Vectors, Hilbert Spaces, and Tensor Products

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Discussion Overview

The discussion revolves around the representation of states in classical mechanics and quantum mechanics, specifically the use of vectors in phase space and Hilbert spaces. Participants explore the transition from classical to quantum frameworks, the motivation behind using Hilbert spaces to represent quantum states, and the implications of tensor products in joint quantum systems.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants propose that a vector in phase space can specify the state of a classical system, suggesting this might facilitate the transition to quantum mechanics.
  • Others argue that a ray in Hilbert space, rather than a vector, represents a pure quantum state, with references to quantum mechanics textbooks for further clarification.
  • There is a suggestion that the state of a classical system can be represented by a vector in a Hilbert space associated with phase space, though this claim is met with requests for elaboration on the differences between classical and quantum representations.
  • One participant notes that phase space cannot be treated as Euclidean space in the same way as vectors in RN, indicating a complexity in the representation of states in classical mechanics.

Areas of Agreement / Disagreement

Participants express differing views on the representation of states in classical and quantum mechanics, with no consensus reached on the nature of the transition between the two frameworks or the appropriate mathematical representations.

Contextual Notes

Limitations include the potential misunderstanding of the relationship between classical and quantum representations, as well as the complexity of phase space not being necessarily Euclidean, which may affect the discussion of vectors and their interpretations.

Bashyboy
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If I ever say anything incorrect, please promptly correct me!

The state of a system in classical mechanics is specified by point in phase space, the point giving us the position and velocity at a given instance. Could we rephrase it by saying a vector in phase space specifies the system? If so, it would seem to make transition to QM slightly more natural.

My next question is, what is the motivation for thinking that a vector in a Hilbert space represents the state of a quantum? I would appreciate an explanation or a reference to some source that nicely answers this question.

My last question, related to the second, is, why is "The situation of two independent observers conducting measurements on a joint quantum system...usually modeled using a Hilbert space of tensor product form, each factor associated to one observer"? Again, is there motivation for this idea?
 
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Take any quantum-mechanics textbook, e.g., Sakurai, Modern Quantum Mechanics. A good book will explain that it is actually a ray in Hilbert space that represents a (pure) state of the system. Most general is the representation of the system in terms of a statistical operator, which is a self-adjoint positive semidefinite operator of trace 1.
 
Bashyboy said:
The state of a system in classical mechanics is specified by point in phase space, the point giving us the position and velocity at a given instance. Could we rephrase it by saying a vector in phase space specifies the system? If so, it would seem to make transition to QM slightly more natural.

Actually It is position and momentum. But in a sense yes, The state of a classical system can be represented by vector in an Hilbert space associated to the phase space

http://arxiv.org/abs/quant-ph/0301172
 
andresB said:
The state of a classical system can be represented by vector in an Hilbert space associated to the phase space

http://arxiv.org/abs/quant-ph/0301172

@andresB You seem to be saying something slightly different than what I said in my question. Would you elaborate on the difference between a vector in phase space describing a classical system and a vector in an Hilbert space associated to the phase space?
 
In general, for the phase space you can't use vectors as in RN (where there is an identification of a point with a vector) because the phase space is not necessarily an euclidean manifolds. I don't have enough mastery on the topic to give a clear picture but there are several good expositions like Arnold's mathematical methods of classical mechanics.
 

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