ar X iv : q ua nt - p h / 02 07 04 4 v 3 2 9 Ju l 2 00 8 Shouldn ’ t there be an antithesis to quantization ? ∗

ua nt - p h / 02 07 04 4 v 2 2 7 Se p 20 04 Shouldn ’ t there be an antithesis to quantization ? ∗ Eric

We raise the possibility of developing a theory of constructing quantum dynamical observables independent from quantization and deriving classical dynamical observables from pure quantum mechanical consideration. We do so by giving a detailed quantum mechanical derivation of the classical time of arrival at arbitrary arrival points for a particle in one dimension. E. A. Galapon J. Math. Phys. 4...

ar X iv : q ua nt - p h / 02 03 04 6 v 1 1 1 M ar 2 00 2 Quantum imaging

We provide a brief overview of the newly born field of quantum imaging, and discuss some concepts that lie at the root of this field.

ar X iv : q ua nt - p h / 04 11 17 2 v 1 2 3 N ov 2 00 4 Information and Entropy in Quantum Theory

ar X iv : q ua nt - p h / 04 07 19 1 v 1 2 3 Ju l 2 00 4 Coherently - assisted incoherent population transfer in a five - level system

A novel effect of population transfer in a five-level system is analyzed. This population transfer effect is found to be a version of a Raman process, which is facilitated and assisted by coherence effects, acting to close other available decay channels.

ar X iv : q ua nt - p h / 04 02 03 5 v 3 9 J un 2 00 5 p - MECHANICS AND FIELD THEORY

The orbit method of Kirillov is used to derive the p-mechanical brackets [25]. They generate the quantum (Moyal) and classical (Poisson) brackets on respective orbits corresponding to representations of the Heisenberg group. The extension of p-mechanics to field theory is made through the De Donder–Weyl Hamiltonian formulation. The principal step is the substitution of the Heisenberg group with...