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1. Group actions and other topics in group theory
1. Group actions and other topics in group theory

... Representation theory is one of the major branches of mathematics. We’ll consider representation theory of finite groups in some detail, especially over C. Example. Let F be a field, and suppose G acts on F via field automorphisms. This is precisely the situation one studies in Galois theory. Exampl ...
Section III.15. Factor-Group Computations and Simple
Section III.15. Factor-Group Computations and Simple

... Z2 and the square of each element (coset) is the identity (H). So H · H = H and (σH) · (σH) = σ2 H = H. So if α ∈ H then α2 ∈ H and if β ∈ / H (then β ∈ σH) then β 2 ∈ H. So, the square of every element of A4 is in H. But in A4 we have (1, 2, 3) = (1, 3, 2)2 and (1, 3, 2) = (1, 2, 3)2 (1, 2, 4) = (1 ...
Group Theory G13GTH
Group Theory G13GTH

... Generalisations of this theorem to multiple products H1 × H2 × · · · × Hk are immediate. The condition (b) can also be rephrased by asking that G = HK and H ∩ K = {1}; see the lemma 1.8 below. Example. Let G be the dihedral group D6 of order 12. Inside the regular hexagon, we find the regular triang ...
LIE ALGEBRAS OF CHARACTERISTIC 2Q
LIE ALGEBRAS OF CHARACTERISTIC 2Q

... form of the root diagrams. Brown retains most of the common properties of root spaces and root diagrams by altering the definitions of root spaces and roots. ...
GENERALIZED CAYLEY`S Ω-PROCESS 1. Introduction We assume
GENERALIZED CAYLEY`S Ω-PROCESS 1. Introduction We assume

... We assume throughout that the base field k is algebraically closed of characteristic zero and that all the geometric and algebraic objetcs are defined over k. A linear algebraic monoid is an affine normal algebraic variety M with an associative product M × M → M which is a morphism of algebraic k–va ...
Chapter 1 ``Semisimple modules
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... of cardinality a positive power of p. Since 0 is a G-fixed point in W , there is, by Eq. (1.7), at least one other G-fixed element in W . The k-span of this element is, on the one hand, a non-zero G-invariant subspace of V and so equals V , and, on the other, trivial as a kG-module. Yet another proo ...
ESCI 342 – Atmospheric Dynamics I Lesson 1 – Vectors and Vector
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...  In spherical coordinates for the Earth, the position of a point is given by its distance from the center of the Earth, r; the latitude, φ ; and the longitude, λ . ο The unit vectors in spherical coordinates are the same as in Cartesian coordinates, with iˆ , ĵ , and k̂ pointing toward the East, N ...
Representations on Hessenberg Varieties and Young`s Rule
Representations on Hessenberg Varieties and Young`s Rule

... Fix G = GLn (C) and let B be the subgroup of upper-triangular matrices. Let the respective Lie algebras be g and b. The flag variety is the homogenous space G/B. It is known to be a smooth complex projective variety [H, Section 21]. Hessenberg varieties are a family of subvarieties of the flag varie ...
Eigenvalues and Eigenvectors
Eigenvalues and Eigenvectors

... We cannot compute L(x1 , x2 ) until we specify which basis G we used. Let’s assume that G = {gg 1 , g 2 }. Then we know that L(gg 1 ) = 2gg 1 + 0gg 2 = 2gg 1 and L(gg 2 ) = 0gg 1 + 3gg 2 = 3gg 2 . Thus, L(gg k ) just multiplies g k by the corresponding element in the main diagonal of A. Figure 5.1 i ...
Notes 11: Roots.
Notes 11: Roots.

... We now proceed to search for the reflections sα in the Weyl group of G. The clue is to study the centralizers of the groups Uα . We shall show, in theorem 1 below, that these centralizers are connected (even though Uα is not necessarily connected) and that their Weyl groups all are of order two. As ...
Representations on Hessenberg Varieties and Young`s Rule
Representations on Hessenberg Varieties and Young`s Rule

... Fix G = GLn (C) and let B be the subgroup of upper-triangular matrices. Let the respective Lie algebras be g and b. The flag variety is the homogenous space G/B. It is known to be a smooth complex projective variety [H, Section 21]. Hessenberg varieties are a family of subvarieties of the flag varie ...
Graded Brauer groups and K-theory with local coefficients
Graded Brauer groups and K-theory with local coefficients

... Lemma 4. — If^ and SS are bundles of [8; %]'s and [8; T^'J'S respectively on X, then w(^0^)==w^).w{^). Proof.—The maps E^—^Zg and E^—^Zg will both be denoted by a\^a. Choose an open cover U=={UJ of X such that the restrictions of ^ and 3§ to each U^ are product bundles. Set U^==U,nUj and U^==U,nU,nU ...
Asymptotic Behavior of the Weyl Function for One
Asymptotic Behavior of the Weyl Function for One

