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Published equation contexts

Hf=HS⊗IB+IS⊗HB+HSBH_f = H_S \otimes I_B + I_S \otimes H_B + H_{SB}

Why this formula appears here

Start with the setting the open-quantum-systems literature calls a fine description: a Hilbert space Hf\mathcal H_f = HS\mathcal H_S ⊗\otimes HB\mathcal H_B holding a system S and everything else, B , that a working physicist has decided not to track in detail — a resonant bath, an environment, a set of nuclear spins, whatever “everything else” means for the apparatus at hand. The fine Hamiltonian is Hf=HS⊗IB+IS⊗HB+HSBH_f = H_S \otimes I_B + I_S \otimes H_B + H_{SB}. three Hermitian terms, each in units of energy: the system’s own generator, the bath’s own generator, and an interaction coupling the two. A fine state is a density operator ρ\rho on Hf\mathcal H_f — trace one, positive semidefinite, dimensionless as a probability object.

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Published contexts (1)

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Hf=HS⊗IB+IS⊗HB+HSB,H_f = H_S \otimes I_B + I_S \otimes H_B + H_{SB},

Equation 4 · Evolutionary Physics

The Entry a Relabeling Cannot Write

This equation states an equality: the expressions on both sides have the same value under the article’s assumptions.

Start with the setting the open-quantum-systems literature calls a fine description: a Hilbert space Hf\mathcal H_f = HS\mathcal H_S ⊗\otimes HB\mathcal H_B holding a system S and everything else, B , that a working physicist has decided not to track in detail — a resonant bath, an environment, a set of nuclear spins, whatever “everything else” means for the apparatus at hand. The fine Hamiltonian is Hf=HS⊗IB+IS⊗HB+HSBH_f = H_S \otimes I_B + I_S \otimes H_B + H_{SB}. three Hermitian terms, each in units of energy: the system’s own generator, the bath’s own generator, and an interaction coupling the two. A fine state is a density operator ρ\rho on Hf\mathcal H_f — trace one, positive semidefinite, dimensionless as a probability object.

Meanings in this article

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