ESSENTIAL DIMENSION of FINITE P-GROUPS
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Essential Dimension of Finite Groups
University of California Los Angeles Essential Dimension of Finite Groups A dissertation submitted in partial satisfaction of the requirements for the degree Doctor of Philosophy in Mathematics by Wanshun Wong 2012 c Copyright by Wanshun Wong 2012 Abstract of the Dissertation Essential Dimension of Finite Groups by Wanshun Wong Doctor of Philosophy in Mathematics University of California, Los Angeles, 2012 Professor Alexander Merkurjev, Chair In this thesis we study the essential dimension of the first Galois cohomology functors of finite groups. Following the result by N. A. Karpenko and A. S. Merkurjev about the essential dimension of finite p-groups over a field containing a primitive p-th root of unity, we compute the essential dimension of finite cyclic groups and finite abelian groups over a field containing all primitive p-th roots of unity for all prime divisors p of the order of the group. For the computation of the upper bound of the essential dimension we apply the techniques about affine group schemes, and for the lower bound we make use of the tools of canonical dimension and fibered categories. We also compute the essential dimension of small groups over the field of rational numbers to illustrate the behavior of essential dimension when the base field does not contain all relevant primitive roots of unity. ii The dissertation of Wanshun Wong is approved. Amit Sahai Richard Elman Paul Balmer Alexander Merkurjev, Committee Chair University of California, Los Angeles 2012 iii Table of Contents 1 Introduction :::::::::::::::::::::::::::::::::::::: -
The General Linear Group
18.704 Gabe Cunningham 2/18/05 [email protected] The General Linear Group Definition: Let F be a field. Then the general linear group GLn(F ) is the group of invert- ible n × n matrices with entries in F under matrix multiplication. It is easy to see that GLn(F ) is, in fact, a group: matrix multiplication is associative; the identity element is In, the n × n matrix with 1’s along the main diagonal and 0’s everywhere else; and the matrices are invertible by choice. It’s not immediately clear whether GLn(F ) has infinitely many elements when F does. However, such is the case. Let a ∈ F , a 6= 0. −1 Then a · In is an invertible n × n matrix with inverse a · In. In fact, the set of all such × matrices forms a subgroup of GLn(F ) that is isomorphic to F = F \{0}. It is clear that if F is a finite field, then GLn(F ) has only finitely many elements. An interesting question to ask is how many elements it has. Before addressing that question fully, let’s look at some examples. ∼ × Example 1: Let n = 1. Then GLn(Fq) = Fq , which has q − 1 elements. a b Example 2: Let n = 2; let M = ( c d ). Then for M to be invertible, it is necessary and sufficient that ad 6= bc. If a, b, c, and d are all nonzero, then we can fix a, b, and c arbitrarily, and d can be anything but a−1bc. This gives us (q − 1)3(q − 2) matrices. -
Normal Subgroups of the General Linear Groups Over Von Neumann Regular Rings L
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 96, Number 2, February 1986 NORMAL SUBGROUPS OF THE GENERAL LINEAR GROUPS OVER VON NEUMANN REGULAR RINGS L. N. VASERSTEIN1 ABSTRACT. Let A be a von Neumann regular ring or, more generally, let A be an associative ring with 1 whose reduction modulo its Jacobson radical is von Neumann regular. We obtain a complete description of all subgroups of GLn A, n > 3, which are normalized by elementary matrices. 1. Introduction. For any associative ring A with 1 and any natural number n, let GLn A be the group of invertible n by n matrices over A and EnA the subgroup generated by all elementary matrices x1'3, where 1 < i / j < n and x E A. In this paper we describe all subgroups of GLn A normalized by EnA for any von Neumann regular A, provided n > 3. Our description is standard (see Bass [1] and Vaserstein [14, 16]): a subgroup H of GL„ A is normalized by EnA if and only if H is of level B for an ideal B of A, i.e. E„(A, B) C H C Gn(A, B). Here Gn(A, B) is the inverse image of the center of GL„(,4/S) (when n > 2, this center consists of scalar invertible matrices over the center of the ring A/B) under the canonical homomorphism GL„ A —►GLn(A/B) and En(A, B) is the normal subgroup of EnA generated by all elementary matrices in Gn(A, B) (when n > 3, the group En(A, B) is generated by matrices of the form (—y)J'lx1'Jy:i''1 with x € B,y £ A,l < i ^ j < n, see [14]). -