... We want to extend the idea of absolutely continuous functions to intervals of infinite length. Definition 1.11. Let (a, b) be an arbitrary interval with −∞ ≤ a < b ≤ +∞ and let µ be a locally finite complex Borel measure. A function f : (a, b) → C is called locally absolutely continuous with respect ...
Reverse mathematics and fully ordered groups 1 Introduction Reed Solomon
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KMS states on self-similar groupoid actions
KMS states on self-similar groupoid actions

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A gentle introduction to von Neumann algebras for model theorists
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... nontrivial conjugacy classes are infinite; we call a group with this property ICC (for infinite conjugacy classes). We have thus established: Proposition 2.7. If Γ is an ICC group, then L(Γ) is a factor. Another example of a factor is B(H) for any Hilbert space H. Fact 2.8. Every von Neumann algebra ...
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... A G-compactification of a G-space X is a G-map ν : X → Y with a dense range into a compact G-space Y . A compactification is proper when ν is a topological embedding. The study of equivariant compactifications goes back to J. de Groot, R. Palais, R. Brook, J. de Vries, Yu. Smirnov and others. The Ge ...
Quaternion Algebras and Quadratic Forms - UWSpace
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... The set D(f ) is always closed under inverses, since d ∈ D(f ) iff d−1 = (d−1 )2 d ∈ D(f ). However, f might not represent 1, so D(f ) might not contain the identity and is thus not a group. Even if it contains 1, it may not be closed under multiplication. Consider the form f = X 2 +Y 2 +Z 2 over Q ...
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... finite lists (also known as words, strings) of elements from A. F is a monad as follows: • Functor: for f : A → B, define f∗ : A∗ → B∗ by f∗[a1, . . . , an] = [f(a1), . . . , f(an)]. • Unit: we define ηA : A → A∗ by ηA(a) = [a] ...
DILATION OF THE WEYL SYMBOL AND BALIAN
DILATION OF THE WEYL SYMBOL AND BALIAN

... rotations, shearing and other operations close to the identity) described in the next theorem. In order to formulate it properly we write ρΛ = (ρλ)λ∈Λ , for Λ ⊂ R2n and a matrix ρ ∈ GL(2n, R). For the regular case, i.e. for the case that Λ is a discrete lattice in R2n , this result has been given in ...
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... Lemma 17. Let Q be a finite double loop in which addition is associative and the right distributive law holds. Then (1) (−a)b = −ab for all a, b ∈ Q, (2) hQ, +, 0i is an elementary abelian p-group, i.e., there is a prime p such that |Q| = pk and every element of Q has additive order p, and (3) prope ...
1. Divisors Let X be a complete non-singular curve. Definition 1.1. A
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... inseparable extensions. We say that ϕ : X → Y is purely inseparable if the corresponding function field extension k(X) ⊃ k(Y ) is purely inseparable. Note that a purely inseparable ϕ : X → Y of degree p is everywhere ramified with ramification index p. If P ∈ X and πP ∈ k(X) is a generator of the ma ...
COMPUTING RAY CLASS GROUPS, CONDUCTORS AND
COMPUTING RAY CLASS GROUPS, CONDUCTORS AND

... Finding a generator g0 of the finite field (ZK /p)∗ is easily done if q − 1 is completely factored, simply by trying random elements. Since the probability of finding a generator is φ(q − 1)/(q − 1) (where φ is Euler’s function), this is close enough to 1 in general, so g0 will be found rapidly. On ...
Non-Commutative Arithmetic Circuits with Division
Non-Commutative Arithmetic Circuits with Division

Non-Commutative Arithmetic Circuits with Division
Non-Commutative Arithmetic Circuits with Division

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Oscillator representation

In mathematics, the oscillator representation is a projective unitary representation of the symplectic group, first investigated by Irving Segal, David Shale, and André Weil. A natural extension of the representation leads to a semigroup of contraction operators, introduced as the oscillator semigroup by Roger Howe in 1988. The semigroup had previously been studied by other mathematicians and physicists, most notably Felix Berezin in the 1960s. The simplest example in one dimension is given by SU(1,1). It acts as Möbius transformations on the extended complex plane, leaving the unit circle invariant. In that case the oscillator representation is a unitary representation of a double cover of SU(1,1) and the oscillator semigroup corresponds to a representation by contraction operators of the semigroup in SL(2,C) corresponding to Möbius transformations that take the unit disk into itself. The contraction operators, determined only up to a sign, have kernels that are Gaussian functions. On an infinitesimal level the semigroup is described by a cone in the Lie algebra of SU(1,1) that can be identified with a light cone. The same framework generalizes to the symplectic group in higher dimensions, including its analogue in infinite dimensions. This article explains the theory for SU(1,1) in detail and summarizes how the theory can be extended.
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