update

Author: mhjensen

doc/pub/week6/html/week6-bs.html

@@ -2132,7 +2132,7 @@ <h2 id="the-hamiltonian-in-terms-of-pauli-boldsymbol-x-and-pauli-boldsymbol-z-ma
 
 <p>with</p>
 $$
-\mathcal{H}_0=\epsilon_{II}\boldsymbol{I}\otimes\boldsymbol{I}+\epsilon_{ZI}\boldsymbol{Z}\otimes\boldsymbol{I}+\epsilon_{IZ}\boldsymbol{I}\otimes\boldsymbol{Z}+\epsilon_{II}+\epsilon_{ZZ}\boldsymbol{Z}\otimes\boldsymbol{Z},
+\mathcal{H}_0=\epsilon_{II}\boldsymbol{I}\otimes\boldsymbol{I}+\epsilon_{ZI}\boldsymbol{Z}\otimes\boldsymbol{I}+\epsilon_{IZ}\boldsymbol{I}\otimes\boldsymbol{Z}+\epsilon_{ZZ}\boldsymbol{Z}\otimes\boldsymbol{Z},
 $$
 
 <p>and</p>
@@ -2166,10 +2166,10 @@ <h2 id="explicit-expressions" class="anchor">Explicit expressions </h2>
 <p>In order to perform our measurements, will then need the following operators \( \boldsymbol{U} \)</p>
 $$
 \begin{align*}
-\boldsymbol{Z}\otimes\boldsymbol{I} & \boldsymbol{U}=\boldsymbol{I}\otimes\boldsymbol{I}\\
-\boldsymbol{I}\otimes\boldsymbol{Z} & \boldsymbol{U}=\text{SWAP}\\
-\boldsymbol{Z}\otimes\boldsymbol{Z} & \boldsymbol{U}=CX_{10}\\
-\boldsymbol{X}\otimes\boldsymbol{X} & \boldsymbol{U}=CX_{10}(\boldsymbol{H}\otimes\boldsymbol{H}\\
+\boldsymbol{Z}\otimes\boldsymbol{I}\hspace{1cm} & \boldsymbol{U}=\boldsymbol{I}\otimes\boldsymbol{I}\\
+\boldsymbol{I}\otimes\boldsymbol{Z}\hspace{1cm} & \boldsymbol{U}=\text{SWAP}\\
+\boldsymbol{Z}\otimes\boldsymbol{Z}\hspace{1cm} & \boldsymbol{U}=CX_{10}\\
+\boldsymbol{X}\otimes\boldsymbol{X}\hspace{1cm} & \boldsymbol{U}=CX_{10}(\boldsymbol{H}\otimes\boldsymbol{H})\\
 \end{align*}
 $$
 

doc/pub/week6/html/week6-reveal.html

@@ -2172,7 +2172,7 @@ <h2 id="the-hamiltonian-in-terms-of-pauli-boldsymbol-x-and-pauli-boldsymbol-z-ma
 <p>with</p>
 <p>&nbsp;<br>
 $$
-\mathcal{H}_0=\epsilon_{II}\boldsymbol{I}\otimes\boldsymbol{I}+\epsilon_{ZI}\boldsymbol{Z}\otimes\boldsymbol{I}+\epsilon_{IZ}\boldsymbol{I}\otimes\boldsymbol{Z}+\epsilon_{II}+\epsilon_{ZZ}\boldsymbol{Z}\otimes\boldsymbol{Z},
+\mathcal{H}_0=\epsilon_{II}\boldsymbol{I}\otimes\boldsymbol{I}+\epsilon_{ZI}\boldsymbol{Z}\otimes\boldsymbol{I}+\epsilon_{IZ}\boldsymbol{I}\otimes\boldsymbol{Z}+\epsilon_{ZZ}\boldsymbol{Z}\otimes\boldsymbol{Z},
 $$
 <p>&nbsp;<br>
 
@@ -2213,10 +2213,10 @@ <h2 id="explicit-expressions">Explicit expressions </h2>
 <p>&nbsp;<br>
 $$
 \begin{align*}
-\boldsymbol{Z}\otimes\boldsymbol{I} & \boldsymbol{U}=\boldsymbol{I}\otimes\boldsymbol{I}\\
-\boldsymbol{I}\otimes\boldsymbol{Z} & \boldsymbol{U}=\text{SWAP}\\
-\boldsymbol{Z}\otimes\boldsymbol{Z} & \boldsymbol{U}=CX_{10}\\
-\boldsymbol{X}\otimes\boldsymbol{X} & \boldsymbol{U}=CX_{10}(\boldsymbol{H}\otimes\boldsymbol{H}\\
+\boldsymbol{Z}\otimes\boldsymbol{I}\hspace{1cm} & \boldsymbol{U}=\boldsymbol{I}\otimes\boldsymbol{I}\\
+\boldsymbol{I}\otimes\boldsymbol{Z}\hspace{1cm} & \boldsymbol{U}=\text{SWAP}\\
+\boldsymbol{Z}\otimes\boldsymbol{Z}\hspace{1cm} & \boldsymbol{U}=CX_{10}\\
+\boldsymbol{X}\otimes\boldsymbol{X}\hspace{1cm} & \boldsymbol{U}=CX_{10}(\boldsymbol{H}\otimes\boldsymbol{H})\\
 \end{align*}
 $$
 <p>&nbsp;<br>

doc/pub/week6/html/week6-solarized.html

@@ -2051,7 +2051,7 @@ <h2 id="the-hamiltonian-in-terms-of-pauli-boldsymbol-x-and-pauli-boldsymbol-z-ma
 
