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- W2792849173 abstract "We need to extend the quantum mechanical theory to the case of N particles; separately, the particles would be described by a Schrodinger equation or the Pauli equation, depending on their spins. As in the classical case, the Hamiltonian of the system will be the sum of those of the particles plus an interaction term (possibly). For independent particles (no interaction), the Hamiltonian is, in obvious notation $$ hat{H}(1,2,ldots , N)= sum _{n}^N hat{h}(n), $$where h(n) describes particle n. The wave function (varPsi (1,2,ldots , N)) depends on all the orbital and spin degrees of freedom of the particles, so it is a spinor in the spin space of each particle." @default.
- W2792849173 created "2018-03-29" @default.
- W2792849173 creator A5056552760 @default.
- W2792849173 date "2018-01-01" @default.
- W2792849173 modified "2023-09-27" @default.
- W2792849173 title "Systems of Particles" @default.
- W2792849173 doi "https://doi.org/10.1007/978-3-319-71330-4_19" @default.
- W2792849173 hasPublicationYear "2018" @default.
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