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  • is called the Feynman slash notation. The slash operation maps the basis of V, or any 4 dimensional vector space, to basis vectors γμ. The transformation...
    60 KB (7,209 words) - 14:01, 14 March 2024
  • Thumbnail for Polylogarithm
    }(2k\pi i-\mu )^{s-1}.} This will hold for Re(s) < 0 and all μ except where = 1. For 0 < Im(µ) ≤ 2π the sum can be split as: Li s ⁡ ( e μ ) = Γ ( 1 − s )...
    60 KB (10,172 words) - 09:02, 23 April 2024
  • Thumbnail for Jhelum
    Jhelum (redirect from Jhelum-I)
    Porus the Elder. Abisares (or Abhisara; in Greek Αβισαρης), called Embisarus ( Oβισαρoς) by Diodorus, was an Indian king of the Abhira tribe. descent beyond...
    50 KB (3,875 words) - 23:56, 5 April 2024
  • Thumbnail for Laplace distribution
    P(μ+Z1>Z2)={(2−μ)4,when μ<01−e−μ(2+μ)4,when μ>0{\displaystyle P(\mu +Z_{1}>Z_{2})={\begin{cases}e^{\mu }{\frac {(2-\mu )}{4}},&{\text{when }}\mu <0\\1-e^{-\mu...
    21 KB (2,870 words) - 19:23, 6 April 2024
  • Thumbnail for Differential operator
    which determine fiber coordinates ξi. In terms of a basis of frames , fν of E and F, respectively, the differential operator P decomposes into components...
    22 KB (3,650 words) - 11:48, 7 November 2023
  • Thumbnail for Minkowski space
    written (v0, v1, v2, v3) where the Einstein notation is used to write v = vμ . The component v0 is called the timelike component of v while the other three...
    79 KB (10,530 words) - 23:01, 19 April 2024
  • that T{\displaystyle e^{\mu T}} is a characteristic multiplier of the system. Notice that Floquet exponents are not unique, since e(μ+2πikT)T=T{\displaystyle...
    9 KB (1,269 words) - 04:12, 15 April 2024
  • calcium are considered, terms such as e2μ appear, which is the square of ; in this case, the formula for the Goldman equation can be solved using the...
    13 KB (2,136 words) - 18:09, 14 March 2024
  • inner product (f,g) = (2π)−2∬ f(x,y) g(x,y) dx dy, so that (Σ aλ eλ, Σ bμ ) = Σ aλbλ. For f in C∞(T'2) and k an integer, define the kth Sobolev norm...
    78 KB (10,756 words) - 22:20, 25 March 2024
  • \gamma _{\mu }} into another frame of vectors {\displaystyle e_{\mu }} by the operation =RγμR†{\displaystyle e_{\mu }=R\gamma _{\mu }R^{\dagger }};: 15 ...
    44 KB (5,961 words) - 00:31, 9 April 2024
  • representations of special linear groups) Eλ⊗=⨁ν(Eν)⊕cλμν.{\displaystyle E^{\lambda }\otimes E^{\mu }=\bigoplus _{\nu }(E^{\nu })^{\oplus c_{\lambda \mu }^{\nu...
    28 KB (3,553 words) - 09:59, 26 March 2024
  • Thumbnail for Dirac equation in curved spacetime
    We use a set of vierbein or frame fields {}={e0,e1,e2,e3}{\displaystyle \{e_{\mu }\}=\{e_{0},e_{1},e_{2},e_{3}\}}, which are a set of vector fields (which...
    13 KB (2,035 words) - 07:45, 30 March 2024
  • Similarly we can construct local coframes in which ∗a(x)=δaμ−16Raσμτ(0)xσxτ+O(x2),{\displaystyle e_{\mu }^{*a}(x)=\delta _{a\mu }-{\frac {1}{6}}R_{a\sigma...
    8 KB (1,200 words) - 16:16, 6 July 2023
  • {\displaystyle f(x)={\frac {1}{2b}}e^{-{\frac {|x-\mu |}{b}}},} then the left-tail TVaR is equal to TVaRα⁡(X)={1−(2α)bb+1if α≤0.5,1−eμ2−bα(b−1)[(1−α)(1−b)−1]if α>0...
    23 KB (4,277 words) - 08:47, 23 December 2023
  • Thumbnail for Log-Cauchy distribution
    >0}. If σ{\displaystyle \sigma } is known, the scale parameter is {\displaystyle e^{\mu }}. μ{\displaystyle \mu } and σ{\displaystyle \sigma } correspond...
    12 KB (1,265 words) - 08:30, 26 June 2023
  • _{\alpha _{i}\in \Delta _{s}}\lambda _{i},} where the sum is calculated in the weight lattice P. The set of linear combinations of the exponentials with...
    12 KB (1,930 words) - 18:49, 26 January 2024
  • 1=e0{\displaystyle 1=\mathbf {e} _{0}}, so that the complete basis can be written in a compact form as {},{\displaystyle \{\mathbf {e} _{\mu }\},} where the...
    30 KB (4,065 words) - 17:24, 10 October 2023
  • polynomial satisfies: Pλ(x;q,t)=∑μ(x1,...,xn;q,t)=∑μ∑Qwt(Q){\displaystyle P_{\lambda }({\textbf {x}};q,t)=\sum _{\mu }E_{\mu }(x_{1},...,x_{n};q,t)=\sum...
    21 KB (3,046 words) - 06:56, 13 January 2024
  • F^{I_{M}}} and FI1⋯IM{\displaystyle F^{I_{1}\cdots I_{M}}} is constructed via the mapping ei11⊗⋯eimm⊗⋯⊗eiMM↦(i1,i2,…,iM),{\displaystyle \mathbf {e} _{i_{1}}^{1}\otimes...
    10 KB (1,978 words) - 22:33, 24 March 2024
  • "Simple symmetric matrix singularities and the subgroups of Weyl groups Aμ, Dμ, ", Mosc. Math. J., 3:2 (2003). J.-P. Gauthier, V. M. Zakalyukin, "On the motion...
    4 KB (255 words) - 06:36, 29 January 2023
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