Difference between revisions of "Deut pair.m"
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==Syntax== | ==Syntax== | ||
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| + | [S,T,Q,Tc,Qc]=deut_pair(spin_system,spin_a,spin_b,options) | ||
==Arguments== | ==Arguments== | ||
Revision as of 15:12, 5 June 2026
All possible states of a spin-1 pair, classified by the total spin into singlet, triplet, and quartet.
Syntax
[S,T,Q,Tc,Qc]=deut_pair(spin_system,spin_a,spin_b,options)
Arguments
spin_a - the number of the first spin
spin_b - the number of the second spin
options.dephasing - set to 1 to eliminate the states that are
not stationary under Az+Bz Hamiltonian,
the default is to keep everything
Outputs
S - singet state density matrix (Hilbert space)
or state vector (Liouville space)
T - triplet state density matrices (Hilbert space)
or state vectors (Liouville space), ordered in
a cell array as {T+,T0,T-}
Q - quintet state density matrices (Hilbert space)
or state vectors (Liouville space), ordered in
a cell array as {Q++,Q+,Q0,Q-,Q--}
Notes
WARNING: the states above are NOT irreducible spherical tensors - Bargon just kroneckered up some Zeeman states and gave them what looked to him like appropriate labels.
See also
Version 2.11, authors: Ilya Kuprov, Anakin Aden