### Abstract

Following constructions in the case of canonical and affine coherent states, a universal propagator for a general Hamiltonian appropriate to a single spin degree of freedom is introduced. The universal propagator is a single function, independent of any particular choice of fiducial vector, which, nonetheless, propagates all coherent state Hubert space representatives correctly. Furthermore, we explicitly construct the universal propagator for several examples.

Original language | English (US) |
---|---|

Pages (from-to) | 2893-2913 |

Number of pages | 21 |

Journal | Journal of Mathematical Physics |

Volume | 34 |

Issue number | 7 |

State | Published - 1993 |

Externally published | Yes |

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### ASJC Scopus subject areas

- Organic Chemistry

### Cite this

*Journal of Mathematical Physics*,

*34*(7), 2893-2913.

**The universal propagator for spin [or SU (2)] coherent states.** / Tome, Wolfgang A.; Klauder, John R.

Research output: Contribution to journal › Article

*Journal of Mathematical Physics*, vol. 34, no. 7, pp. 2893-2913.

}

TY - JOUR

T1 - The universal propagator for spin [or SU (2)] coherent states

AU - Tome, Wolfgang A.

AU - Klauder, John R.

PY - 1993

Y1 - 1993

N2 - Following constructions in the case of canonical and affine coherent states, a universal propagator for a general Hamiltonian appropriate to a single spin degree of freedom is introduced. The universal propagator is a single function, independent of any particular choice of fiducial vector, which, nonetheless, propagates all coherent state Hubert space representatives correctly. Furthermore, we explicitly construct the universal propagator for several examples.

AB - Following constructions in the case of canonical and affine coherent states, a universal propagator for a general Hamiltonian appropriate to a single spin degree of freedom is introduced. The universal propagator is a single function, independent of any particular choice of fiducial vector, which, nonetheless, propagates all coherent state Hubert space representatives correctly. Furthermore, we explicitly construct the universal propagator for several examples.

UR - http://www.scopus.com/inward/record.url?scp=21144479440&partnerID=8YFLogxK

UR - http://www.scopus.com/inward/citedby.url?scp=21144479440&partnerID=8YFLogxK

M3 - Article

AN - SCOPUS:21144479440

VL - 34

SP - 2893

EP - 2913

JO - Journal of Mathematical Physics

JF - Journal of Mathematical Physics

SN - 0022-2488

IS - 7

ER -