Variational Problems on Flows of Diffeomorphisms for Image Matching
QUARTERLY OF APPLIED MATHEMATICS VOLUME LVI, NUMBER 3 SEPTEMBER 1998, PAGES 587-600 VARIATIONAL PROBLEMS ON FLOWS OF DIFFEOMORPHISMS FOR IMAGE MATCHING By PAUL DUPUIS (LCDS, Division of Applied Mathematics, Brown University, Providence, RI), ULF GRENANDER (Division of Applied Mathematics, Brown University, Providence, Rl), AND MICHAEL I. MILLER (Dept. of Electrical Engineering, Washington University, St. Louis, MO) Abstract. This paper studies a variational formulation of the image matching prob- lem. We consider a scenario in which a canonical representative image T is to be carried via a smooth change of variable into an image that is intended to provide a good fit to the observed data. The images are all defined on an open bounded set GcR3, The changes of variable are determined as solutions of the nonlinear Eulerian transport equation ==v(rj(s;x),s), r)(t;x)=x, (0.1) with the location 77(0;x) in the canonical image carried to the location x in the deformed image. The variational problem then takes the form arg mm ;||2 + [ |Tor?(0;a;) - D(x)\2dx (0.2) JG where ||v|| is an appropriate norm on the velocity field v(-, •), and the second term at- tempts to enforce fidelity to the data. In this paper we derive conditions under which the variational problem described above is well posed. The key issue is the choice of the norm. Conditions are formulated under which the regularity of v(-, ■) imposed by finiteness of the norm guarantees that the associated flow is supported on a space of diffeomorphisms. The problem (0.2) can Received March 15, 1996. -
On the Essential Dimension of Cyclic P-Groups
1 On the essential dimension of cyclic p-groups Mathieu Florence1 December 2006 Abstract. Let p be a prime number and r ≥ 1 an integer. We compute the essential dimension of Z/prZ over fields of characteristic not p, containing the p-th roots of unity (theorem 3.1). In particular, we have edQ(Z/8Z) = 4, a result which was conjectured by Buhler and Reichstein in 1995 (unpublished). Keywords and Phrases: Galois cohomology, essential dimension, Severi-Brauer varieties. A la m´emoire de mon p`ere. Acknowledgements We thank Jean Fasel and Giordano Favi for fruitful discussions about essential dimension. Contents Acknowledgements 1 1. Introduction 1 2. Some auxiliary results 2 3. The main theorem 5 References 6 1. Introduction The notion of essential dimension was introduced by Buhler and Reichstein for finite groups in [BR]. It was later generalized by Reichstein to arbitrary linear algebraic groups ([Re]). Throughout this paper, we shall assume that the reader is somewhat familiar with this concept. A convenient and comprehensive reference on this subject is [BF]. Definition 1.1. Let k be a field, and G a (smooth) linear algebraic k-group. The essential dimension of G over k, denoted by edk(G), is the smallest nonnegative integer n with the following property. For each field extension K/k, and each GK -torsor T −→ Spec(K), there exists a ′ ′ ′ subfield K of K, containing k, and a GK′ -torsor T −→ Spec(K ), such that ′ i) The GK -torsors T and TK are isomorphic, ii) The transcendence degree of K′/k is equal to n. -
On Generalizations of Sylow Tower Groups
