Difference between revisions of "Deut pair.m"

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==Syntax==
 
==Syntax==
  
    [S,T,Q]=deut_pair(spin_system,spin_a,spin_b,options)
+
 
 +
    [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

Elementary_states

Version 2.11, authors: Ilya Kuprov, Anakin Aden