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  2. Interaction picture - Wikipedia

    en.wikipedia.org/wiki/Interaction_picture

    By utilizing the interaction picture, one can use time-dependent perturbation theory to find the effect of H 1,I, [15]: 355ff e.g., in the derivation of Fermi's golden rule, [15]: 359–363 or the Dyson series [15]: 355–357 in quantum field theory: in 1947, Shin'ichirō Tomonaga and Julian Schwinger appreciated that covariant perturbation ...

  3. Heisenberg picture - Wikipedia

    en.wikipedia.org/wiki/Heisenberg_picture

    For the sake of pedagogy, the Heisenberg picture is introduced here from the subsequent, but more familiar, Schrödinger picture. According to Schrödinger's equation, the quantum state at time is | = | , where () = is the time-evolution operator induced by a Hamiltonian () that could depend on time, and | is the initial state.

  4. Dynamical pictures - Wikipedia

    en.wikipedia.org/wiki/Dynamical_pictures

    The Heisenberg picture is closest to classical Hamiltonian mechanics (for example, the commutators appearing in the above equations directly correspond to classical Poisson brackets). The Schrödinger picture, the preferred formulation in introductory texts, is easy to visualize in terms of Hilbert space rotations of state vectors, although it ...

  5. Matrix mechanics - Wikipedia

    en.wikipedia.org/wiki/Matrix_mechanics

    Heisenberg went on to say that Born and Jordan's contribution to quantum mechanics cannot be changed by "a wrong decision from the outside". [28] In 1954, Heisenberg wrote an article honoring Max Planck for his insight in 1900. In the article, Heisenberg credited Born and Jordan for the final mathematical formulation of matrix mechanics and ...

  6. Schrödinger picture - Wikipedia

    en.wikipedia.org/wiki/Schrödinger_picture

    In physics, the Schrödinger picture or Schrödinger representation is a formulation of quantum mechanics in which the state vectors evolve in time, but the operators (observables and others) are mostly constant with respect to time (an exception is the Hamiltonian which may change if the potential changes).

  7. Bethe ansatz - Wikipedia

    en.wikipedia.org/wiki/Bethe_ansatz

    In physics, the Bethe ansatz is an ansatz for finding the exact wavefunctions of certain quantum many-body models, most commonly for one-dimensional lattice models.It was first used by Hans Bethe in 1931 to find the exact eigenvalues and eigenvectors of the one-dimensional antiferromagnetic isotropic (XXX) Heisenberg model.

  8. Heisenberg model - Wikipedia

    en.wikipedia.org/wiki/Heisenberg_model

    Heisenberg model can refer to two models in statistical mechanics: Heisenberg model (classical), a classical nearest neighbour spin model; Heisenberg model (quantum ...

  9. Quantum Heisenberg model - Wikipedia

    en.wikipedia.org/wiki/Quantum_Heisenberg_model

    It is common to name the model depending on the values of , and : if , the model is called the Heisenberg XYZ model; in the case of = = =, it is the Heisenberg XXZ model; if = = =, it is the Heisenberg XXX model. The spin 1/2 Heisenberg model in one dimension may be solved exactly using the Bethe ansatz. [1]