Dynamically Equivalent & Kinematically Distinct Pseudo-Hermitian Quantum Systems Ali Mostafazadeh...

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Dynamically Equivalent & Kinematically Distinct Pseudo- Hermitian Quantum Systems Ali Mostafazadeh Koç University

Transcript of Dynamically Equivalent & Kinematically Distinct Pseudo-Hermitian Quantum Systems Ali Mostafazadeh...

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Dynamically Equivalent & Kinematically Distinct Pseudo-Hermitian

Quantum Systems

Ali MostafazadehKoç University

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Outline- Motivation

- Pseudo-Hermitian QM & Its Classical Limit

- Indefinite-Metric QM & the C-operator

- Perturbative Determination of the Most General Metric Operator

- Imaginary Cubic Potential

- QM of Klein-Gordon Fields

- Conclusion

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In Classical Mechanics the geometry of the phase space is fixed.

In Quantum Mechanics the geometry of the Hilbert Space is fixed.

Is this absolutism justified in QM?

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Answer: Yes, because up to unitary-equivalence there is a single separable Hilbert space.

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Though these representations are equivalent, the very fact that they exist reveals a symmetry of the

formulation of QM.

Different reprsentations may prove appropriate for different systems.

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Classical Phase Space Orbits ofImaginary Cubic Potential

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QM of Klein-Gordon Fields

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Conclusion• Not fixing the geometry of the Hilbert space

reveals an infinite class of equivalent representations of QM.

• The classical limit of PT-symmetric non-Hermitian Hamiltonians may be obtained using the Hermitian rep. of the corresponding systems.

• CPT-inner product is not the most general permissible inner product.

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• For imaginary cubic potential the classical Hamiltonian is insensitive to the choice of the metric.

• In the Hermitian rep. the Hamiltonian is generally nonlocal while in the pseudo-Hermitian rep. the basic observables are nonlocal. This seems to indicate a duality between non-Hermiticity and nonlocality.

• Pseudo-Hermiticity yields a consistent QM of free KG fields with a genuine probabilistic interpretation. The same holds for real fields and fields interacting with a time-independent magnetic field.

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• A direct application of the method fails for interactions with other EM fields, for one can prove that in this case time-translations are non-unitary for every choice of an inner product on the space of KG fields (Klein Paradox).

• Application: Construction of Relativistic Coherent States [A.M. & F. Zamani].

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