The Concept of Dimension: a Theoretical and an Informal Approach
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Dimension Theory and Systems of Parameters
Dimension theory and systems of parameters Krull's principal ideal theorem Our next objective is to study dimension theory in Noetherian rings. There was initially amazement that the results that follow hold in an arbitrary Noetherian ring. Theorem (Krull's principal ideal theorem). Let R be a Noetherian ring, x 2 R, and P a minimal prime of xR. Then the height of P ≤ 1. Before giving the proof, we want to state a consequence that appears much more general. The following result is also frequently referred to as Krull's principal ideal theorem, even though no principal ideals are present. But the heart of the proof is the case n = 1, which is the principal ideal theorem. This result is sometimes called Krull's height theorem. It follows by induction from the principal ideal theorem, although the induction is not quite straightforward, and the converse also needs a result on prime avoidance. Theorem (Krull's principal ideal theorem, strong version, alias Krull's height theorem). Let R be a Noetherian ring and P a minimal prime ideal of an ideal generated by n elements. Then the height of P is at most n. Conversely, if P has height n then it is a minimal prime of an ideal generated by n elements. That is, the height of a prime P is the same as the least number of generators of an ideal I ⊆ P of which P is a minimal prime. In particular, the height of every prime ideal P is at most the number of generators of P , and is therefore finite. -
23. Dimension Dimension Is Intuitively Obvious but Surprisingly Hard to Define Rigorously and to Work With
58 RICHARD BORCHERDS 23. Dimension Dimension is intuitively obvious but surprisingly hard to define rigorously and to work with. There are several different concepts of dimension • It was at first assumed that the dimension was the number or parameters something depended on. This fell apart when Cantor showed that there is a bijective map from R ! R2. The Peano curve is a continuous surjective map from R ! R2. • The Lebesgue covering dimension: a space has Lebesgue covering dimension at most n if every open cover has a refinement such that each point is in at most n + 1 sets. This does not work well for the spectrums of rings. Example: dimension 2 (DIAGRAM) no point in more than 3 sets. Not trivial to prove that n-dim space has dimension n. No good for commutative algebra as A1 has infinite Lebesgue covering dimension, as any finite number of non-empty open sets intersect. • The "classical" definition. Definition 23.1. (Brouwer, Menger, Urysohn) A topological space has dimension ≤ n (n ≥ −1) if all points have arbitrarily small neighborhoods with boundary of dimension < n. The empty set is the only space of dimension −1. This definition is mostly used for separable metric spaces. Rather amazingly it also works for the spectra of Noetherian rings, which are about as far as one can get from separable metric spaces. • Definition 23.2. The Krull dimension of a topological space is the supre- mum of the numbers n for which there is a chain Z0 ⊂ Z1 ⊂ ::: ⊂ Zn of n + 1 irreducible subsets. DIAGRAM pt ⊂ curve ⊂ A2 For Noetherian topological spaces the Krull dimension is the same as the Menger definition, but for non-Noetherian spaces it behaves badly. -
UC Berkeley UC Berkeley Previously Published Works
UC Berkeley UC Berkeley Previously Published Works Title Operator bases, S-matrices, and their partition functions Permalink https://escholarship.org/uc/item/31n0p4j4 Journal Journal of High Energy Physics, 2017(10) ISSN 1126-6708 Authors Henning, B Lu, X Melia, T et al. Publication Date 2017-10-01 DOI 10.1007/JHEP10(2017)199 Peer reviewed eScholarship.org Powered by the California Digital Library University of California Published for SISSA by Springer Received: July 7, 2017 Accepted: October 6, 2017 Published: October 27, 2017 Operator bases, S-matrices, and their partition functions JHEP10(2017)199 Brian Henning,a Xiaochuan Lu,b Tom Meliac;d;e and Hitoshi Murayamac;d;e aDepartment of Physics, Yale University, New Haven, Connecticut 06511, U.S.A. bDepartment of Physics, University of California, Davis, California 95616, U.S.A. cDepartment of Physics, University of California, Berkeley, California 94720, U.S.A. dTheoretical Physics Group, Lawrence Berkeley National Laboratory, Berkeley, California 94720, U.S.A. eKavli Institute for the Physics and Mathematics of the Universe (WPI), Todai Institutes for Advanced Study, University of Tokyo, Kashiwa 277-8583, Japan E-mail: [email protected], [email protected], [email protected], [email protected] Abstract: Relativistic quantum systems that admit scattering experiments are quan- titatively described by effective field theories, where S-matrix kinematics and symmetry considerations are encoded in the operator spectrum of the EFT. In this paper we use the S-matrix to derive the structure of the EFT operator basis, providing complementary de- scriptions in (i) position space utilizing the conformal algebra and cohomology and (ii) mo- mentum space via an algebraic formulation in terms of a ring of momenta with kinematics implemented as an ideal. -
