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1
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0003490204
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S. Das Sarma, A. Pinczuk, Wiley, New York, edited by, and
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Perspectives in Quantum Hall Effects, edited by S. Das Sarma and A. Pinczuk (Wiley, New York, 1997);
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(1997)
Perspectives in Quantum Hall Effects
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2
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0004308006
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Olle Heinonen, World Scientific, New York, edited by
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Composite Fermions, edited by Olle Heinonen (World Scientific, New York, 1998);
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(1998)
Composite Fermions
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18
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85038966112
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At electron filling (formula presented), the system maps into composite fermions at an effective filling (formula presented), with an effective magnetic field (formula presented). The Landau mass, (formula presented), is defined by (formula presented). Assuming that electrons are confined to their lowest LL, the only energy scale in the problem is the interaction energy, and therefore we must have (formula presented), where (formula presented) is the magnetic length, (formula presented) is the dielectric constant of the background material (which will be taken to be (formula presented), as appropriate for GaAs), and (formula presented) is the dimensionless cyclotron energy in units of (formula presented). For GaAs, the relation (formula presented) can be conveniently expressed as (formula presented) where (formula presented) is the electron mass in vacuum, (formula presented) is the magnetic field measured in Tesla, and the “normalized” Landau mass is given by (formula presented) for GaAs. Here, (formula presented) is only a convenient unit; the composite fermion mass is not related to it in any way
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At electron filling (formula presented), the system maps into composite fermions at an effective filling (formula presented), with an effective magnetic field (formula presented). The Landau mass, (formula presented), is defined by (formula presented). Assuming that electrons are confined to their lowest LL, the only energy scale in the problem is the interaction energy, and therefore we must have (formula presented), where (formula presented) is the magnetic length, (formula presented) is the dielectric constant of the background material (which will be taken to be (formula presented), as appropriate for GaAs), and (formula presented) is the dimensionless cyclotron energy in units of (formula presented). For GaAs, the relation (formula presented) can be conveniently expressed as (formula presented) where (formula presented) is the electron mass in vacuum, (formula presented) is the magnetic field measured in Tesla, and the “normalized” Landau mass is given by (formula presented) for GaAs. Here, (formula presented) is only a convenient unit; the composite fermion mass is not related to it in any way.
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21
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85038904253
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We have considered only the CF LLs with (formula presented). For (formula presented), this restricts us to particle-hole pairs with (formula presented). However, for (formula presented), we are able to go to much larger, thanks to the fact that the states involving excitations into high CF LLs are spurious, as explained in the text
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We have considered only the CF LLs with (formula presented). For (formula presented), this restricts us to particle-hole pairs with (formula presented). However, for (formula presented), we are able to go to much larger L, thanks to the fact that the states involving excitations into high CF LLs are spurious, as explained in the text.
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