2001
DOI: 10.1006/spmi.2001.0985
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1 s–2 p±transitions between hydrogenic states in GaAs low-dimensional systems under external fields

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Cited by 7 publications
(2 citation statements)
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“…x \left.\right) - E_{1 p}^{\text{sub}} \left.\right) / �?^{2}}$$where E1ssub$E_{1 s}^{\text{sub}}$ and E1psub$E_{1 p}^{\text{sub}}$ are the 1 s ‐ground state and 1 p ‐excites state subband energies, and these energies are found from the ground and excited state transcendental equations, respectively. [ 41,47 ] Energies are given as follows for 1 s and 1 p impurity states [ 13 ] E1simp=minλ1s ψ1simp3extrue|HA=1,B=03extrue|ψ1simp3extrue/ψ1simp3extrue|ψ1simp$$E_{1 s}^{\text{imp}} = \left(\text{min}\right)_{\left(\lambda\right)_{1 s} \textrm{ }} \psi_{1 s}^{\text{imp}} \text{|} H^{A = 1 , B = 0} \text{|} \psi_{1 s}^{\text{imp}} / \psi_{1 s}^{\text{imp}} \text{|} \psi_{1 s}^{\text{imp}}$$andE1pimp=minλ1p ψ1pimp3extrue|HA=1,B=13extrue|ψ1pimp3extrue/ψ1pimp3extrue|ψ1pimp$$E_{1 p}^{\text{imp}} = \left(\text{min}\right)_{\left(\lambda\right)_{1 p} \textrm{ }} \psi_{1 p}^{\text{imp}} \text{|} H^{A = 1 , B = 1} \text{|} \psi_{1 p}^{\text{imp}} / \psi_{1 p}^{\text{imp}} \text{|} \psi_{1 p}^{\text{imp}}$$The intradonor transition energy between ground state 1 s and excited state 1 p is defined as [ 43,47 ] …”
Section: Theorymentioning
confidence: 99%
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“…x \left.\right) - E_{1 p}^{\text{sub}} \left.\right) / �?^{2}}$$where E1ssub$E_{1 s}^{\text{sub}}$ and E1psub$E_{1 p}^{\text{sub}}$ are the 1 s ‐ground state and 1 p ‐excites state subband energies, and these energies are found from the ground and excited state transcendental equations, respectively. [ 41,47 ] Energies are given as follows for 1 s and 1 p impurity states [ 13 ] E1simp=minλ1s ψ1simp3extrue|HA=1,B=03extrue|ψ1simp3extrue/ψ1simp3extrue|ψ1simp$$E_{1 s}^{\text{imp}} = \left(\text{min}\right)_{\left(\lambda\right)_{1 s} \textrm{ }} \psi_{1 s}^{\text{imp}} \text{|} H^{A = 1 , B = 0} \text{|} \psi_{1 s}^{\text{imp}} / \psi_{1 s}^{\text{imp}} \text{|} \psi_{1 s}^{\text{imp}}$$andE1pimp=minλ1p ψ1pimp3extrue|HA=1,B=13extrue|ψ1pimp3extrue/ψ1pimp3extrue|ψ1pimp$$E_{1 p}^{\text{imp}} = \left(\text{min}\right)_{\left(\lambda\right)_{1 p} \textrm{ }} \psi_{1 p}^{\text{imp}} \text{|} H^{A = 1 , B = 1} \text{|} \psi_{1 p}^{\text{imp}} / \psi_{1 p}^{\text{imp}} \text{|} \psi_{1 p}^{\text{imp}}$$The intradonor transition energy between ground state 1 s and excited state 1 p is defined as [ 43,47 ] …”
Section: Theorymentioning
confidence: 99%
“…[39,40] In the literature, there are many studies on binding energy and transition energy calculations for different structures. [12,[41][42][43] One of the most important reasons for calculating the binding energy and transition energy is that it is of great importance in determining the optical properties of the system. Çakır et al [44] have calculated the variation of the difference between the energy levels of the QD1 with impurity as a function of dot radius.…”
Section: Introductionmentioning
confidence: 99%