Dimension and Dimensional Reduction in Quantum Gravity
May 2017 Dimension and Dimensional Reduction in Quantum Gravity S. Carlip∗ Department of Physics University of California Davis, CA 95616 USA Abstract , A number of very different approaches to quantum gravity contain a common thread, a hint that spacetime at very short distances becomes effectively two dimensional. I review this evidence, starting with a discussion of the physical meaning of “dimension” and concluding with some speculative ideas of what dimensional reduction might mean for physics. arXiv:1705.05417v2 [gr-qc] 29 May 2017 ∗email: [email protected] 1 Why Dimensional Reduction? What is the dimension of spacetime? For most of physics, the answer is straightforward and uncontroversial: we know from everyday experience that we live in a universe with three dimensions of space and one of time. For a condensed matter physicist, say, or an astronomer, this is simply a given. There are a few exceptions—surface states in condensed matter that act two-dimensional, string theory in ten dimensions—but for the most part dimension is simply a fixed, and known, external parameter. Over the past few years, though, hints have emerged from quantum gravity suggesting that the dimension of spacetime is dynamical and scale-dependent, and shrinks to d 2 at very small ∼ distances or high energies. The purpose of this review is to summarize this evidence and to discuss some possible implications for physics. 1.1 Dimensional reduction and quantum gravity As early as 1916, Einstein pointed out that it would probably be necessary to combine the newly formulated general theory of relativity with the emerging ideas of quantum mechanics [1]. -
The Small Inductive Dimension Can Be Raised by the Adjunction of a Single Point
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector MATHEMATICS THE SMALL INDUCTIVE DIMENSION CAN BE RAISED BY THE ADJUNCTION OF A SINGLE POINT BY ERIC K. VAN DOUWEN (Communicated by Prof. R. TIBXMAN at the meeting of June 30, 1973) Unless otherwise indicated, all spaces are metrizable. 1. INTRODUCTION In this note we construct a metrizable space P containing a point p such that ind P\@} = 0 and yet ind P = 1, thus showing that the small inductive dimension of a metrizable space can be raised by the adjunction of a single point. (Without the metrizsbility condition such on example has already been constructed by Dowker [3, p. 258, exercise Cl). So the behavior of the small inductive dimension is in contrast with that of the dimension functions Ind and dim, which, as is well known, cannot be raised by the edjunction of a single point [3, p. 274, exercises B and C]. The construction of our example stems from the proof of the equality of ind and Ind on the class of separable metrizable spaces, as given in [lo, p. 1781. We make use of the fact that there exists a metrizable space D with ind D = 0 and Ind D = 1 [ 141. This space is completely metrizable. Hence our main example, and the two related examples, also are com- pletely metrizable. Following [7, p, 208, example 3.3.31 the example is used to show that there is no finite closed sum theorem for the small inductive dimension, even on the class of metrizable spaces. -
Arxiv:1012.0864V3 [Math.AG] 14 Oct 2013 Nbt Emtyadpr Ler.Ltu Mhsz H Olwn Th Following the Emphasize Us H Let Results Cit.: His Algebra
ORLOV SPECTRA: BOUNDS AND GAPS MATTHEW BALLARD, DAVID FAVERO, AND LUDMIL KATZARKOV Abstract. The Orlov spectrum is a new invariant of a triangulated category. It was intro- duced by D. Orlov building on work of A. Bondal-M. van den Bergh and R. Rouquier. The supremum of the Orlov spectrum of a triangulated category is called the ultimate dimension. In this work, we study Orlov spectra of triangulated categories arising in mirror symmetry. We introduce the notion of gaps and outline their geometric significance. We provide the first large class of examples where the ultimate dimension is finite: categories of singular- ities associated to isolated hypersurface singularities. Similarly, given any nonzero object in the bounded derived category of coherent sheaves on a smooth Calabi-Yau hypersurface, we produce a new generator by closing the object under a certain monodromy action and uniformly bound this new generator’s generation time. In addition, we provide new upper bounds on the generation times of exceptional collections and connect generation time to braid group actions to provide a lower bound on the ultimate dimension of the derived Fukaya category of a symplectic surface of genus greater than one. 1. Introduction The spectrum of a triangulated category was introduced by D. Orlov in [39], building on work of A. Bondal, R. Rouquier, and M. van den Bergh, [44] [11]. This categorical invariant, which we shall call the Orlov spectrum, is simply a list of non-negative numbers. Each number is the generation time of an object in the triangulated category. Roughly, the generation time of an object is the necessary number of exact triangles it takes to build the category using this object. -
