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An Introduction to Algebra and Geometry via Matrix Groups
An Introduction to Algebra and Geometry via Matrix Groups

... theory of vector spaces over arbitrary fields, and bilinear forms on such vector spaces. We can then define the orthogonal and symplectic group with respect to the bilinear forms. The tools we introduce allow us to determine the generators for the general linear group, the orthogonal group, the symp ...
SURFACE WAVE PROPAGATION IN A DIELECTRIC WAVEGUIDE
SURFACE WAVE PROPAGATION IN A DIELECTRIC WAVEGUIDE

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On Fitting ideals of logarithmic vector fields and Saito`s criterion
On Fitting ideals of logarithmic vector fields and Saito`s criterion

PROJECTIVE MODULES AND VECTOR BUNDLES The basic
PROJECTIVE MODULES AND VECTOR BUNDLES The basic

... of any surjective m × n matrix σ: Rn → Rm is a stably free module, because a lift of a basis for Rm yields a decomposition P ⊕ Rm ∼ = Rn . This raises a question: when are stably free modules free? Over some rings every stably free module is free (fields, Z and the matrix rings Mn (F ) of Example 1. ...
5 Markov Chains
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Nonequilibrium fluctuations, fluctuation theorems
Nonequilibrium fluctuations, fluctuation theorems

Stan: A Probabilistic Programming Language
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Introduction to Modern Canonical Quantum General Relativity

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MATH 22A: LINEAR ALGEBRA Chapter 2

Newtonian Dynamics - Richard Fitzpatrick
Newtonian Dynamics - Richard Fitzpatrick

The geometry and topology of toric hyperkahler manifolds
The geometry and topology of toric hyperkahler manifolds

... We shall study various topological and metric properties of toric hyperkahler manifolds. First we give necessary and sufficient conditions for a hyperkahler quotient M of quaternionic space by our torus actions to be smooth (Theorem 3.2) or an orbifold (Theorem 3.3). When smooth, M is complete as a ...
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Armstrong on Quantities and Resemblance

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Longitudinal and transverse response of the electron gas

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VECTOR BUNDLES ON RIEMANN SURFACES

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Limit theorems for conditioned multitype Dawson

... Let us remark that we introduced a variance parameter c which is typeindependent. In fact we could replace it by a vector c = (c1 ; · · · ; ck ), where ci corresponds to type i. If inf 1≤i≤k ci > 0, then all the results of this paper are still true. We decided to take c independent of the type to si ...
PDF of Version 2.01-B of GIAA here.
PDF of Version 2.01-B of GIAA here.

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... notes were invaluable and reasonably well written. However, they also told me that the notes were next to useless without also attending the lectures. So, don’t get caught in the trap of thinking ‘well, I have the notes, maybe it’s OK if I skip class today to take care of an important errand....’ Ye ...
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Chapter 3 Electric Flux Density, Gauss` Law, and Divergence

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Factoring Integers with the Self-Initializing Quadratic - crypto

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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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