Pacific Journal of Mathematics ON GENERALIZATIONS OF SYLOW TOWER GROUPS ABI (ABIADBOLLAH)FATTAHI Vol. 45, No. 2 October 1973 PACIFIC JOURNAL OF MATHEMATICS Vol. 45, No. 2, 1973 ON GENERALIZATIONS OF SYLOW TOWER GROUPS ABIABDOLLAH FATTAHI In this paper two different generalizations of Sylow tower groups are studied. In Chapter I the notion of a fc-tower group is introduced and a bound on the nilpotence length (Fitting height) of an arbitrary finite solvable group is found. In the same chapter a different proof to a theorem of Baer is given; and the list of all minimal-not-Sylow tower groups is obtained. Further results are obtained on a different generalization of Sylow tower groups, called Generalized Sylow Tower Groups (GSTG) by J. Derr. It is shown that the class of all GSTG's of a fixed complexion form a saturated formation, and a structure theorem for all such groups is given. NOTATIONS The following notations will be used throughont this paper: N<]G N is a normal subgroup of G ΛΓCharG N is a characteristic subgroup of G ΛΓ OG N is a minimal normal subgroup of G M< G M is a proper subgroup of G M<- G M is a maximal subgroup of G Z{G) the center of G #>-part of the order of G, p a prime set of all prime divisors of \G\ Φ(G) the Frattini subgroup of G — the intersec- tion of all maximal subgroups of G [H]K semi-direct product of H by K F(G) the Fitting subgroup of G — the maximal normal nilpotent subgroup of G C(H) = CG(H) the centralizer of H in G N(H) = NG(H) the normalizer of H in G PeSy\p(G) P is a Sylow ^-subgroup of G P is a Sy-subgroup of G PeSγlp(G) Core(H) = GoreG(H) the largest normal subgroup of G contained in H= ΓioeoH* KG) the nilpotence length (Fitting height) of G h(G) p-length of G d(G) minimal number of generators of G c(P) nilpotence class of the p-group P some nonnegative power of prime p OP(G) largest normal p-subgroup of G 453 454 A. -
LM2931-N SNOSBE5G –MARCH 2000–REVISED APRIL 2013 LM2931-N Series Low Dropout Regulators Check for Samples: LM2931-N
LM2931-N www.ti.com SNOSBE5G –MARCH 2000–REVISED APRIL 2013 LM2931-N Series Low Dropout Regulators Check for Samples: LM2931-N 1FEATURES DESCRIPTION The LM2931-N positive voltage regulator features a 2• Very Low Quiescent Current very low quiescent current of 1mA or less when • Output Current in Excess of 100 mA supplying 10mA loads. This unique characteristic and • Input-output Differential Less than 0.6V the extremely low input-output differential required for • Reverse Battery Protection proper regulation (0.2V for output currents of 10mA) make the LM2931-N the ideal regulator for standby • 60V Load Dump Protection power systems. Applications include memory standby • −50V Reverse Transient Protection circuits, CMOS and other low power processor power • Short Circuit Protection supplies as well as systems demanding as much as • Internal Thermal Overload Protection 100mA of output current. • Mirror-image Insertion Protection Designed originally for automotive applications, the LM2931-N and all regulated circuitry are protected • Available in TO-220, TO-92, TO-263, or SOIC-8 from reverse battery installations or 2 battery jumps. Packages During line transients, such as a load dump (60V) • Available as Adjustable with TTL Compatible when the input voltage to the regulator can Switch momentarily exceed the specified maximum operating voltage, the regulator will automatically shut down to protect both internal circuits and the load. The LM2931-N cannot be harmed by temporary mirror-image insertion. Familiar regulator features such as short circuit and thermal overload protection are also provided. The LM2931-N family includes a fixed 5V output (±3.8% tolerance for A grade) or an adjustable output with ON/OFF pin. -
Essential Dimension
BULLETIN (New Series) OF THE AMERICAN MATHEMATICAL SOCIETY Volume 54, Number 4, October 2017, Pages 635–661 http://dx.doi.org/10.1090/bull/1564 Article electronically published on December 19, 2016 ESSENTIAL DIMENSION ALEXANDER S. MERKURJEV Abstract. In this paper we survey research on the essential dimension that was introduced by J. Buhler and Z. Reichstein. Informally speaking, the es- sential dimension of a class of algebraic objects is the minimal number of algebraically independent parameters one needs to define any object in the class. The notion of essential dimension, which is defined in elementary terms, has surprising connections to many areas of algebra, such as algebraic geome- try, algebraic K-theory, Galois cohomology, representation theory of algebraic groups, theory of fibered categories and valuation theory. The highlights of the survey are the computations of the essential dimensions of finite groups, groups of multiplicative type and the spinor groups. 