Metrizable Spaces Where the Inductive Dimensions Disagree
TRANSACTIONS OF THE AMERICAN MATHEMATICALSOCIETY Volume 318, Number 2, April 1990 METRIZABLE SPACES WHERE THE INDUCTIVE DIMENSIONS DISAGREE JOHN KULESZA Abstract. A method for constructing zero-dimensional metrizable spaces is given. Using generalizations of Roy's technique, these spaces can often be shown to have positive large inductive dimension. Examples of N-compact, complete metrizable spaces with ind = 0 and Ind = 1 are provided, answering questions of Mrowka and Roy. An example with weight c and positive Ind such that subspaces with smaller weight have Ind = 0 is produced in ZFC. Assuming an additional axiom, for each cardinal X a space of positive Ind with all subspaces with weight less than A strongly zero-dimensional is constructed. I. Introduction There are three classical notions of dimension for a normal topological space X. The small inductive dimension, denoted ind(^T), is defined by ind(X) = -1 if X is empty, ind(X) < n if each p G X has a neighborhood base of open sets whose boundaries have ind < n - 1, and ind(X) = n if ind(X) < n and n is as small as possible. The large inductive dimension, denoted Ind(Jf), is defined by Ind(X) = -1 if X is empty, \t\c\(X) < n if each closed C c X has a neighborhood base of open sets whose boundaries have Ind < n — 1, and Ind(X) = n if Ind(X) < n and n is as small as possible. The covering dimension, denoted by dim(X), is defined by dim(A') = -1 if X is empty, dim(A') < n if for each finite open cover of X there is a finite open refining cover such that no point is in more than n + 1 of the sets in the refining cover and, dim(A") = n if dim(X) < n and n is as small as possible. -
Quasiorthogonal Dimension
Quasiorthogonal Dimension Paul C. Kainen1 and VˇeraK˚urkov´a2 1 Department of Mathematics and Statistics, Georgetown University Washington, DC, USA 20057 [email protected] 2 Institute of Computer Science, Czech Academy of Sciences Pod Vod´arenskou vˇeˇz´ı 2, 18207 Prague, Czech Republic [email protected] Abstract. An interval approach to the concept of dimension is pre- sented. The concept of quasiorthogonal dimension is obtained by relax- ing exact orthogonality so that angular distances between unit vectors are constrained to a fixed closed symmetric interval about π=2. An ex- ponential number of such quasiorthogonal vectors exist as the Euclidean dimension increases. Lower bounds on quasiorthogonal dimension are proven using geometry of high-dimensional spaces and a separate argu- ment is given utilizing graph theory. Related notions are reviewed. 1 Introduction The intuitive concept of dimension has many mathematical formalizations. One version, based on geometry, uses \right angles" (in Greek, \ortho gonia"), known since Pythagoras. The minimal number of orthogonal vectors needed to specify an object in a Euclidean space defines its orthogonal dimension. Other formalizations of dimension are based on different aspects of space. For example, a topological definition (inductive dimension) emphasizing the recur- sive character of d-dimensional objects having d−1-dimensional boundaries, was proposed by Poincar´e,while another topological notion, covering dimension, is associated with Lebesgue. A metric-space version of dimension was developed -
Commutative Algebra Ii, Spring 2019, A. Kustin, Class Notes
COMMUTATIVE ALGEBRA II, SPRING 2019, A. KUSTIN, CLASS NOTES 1. REGULAR SEQUENCES This section loosely follows sections 16 and 17 of [6]. Definition 1.1. Let R be a ring and M be a non-zero R-module. (a) The element r of R is regular on M if rm = 0 =) m = 0, for m 2 M. (b) The elements r1; : : : ; rs (of R) form a regular sequence on M, if (i) (r1; : : : ; rs)M 6= M, (ii) r1 is regular on M, r2 is regular on M=(r1)M, ::: , and rs is regular on M=(r1; : : : ; rs−1)M. Example 1.2. The elements x1; : : : ; xn in the polynomial ring R = k[x1; : : : ; xn] form a regular sequence on R. Example 1.3. In general, order matters. Let R = k[x; y; z]. The elements x; y(1 − x); z(1 − x) of R form a regular sequence on R. But the elements y(1 − x); z(1 − x); x do not form a regular sequence on R. Lemma 1.4. If M is a finitely generated module over a Noetherian local ring R, then every regular sequence on M is a regular sequence in any order. Proof. It suffices to show that if x1; x2 is a regular sequence on M, then x2; x1 is a regular sequence on M. Assume x1; x2 is a regular sequence on M. We first show that x2 is regular on M. If x2m = 0, then the hypothesis that x1; x2 is a regular sequence on M guarantees that m 2 x1M; thus m = x1m1 for some m1. -
