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In the BLS phase at (Formula presented) the value of (Formula presented) obtained by exact diagonalization (full symbols) demonstrates some increase with the change of L from (Formula presented) to (Formula presented). We attribute this to the fact that at larger L the pair in the ground state can choose a more profound minimum appearing due to statistical fluctuations that gives some growth of (Formula presented)
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In the BLS phase at (Formula presented) the value of (Formula presented) obtained by exact diagonalization (full symbols) demonstrates some increase with the change of L from (Formula presented) to (Formula presented). We attribute this to the fact that at larger L the pair in the ground state can choose a more profound minimum appearing due to statistical fluctuations that gives some growth of (Formula presented).
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The first step in direct numerical investigations of a few interacting spin fermions above the frozen Fermi sea was done in J. Lages, G. Benenti, and D.L. Shepelyansky, Phys. Rev. B 63, 214516 (2001). However in this approach it is difficult to reach large system sizes since the condition (Formula presented) leads to a strong growth of the matrix size with the number of particles.
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