1995
DOI: 10.1016/0038-1098(95)00514-5
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Bound magneto-acceptor and magneto-donor states in the conduction band of GaAsGaAlAs heterostructures

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Cited by 18 publications
(14 citation statements)
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“…This has also been confirmed experimentally. 18 Taking the advantage of the double-well structure of the potential U h , we can solve the hole motion by independently studying the motions in the two wells, and later including the coupling between the wells via the off-diagonal tunneling matrix element. Thus the pair of lowest-energy hole states will be approximated by diagonalizing the Hamiltonian H h in the subspace spanned by the pair of ground states in the two wells treated separately: Lh and Rh , with the energies E Lh and E Rh , respectively.…”
Section: ͑10͒mentioning
confidence: 99%
“…This has also been confirmed experimentally. 18 Taking the advantage of the double-well structure of the potential U h , we can solve the hole motion by independently studying the motions in the two wells, and later including the coupling between the wells via the off-diagonal tunneling matrix element. Thus the pair of lowest-energy hole states will be approximated by diagonalizing the Hamiltonian H h in the subspace spanned by the pair of ground states in the two wells treated separately: Lh and Rh , with the energies E Lh and E Rh , respectively.…”
Section: ͑10͒mentioning
confidence: 99%
“…Magneto-donors in symmetric wells were described theoretically by Green and coworkers [3] and by MacDonald and Ritchie [4], while the case of triangular-like wells was treated by Kubisa and Zawadzki [5]. Vicente et al [6] presented evidence for new localized magneto-impurity states in 2D systems, created by conduction electrons bound to ionized acceptors (as originally proposed in [5]). Recently, Raymond et al [7] observed oscillatory binding energy of magneto-donors in GaAs/GaAlAs heterostructure in the Quantum Hall regime.…”
mentioning
confidence: 96%
“…Below these three excitations we observe three additional transitions not accounted for by the free-carrier picture. The lowest transition A was identified as excitation originating from the ground MD state and the 1b state in the valence band [6,7]. We identify transitions C and G as originating from the excited MD states associated with LLs 1 ± ± and 2 + , respectively.…”
mentioning
confidence: 99%
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