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We work with the convention that for any bipartite split of a system, (Formula presented) the symbol A is equivalent to a list of the particles residing on its side of the split, and likewise for B. (Formula presented) and (Formula presented) are the number of particles on each side of the split; (Formula presented) and (Formula presented) are the Hilbert space dimensions of each side, generally (Formula presented) and (Formula presented) for nonsymmetric collections of spin-1/2 particles
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We work with the convention that for any bipartite split of a system, (Formula presented) the symbol A is equivalent to a list of the particles residing on its side of the split, and likewise for B. (Formula presented) and (Formula presented) are the number of particles on each side of the split; (Formula presented) and (Formula presented) are the Hilbert space dimensions of each side, generally (Formula presented) and (Formula presented) for nonsymmetric collections of spin-1/2 particles.
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We use the convention that for any bipartite measure X if (Formula presented) is less than the number of spins N in (Formula presented) the possibly mixed state that the measure (Formula presented) should act on is actually (Formula presented) For the concurrence, we use the similar convention (Formula presented)
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We use the convention that for any bipartite measure X if (Formula presented) is less than the number of spins N in (Formula presented) the possibly mixed state that the measure (Formula presented) should act on is actually (Formula presented) For the concurrence, we use the similar convention (Formula presented)
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