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Varenna Lectures
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0000318843
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For discussions of bosonization in more than one dimension see Luther A 1979 Phys. Rev. B 19 320 Haldane F D M 1992 Varenna Lectures (Amsterdam: North-Holland) Haldane F D M 1992 Helv. Phys. Acta 65 152 Houghton A and Marston J B 1993 Phys. Rev. B 48 7790 Castro Neto A H and Fradkin E 1994 Phys. Rev. B 49 10877 Westfahl H, Castro Neto A H and Caldeira A O 1997 Phys. Rev. B 55 7347
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For discussions of bosonization in more than one dimension see Luther A 1979 Phys. Rev. B 19 320 Haldane F D M 1992 Varenna Lectures (Amsterdam: North-Holland) Haldane F D M 1992 Helv. Phys. Acta 65 152 Houghton A and Marston J B 1993 Phys. Rev. B 48 7790 Castro Neto A H and Fradkin E 1994 Phys. Rev. B 49 10877 Westfahl H, Castro Neto A H and Caldeira A O 1997 Phys. Rev. B 55 7347
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Westfahl, H.1
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Caldeira, A.O.3
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37
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11344291398
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note
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The compressible state at v = 1/2 is anomalous from the present point of view, being the accumulation point of an infinite series of incompressible states [13]. Its description requires the inclusion of q-dependent viscosity terms.
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38
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11344260427
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note
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n. The fact that the positive-frequency eigenfunctions (n > 0) are the ones with positive norm follows from the stability of the ground state.
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39
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11344276774
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note
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For example, in Laughlin's thought experiment [2] to generate a quasiparticle, the addition of a magnetic flux at the origin causes a radial displacement of all the electrons, with vanishing curl.
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40
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11344271283
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note
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R→ is to shift the zero of the energy to the chemical potential μ.
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47
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11344250536
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Preprint cond-mat/9710137
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Shytov A V, Levitov L S and Halperin B I 1998 Phys. Rev. Lett. 80 141 Khveshchenko D V 1997 Preprint cond-mat/9710137 Zülicke U and MacDonald A H 1998 Preprint cond-mat/9802019
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(1997)
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Khveshchenko, D.V.1
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48
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11344293366
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Preprint cond-mat/9802019
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Shytov A V, Levitov L S and Halperin B I 1998 Phys. Rev. Lett. 80 141 Khveshchenko D V 1997 Preprint cond-mat/9710137 Zülicke U and MacDonald A H 1998 Preprint cond-mat/9802019
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(1998)
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Zülicke, U.1
MacDonald, A.H.2
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49
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11344257375
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note
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The derivation of the edge Hamiltonian (16) makes use of the 'weak-incompressibility' condition ∇→ · u→ = 0 and neglects the (small) shear modulus of the edge. Details will be given elsewhere.
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