We may denote an electron pair α at ξα = (rα,1, rα,2) = ( Rα, rα) in the state µ = ( NM,nm ) with wavefunction ψ µ(ξα) = Ψ N M,nm(rα,1, rα,2) given by Eq

becomes, ˆH = Np∑ α=1 ˆHp(rα,1, rα,2) + Np∑ β <α 2∑ i,j=1 γB |rα,i − rβ,j |, (22) where rα,i represents the pair α with two electrons i=1

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Sub-Landau levels in two-dimensional electron system in magnetic field

cond-mat.str-el · 2024-06-10 · unverdicted · novelty 5.0

Exact two-electron solutions in strong magnetic field organize into sub-Landau levels by relative angular momentum m, defining correlation subspaces that retain center-of-mass degeneracy and enable construction of pair-based many-body trial states.

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Sub-Landau levels in two-dimensional electron system in magnetic field cond-mat.str-el · 2024-06-10 · unverdicted · none · ref 6
Exact two-electron solutions in strong magnetic field organize into sub-Landau levels by relative angular momentum m, defining correlation subspaces that retain center-of-mass degeneracy and enable construction of pair-based many-body trial states.

We may denote an electron pair α at ξα = (rα,1, rα,2) = ( Rα, rα) in the state µ = ( NM,nm ) with wavefunction ψ µ(ξα) = Ψ N M,nm(rα,1, rα,2) given by Eq

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