Can QM be described by Markov chain theory?

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SUMMARY

The discussion centers on the inadequacy of Markov chain theory to describe quantum mechanics (QM), particularly in relation to the intensity of spectral lines. It is established that regardless of the initial state vector, QM transitions to a stationary vector that does not align with classical probability theory's constraints. The conversation references the paper "From quantum mechanics to classical statistical physics" which discusses the correspondence between stochastic classical systems and quantum phase diagrams, emphasizing the limitations of Markov theory in capturing continuous transformations in QM.

PREREQUISITES
  • Quantum Mechanics fundamentals
  • Markov Chain Theory
  • Stochastic Processes
  • Matrix Theory in statistical physics
NEXT STEPS
  • Study the implications of the "Stochastic Matrix Form" decomposition in quantum systems
  • Explore the relationship between equilibrium partition functions and quantum phase diagrams
  • Investigate the role of relaxation rates in quantum excitation spectra
  • Review the paper "From quantum mechanics to classical statistical physics" for deeper insights
USEFUL FOR

Physicists, quantum mechanics researchers, and anyone interested in the intersection of quantum theory and classical statistical mechanics.

Adel Makram
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Can we describe the intensity of spectral lines using Markov theory? No matter what is the initial state vector of the system, the final state will be reduced to a stationary vector whose elements represent the intensity of the spectral lines.
 
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http://arxiv.org/abs/cond-mat/0502068
From quantum mechanics to classical statistical physics: generalized Rokhsar-Kivelson Hamiltonians and the "Stochastic Matrix Form" decomposition

"Matrices that are SMF decomposable are shown to be in one-to-one correspondence with stochastic classical systems described by a Master equation of the matrix type, hence their name. It then follows that the equilibrium partition function of the stochastic classical system partly controls the zero-temperature quantum phase diagram, while the relaxation rates of the stochastic classical system coincide with the excitation spectrum of the quantum problem."
 

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