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Another way to write Ψ would be to use the form of Eq. (2.16) of Ref. with k=2 modifying the function χ to have the form χ (z1, z2; z3, z4) = (z1 - z3) 2 (z2 - z4) 2 (z1 - z4) (z2 - z3). Many generalizations of this form to clusters rather than pairs are possible (analogous to Appendix).
-
Another way to write Ψ would be to use the form of Eq. (2.16) of Ref. with k=2 modifying the function χ to have the form χ (z1, z2; z3, z4) = (z1 - z3) 2 (z2 - z4) 2 (z1 - z4) (z2 - z3). Many generalizations of this form to clusters rather than pairs are possible (analogous to Appendix).
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4344564550
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A nonrigorous argument can be made, however, that any quantum Hall phase of matter should be adiabatically connected to a wave function that can be expressed as a correlator of a conformal field theory.
-
A nonrigorous argument can be made, however, that any quantum Hall phase of matter should be adiabatically connected to a wave function that can be expressed as a correlator of a conformal field theory.
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30
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33846968507
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Numerically we define the hierarchy 2/5 state as the ground state of a V1 only Hamiltonian. For system sizes for which composite fermion trial wave functions can be generated, the hierarchy and composite fermion wave function have near perfect overlap.
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Numerically we define the hierarchy 2/5 state as the ground state of a V1 only Hamiltonian. For system sizes for which composite fermion trial wave functions can be generated, the hierarchy and composite fermion wave function have near perfect overlap..
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