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  2. Poisson bracket - Wikipedia

    en.wikipedia.org/wiki/Poisson_bracket

    In a more general sense, the Poisson bracket is used to define a Poisson algebra, of which the algebra of functions on a Poisson manifold is a special case. There are other general examples, as well: it occurs in the theory of Lie algebras , where the tensor algebra of a Lie algebra forms a Poisson algebra; a detailed construction of how this ...

  3. Four-momentum - Wikipedia

    en.wikipedia.org/wiki/Four-momentum

    Momentum is a vector in three dimensions; similarly four-momentum is a four-vector in spacetime. The contravariant four-momentum of a particle with relativistic energy E and three-momentum p = (p x, p y, p z) = γmv, where v is the particle's three-velocity and γ the Lorentz factor, is = (,,,) = (,,,). The quantity mv of above is the ordinary ...

  4. 4th Dimension (software) - Wikipedia

    en.wikipedia.org/wiki/4th_Dimension_(software)

    There are also over 100 third-party plugins, free and commercial. 4D can also be used as a web server , to run compiled database applications. Today, 4D is published by the French company 4D SAS and has a sales, distribution and support presence in most major markets, with the United States, the United Kingdom, and France being the primary markets.

  5. Canonical commutation relation - Wikipedia

    en.wikipedia.org/wiki/Canonical_commutation_relation

    In 1946, Hip Groenewold demonstrated that a general systematic correspondence between quantum commutators and Poisson brackets could not hold consistently. [4] [5] However, he further appreciated that such a systematic correspondence does, in fact, exist between the quantum commutator and a deformation of the Poisson bracket, today called the ...

  6. Constant of motion - Wikipedia

    en.wikipedia.org/wiki/Constant_of_motion

    Another useful result is Poisson's theorem, which states that if two quantities and are constants of motion, so is their Poisson bracket {,}. A system with n degrees of freedom, and n constants of motion, such that the Poisson bracket of any pair of constants of motion vanishes, is known as a completely integrable system .

  7. Hamiltonian mechanics - Wikipedia

    en.wikipedia.org/wiki/Hamiltonian_mechanics

    The symplectic structure induces a Poisson bracket. The Poisson bracket gives the space of functions on the manifold the structure of a Lie algebra. If F and G are smooth functions on M then the smooth function ω(J(dF), J(dG)) is properly defined; it is called a Poisson bracket of functions F and G and is denoted {F, G}. The Poisson bracket ...

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