On the Hilbert Function of a Graded Cohen-Macaulay Domain
Journal of Pure and Applied Algebra 73 (lW1) 307-314 307 North-Holland Richard P. Stsnley” Department of Mathematics, Massachusetts Institute of Teclmology . Carnhridge. MA 02139. USA Communicated by A. Blass Received 7 May 1990 Revised 6 August 1990 Abstract Stanley, R.P., On the Hilbert function of a graded Cohen-Macaulay domain. Journal of Pure and Applied Algebra 73 (1991) 307-314. A condition is obtained on the Hilbert function of a graded Cohen-Macaulay domain R=R,$f?,G+. - over a field R, = K when R is integral over the subalgebra generated by R,. A result of Eisenbud and Harris leads to a stronger condition when char K = 0 and R is generated as a K-aigebra by R,. An application is given to the Ehrhart polynomial of an :,r____:-&W’ ^ ,,-l -u-i.-I\*..- _- c- --1..+,q,__~“t..‘. ... -_ _ _,_-_. 1. Introduction By a graded algebra over a field K, we mean here a commutative K-algebra R with identity, together with a vector space direct sum decompo&ion & = &_,l R;. such that: (a) RiRi c Ri+i, (b) R, = K (i.e., R is connected), and (c) R is finitely-generated as a K-algebra. R is standard if R is generated as a K-algebra by R,, and semistandard if R is integral over the subalgebra K[ R,] of R generated by R,. The Hilbert function H( R, -) of R is defined by H( R, i) = dim,R,, for i 2 0. while the Hilbert series is given by F(R, A) = 2 H(R, i)A’. -
Commutative Algebra) Notes, 2Nd Half
Math 221 (Commutative Algebra) Notes, 2nd Half Live [Locally] Free or Die. This is Math 221: Commutative Algebra as taught by Prof. Gaitsgory at Harvard during the Fall Term of 2008, and as understood by yours truly. There are probably typos and mistakes (which are all mine); use at your own risk. If you find the aforementioned mistakes or typos, and are feeling in a generous mood, then you may consider sharing this information with me.1 -S. Gong [email protected] 1 CONTENTS Contents 1 Divisors 2 1.1 Discrete Valuation Rings (DVRs), Krull Dimension 1 . .2 1.2 Dedekind Domains . .6 1.3 Divisors and Fractional Ideals . .8 1.4 Dedekind Domains and Integral Closedness . 11 1.5 The Picard Group . 16 2 Dimension via Hilbert Functions 21 2.1 Filtrations and Gradations . 21 2.2 Dimension of Modules over a Polynomial Algebra . 24 2.3 For an arbitrary finitely generated algebra . 27 3 Dimension via Transcendency Degree 31 3.1 Definitions . 31 3.2 Agreement with Hilbert dimension . 32 4 Dimension via Chains of Primes 34 4.1 Definition via chains of primes and Noether Normalization . 34 4.2 Agreement with Hilbert dimension . 35 5 Kahler Differentials 37 6 Completions 42 6.1 Introduction to inverse limits and completions . 42 6.2 Artin Rees Pattern . 46 7 Local Rings and Other Notions of Dimension 50 7.1 Dimension theory for Local Noetherian Rings . 50 8 Smoothness and Regularity 53 8.1 Regular Local Rings . 53 8.2 Smoothness/Regularity for algebraically closed fields . 55 8.3 A taste of smoothness and regularity for non-algebraically closed fields . -
New Methods for Estimating Fractal Dimensions of Coastlines
New Methods for Estimating Fractal Dimensions of Coastlines by Jonathan David Klotzbach A Thesis Submitted to the Faculty of The College of Science in Partial Fulfillment of the Requirements for the Degree of Master of Science Florida Atlantic University Boca Raton, Florida May 1998 New Methods for Estimating Fractal Dimensions of Coastlines by Jonathan David Klotzbach This thesis was prepared under the direction of the candidate's thesis advisor, Dr. Richard Voss, Department of Mathematical Sciences, and has been approved by the members of his supervisory committee. It was submitted to the faculty of The College of Science and was accepted in partial fulfillment of the requirements for the degree of Master of Science. SUPERVISORY COMMITTEE: ~~~y;::ThesisAMo/ ~-= Mathematical Sciences Date 11 Acknowledgements I would like to thank my advisor, Dr. Richard Voss, for all of his help and insight into the world of fractals and in the world of computer programming. You have given me guidance and support during this process and without you, this never would have been completed. You have been an inspiration to me. I would also like to thank my committee members, Dr. Heinz- Otto Peitgen and Dr. Mingzhou Ding, for their help and support. Thanks to Rich Roberts, a graduate student in the Geography Department at Florida Atlantic University, for all of his help converting the data from the NOAA CD into a format which I could use in my analysis. Without his help, I would have been lost. Thanks to all of the faculty an? staff in the Math Department who made my stay here so enjoyable.