| = 2 |\\cos(\\frac{\\Omega}{2})|,\n",
+    "|H(\\Omega)| = 2 |\\cos(\\frac{\\Omega}{2})|,\n",
     "\\end{equation}\n",
     "\n",
     "which is confirmed by the below plot (left, top). The magnitude response exhibits lowpass characteristics.\n",
@@ -484,11 +484,11 @@
     "## Example FIR M=1, b0=1, b1=-1\n",
     "\n",
     "\\begin{equation}\n",
-    "|H(\\mathrm{e}^{\\mathrm{j}\\Omega})|^2 = 4 \\sin^2(\\frac{\\Omega}{2}).\n",
+    "|H(\\Omega)|^2 = 4 \\sin^2(\\frac{\\Omega}{2}).\n",
     "\\end{equation}\n",
     "\n",
     "\\begin{equation}\n",
-    "|H(\\mathrm{e}^{\\mathrm{j}\\Omega})| = 2 |\\sin(\\frac{\\Omega}{2})|.\n",
+    "|H(\\Omega)| = 2 |\\sin(\\frac{\\Omega}{2})|.\n",
     "\\end{equation}\n",
     "\n",
     "$z_{\\infty,1}=0$,\n",
@@ -521,11 +521,11 @@
     "Filter order $M=2$, number of coefficients $M+1=3$, although one coefficient is zero, namely $b_1=0$.\n",
     "\n",
     "\\begin{equation}\n",
-    "|H(\\mathrm{e}^{\\mathrm{j}\\Omega})|^2 = 4 \\cos^2(\\Omega).\n",
+    "|H(\\Omega)|^2 = 4 \\cos^2(\\Omega).\n",
     "\\end{equation}\n",
     "\n",
     "\\begin{equation}\n",
-    "|H(\\mathrm{e}^{\\mathrm{j}\\Omega})| = 2 |\\cos(\\Omega)|.\n",
+    "|H(\\Omega)| = 2 |\\cos(\\Omega)|.\n",
     "\\end{equation}\n",
     "\n",
     "double pole in origin $z_{\\infty,1,2}=0$\n",
@@ -559,11 +559,11 @@
     "Filter order $M=2$, number of coefficients $M+1=3$, although one coefficient is zero, namely $b_1=0$.\n",
     "\n",
     "\\begin{equation}\n",
-    "|H(\\mathrm{e}^{\\mathrm{j}\\Omega})|^2 = 4 \\sin^2(\\Omega).\n",
+    "|H(\\Omega)|^2 = 4 \\sin^2(\\Omega).\n",
     "\\end{equation}\n",
     "\n",
     "\\begin{equation}\n",
-    "|H(\\mathrm{e}^{\\mathrm{j}\\Omega})| = 2 |\\sin(\\Omega)|.\n",
+    "|H(\\Omega)| = 2 |\\sin(\\Omega)|.\n",
     "\\end{equation}\n",
     "\n",
     "double pole in origin $z_{\\infty,1,2}=0$\n",
@@ -599,11 +599,11 @@
     "The manual derivation of analytic magnitude response starts to get tedious, however:\n",
     "\n",
     "\\begin{equation}\n",
-    "|H(\\mathrm{e}^{\\mathrm{j}\\Omega})|^2 = 16 \\cos^4(\\Omega).\n",
+    "|H(\\Omega)|^2 = 16 \\cos^4(\\Omega).\n",
     "\\end{equation}\n",
     "\n",
     "\\begin{equation}\n",
-    "|H(\\mathrm{e}^{\\mathrm{j}\\Omega})| = 4 \\cos^2(\\Omega).\n",
+    "|H(\\Omega)| = 4 \\cos^2(\\Omega).\n",
     "\\end{equation}\n",
     "\n",
     "double pole in origin $z_{\\infty,1,2}=0$\n",
@@ -639,11 +639,11 @@
     "Filter order $M=2$, number of coefficients $M+1=3$.\n",
     "\n",
     "\\begin{equation}\n",
-    "|H(\\mathrm{e}^{\\mathrm{j}\\Omega})|^2 = 16 \\sin^4(\\Omega).\n",
+    "|H(\\Omega)|^2 = 16 \\sin^4(\\Omega).\n",
     "\\end{equation}\n",
     "\n",
     "\\begin{equation}\n",
-    "|H(\\mathrm{e}^{\\mathrm{j}\\Omega})| = 4 \\sin^2(\\Omega).\n",
+    "|H(\\Omega)| = 4 \\sin^2(\\Omega).\n",
     "\\end{equation}\n",
     "\n",
     "double pole in origin $z_{\\infty,1,2}=0$\n",
@@ -798,10 +798,10 @@
     "A linear-phase FIR filter exhibits the DTFT spectrum\n",
     "\n",
     "\\begin{equation}\n",
-    "H(\\mathrm{e}^{\\mathrm{j}\\Omega}) = A(\\mathrm{e}^{\\mathrm{j}\\Omega})\\,\\mathrm{e}^{-\\mathrm{j}\\,\\alpha\\,\\Omega}\\,\\mathrm{e}^{\\mathrm{j}\\,\\beta}\n",
+    "H(\\Omega) = A(\\Omega)\\,\\mathrm{e}^{-\\mathrm{j}\\,\\alpha\\,\\Omega}\\,\\mathrm{e}^{\\mathrm{j}\\,\\beta}\n",
     "\\end{equation}\n",
     "\n",
-    "with the magnitude spectrum $A(\\mathrm{e}^{\\mathrm{j}\\Omega})\\in\\mathbb{R}$ and the phase $\\mathrm{e}^{-\\mathrm{j}\\,\\alpha\\,\\Omega}\\,\\mathrm{e}^{\\mathrm{j}\\,\\beta}$ with $\\alpha,\\beta\\in\\mathbb{R}^+$.\n",
+    "with the magnitude spectrum $A(\\Omega)\\in\\mathbb{R}$ and the phase $\\mathrm{e}^{-\\mathrm{j}\\,\\alpha\\,\\Omega}\\,\\mathrm{e}^{\\mathrm{j}\\,\\beta}$ with $\\alpha,\\beta\\in\\mathbb{R}^+$.\n",
     "\n",
     "There are four different basic types of linear-phase FIR filters that differ by the symmetry of the impulse response and the length of the finite impulse response.\n",
     "\n",