Klaus Mølmer 2026-11-05
Klaus Mølmer helped develop a wave-function description of dissipative quantum evolution with Yvan Castin and Jean Dalibard. Their 1992 manuscript, reproduced in 2008, represents individual conditioned evolutions through stochastic jumps and intervening nonunitary evolution.[ref]
Averaging many trajectories recovers the corresponding Lindblad equation. This quantum-trajectory unravelling connects an ensemble density operator with possible individual measurement records; the trajectory depends on how the environment is monitored.
Quantum Trajectory Theory Created 2026-10-14 Updated 2026-11-05
A quantum Trajectory Theory unravelling represents a Lindblad equation by an ensemble of stochastic pure states. In units , define the non-Hermitian effective Hamiltonian
For a normalized state , channel has instantaneous jump rate . During a small interval , that jump occurs with probability and sends the state to . A zero rate means that channel cannot jump. Otherwise, with total no-jump probability , evolve with and renormalize.
To verify the ensemble evolution, put . The conditional normalizations cancel their probability weights, giving
Expanding recovers the Lindblad equation. Different monitoring choices can give different trajectories with the same ensemble density matrix. For spontaneous emission, gives jump rate and resets the atom to its ground state.[ref]
Yvan Castin 2026-11-05
Yvan Castin, with Jean Dalibard and Klaus Mølmer, formulated a stochastic wave-function approach to dissipative quantum systems. Their construction samples conditional jumps and no-jump evolution so that the ensemble reproduces a density-operator master equation.[ref]
Using state vectors can reduce the cost of numerical simulations compared with directly storing a full density matrix, although many trajectories may be needed for precise averages. The 2008 posting reproduces a 1992 manuscript and explicitly acknowledges earlier related quantum-filtering work.