“…In the case of Cu 2 O ν means p, f, h, K excitonic states. The equations have been described in [2,6] (see also [11,16]) and have the form…”
Section: Theorymentioning
confidence: 99%
“…Again, note that transition to intermediate field regime is earlier for higher states. We have to remark that for these two regimes of magnetic field, we use two different methods of solution of the constitutive equation (2) and as the consequence one can not expect interpolation to be perfect. For the weak field we have used the perturbation calculus, where the unperturbed, spherically symmetric eigen-functions serve as a basis.…”
Section: Intermediate Fieldsmentioning
confidence: 99%
“…Extraordinary properties of RE attracted an increasing attention during the last few years, specifically for excitons in high external magnetic fields ( [2][3][4][5][6] and references therein). This model system is well-recognized as a convenient analog to a hydrogen atom, in which the high field' physics occurs already at moderate field strengths achievable in a laboratory.…”
Section: Introductionmentioning
confidence: 99%
“…The upper value corresponds to B>0 and m=−1, and the lower to the quantum number m=+1 for the same field orientation.The Green's function allows one to calculate the amplitude Y from the (16) is the amplitude of the propagating wave and M the dipole density in scaled variables. The detailed calculations follow the pattern presented for the electric field using the trial wave functions[2]. For p excitons the trial function has the form[11] Y nm (ζ).…”
mentioning
confidence: 99%
“…For p excitons the trial function has the form[11] Y nm (ζ). Furthermore, the y component of the dipole density of the form[2]…”
Recent experimental and theoretical work on hydrogen-like absorption spectra of excitons in external magnetic fields revealed new effects when the Coulomb interaction becomes comparable to the magnetic perturbation. We present a theoretical approach that allows for calculation of absorption spectra for any value of magnetic field. This approach opens the possibility to compute the optical functions i.e. reflectivity, transmission and absorption including the excitonic effects for various strength of external magnetic field.
“…In the case of Cu 2 O ν means p, f, h, K excitonic states. The equations have been described in [2,6] (see also [11,16]) and have the form…”
Section: Theorymentioning
confidence: 99%
“…Again, note that transition to intermediate field regime is earlier for higher states. We have to remark that for these two regimes of magnetic field, we use two different methods of solution of the constitutive equation (2) and as the consequence one can not expect interpolation to be perfect. For the weak field we have used the perturbation calculus, where the unperturbed, spherically symmetric eigen-functions serve as a basis.…”
Section: Intermediate Fieldsmentioning
confidence: 99%
“…Extraordinary properties of RE attracted an increasing attention during the last few years, specifically for excitons in high external magnetic fields ( [2][3][4][5][6] and references therein). This model system is well-recognized as a convenient analog to a hydrogen atom, in which the high field' physics occurs already at moderate field strengths achievable in a laboratory.…”
Section: Introductionmentioning
confidence: 99%
“…The upper value corresponds to B>0 and m=−1, and the lower to the quantum number m=+1 for the same field orientation.The Green's function allows one to calculate the amplitude Y from the (16) is the amplitude of the propagating wave and M the dipole density in scaled variables. The detailed calculations follow the pattern presented for the electric field using the trial wave functions[2]. For p excitons the trial function has the form[11] Y nm (ζ).…”
mentioning
confidence: 99%
“…For p excitons the trial function has the form[11] Y nm (ζ). Furthermore, the y component of the dipole density of the form[2]…”
Recent experimental and theoretical work on hydrogen-like absorption spectra of excitons in external magnetic fields revealed new effects when the Coulomb interaction becomes comparable to the magnetic perturbation. We present a theoretical approach that allows for calculation of absorption spectra for any value of magnetic field. This approach opens the possibility to compute the optical functions i.e. reflectivity, transmission and absorption including the excitonic effects for various strength of external magnetic field.
An efficient and precise tool for steering on-demand the periodicity and amplitude of electro-modulations based on solid-state is of great importance for quantum engineering. In Cu 2 O crystal, the excitons created by electromagnetic waves can be used to design a flexible device which enables the control of absorption oscillations above the gap. The influence of exterior parameters such as temperature and electric field, which influence the dynamic of these oscillations, is discussed.
This topical review addresses how semiconductor systems may reveal scalable properties similar to those known from Rydberg atoms and in which ways they may be utilized for precision sensing and to realize huge long‐range interactions in semiconductor systems. Due to the interdisciplinary nature of the field, it has a twofold purpose: First, it may serve as an introduction to Rydberg physics for semiconductor physicists unfamiliar with the topic. Second, it may also serve as an overview of the specific opportunities and challenges arising in semiconductor physics for researchers who are familiar with Rydberg physics of cold atom gases, but new to the field of semiconductor physics. The review starts with an introduction on the general properties of excitons in semiconductors. Then, the material system Cu2O, which is the best developed platform for semiconductor Rydberg physics at the moment, is discussed in detail.
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