 <p>with</p>
 $$
-\mathcal{H}_0=\epsilon_{II}\boldsymbol{I}\otimes\boldsymbol{I}+\epsilon_{ZI}\boldsymbol{Z}\otimes\boldsymbol{I}+\epsilon_{IZ}\boldsymbol{I}\otimes\boldsymbol{Z}+\epsilon_{II}+\epsilon_{ZZ}\boldsymbol{Z}\otimes\boldsymbol{Z},
+\mathcal{H}_0=\epsilon_{II}\boldsymbol{I}\otimes\boldsymbol{I}+\epsilon_{ZI}\boldsymbol{Z}\otimes\boldsymbol{I}+\epsilon_{IZ}\boldsymbol{I}\otimes\boldsymbol{Z}+\epsilon_{ZZ}\boldsymbol{Z}\otimes\boldsymbol{Z},
 $$
 
 <p>and</p>
@@ -2085,10 +2085,10 @@ <h2 id="explicit-expressions">Explicit expressions </h2>
 <p>In order to perform our measurements, will then need the following operators \( \boldsymbol{U} \)</p>
 $$
 \begin{align*}
-\boldsymbol{Z}\otimes\boldsymbol{I} & \boldsymbol{U}=\boldsymbol{I}\otimes\boldsymbol{I}\\
-\boldsymbol{I}\otimes\boldsymbol{Z} & \boldsymbol{U}=\text{SWAP}\\
-\boldsymbol{Z}\otimes\boldsymbol{Z} & \boldsymbol{U}=CX_{10}\\
-\boldsymbol{X}\otimes\boldsymbol{X} & \boldsymbol{U}=CX_{10}(\boldsymbol{H}\otimes\boldsymbol{H}\\
+\boldsymbol{Z}\otimes\boldsymbol{I}\hspace{1cm} & \boldsymbol{U}=\boldsymbol{I}\otimes\boldsymbol{I}\\
+\boldsymbol{I}\otimes\boldsymbol{Z}\hspace{1cm} & \boldsymbol{U}=\text{SWAP}\\
+\boldsymbol{Z}\otimes\boldsymbol{Z}\hspace{1cm} & \boldsymbol{U}=CX_{10}\\
+\boldsymbol{X}\otimes\boldsymbol{X}\hspace{1cm} & \boldsymbol{U}=CX_{10}(\boldsymbol{H}\otimes\boldsymbol{H})\\
 \end{align*}
 $$
 

doc/pub/week6/html/week6.html

@@ -2128,7 +2128,7 @@ <h2 id="the-hamiltonian-in-terms-of-pauli-boldsymbol-x-and-pauli-boldsymbol-z-ma
 
 <p>with</p>
 $$
-\mathcal{H}_0=\epsilon_{II}\boldsymbol{I}\otimes\boldsymbol{I}+\epsilon_{ZI}\boldsymbol{Z}\otimes\boldsymbol{I}+\epsilon_{IZ}\boldsymbol{I}\otimes\boldsymbol{Z}+\epsilon_{II}+\epsilon_{ZZ}\boldsymbol{Z}\otimes\boldsymbol{Z},
+\mathcal{H}_0=\epsilon_{II}\boldsymbol{I}\otimes\boldsymbol{I}+\epsilon_{ZI}\boldsymbol{Z}\otimes\boldsymbol{I}+\epsilon_{IZ}\boldsymbol{I}\otimes\boldsymbol{Z}+\epsilon_{ZZ}\boldsymbol{Z}\otimes\boldsymbol{Z},
 $$
 
 <p>and</p>
@@ -2162,10 +2162,10 @@ <h2 id="explicit-expressions">Explicit expressions </h2>
 <p>In order to perform our measurements, will then need the following operators \( \boldsymbol{U} \)</p>
 $$
 \begin{align*}
-\boldsymbol{Z}\otimes\boldsymbol{I} & \boldsymbol{U}=\boldsymbol{I}\otimes\boldsymbol{I}\\
-\boldsymbol{I}\otimes\boldsymbol{Z} & \boldsymbol{U}=\text{SWAP}\\
-\boldsymbol{Z}\otimes\boldsymbol{Z} & \boldsymbol{U}=CX_{10}\\
-\boldsymbol{X}\otimes\boldsymbol{X} & \boldsymbol{U}=CX_{10}(\boldsymbol{H}\otimes\boldsymbol{H}\\
+\boldsymbol{Z}\otimes\boldsymbol{I}\hspace{1cm} & \boldsymbol{U}=\boldsymbol{I}\otimes\boldsymbol{I}\\
+\boldsymbol{I}\otimes\boldsymbol{Z}\hspace{1cm} & \boldsymbol{U}=\text{SWAP}\\
+\boldsymbol{Z}\otimes\boldsymbol{Z}\hspace{1cm} & \boldsymbol{U}=CX_{10}\\
+\boldsymbol{X}\otimes\boldsymbol{X}\hspace{1cm} & \boldsymbol{U}=CX_{10}(\boldsymbol{H}\otimes\boldsymbol{H})\\
 \end{align*}
 $$