classical state (changes) in nLab
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Context
Physics
physics, mathematical physics, philosophy of physics
Surveys, textbooks and lecture notes
theory (physics), model (physics)
experiment, measurement, computable physics
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Axiomatizations
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Tools
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Structural phenomena
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Types of quantum field thories
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Measure and probability theory
Contents
Idea
A classical state is a state of a system of classical mechanics.
In principle, a pure state in classical mechanics specifies completely all information about the state of the system, while a mixed state is a probability measure on the space of pure states. This space of pure states my may be identified with thestate space? in Lagrangian mechanics or with the phase space in Hamiltonian mechanics.
Definition
We give a definition in a very general context.
For AA a commutative unital associative algebra that encodes a system of classical mechanics (say, the associative algebra underlying a Poisson algebra), a classical state is an ℝ\mathbb{R}-linear function
ρ:A→ℝ \rho\colon A \to \mathbb{R}
that satisfies
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normalization ρ(1)=1\rho(1) = 1;
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positivity for all a∈Aa \in A we have ρ(a 2)≥0\rho(a^2) \geq 0.
This is essentially the definition of quantum state, but formulated for commutative algebras and over the real numbers.
If we take AA to be a **-algebra over the complex numbers, then we may take ρ\rho to be a ℂ\mathbb{C}-linear function from AA to ℂ\mathbb{C} instead.
classical mechanics | semiclassical approximation | … | formal deformation quantization | quantum mechanics | |
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order of Planck's constant ℏ\hbar | 𝒪(ℏ 0)\mathcal{O}(\hbar^0) | 𝒪(ℏ 1)\mathcal{O}(\hbar^1) | 𝒪(ℏ n)\mathcal{O}(\hbar^n) | 𝒪(ℏ ∞)\mathcal{O}(\hbar^\infty) | |
states | classical state | semiclassical state | quantum state | ||
observables | classical observable | quantum observable |
quantum probability theory – observables and states
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Last revised on July 10, 2022 at 15:42:19. See the history of this page for a list of all contributions to it.