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First quantization is a procedure for converting equations of classical particle equations into quantum wave equations. The companion concept of second quantization converts classical field equations in to quantum field equations.
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quantization displaystyle quantum theory classical state first function schrödinger mechanics second system equation particle wave particles however mass two single
| Subject | Predicate | Object | Confidence | Src |
|---|---|---|---|---|
| First quantization | is a | procedure for converting equations of classical particle equations into quantum wave equations | 0.90 | text |
| Wien's displacement law | instance of | this era was based solely on purely classical arguments | 0.80 | text |
| thermodynamics | instance of | this era was based solely on purely classical arguments | 0.80 | text |
| statistical mechanics | instance of | this era was based solely on purely classical arguments | 0.80 | text |
| and the electromagnetic theory | instance of | this era was based solely on purely classical arguments | 0.80 | text |
| the position of the system | instance of | it is natural to seek solutions of the Newton equation that are at least second order differentiable.Quantum theory differs dramatically in that it replaces physical observables | 0.80 | text |
| the time at which that observation is made | instance of | it is natural to seek solutions of the Newton equation that are at least second order differentiable.Quantum theory differs dramatically in that it replaces physical observables | 0.80 | text |
| the mass | instance of | it is natural to seek solutions of the Newton equation that are at least second order differentiable.Quantum theory differs dramatically in that it replaces physical observables | 0.80 | text |
| and the velocity of the system at the instant of observation with the notion of operator observables | instance of | it is natural to seek solutions of the Newton equation that are at least second order differentiable.Quantum theory differs dramatically in that it replaces physical observables | 0.80 | text |
| mass | instance of | systems containing N identical particles i.e. particles characterized by the same physical parameters | 0.80 | text |
| charge | instance of | systems containing N identical particles i.e. particles characterized by the same physical parameters | 0.80 | text |
| spin | instance of | systems containing N identical particles i.e. particles characterized by the same physical parameters | 0.80 | text |
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