Manuscript Em05-A@1 · Em05-A-v1.tex · theorem · 9cac0def
Theorem: Exact marginal matrices and diagnostics
Excitation, coherence, and subsystem purity · lines 422–494 · proof included or linked
Em05-A@1#thm:marginals, Em05-A@1#eq:rhoR, Em05-A@1#eq:rhoE, Em05-A@1#eq:occupation, Em05-A@1#eq:coherence, Em05-A@1#eq:purity
In the declared occupation bases,
\rho_R=\mathcal N_\eta(\rho_M)
&=
\begin{pmatrix}
1-p+pt^2&0&0&\eta z\\
0&p\eta t&0&0\\
0&0&p\eta t&0\\
\eta z^*&0&0&p\eta^2
\end{pmatrix},
\label{eq:rhoR}\\
\rho_E=\mathcal C_\eta(\rho_M)
&=
\begin{pmatrix}
1-p+p\eta^2&0&0&t z\\
0&p\eta t&0&0\\
0&0&p\eta t&0\\
t z^*&0&0&pt^2
\end{pmatrix}.
\label{eq:rhoE}For
on the respective subsystems,
The distinguished occupation-basis coherences are
The accessible purity is
The residual purity follows by interchanging and .
Proof. Insert (eq:input) into the Kraus expressions. Only contributes the accessible coherence. For the complement, the only off-diagonal residual matrix units are and their adjoints, with coefficient . This gives (eq:rhoR) and (eq:rhoE).
Tracing either marginal against its number operator gives
The coherence formulas are their displayed entries. For a Hermitian matrix, . Applying this identity to (eq:rhoR) gives (eq:purity).
Displayed formulas in this passage
Em05-A@1#eq:rhoR · line 425
\rho_R=\mathcal N_\eta(\rho_M) &= \begin{pmatrix} 1-p+pt^2&0&0&\eta z\\ 0&p\eta t&0&0\\ 0&0&p\eta t&0\\ \eta z^*&0&0&p\eta^2 \end{pmatrix}, \label{eq:rhoR}\\ \rho_E=\mathcal C_\eta(\rho_M) &= \begin{pmatrix} 1-p+p\eta^2&0&0&t z\\ 0&p\eta t&0&0\\ 0&0&p\eta t&0\\ t z^*&0&0&pt^2 \end{pmatrix}. \label{eq:rhoE}Em05-A@1#eq:rhoE · line 425
\rho_R=\mathcal N_\eta(\rho_M) &= \begin{pmatrix} 1-p+pt^2&0&0&\eta z\\ 0&p\eta t&0&0\\ 0&0&p\eta t&0\\ \eta z^*&0&0&p\eta^2 \end{pmatrix}, \label{eq:rhoR}\\ \rho_E=\mathcal C_\eta(\rho_M) &= \begin{pmatrix} 1-p+p\eta^2&0&0&t z\\ 0&p\eta t&0&0\\ 0&0&p\eta t&0\\ t z^*&0&0&pt^2 \end{pmatrix}. \label{eq:rhoE}Em05-A@1#eq:occupation · line 450
Em05-A@1#eq:coherence · line 458
Em05-A@1#eq:purity · line 465
unlabeled · line 446
unlabeled · line 484