Ideal Bose Gas and Blackbody Radiation in the Dunkl Formalism
arXiv:2301.12236 · doi:10.1088/1742-5468/acd106
Abstract
Recently, deformed quantum systems gather lots of attention in the literature. Dunkl formalism differs from others by containing the difference-differential and reflection operator. It is one of the most interesting deformations since it let us discuss the solutions according to the even and odd solutions. In this work, we studied the ideal Bose gas and the blackbody radiation via the Dunkl formalism. To this end, we made a liaison between the coordinate and momentum operators with the creation and annihilation operators which allowed us to obtain the expressions of the partition function, the condensation temperature, and the ground state population of the Bose gas. We found that Dunkl-condensation temperature increases with increasing θ value. In the blackbody radiation phenomena, we found how the Dunkl formalism modifies total radiated energy. Then, we examined the thermal quantities of the system. We found that the Dunkl deformation causes an increase in entropy and specific heat functions as well as in the total radiation energy. However, we observed a decrease in the Dunk-corrected Helmholtz free energy in this scenario. Finally, we found that the equation of state is invariant even in the considered formalism.
12 pages, 7 figures
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- The Dunkl-Fokker-Planck Equation in Dimensions
- Time-Dependent Dunkl-Schrödinger Equation with an Angular-Dependent Potential
- The Condensation of Ideal Dunkl-Bose Gas in Power-Law Traps
- One-dimensional Dunkl Quantum Mechanics: A Path Integral Approach
- A Path Integral Treatment of Time-dependent Dunkl Quantum Mechanics
- On Dunkl-Bose-Einstein Condensation in Harmonic Traps
- Dunkl-Klein-Gordon Equation in Higher Dimensions
- Bounding the Wigner Deformation Parameter in Harmonically Trapped Bose Gases
- Spectral and Thermal Analysis of the Morse Potential within the Dunkl Formalism: Analytical Approximations and Applications
- Impact of the non-canonical approach to the exact solution of the ideal one-dimensional electron gas confined with an anisotropic quantum wire of oscillator-shaped profile