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Open Questions in Physics
Open Questions in Physics

LOYOLA COLLEGE (AUTONOMOUS), CHENNAI – 600 034
LOYOLA COLLEGE (AUTONOMOUS), CHENNAI – 600 034

... 16. State and prove Ehernfest’s theorem 17. Solve the Schrodinger equation for a linear harmonic oscillator. Sketch the first two eigenfunctions of the system. 18. Determine the eigenvalue spectrum of angular momentum operators Jz and Jz 19. What are symmetric and antisymmetric wave functions? Show ...
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... A coherent state is the specific quantum state of the quantum harmonic oscillator whose dynamics most closely resembles the oscillating behaviour of a classical harmonic oscillator. Further, in contrast to the energy eigenstates of the system, the time evolution of a coherent state is concentrated a ...
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... Find the ordering momentum and the energy of the ground state configuration as a function of the dimensionless ratio w = −J2 /J1 in the full possible range 0 ≤ w ≤ ∞. [The problem is motivated by recently discovered frustrated ferromagnets LiCuVO4 and LiCu2 O2 .] ~ and the ground state energy E0 of ...
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Canonical quantization

In physics, canonical quantization is a procedure for quantizing a classical theory, while attempting to preserve the formal structure, such as symmetries, of the classical theory, to the greatest extent possible.Historically, this was not quite Werner Heisenberg's route to obtaining quantum mechanics, but Paul Dirac introduced it in his 1926 doctoral thesis, the ""method of classical analogy"" for quantization, and detailed it in his classic text. The word canonical arises from the Hamiltonian approach to classical mechanics, in which a system's dynamics is generated via canonical Poisson brackets, a structure which is only partially preserved in canonical quantization.This method was further used in the context of quantum field theory by Paul Dirac, in his construction of quantum electrodynamics. In the field theory context, it is also called second quantization, in contrast to the semi-classical first quantization for single particles.
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