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        <title>Kollektanee - Samuel Gyger - topic:qm</title>
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       <dc:date>2026-07-26T07:23:02+00:00</dc:date>
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        <title>Kollektanee - Samuel Gyger</title>
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        <dc:date>2023-02-15T18:56:35+00:00</dc:date>
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        <title>density-matrix</title>
        <link>https://wiki.gyger.at/topic:qm:density-matrix?rev=1676487395&amp;do=diff</link>
        <description>Density Operator (matrix)

While a system state in quantum mechanics can be described by its state vector $\ket{\psi}$, 
it can also be described by a so called density operator $\rho$.

We define the density operator to be a positive operator $\rho$ with a trace equal to one ($\tr{\rho} = 1$$\rho$$\rho_i$$p_i$$\sum_i{p_i \rho_i}$$\rho$$t_1$$\rho&#039;$$t_2$$U$$t_1$$t_2$$$\rho&#039; = U \rho U^\dagger$$$\tr(\rho^2) &lt;= 1$$\rho$$\tr(\rho^2) == 1$$$ \rho = \sum_i p_i{\ket{\psi_i}\bra{\psi_i}} $$</description>
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        <dc:date>2023-02-15T18:37:40+00:00</dc:date>
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        <title>measurements</title>
        <link>https://wiki.gyger.at/topic:qm:measurements?rev=1676486260&amp;do=diff</link>
        <description>Quantum measurements

From the general postulates by Nielsen and Chuang, 3 talks about measurements.

Quantum measurements are described by a collection ${M_m}$ of measurement operators. 
These are operators acting on the state space of the system being measured. 
The index $m$$\ket{\psi}$$m$$$p(m) = \Braket{\psi | M_m^\dag M_m | \psi}$$$$\frac{M_m \ket{\psi}}{\sqrt{\Braket{\psi | M_m^\dag M_m | \psi}}}.$$$p(m)$$1$$$\sum_m{M_m^\dag M_m} = I$$$M$$ M = \sum_m m P_m $$P_m$$M$$m$$m$$m$$$p(m) = \Brak…</description>
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        <dc:date>2022-12-14T22:19:16+00:00</dc:date>
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        <title>nok</title>
        <link>https://wiki.gyger.at/topic:qm:nok?rev=1671056356&amp;do=diff</link>
        <description>Nuggets of Knowledge (NoK)

Werner State

A mixture of (1-a):a of the Bell State $\ket{\Phi^+}$ and a fully mixed state is called the Werner state.\cite{Werner:1989}
$$
\begin{aligned}
\rho &amp; =\frac{1-a}{2}(\ket{00}+\ket{11})(\bra{00}+\bra{11})+\frac{a}{4} I \\
&amp; =\frac{1}{2}\left(\begin{array}{cccc}
1-a / 2 &amp; 0 &amp; 0 &amp; 1-a \\
0 &amp; a / 2 &amp; 0 &amp; 0 \\
0 &amp; 0 &amp; a / 2 &amp; 0 \\
1-a &amp; 0 &amp; 0 &amp; 1-a / 2
\end{array}\right) .
\end{aligned}
$$</description>
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        <dc:date>2023-02-15T18:26:39+00:00</dc:date>
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        <title>postulates</title>
        <link>https://wiki.gyger.at/topic:qm:postulates?rev=1676485599&amp;do=diff</link>
        <description>Postulates of Quantum Mechanics

This follows (verbatim) the Postulates as written in \cite{Nielsen.Chuang:2010}.

Four postulates are defined to outline the space quantum mechanics exists in. 1., describes the state of a closed system. 2. describes the evolution of such system in time. 3. describes the influence of observations or information gathering from such a system and 4. defines how multiple systems can be combined.$\ket{\psi}$$\ket{\psi&#039;}$$\ket{\psi&#039;} = U \ket{\psi}$$$ i\hbar \partial_t…</description>
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