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Week 1: an Overview of Circuit Complexity 1 Welcome 2
Topics in Circuit Complexity (CS354, Fall’11) Week 1: An Overview of Circuit Complexity Lecture Notes for 9/27 and 9/29 Ryan Williams 1 Welcome The area of circuit complexity has a long history, starting in the 1940’s. It is full of open problems and frontiers that seem insurmountable, yet the literature on circuit complexity is fairly large. There is much that we do know, although it is scattered across several textbooks and academic papers. I think now is a good time to look again at circuit complexity with fresh eyes, and try to see what can be done. 2 Preliminaries An n-bit Boolean function has domain f0; 1gn and co-domain f0; 1g. At a high level, the basic question asked in circuit complexity is: given a collection of “simple functions” and a target Boolean function f, how efficiently can f be computed (on all inputs) using the simple functions? Of course, efficiency can be measured in many ways. The most natural measure is that of the “size” of computation: how many copies of these simple functions are necessary to compute f? Let B be a set of Boolean functions, which we call a basis set. The fan-in of a function g 2 B is the number of inputs that g takes. (Typical choices are fan-in 2, or unbounded fan-in, meaning that g can take any number of inputs.) We define a circuit C with n inputs and size s over a basis B, as follows. C consists of a directed acyclic graph (DAG) of s + n + 2 nodes, with n sources and one sink (the sth node in some fixed topological order on the nodes). -
The Complexity Zoo
The Complexity Zoo Scott Aaronson www.ScottAaronson.com LATEX Translation by Chris Bourke [email protected] 417 classes and counting 1 Contents 1 About This Document 3 2 Introductory Essay 4 2.1 Recommended Further Reading ......................... 4 2.2 Other Theory Compendia ............................ 5 2.3 Errors? ....................................... 5 3 Pronunciation Guide 6 4 Complexity Classes 10 5 Special Zoo Exhibit: Classes of Quantum States and Probability Distribu- tions 110 6 Acknowledgements 116 7 Bibliography 117 2 1 About This Document What is this? Well its a PDF version of the website www.ComplexityZoo.com typeset in LATEX using the complexity package. Well, what’s that? The original Complexity Zoo is a website created by Scott Aaronson which contains a (more or less) comprehensive list of Complexity Classes studied in the area of theoretical computer science known as Computa- tional Complexity. I took on the (mostly painless, thank god for regular expressions) task of translating the Zoo’s HTML code to LATEX for two reasons. First, as a regular Zoo patron, I thought, “what better way to honor such an endeavor than to spruce up the cages a bit and typeset them all in beautiful LATEX.” Second, I thought it would be a perfect project to develop complexity, a LATEX pack- age I’ve created that defines commands to typeset (almost) all of the complexity classes you’ll find here (along with some handy options that allow you to conveniently change the fonts with a single option parameters). To get the package, visit my own home page at http://www.cse.unl.edu/~cbourke/. -
Discrete Calculus with Cubic Cells on Discrete Manifolds 3
DISCRETE CALCULUS WITH CUBIC CELLS ON DISCRETE MANIFOLDS LEONARDO DE CARLO Abstract. This work is thought as an operative guide to ”discrete exterior calculus” (DEC), but at the same time with a rigorous exposition. We present a version of (DEC) on ”cubic” cell, defining it for discrete manifolds. An example of how it works, it is done on the discrete torus, where usual Gauss and Stokes theorems are recovered. Keywords: Discrete Calculus, discrete differential geometry AMS 2010 Subject Classification: 97N70 1. Introduction Discrete exterior calculus (DEC) is motivated by potential applications in com- putational methods for field theories (elasticity, fluids, electromagnetism) and in areas of computer vision/graphics, for these applications see for example [DDT15], [DMTS14] or [BSSZ08]. DEC is developing as an alternative approach for com- putational science to the usual discretizing process from the continuous theory. It considers the discrete mesh as the only thing given and develops an entire calcu- lus using only discrete combinatorial and geometric operations. The derivations may require that the objects on the discrete mesh, but not the mesh itself, are interpolated as if they come from a continuous model. Therefore DEC could have interesting applications in fields where there isn’t any continuous underlying struc- ture as Graph theory [GP10] or problems that are inherently discrete since they are defined on a lattice [AO05] and it can stand in its own right as theory that parallels the continuous one. The language of DEC is founded on the concept of discrete differential form, this characteristic allows to preserve in the discrete con- text some of the usual geometric and topological structures of continuous models, arXiv:1906.07054v2 [cs.DM] 8 Jul 2019 in particular the Stokes’theorem dω = ω. -
High Order Gradient, Curl and Divergence Conforming Spaces, with an Application to NURBS-Based Isogeometric Analysis