1. Introduction The essential dimension of an algebraic object is an integer that measures the complexity of the object. For example, let Q =(a, b)K be a quaternion algebra over a field extension K of a base field F of characteristic not 2. That is, let Q be a four-dimensional algebra over K with basis {1,i,j,ij} and multiplication table i2 = a, j2 = b, ij = −ji,wherea and b are nonzero elements in K.Thus,Q is determined by two parameters a and b. Equivalently, we can say that the algebra Q is defined over the subfield K = F (a, b)ofK,namely,Q Q ⊗K K for the quaternion algebra Q =(a, b)K over the field K of transcendence degree at most 2overF . -
Quasi P Or Not Quasi P? That Is the Question
Rose-Hulman Undergraduate Mathematics Journal Volume 3 Issue 2 Article 2 Quasi p or not Quasi p? That is the Question Ben Harwood Northern Kentucky University, [email protected] Follow this and additional works at: https://scholar.rose-hulman.edu/rhumj Recommended Citation Harwood, Ben (2002) "Quasi p or not Quasi p? That is the Question," Rose-Hulman Undergraduate Mathematics Journal: Vol. 3 : Iss. 2 , Article 2. Available at: https://scholar.rose-hulman.edu/rhumj/vol3/iss2/2 Quasi p- or not quasi p-? That is the Question.* By Ben Harwood Department of Mathematics and Computer Science Northern Kentucky University Highland Heights, KY 41099 e-mail: [email protected] Section Zero: Introduction The question might not be as profound as Shakespeare’s, but nevertheless, it is interesting. Because few people seem to be aware of quasi p-groups, we will begin with a bit of history and a definition; and then we will determine for each group of order less than 24 (and a few others) whether the group is a quasi p-group for some prime p or not. This paper is a prequel to [Hwd]. In [Hwd] we prove that (Z3 £Z3)oZ2 and Z5 o Z4 are quasi 2-groups. Those proofs now form a portion of Proposition (12.1) It should also be noted that [Hwd] may also be found in this journal. Section One: Why should we be interested in quasi p-groups? In a 1957 paper titled Coverings of algebraic curves [Abh2], Abhyankar conjectured that the algebraic fundamental group of the affine line over an algebraically closed field k of prime characteristic p is the set of quasi p-groups, where by the algebraic fundamental group of the affine line he meant the family of all Galois groups Gal(L=k(X)) as L varies over all finite normal extensions of k(X) the function field of the affine line such that no point of the line is ramified in L, and where by a quasi p-group he meant a finite group that is generated by all of its p-Sylow subgroups. -
A Fast Diffeomorphic Image Registration Algorithm
www.elsevier.com/locate/ynimg NeuroImage 38 (2007) 95–113 A fast diffeomorphic image registration algorithm John Ashburner Wellcome Trust Centre for Neuroimaging, 12 Queen Square, London, WC1N 3BG, UK Received 26 October 2006; revised 14 May 2007; accepted 3 July 2007 Available online 18 July 2007 This paper describes DARTEL, which is an algorithm for diffeo- Many registration approaches still use a small deformation morphic image registration. It is implemented for both 2D and 3D model. These models parameterise a displacement field (u), which image registration and has been formulated to include an option for is simply added to an identity transform (x). estimating inverse consistent deformations. Nonlinear registration is considered as a local optimisation problem, which is solved using a Φ x x u x 1 Levenberg–Marquardt strategy. The necessary matrix solutions are ð Þ ¼ þ ð Þ ð Þ obtained in reasonable time using a multigrid method. A constant In such parameterisations, the inverse transformation is sometimes Eulerian velocity framework is used, which allows a rapid scaling and