What is the meaning of canonical in quantum mechanics?

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Canonical variables in quantum mechanics refer to pairs of variables, such as position and canonical momentum, that satisfy specific commutation relations, indicating their fundamental relationship. The distinction between canonical momentum and regular momentum arises in contexts like electromagnetic fields, where canonical momentum incorporates additional terms related to the field, while mechanical momentum does not. Both types of momentum can satisfy the same commutation relations, but only the canonical momentum is designated as such due to its role in the formulation of quantum mechanics. The conservation of one canonical variable implies the conservation of its counterpart, reflecting symmetries in the system. Understanding these concepts is crucial for grasping the underlying principles of quantum mechanics.
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what does it mean in quantum mechanics when they say canonical variables or canonical momentum? what is the difference from regular momentum?
 
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Read the bottom of this page under physics:

http://www.answers.com/canonical&r=67

To paraphrase: Any two variables whose Poisson Bracket (or Commutator in Quantum) that give a delta are canonical. A symmetry in one canonical variable implies the other is conserved. For example, translational invariance and conservation of momentum.

Cheers,
Norm
 
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Norman said:
...To paraphrase: Any two variables whose Poisson Bracket (or Commutator in Quantum) that give a delta are canonical.

Not exactly. For example, in single particle quantum mechanics in the presence of an external electromagnetic field the canonical variables are the position \vec x and the *canonical* momentum \vec p which satisfy:
<br /> [x_j,p_k]=i\hbar\delta_{jk}\;.<br />

But, if the above holds, it should also be obvious that the *mechanical* momentum \vec \pi =\vec p-e\vec A where e is the charge also satisfies:
<br /> [x_j,\pi_k]=i\hbar\delta_{jk}\;.<br />

Thus, both sets of variables satisfy canonical communtation relations even though only the set (x,p) are called "canonical variables."
 
thanks for your help
 
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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