More Problems with Bohr
... corrections will serve me well in what is upcoming. But what I would like to do now is go through a recent graduate level textbook, pulling apart the historical equations and assumptions once more. I will use Lawrence Lerner's 1996 textbook Modern Physics for Scientists and Engineers, volume 2. I us ...
... corrections will serve me well in what is upcoming. But what I would like to do now is go through a recent graduate level textbook, pulling apart the historical equations and assumptions once more. I will use Lawrence Lerner's 1996 textbook Modern Physics for Scientists and Engineers, volume 2. I us ...
Relaxation dynamics of a quantum Brownian particle in an ideal gas
... The simplest realistic environment in that sense is clearly given by an ideal gas in a thermal state. The gas particles then do not interact with each other, but they influence the Brownian particle via two-body forces, which should be taken sufficiently short-ranged to permit a scattering theory descr ...
... The simplest realistic environment in that sense is clearly given by an ideal gas in a thermal state. The gas particles then do not interact with each other, but they influence the Brownian particle via two-body forces, which should be taken sufficiently short-ranged to permit a scattering theory descr ...
Chapter 2 Wave Mechanics and the Schrödinger equation
... In the classically allowed area, where the energy of the electron is larger then the potential, the solution is oscillatory, whereas in the classically forbidden realm of E < V (x) we find a superposition of exponential growth and of exponential decay. Normalizability of the solution requires that t ...
... In the classically allowed area, where the energy of the electron is larger then the potential, the solution is oscillatory, whereas in the classically forbidden realm of E < V (x) we find a superposition of exponential growth and of exponential decay. Normalizability of the solution requires that t ...
instroduction_a_final
... Note: Iz is the Operator, represents the z component of nuclear spin angular momentum. (Also Ix and Iy, represents x component and y component respectively. We will use them late on). At this point, we don't know the WaveFunction, and we don't have to know the WaveFunction to get the EigenValue. Now ...
... Note: Iz is the Operator, represents the z component of nuclear spin angular momentum. (Also Ix and Iy, represents x component and y component respectively. We will use them late on). At this point, we don't know the WaveFunction, and we don't have to know the WaveFunction to get the EigenValue. Now ...
an exact solution of the dirac oscillator problem in
... equal weight, to obtain exact energy spectrum. Our result fully coincides with existing result in the literature [34]. Therefore, this paper presents a handy alternative method of an exact solution of the Dirac oscillator in one dimension with GUP. The paper also manifests the super symmetry aspects ...
... equal weight, to obtain exact energy spectrum. Our result fully coincides with existing result in the literature [34]. Therefore, this paper presents a handy alternative method of an exact solution of the Dirac oscillator in one dimension with GUP. The paper also manifests the super symmetry aspects ...
