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We put quotes here because Eq. 20 is decoupled only in its face form. As shown explicitly in Ref., in the balanced case, there is a spin-charge separation only in the ground state. However, in any excited states such as meron excitations, there are spin-charge connection which leads to the correct meron fractional charge and polarization listed in Table 1 in Ref.. It is this spin-charge connection which leads to the constraint of the vortices in the two layers J0 v+ (x)= J0 v- (x)=-δ(x) used in this section and J0 v± =δ (x - z0) ±δ (x - w0) used in the next section.
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We put quotes here because Eq. 20 is decoupled only in its face form. As shown explicitly in Ref., in the balanced case, there is a spin-charge separation only in the ground state. However, in any excited states such as meron excitations, there are spin-charge connection which leads to the correct meron fractional charge and polarization listed in Table 1 in Ref.. It is this spin-charge connection which leads to the constraint of the vortices in the two layers J0 v+ (x)= J0 v- (x)=-δ(x) used in this section and J0 v± =δ (x - z0) ±δ (x - w0) used in the next section.
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As shown in detail in Ref., the functional form achieved from the composite boson theory is the same at that achieved from the microscopic LLL+HF approach. But the coefficients should be taken from the LLL+HF approach.
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