Within the framework of the q-deformed Heisenberg algebra a dynamical equation of q-deformed quantum mechanics is discussed. The perturbative aspects of the q-deformed Schrödinger equation are analyzed. General representations of the additional momentum-dependent interaction originating from the q-deformed effects are presented in two approaches. As examples, such additional interactions related to the harmonic-oscillator potential and the Morse potential are demonstrated. §
The possibility of testing spatial noncommutativity via Rydberg atoms is explored. An atomic dipole of a cold Rydberg atom is arranged in appropriate electric and magnetic field, so that the motion of the dipole is constrained to be planar and rotationally symmetric. Spatial noncommutativity leads to that the canonical angular momentum possesses fractional values. In the limit of vanishing kinetic energy, the dominate value of the lowest canonical angular momentum takesh/2. Furthermore, in the limit of eliminating magnetic field, the dominate value of the lowest canonical angular momentum changes fromh/2 toh/4. This result is a clear signal of spatial noncommutativity. An experimental verification of this prediction is suggested. *
Standard methods of nonlinear dynamics are used to investigate the stability of particles, branes and D-branes of abelian Born-Infeld theory. In particular the equation of small fluctuations about the D-brane is derived and converted into a modified Mathieu equation and -complementing earlier low-energy investigations in the case of the dilaton-axion system -studied in the high-energy domain. Explicit expressions are derived for the S-matrix and absorption and reflection amplitudes of the scalar fluctuation in the presence of the D-brane. The results confirm physical expectations and numerical studies of others. With the derivation and use of the (hitherto practically unknown) high energy expansion of the Floquet exponent our considerations also close a gap in earlier treatments of the Mathieu equation. *
Semiunitary transformation is applied to discuss supersymmetrization of cold
Rydberg atoms. In the limit of vanishing kinetic energy the lowest angular
momentum of the supersymmetric cold Rydberg atom is $3\hbar/2$. A possible
experimental verification is suggested.Comment: 11 pages, no figur
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