Undergrad Unitary Time Evolution: Explaining Open Quantum Systems

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Unitary time evolution applies to closed quantum systems, ensuring the total probability remains 1. In contrast, open quantum systems cannot generally be described by unitary evolution due to their interaction with the environment. The density matrix for an open system, while maintaining the trace condition, does not evolve unitarily after tracing out environmental degrees of freedom. This leads to a situation where the total density matrix may evolve unitarily, but the reduced density matrix for the system does not. The collapse interpretation further complicates this, as it involves non-invertible processes that preserve the trace condition but do not adhere to unitary evolution principles.
jamie.j1989
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Hi, I am a bit confused about unitary time evolution, I understand that a closed quantum system can be explained by unitary time evolution which ensures that the probability of all possible outcomes is always 1. But for an open quantum system we can't in general explain it with a unitary time evolution. This is where I get confused, we explain the evolution of an open quantum systems with the density matrix ##\rho(t)##, which must always satisfy ##Tr[\rho(t)]=1##, so my question is, how is this not unitary time evolution? Thanks.
 
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The density matrix may refer to the state of the system+environment which we expect to have a unitary evolution. But when we trace out the environmental degrees of freedom, we are left with a density matrix which describes what we should expect if we have don't have access to the environmental degrees the freedom. So ## \rho_{total} ## has a unitary evolution but ## \rho_{system}=Tr_{environment}(\rho_{total}) ## doesn't!
 
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More often than not open system measurements are described by the Copenhagen/Collapse Interpretation. Collapse is not invertible let alone unitary.
 
Collapse preserves the condition ##\mbox{Tr}~ \rho=1##. This is a much weaker condition than nitarity, which says that ##\rho(t)=U(t)\rho(0)U(t)^*## with a unitary ##U(t)##.
 
A. Neumaier said:
Collapse preserves the condition ##\mbox{Tr}~ \rho=1##. This is a much weaker condition than nitarity, which says that ##\rho(t)=U(t)\rho(0)U(t)^*## with a unitary ##U(t)##.

Indeed, ρ becomes the projection onto the collapsed eigenvector.
 
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