• Thumbnail for Covariant transformation
    In physics, a covariant transformation is a rule that specifies how certain entities, such as vectors or tensors, change under a change of basis. The transformation...
    15 KB (2,544 words) - 05:20, 3 June 2024
  • Thumbnail for Covariance and contravariance of vectors
    and a covariant vector is a list of numbers that transforms in the same way. Contravariant vectors are often just called vectors and covariant vectors...
    35 KB (5,573 words) - 06:38, 14 July 2024
  • derivative transforms covariantly under a general coordinate transformation, that is, linearly via the Jacobian matrix of the transformation. This article presents...
    36 KB (6,354 words) - 20:38, 2 May 2024
  • general covariant transformations are symmetries of gravitation theory on a world manifold X {\displaystyle X} . They are gauge transformations whose parameter...
    5 KB (784 words) - 14:58, 23 July 2022
  • Thumbnail for Tensor
    some combination of covariant and contravariant transformations, with one transformation law for each index. If the transformation matrix of an index is...
    69 KB (9,354 words) - 17:48, 12 July 2024
  • such gauge transformations, because they depend on the local frame. However, when gauge transformations act on fields and the gauge covariant derivative...
    25 KB (4,483 words) - 03:08, 22 May 2024
  • Thumbnail for Lorentz transformation
    In physics, the Lorentz transformations are a six-parameter family of linear transformations from a coordinate frame in spacetime to another frame that...
    103 KB (14,094 words) - 22:06, 27 May 2024
  • contravariance Covariant derivative Fictitious force Galilean invariance Gauge covariant derivative General covariant transformations Harmonic coordinate...
    6 KB (657 words) - 00:01, 23 May 2024
  • linear transformations. Covariance and contravariance of vectors, properties of how vector coordinates change under a change of basis Covariant transformation...
    2 KB (285 words) - 12:08, 16 November 2019
  • one-form has a covariant transformation law on passing from one coordinate system to another. Thus a one-form is an order 1 covariant tensor field. The...
    5 KB (744 words) - 16:50, 12 July 2024
  • In particular, a Lorentz covariant scalar (e.g., the space-time interval) remains the same under Lorentz transformations and is said to be a Lorentz...
    21 KB (2,917 words) - 07:22, 22 June 2024
  • linear algebra, a linear map (also called a linear mapping, linear transformation, vector space homomorphism, or in some contexts linear function) is...
    43 KB (7,001 words) - 21:10, 13 July 2024
  • Thumbnail for Gauge theory
    \mathbf {F} } transforms covariantly. Not all gauge transformations can be generated by infinitesimal gauge transformations in general. An example is...
    47 KB (6,757 words) - 00:00, 10 April 2024
  • vector is called covariant or contravariant depending on how the transformation of the vector's components is related to the transformation of coordinates...
    27 KB (3,173 words) - 02:08, 2 May 2024
  • Thumbnail for Cartesian tensor
    components from one such basis to another is done through an orthogonal transformation. The most familiar coordinate systems are the two-dimensional and three-dimensional...
    67 KB (11,700 words) - 19:53, 26 February 2024
  • Thumbnail for Covariant formulation of classical electromagnetism
    The covariant formulation of classical electromagnetism refers to ways of writing the laws of classical electromagnetism (in particular, Maxwell's equations...
    24 KB (3,930 words) - 17:09, 22 June 2024
  • G^{\text{op}}} are thus "turned around". Forming the opposite group becomes a (covariant) functor from Grp {\displaystyle {\textbf {Grp}}} to Grp {\displaystyle...
    33 KB (5,663 words) - 12:43, 25 June 2024
  • In physics, a Galilean transformation is used to transform between the coordinates of two reference frames which differ only by constant relative motion...
    17 KB (2,572 words) - 15:35, 14 July 2023
  • Functor (redirect from Covariant functor)
    called covariant functors in order to distinguish them from contravariant ones. Note that one can also define a contravariant functor as a covariant functor...
    24 KB (3,336 words) - 07:27, 6 June 2024
  • internal symmetries encountered a problem of treating general covariant transformations and establishing the gauge status of a pseudo-Riemannian metric...
    9 KB (1,155 words) - 00:01, 25 December 2023
  • matrix whose entries transform covariantly under changes to the coordinate system. Thus a metric tensor is a covariant symmetric tensor. From the coordinate-independent...
    56 KB (8,866 words) - 03:18, 8 July 2024
  • on a principal frame bundle whose gauge symmetries are general covariant transformations which are not elements of a gauge group. In the physical literature...
    3 KB (529 words) - 21:30, 12 May 2024
  • are used to label a variable object as covariant (lower index), contravariant (upper index), or mixed covariant and contravariant (having both upper and...
    13 KB (1,906 words) - 17:49, 5 July 2024
  • Thumbnail for Curvilinear coordinates
    components, Si j the mixed right-covariant components, Si j the mixed left-covariant components, and Sij the covariant components of the second-order tensor...
    52 KB (8,289 words) - 07:39, 16 May 2024
  • Thumbnail for Gauge fixing
    however, not Lorentz covariant. If a Lorentz transformation to a new inertial frame is carried out, a further gauge transformation has to be made to retain...
    28 KB (4,271 words) - 21:58, 2 May 2024
  • ^{i}}_{jk}={\Gamma ^{i}}_{kj}.} The index-less transformation properties of a tensor are given by pullbacks for covariant indices, and pushforwards for contravariant...
    42 KB (7,076 words) - 16:07, 8 July 2024
  • A = H o m ( A , − ) {\displaystyle h_{A}=\mathrm {Hom} (A,-)} . The (covariant) hom-functor h A {\displaystyle h_{A}} sends X ∈ C {\displaystyle X\in...
    20 KB (3,358 words) - 13:16, 28 May 2024
  • Thumbnail for Gluon field
    position r and time t. Matrix exponentiation is used in the transformation. The gauge covariant derivative transforms similarly. The functions θn here are...
    12 KB (1,542 words) - 08:42, 4 March 2023
  • Thumbnail for Special relativity
    coordinates. More generally, the covariant components of a 4-vector transform according to the inverse Lorentz transformation: T μ ′ = Λ μ ′ ν T ν , {\displaystyle...
    187 KB (25,128 words) - 16:44, 12 July 2024
  • quantities must transform covariantly, that is, under a certain representation of the group of coordinate transformations between admissible frames of...
    4 KB (471 words) - 01:47, 13 March 2024