Mutli-partite states and operators

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SUMMARY

The discussion centers on the relationship between multi-partite states in quantum mechanics and their interpretation as operators acting on other quantum systems. It establishes that the space of operators on a Hilbert space is isomorphic to the tensor product of the Hilbert space and its dual, expressed as H ⊗ H* ~ L(H). The conversation emphasizes that composite quantum systems can be viewed as observables on other systems, reinforcing the axioms of quantum mechanics regarding tensor products in multi-degree freedom scenarios. Additionally, it clarifies that operators are defined by their matrix representations, highlighting the dimensionality of operator spaces in finite dimensions.

PREREQUISITES
  • Understanding of Hilbert spaces in quantum mechanics
  • Familiarity with tensor products and dual spaces
  • Knowledge of quantum operators and their matrix representations
  • Basic concepts of composite quantum systems
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  • Study the properties of tensor products in quantum mechanics
  • Explore the significance of dual spaces in quantum theory
  • Learn about the representation of quantum operators in various bases
  • Investigate the implications of composite systems acting as observables
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Quantum physicists, researchers in quantum information theory, and students studying advanced quantum mechanics concepts will benefit from this discussion.

MaverickMenzies
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Hi, I've seen the following in quantum info textbooks and papers and I was just wondering if anyone knows if it has any phsical interpretation or significance?

The space of operators that act on a HIlbert space is isomorphic to the tensor product of the original Hilbert space with its dual:

H otimes H* ~ L(H)

This means that if we start with a tensor product Hilbert space then it is possible to regard the states in this space as operators acting on another space. I.e. there is a one-to-one relationship between the vectors of this tensor product space and operators acting on a separate space.

Ok, the axioms of QM require that the tensor product be used when the system has more than one degree of freedom. Does this then mean that perhaps composite quantum systems in certain states can be imagined as acting as observables on other quantum systems?

What do you guys think? Am I reading too much into it?
 
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You're reading too much into it. Operators are uniquely defined by their matrix representation in a basis - which looks like

[tex]\begin{align*}\hat{A} &= \sum_{a} \sum_{a'} | a \rangle \langle a | \hat{A} | a' \rangle \langle a' | \\<br /> &= \sum_{a} \sum_{a'} \left( \langle a | \hat{A} | a' \rangle \right) | a \rangle \langle a' | \end{align}[/tex]

with matrix elements [tex]\left( \langle a | \hat{A} | a' \rangle \right)[/tex]. So an arbitary operator is a linear combination of operators of the form [tex]| a \rangle \langle a' |[/tex] - i.e. tensor products of basis vectors and dual basis vectors - which themselves form a basis for the space of operators.

To check your intuition, note that in finite spaces, the dimension of the space of NxN matrices (operators) is N^2, the square of the dimension N of the vector (Hilbert) space.
 
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