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  2. Lorentz group - Wikipedia

    en.wikipedia.org/wiki/Lorentz_group

    Hendrik Antoon Lorentz (1853–1928), after whom the Lorentz group is named. In physics and mathematics, the Lorentz group is the group of all Lorentz transformations of Minkowski spacetime, the classical and quantum setting for all (non-gravitational) physical phenomena. The Lorentz group is named for the Dutch physicist Hendrik Lorentz.

  3. Hendrik Lorentz - Wikipedia

    en.wikipedia.org/wiki/Hendrik_Lorentz

    Hendrik Antoon Lorentz (/ ˈ l ɒr ən t s /, LORR-ənts; Dutch: [ˈɦɛndrɪk ˈloːrɛnts]; 18 July 1853 – 4 February 1928) was a Dutch theoretical physicist who shared the 1902 Nobel Prize in Physics with Pieter Zeeman for his theoretical explanation of the Zeeman effect.

  4. Representation theory of the Lorentz group - Wikipedia

    en.wikipedia.org/wiki/Representation_theory_of...

    Then, for example, (0, ⁠ 3 / 2 ⁠) and (1, ⁠ 1 / 2 ⁠) are a spin representations of dimensions 2⋅ ⁠ 3 / 2 ⁠ + 1 = 4 and (2 + 1)(2⋅ ⁠ 1 / 2 ⁠ + 1) = 6 respectively. According to the above paragraph, there are subspaces with spin both ⁠ 3 / 2 ⁠ and ⁠ 1 / 2 ⁠ in the last two cases, so these representations cannot likely ...

  5. Derivations of the Lorentz transformations - Wikipedia

    en.wikipedia.org/wiki/Derivations_of_the_Lorentz...

    In the fundamental branches of modern physics, namely general relativity and its widely applicable subset special relativity, as well as relativistic quantum mechanics and relativistic quantum field theory, the Lorentz transformation is the transformation rule under which all four-vectors and tensors containing physical quantities transform from one frame of reference to another.

  6. Covariant formulation of classical electromagnetism - Wikipedia

    en.wikipedia.org/wiki/Covariant_formulation_of...

    The covariant formulation of classical electromagnetism refers to ways of writing the laws of classical electromagnetism (in particular, Maxwell's equations and the Lorentz force) in a form that is manifestly invariant under Lorentz transformations, in the formalism of special relativity using rectilinear inertial coordinate systems.

  7. Lorentz transformation - Wikipedia

    en.wikipedia.org/wiki/Lorentz_transformation

    The quantity on the left is called the spacetime interval between events a 1 = (t 1, x 1, y 1, z 1) and a 2 = (t 2, x 2, y 2, z 2). The interval between any two events, not necessarily separated by light signals, is in fact invariant, i.e., independent of the state of relative motion of observers in different inertial frames, as is shown using ...

  8. Category:Hendrik Lorentz - Wikipedia

    en.wikipedia.org/wiki/Category:Hendrik_Lorentz

    This is a topic category for the topic Hendrik Lorentz ... Lorentz–Lorenz equation; Lorentz-violating electrodynamics; Lorentzian algebra;

  9. Heaviside–Lorentz units - Wikipedia

    en.wikipedia.org/wiki/Heaviside–Lorentz_units

    Coulomb's equation, used to define charge in these systems, is F = q G 1 q G 2 / r 2 in the Gaussian system, and F = q HL 1 q HL 2 / (4πr 2) in the HL system. The unit of charge then connects to 1 dyn⋅cm 2 = 1 statC 2 = 4π HLC 2, where 'HLC' is the HL unit of charge.

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