update

Author: mhjensen

doc/pub/week4/html/week4-bs.html

@@ -330,7 +330,7 @@ <h2 id="gates-the-whys-and-hows" class="anchor">Gates, the whys and hows </h2>
 <h2 id="structure-of-the-lecture" class="anchor">Structure of the lecture </h2>
 
 <ol>
-<li> First we review some of the basic ways of representing the solution to the Schr&#246;dinger equation, introducing the so-called Interaction, Heisenberg and Schr&#246;dinger prictures and unitary transformations. These material is meant mainly as background material</li>
+<li> First we review some of the basic ways of representing the solution to the Schr&#246;dinger equation, introducing the so-called Interaction, Heisenberg and Schr&#246;dinger prictures and unitary transformations. This part is meant mainly as background material</li>
 <li> Secondly, we present examples of physical processes and how they can be represented as unitary operations on a given state.</li>
 <li> These unitary transformations are then represented as gates. Setting gates together gives us a final circuit which can represent a specific physical system</li>
 </ol>

doc/pub/week4/html/week4-reveal.html

@@ -240,7 +240,7 @@ <h2 id="gates-the-whys-and-hows">Gates, the whys and hows </h2>
 <h2 id="structure-of-the-lecture">Structure of the lecture </h2>
 
 <ol>
-<p><li> First we review some of the basic ways of representing the solution to the Schr&#246;dinger equation, introducing the so-called Interaction, Heisenberg and Schr&#246;dinger prictures and unitary transformations. These material is meant mainly as background material</li>
+<p><li> First we review some of the basic ways of representing the solution to the Schr&#246;dinger equation, introducing the so-called Interaction, Heisenberg and Schr&#246;dinger prictures and unitary transformations. This part is meant mainly as background material</li>
 <p><li> Secondly, we present examples of physical processes and how they can be represented as unitary operations on a given state.</li>
 <p><li> These unitary transformations are then represented as gates. Setting gates together gives us a final circuit which can represent a specific physical system</li>
 </ol>

doc/pub/week4/html/week4-solarized.html

@@ -243,7 +243,7 @@ <h2 id="gates-the-whys-and-hows">Gates, the whys and hows </h2>
 <h2 id="structure-of-the-lecture">Structure of the lecture </h2>
 
 <ol>
-<li> First we review some of the basic ways of representing the solution to the Schr&#246;dinger equation, introducing the so-called Interaction, Heisenberg and Schr&#246;dinger prictures and unitary transformations. These material is meant mainly as background material</li>
+<li> First we review some of the basic ways of representing the solution to the Schr&#246;dinger equation, introducing the so-called Interaction, Heisenberg and Schr&#246;dinger prictures and unitary transformations. This part is meant mainly as background material</li>
 <li> Secondly, we present examples of physical processes and how they can be represented as unitary operations on a given state.</li>
 <li> These unitary transformations are then represented as gates. Setting gates together gives us a final circuit which can represent a specific physical system</li>
 </ol>

doc/pub/week4/html/week4.html

@@ -320,7 +320,7 @@ <h2 id="gates-the-whys-and-hows">Gates, the whys and hows </h2>
 <h2 id="structure-of-the-lecture">Structure of the lecture </h2>
 
 <ol>
-<li> First we review some of the basic ways of representing the solution to the Schr&#246;dinger equation, introducing the so-called Interaction, Heisenberg and Schr&#246;dinger prictures and unitary transformations. These material is meant mainly as background material</li>
+<li> First we review some of the basic ways of representing the solution to the Schr&#246;dinger equation, introducing the so-called Interaction, Heisenberg and Schr&#246;dinger prictures and unitary transformations. This part is meant mainly as background material</li>
 <li> Secondly, we present examples of physical processes and how they can be represented as unitary operations on a given state.</li>
 <li> These unitary transformations are then represented as gates. Setting gates together gives us a final circuit which can represent a specific physical system</li>
 </ol>