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- is called the Feynman slash notation. The slash operation maps the basis eμ of V, or any 4 dimensional vector space, to basis vectors γμ. The transformation...60 KB (7,209 words) - 14:01, 14 March 2024
- that eμT{\displaystyle e^{\mu T}} is a characteristic multiplier of the system. Notice that Floquet exponents are not unique, since e(μ+2πikT)T=eμT{\displaystyle...9 KB (1,269 words) - 04:12, 15 April 2024
- calcium are considered, terms such as e2μ appear, which is the square of eμ; 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 eμ) = 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 eμ{\displaystyle e_{\mu }} by the operation eμ=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⊗Eμ=⨁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
- Similarly we can construct local coframes in which eμ∗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−eμ(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
- _{\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 eμ 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 {eμ},{\displaystyle \{\mathbf {e} _{\mu }\},} where the...30 KB (4,065 words) - 17:24, 10 October 2023
- polynomial satisfies: Pλ(x;q,t)=∑μEμ(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↦eμ(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, Eμ", Mosc. Math. J., 3:2 (2003). J.-P. Gauthier, V. M. Zakalyukin, "On the motion...4 KB (255 words) - 06:36, 29 January 2023
- same quadric. If the equation of a linear complex is Al + Bm + Cn + Dλ + Eμ + Fν = 0, then for a line not belonging to the complex we may regard the expression
- because eμ+σ2/2=⟨VfVi⟩=⟨Vf⟩Vi{\displaystyle e^{\mu +\sigma ^{2}/2}=\langle {\frac {V_{f}}{V_{i}}}\rangle ={\frac {\langle V_{f}\rangle }{V_{i}}}} but