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Genus Two Zhu Theory for Vertex Operator Algebras
Genus Two Zhu Theory for Vertex Operator Algebras

Lectures on Lie groups and geometry
Lectures on Lie groups and geometry

02PCYQW_2016_Lagrange_approach - LaDiSpe
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The Magnitude of Metric Spaces
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gravitation, gauge theories and differential geometry

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Ab Initio Nuclear Structure Calculations for Light Nuclei

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... Frictional force depends on the materials that the surfaces are made of. For example, there is more friction between skis and concrete than there is between skis and snow. The normal force between the two objects also matters. The harder one object is pushed against the other, the greater the force ...
An introduction to Lagrangian and Hamiltonian mechanics
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MODULE : 1 Lecture 1 : Key words : Scalar, Vector, Field, position
MODULE : 1 Lecture 1 : Key words : Scalar, Vector, Field, position

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Universal Identities I

... for indeterminates A, B, C, A0 , B 0 , and C 0 and f, g, and h in Z[A, B, C, A0 , B 0 , C 0 ]. Notice (2.1) implies a similar formula for sums of three squares in any commutative ring by specializing the 6 indeterminates to any 6 elements of any commutative ring. So (2.1) implies that sums of three ...
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array-expr i

Quadratic sieve
Quadratic sieve

R -1 - WordPress.com
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Linear Dependence and Linear Independence
Linear Dependence and Linear Independence

Lectures on Atomic Physics
Lectures on Atomic Physics

sparse matrices in matlab: design and implementation
sparse matrices in matlab: design and implementation

Notes 4: The exponential map.
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Introduction to representation theory of finite groups
Introduction to representation theory of finite groups

... Thus, the linear span of v is a one-dimensional subrepresentation of K[G], which is isomorphic to the trivial representation. In particular, the regular representation is never irreducible, unless |G| = 1. Definition 1.9. Let V and W be two representations of G. The direct sum of V and W is the repr ...
INTRODUCTORY LINEAR ALGEBRA
INTRODUCTORY LINEAR ALGEBRA

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Four-vector

In the theory of relativity, a four-vector or 4-vector is a vector in Minkowski space, a four-dimensional real vector space. It differs from a Euclidean vector in how its magnitude is determined. The transformations that preserve this magnitude are the Lorentz transformations, which include spatial rotations, boosts (a change by a constant velocity to another inertial reference frame), and temporal and spatial inversions. Regarded as a homogeneous space, the transformation group of Minkowski space is the Poincaré group, which adds to the Lorentz group the group of translations. The Lorentz group may be represented by 4×4 matrices.The article considers four-vectors in the context of special relativity. Although the concept of four-vectors also extends to general relativity, some of the results stated in this article require modification in general relativity.
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