Partial trace and the reduced density matrix

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SUMMARY

The discussion focuses on the equation of motion for the reduced density matrix in the interaction picture, specifically addressing the trace paradox associated with the partial trace operation. The corrected LaTeX formula presented is: $$i \hbar \dot{\rho}_A (t) = Tr_B[V(t), \rho_{AB}(t)] = \Sigma_b \langle \phi_b | V \rho_{AB} -\rho_{AB} V | \phi_b \rangle$$. The resolution of the paradox lies in the non-cyclic nature of the partial trace. Additionally, a separate trace paradox involving the commutation of position and momentum operators is introduced, emphasizing the infinite nature of the trace of the identity operator.

PREREQUISITES
  • Understanding of quantum mechanics and the concept of density matrices.
  • Familiarity with the interaction picture in quantum mechanics.
  • Knowledge of the partial trace operation and its implications in quantum systems.
  • Basic understanding of operator commutation relations in quantum mechanics.
NEXT STEPS
  • Study the properties of the partial trace in quantum mechanics.
  • Explore the implications of non-cyclic traces in quantum systems.
  • Investigate the relationship between position and momentum operators, particularly in the context of trace operations.
  • Learn about the mathematical foundations of Hilbert spaces and their role in quantum mechanics.
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Quantum physicists, researchers in quantum information theory, and students studying advanced quantum mechanics concepts will benefit from this discussion.

yucheng
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TL;DR
Trace paradox?
From Rand Lectures on Light, we have, in the interaction picture, the equation of motion of the reduced density matrix:
$$i \hbar \rho \dot_A (t) = Tr_B[V(t), \rho_{AB}(t)] = \Sigma_b \langle \phi_b | V \rho_{AB} -\rho_{AB} V | \phi_b \rangle = \Sigma_b \phi_b | \langle V \rho_{AB} | \phi_b \rangle - \langle \phi_b| \rho_{AB} V | \phi_b \rangle = Tr_B(V \rho_AB) - Tr_B(\rho_AB V) = 0???$$
 
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yucheng said:
TL;DR Summary: Trace paradox?
I have corrected your LaTeX formula to make it readable and meaningful:
$$i \hbar \dot{\rho}_A (t) = Tr_B[V(t), \rho_{AB}(t)] = \Sigma_b \langle \phi_b | V \rho_{AB} -\rho_{AB} V | \phi_b \rangle $$
$$= \Sigma_b \langle\phi_b | V \rho_{AB} | \phi_b \rangle - \langle \phi_b| \rho_{AB} V | \phi_b \rangle = Tr_B(V \rho_{AB}) - Tr_B(\rho_{AB} V) = 0???$$
 
By the way, there is also another instructive trace paradox. Since ##[x,p]=i\hbar 1##, we have
$${\rm Tr} [x,p] ={\rm Tr}(i\hbar 1)=i\hbar {\rm Tr}1=i\hbar\infty$$
but also
$${\rm Tr} [x,p] ={\rm Tr} (xp) - {\rm Tr} (px) =0$$
so
$$0=i\hbar\infty$$
Can you resolve this one? :wink:

Hint: The solution of this paradox is entirely unrelated to the solution of the previous one. The key is to understand the meaning of ##{\rm Tr}1=\infty##, can we pretend that it is actually a big but finite number?
 
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@Demystifier
OMG I did not even realize it was published! I thought I just left it as a draft, but thanks for replying!

After doing some other problems, I realized that a partial trace is defined for a composite Hilbert space, which means that taking the trace with respect to the ##| b \rangle## basis breaks the common argument for commutation under the trace i,e, using the resolution of the identity because we have ##\Sigma \langle b' |\rho_{AB}| a,b \rangle \langle a,b| V |b' \rangle## instead.
 
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