approximated by subtracting the displacement. It is worth noting that squaring method to be used in the computations. DARTEL has been this is only a very approximate inverse, which fails badly for larger applied to intersubject registration of 471 whole brain images, and the deformations. As shown in Fig. 1, compositions of these forward resulting deformations were evaluated in terms of how well they encode and “inverse” deformations do not produce an identity transform. the shape information necessary to separate male and female subjects Small deformation models do not necessarily enforce a one-to-one and to predict the ages of the subjects. -
Essential Dimension and Canonical Dimension of Gerbes Banded by Groups of Multiplicative Type
ESSENTIAL DIMENSION AND CANONICAL DIMENSION OF GERBES BANDED BY GROUPS OF MULTIPLICATIVE TYPE ROLAND LOTSCHER¨ Abstract. We prove the formula ed(X ) = cdim(X ) + ed(A) for any gerbe X banded by an algebraic group A which is the kernel of a homomorphism of algebraic tori Q → S with Q invertible and S split. This result is applied to prove new results on the essential dimension of algebraic groups. 1. Introduction Essential dimension is a notion of complexity of algebraic and geometric objects, introduced by J. Buhler and Z. Reichstein [BR97] around 1995 and in its most general form by A. Merkurjev [BF03]. The essential dimension of an algebraic group G over a field F is defined as the least integer n such that every G-torsor over a field extension K/F is obtained up to isomorphism by scalar extension from a G-torsor over an intermediate field K0 of transcendence degree at most n over F . It is denoted by ed(G). The essential dimension of an algebraic stack X over F is defined similarly (see section 2), where G-torsors are replaced by objects of X . For every algebraic group (and every group algebraic space) G over F there is the classifying stack BG, whose objects are G-torsors. In particular ed(G) = ed(BG). An algebraic stack X of finite type over F is called a gerbe, if it becomes iso- morphic to BG for some group algebraic space G over a finite extension of F (see [Stacks, Definition 06QC and Lemma 06QH]). In particular BG is a gerbe for any algebraic group G. -
Deep Compositing Using Lie Algebras
Deep Compositing Using Lie Algebras TOM DUFF Pixar Animation Studios Deep compositing is an important practical tool in creating digital imagery, Deep images extend Porter-Duff compositing by storing multiple but there has been little theoretical analysis of the underlying mathematical values at each pixel with depth information to determine composit- operators. Motivated by finding a simple formulation of the merging oper- ing order. The OpenEXR deep image representation stores, for each ation on OpenEXR-style deep images, we show that the Porter-Duff over pixel, a list of nonoverlapping depth intervals, each containing a function is the operator of a Lie group. In its corresponding Lie algebra, the single pixel value [Kainz 2013]. An interval in a deep pixel can splitting and mixing functions that OpenEXR deep merging requires have a represent contributions either by hard surfaces if the interval has particularly simple form. Working in the Lie algebra, we present a novel, zero extent or by volumetric objects when the interval has nonzero simple proof of the uniqueness of the mixing function. extent. Displaying a single deep image requires compositing all the The Lie group structure has many more applications, including new, values in each deep pixel in depth order. When two deep images correct resampling algorithms for volumetric images with alpha channels, are merged, splitting and mixing of these intervals are necessary, as and a deep image compression technique that outperforms that of OpenEXR. described in the following paragraphs. 26 r Merging the pixels of two deep images requires that correspond- CCS Concepts: Computing methodologies → Antialiasing; Visibility; ing pixels of the two images be reconciled so that all overlapping Image processing; intervals are identical in extent.