update week 1

Author: mhjensen

doc/pub/week1/html/week1-bs.html

@@ -1593,8 +1593,6 @@ <h2 id="exercise-2-entangled-state" class="anchor">Exercise 2: Entangled state
 
 <p>Show that the state \( \alpha \vert 00\rangle+\beta\vert 11\rangle \) cannot be written as the product of the tensor product of two states and is thus entangle. The constants  \( \alpha \) and \( \beta \) are both nonzero.</p>
 
-<p>Write a function which sets up a one-qubit basis and apply the various Pauli matrices to these basis states.</p>
-
 <!-- !split -->
 <h2 id="exercise-3-commutator-identities" class="anchor">Exercise 3: Commutator identities  </h2>
 <p>Prove the following commutator relations for different operators (marked with a hat)</p>
@@ -1605,6 +1603,7 @@ <h2 id="exercise-3-commutator-identities" class="anchor">Exercise 3: Commutator
 </ol>
 <!-- !split -->
 <h2 id="exercise-4-shared-eigenvectors" class="anchor">Exercise 4: Shared eigenvectors </h2>
+
 <p>Prove that if two operators \( \hat{A} \) and \( \hat{B} \) commute they will share a basis of eigenstates</p>
 
 <!-- !split -->

doc/pub/week1/html/week1-reveal.html

@@ -1696,8 +1696,6 @@ <h2 id="and-the-next-two">And the next two  </h2>
 <h2 id="exercise-2-entangled-state">Exercise 2: Entangled state  </h2>
 
 <p>Show that the state \( \alpha \vert 00\rangle+\beta\vert 11\rangle \) cannot be written as the product of the tensor product of two states and is thus entangle. The constants  \( \alpha \) and \( \beta \) are both nonzero.</p>
-
-<p>Write a function which sets up a one-qubit basis and apply the various Pauli matrices to these basis states.</p>
 </section>
 
 <section>
@@ -1712,6 +1710,7 @@ <h2 id="exercise-3-commutator-identities">Exercise 3: Commutator identities  </h
 
 <section>
 <h2 id="exercise-4-shared-eigenvectors">Exercise 4: Shared eigenvectors </h2>
+
 <p>Prove that if two operators \( \hat{A} \) and \( \hat{B} \) commute they will share a basis of eigenstates</p>
 </section>
 

doc/pub/week1/html/week1-solarized.html

@@ -1506,8 +1506,6 @@ <h2 id="exercise-2-entangled-state">Exercise 2: Entangled state  </h2>
 
 <p>Show that the state \( \alpha \vert 00\rangle+\beta\vert 11\rangle \) cannot be written as the product of the tensor product of two states and is thus entangle. The constants  \( \alpha \) and \( \beta \) are both nonzero.</p>
 
-<p>Write a function which sets up a one-qubit basis and apply the various Pauli matrices to these basis states.</p>
-
 <!-- !split --><br><br><br><br><br><br><br><br><br><br>
 <h2 id="exercise-3-commutator-identities">Exercise 3: Commutator identities  </h2>
 <p>Prove the following commutator relations for different operators (marked with a hat)</p>
@@ -1518,6 +1516,7 @@ <h2 id="exercise-3-commutator-identities">Exercise 3: Commutator identities  </h
 </ol>
 <!-- !split --><br><br><br><br><br><br><br><br><br><br>
 <h2 id="exercise-4-shared-eigenvectors">Exercise 4: Shared eigenvectors </h2>
+
 <p>Prove that if two operators \( \hat{A} \) and \( \hat{B} \) commute they will share a basis of eigenstates</p>
 
 <!-- !split --><br><br><br><br><br><br><br><br><br><br>

doc/pub/week1/html/week1.html

@@ -1583,8 +1583,6 @@ <h2 id="exercise-2-entangled-state">Exercise 2: Entangled state  </h2>
 
 <p>Show that the state \( \alpha \vert 00\rangle+\beta\vert 11\rangle \) cannot be written as the product of the tensor product of two states and is thus entangle. The constants  \( \alpha \) and \( \beta \) are both nonzero.</p>
 
-<p>Write a function which sets up a one-qubit basis and apply the various Pauli matrices to these basis states.</p>
-
 <!-- !split --><br><br><br><br><br><br><br><br><br><br>
 <h2 id="exercise-3-commutator-identities">Exercise 3: Commutator identities  </h2>
 <p>Prove the following commutator relations for different operators (marked with a hat)</p>
@@ -1595,6 +1593,7 @@ <h2 id="exercise-3-commutator-identities">Exercise 3: Commutator identities  </h
 </ol>
 <!-- !split --><br><br><br><br><br><br><br><br><br><br>
 <h2 id="exercise-4-shared-eigenvectors">Exercise 4: Shared eigenvectors </h2>
+
 <p>Prove that if two operators \( \hat{A} \) and \( \hat{B} \) commute they will share a basis of eigenstates</p>
 
 <!-- !split --><br><br><br><br><br><br><br><br><br><br>