Density matrix off-diagonal elements

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SUMMARY

The discussion centers on the restrictions of off-diagonal elements in density matrices, particularly in quantum mechanics. It establishes that the magnitude of coherence between two levels is constrained by the populations of those levels, expressed as |\rho_{nm}|^2 ≤ \rho_{nn}\rho_{mm} ≤ 1. Additionally, it highlights the significance of phase differences, which influence the time-dependent properties of quantum systems, and emphasizes the role of time and frequency shaped laser pulses in optical quantum control. Recommended readings include Ben Fain's "Irreversibilities in Quantum Mechanics" and David Tannor's "Introduction to Quantum Mechanics: A Time-Dependent Perspective."

PREREQUISITES
  • Understanding of density matrices in quantum mechanics
  • Familiarity with coherence and population in quantum states
  • Knowledge of time-dependent quantum mechanics
  • Basic principles of optical quantum control
NEXT STEPS
  • Study the implications of coherence in quantum systems
  • Learn about time-dependent Hamiltonians in quantum mechanics
  • Explore the techniques of optical quantum control
  • Read David Tannor's "Introduction to Quantum Mechanics: A Time-Dependent Perspective"
USEFUL FOR

Quantum physicists, researchers in optical quantum control, and students studying advanced quantum mechanics concepts will benefit from this discussion.

auctor
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The possible values of the diagonal elements of a density matrix are restricted by the condition \mathrm{Tr}~\rho = 1. Are there any restrictions on the possible values of off-diagonal elements, apart from the obvious \mathrm{Re}~\rho_{nm} = \mathrm{Re}~\rho_{mn}, \mathrm{Im}~\rho_{nm} = - \mathrm{Im}~\rho_{mn}? If the off-diagonals are written in the form \left| \rho_{nm} \right| \exp{i \phi_{nm}}, do the absolute value and the phase have a simple physical meaning?
 
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auctor said:
The possible values of the diagonal elements of a density matrix are restricted by the condition \mathrm{Tr}~\rho = 1. Are there any restrictions on the possible values of off-diagonal elements, apart from the obvious \mathrm{Re}~\rho_{nm} = \mathrm{Re}~\rho_{mn}, \mathrm{Im}~\rho_{nm} = - \mathrm{Im}~\rho_{mn}? If the off-diagonals are written in the form \left| \rho_{nm} \right| \exp{i \phi_{nm}}, do the absolute value and the phase have a simple physical meaning?


The magnitude of a coherence between two levels is bounded by the population in those levels:
|\rho_{nm}|^2 \le \rho_{nn}\rho_{mm}\le 1.

The phase differences determine the time dependent properties of the total system. These phases can be set by time and frequency shaped laser pulses in order to enhance or suppress properties of the system. This is the field of "optical quantum control". Take a look at, for example, Ben Fain's book "Irreveribilities in Quantum Mechanics" or better yet, David Tannor's EXCELLENT "Introduction to Quantum Mechanics: A Time-Dependent Perspective". There's also a review called "Optical control of molecular dynamics" edited by Stuart Rice. It's not that great of a source to learn from, but it's a nice collection of the ideas. Most of it will discuss the interference in the wave function formalism, but you'll get the basic picture.
 
For a system with time Independent hamiltonian , in the basis of energy eigen kets, every off diagonal element between two kets corresponding to two distinct energy eigen values will oscillate with Bohr Frequency.
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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