Undergrad Coherence time for repeated spin measurements

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SUMMARY

The discussion centers on the coherence time for repeated spin measurements on the same electron, specifically how the correlation function C(t,0) evolves over time. For small time intervals (t), the correlation is maximal (C(t,0)=1), while for larger intervals, it approaches zero (C(t,0) -> 0). The coherence time, denoted as T_coh, plays a critical role in this decay, with the correlation function modeled as C(t,0) = e^[-t/T_coh]. The conversation also touches on the relevance of the Hamiltonian and density matrix in understanding these dynamics.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly spin measurements.
  • Familiarity with the concept of coherence time (T_coh) in quantum systems.
  • Knowledge of Hamiltonians and their role in quantum state evolution.
  • Basic grasp of density matrices and their application in quantum mechanics.
NEXT STEPS
  • Research the implications of coherence time (T_coh) in quantum computing applications.
  • Explore the role of Hamiltonians in modeling quantum noise and its effects on spin states.
  • Study the density matrix formalism and its application in predicting quantum behavior over time.
  • Investigate the relationship between spin measurements and Bell tests in quantum mechanics.
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Quantum physicists, researchers in quantum computing, and anyone studying the dynamics of quantum states and their measurement processes.

aa2ll2
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TL;DR
"What is the half life of the correlation between repeated spin measurements on the same electron?
Consider repeated spin measurements, along the same axis, on the same electron, at t=0 and at t=t. For small t, the results are identical, so the correlation function, C(t,0)=1, but for large t, C(t,0) -> 0.

Define C(t,0) = P(same) - P(different) = N(same) - N(different) / N(same) + N(different), where N(same) is the number of trials where the measurements at t=0 and at t=t return the same result etc.

How does this correlation function depend on t?
 
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aa2ll2 said:
TL;DR Summary: "What is the half life of the correlation between repeated spin measurements on the same electron?

Consider repeated spin measurements, along the same axis, on the same electron, at t=0 and at t=t. For small t, the results are identical, so the correlation function, C(t,0)=1, but for large t, C(t,0) -> 0.

Define C(t,0) = P(same) - P(different) = N(same) - N(different) / N(same) + N(different), where N(same) is the number of trials where the measurements at t=0 and at t=t return the same result etc.

How does this correlation function depend on t?
It depends on the Hamiltonian for the system. For a free electron, the spin state does not evolve. The spin state would evolve in a magnetic field.
 
It's a noise question. So, the free particle spin evolving in noise, does not remain forever the same, with prob. 1, right? I actually have in mind an NV centre, which I think is free for the purpose to hand.
 
aa2ll2 said:
It's a noise question. So, the free particle spin evolving in noise, does not remain forever the same, with prob. 1, right? I actually have in mind an NV centre, which I think is free for the purpose to hand.
You'll need to specify a Hamiltonian for your "noise".
 
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The standard, coupling to bath, model. A bit of context may help. The single qubit coherence time is T_coh. I'm anticipating the time dependence should involve T_coh, something like C(t,0) = e^[-t/T_coh]. Or, are you saying coherence time is not pertinent?
 
aa2ll2 said:
The standard, coupling to bath, model. A bit of context may help. The single qubit coherence time is T_coh. I'm anticipating the time dependence should involve T_coh, something like C(t,0) = e^[-t/T_coh]. Or, are you saying coherence time is not pertinent?
Is this to do with quantum computing?
 
It is actually something that came up with loophole free Bell tests, but quite similar to computing.
 
Hi Perok,

Looking at some papers, the question of what hamiltonian to use seems a bit of a red herring. The starting point is the density matrix, where off diagonal terms decay as exp[-t/T_coh] In the model used for predicting the Bell violation in noise. My question should then be quite simple . How does the C(t,0) defined above depend on time?
 
aa2ll2 said:
Hi Perok,

Looking at some papers, the question of what hamiltonian to use seems a bit of a red herring. The starting point is the density matrix, where off diagonal terms decay as exp[-t/T_coh] In the model used for predicting the Bell violation in noise. My question should then be quite simple . How does the C(t,0) defined above depend on time?
There's not enough context in this thread for me to comment. Perhaps someone else who is more familiar with the specific subject matter may be able to help. But, in such specific cases, you ought to provide the full background to the question.
 
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Thanks for your attention to this matter.
 

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