Universal Subspaces for Local Unitary Groups of Fermionic Systems

preprint2013arXivOpen access

Abstract

Let V=∧NV\mathcal{V}=\wedge^N V be the NN-fermion Hilbert space with MM-dimensional single particle space VV and 2N≤M2N\le M. We refer to the unitary group GG of VV as the local unitary (LU) group. We fix an orthonormal (o.n.) basis ∣v1⟩,...,∣vM⟩\ket{v_1},...,\ket{v_M} of VV. Then the Slater determinants $e_{i_1,...,i_N}:= \ket{v_{i_1}\we v_{i_2}\we...\we v_{i_N}}$ with i1<...<iNi_1<...<i_N form an o.n. basis of $\cV$. Let $\cS\subseteq\cV$ be the subspace spanned by all ei1,...,iNe_{i_1,...,i_N} such that the set {i1,...,iN}\{i_1,...,i_N\} contains no pair {2k−1,2k}\{2k-1,2k\}, kk an integer. We say that the $\ketψ\in\cS$ are single occupancy states (with respect to the basis ∣v1⟩,...,∣vM⟩\ket{v_1},...,\ket{v_M}). We prove that for N=3 the subspace $\cS$ is universal, i.e., each GG-orbit in $\cV$ meets $\cS$, and that this is false for N>3. If MM is even, the well known BCS states are not LU-equivalent to any single occupancy state. Our main result is that for N=3 and MM even there is a universal subspace $\cW\subseteq\cS$ spanned by M(M−1)(M−5)/6M(M-1)(M-5)/6 states ei1,...,iNe_{i_1,...,i_N}. Moreover the number M(M−1)(M−5)/6M(M-1)(M-5)/6 is minimal.

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