High order gradient, curl and divergence conforming spaces, with an application to compatible NURBS-based IsoGeometric Analysis R.R. Hiemstraa, R.H.M. Huijsmansa, M.I.Gerritsmab aDepartment of Marine Technology, Mekelweg 2, 2628CD Delft bDepartment of Aerospace Technology, Kluyverweg 2, 2629HT Delft Abstract Conservation laws, in for example, electromagnetism, solid and fluid mechanics, allow an exact discrete representation in terms of line, surface and volume integrals. We develop high order interpolants, from any basis that is a partition of unity, that satisfy these integral relations exactly, at cell level. The resulting gradient, curl and divergence conforming spaces have the propertythat the conservationlaws become completely independent of the basis functions. This means that the conservation laws are exactly satisfied even on curved meshes. As an example, we develop high ordergradient, curl and divergence conforming spaces from NURBS - non uniform rational B-splines - and thereby generalize the compatible spaces of B-splines developed in [1]. We give several examples of 2D Stokes flow calculations which result, amongst others, in a point wise divergence free velocity field. Keywords: Compatible numerical methods, Mixed methods, NURBS, IsoGeometric Analyis Be careful of the naive view that a physical law is a mathematical relation between previously defined quantities. The situation is, rather, that a certain mathematical structure represents a given physical structure. Burke [2] 1. Introduction In deriving mathematical models for physical theories, we frequently start with analysis on finite dimensional geometric objects, like a control volume and its bounding surfaces. We assign global, ’measurable’, quantities to these different geometric objects and set up balance statements. -
Discrete Mechanics and Optimal Control: an Analysis ∗
ESAIM: COCV 17 (2011) 322–352 ESAIM: Control, Optimisation and Calculus of Variations DOI: 10.1051/cocv/2010012 www.esaim-cocv.org DISCRETE MECHANICS AND OPTIMAL CONTROL: AN ANALYSIS ∗ Sina Ober-Blobaum¨ 1, Oliver Junge 2 and Jerrold E. Marsden3 Abstract. The optimal control of a mechanical system is of crucial importance in many application areas. Typical examples are the determination of a time-minimal path in vehicle dynamics, a minimal energy trajectory in space mission design, or optimal motion sequences in robotics and biomechanics. In most cases, some sort of discretization of the original, infinite-dimensional optimization problem has to be performed in order to make the problem amenable to computations. The approach proposed in this paper is to directly discretize the variational description of the system’s motion. The resulting optimization algorithm lets the discrete solution directly inherit characteristic structural properties Rapide Not from the continuous one like symmetries and integrals of the motion. We show that the DMOC (Discrete Mechanics and Optimal Control) approach is equivalent to a finite difference discretization of Hamilton’s equations by a symplectic partitioned Runge-Kutta scheme and employ this fact in order to give a proof of convergence. The numerical performance of DMOC and its relationship to other existing optimal control methods are investigated. Mathematics Subject Classification. 49M25, 49N99, 65K10. Received October 8, 2008. Revised September 17, 2009. Highlight Published online March 31, 2010. Introduction In order to solve optimal control problems for mechanical systems, this paper links two important areas of research: optimal control and variational mechanics. The motivation for combining these fields of investigation is twofold. -
Lower Bounds from Learning Algorithms
Circuit Lower Bounds from Nontrivial Learning Algorithms Igor C. Oliveira Rahul Santhanam Charles University in Prague University of Oxford Motivation and Background Previous Work Lemma 1 [Speedup Phenomenon in Learning Theory]. From PSPACE BPTIME[exp(no(1))], simple padding argument implies: DSPACE[nω(1)] BPEXP. Some connections between algorithms and circuit lower bounds: Assume C[poly(n)] can be (weakly) learned in time 2n/nω(1). Lower bounds Lemma [Diagonalization] (3) (the proof is sketched later). “Fast SAT implies lower bounds” [KL’80] against C ? Let k N and ε > 0 be arbitrary constants. There is L DSPACE[nω(1)] that is not in C[poly]. “Nontrivial” If Circuit-SAT can be solved efficiently then EXP ⊈ P/poly. learning algorithm Then C-circuits of size nk can be learned to accuracy n-k in Since DSPACE[nω(1)] BPEXP, we get BPEXP C[poly], which for a circuit class C “Derandomization implies lower bounds” [KI’03] time at most exp(nε). completes the proof of Theorem 1. If PIT NSUBEXP then either (i) NEXP ⊈ P/poly; or 0 0 Improved algorithmic ACC -SAT ACC -Learning It remains to prove the following lemmas. upper bounds ? (ii) Permanent is not computed by poly-size arithmetic circuits. (1) Speedup Lemma (relies on recent work [CIKK’16]). “Nontrivial SAT implies lower bounds” [Wil’10] Nontrivial: 2n/nω(1) ? (Non-uniform) Circuit Classes: If Circuit-SAT for poly-size circuits can be solved in time (2) PSPACE Simulation Lemma (follows [KKO’13]). 2n/nω(1) then NEXP ⊈ P/poly. SETH: 2(1-ε)n ? ? (3) Diagonalization Lemma [Folklore]. -
A Superpolynomial Lower Bound on the Size of Uniform Non-Constant-Depth Threshold Circuits for the Permanent
A Superpolynomial Lower Bound on the Size of Uniform Non-constant-depth Threshold Circuits for the Permanent Pascal Koiran Sylvain Perifel LIP LIAFA Ecole´ Normale Superieure´ de Lyon Universite´ Paris Diderot – Paris 7 Lyon, France Paris, France [email protected] [email protected] Abstract—We show that the permanent cannot be computed speak of DLOGTIME-uniformity), Allender [1] (see also by DLOGTIME-uniform threshold or arithmetic circuits of similar results on circuits with modulo gates in [2]) has depth o(log log n) and polynomial size. shown that the permanent does not have threshold circuits of Keywords-permanent; lower bound; threshold circuits; uni- constant depth and “sub-subexponential” size. In this paper, form circuits; non-constant depth circuits; arithmetic circuits we obtain a tradeoff between size and depth: instead of sub-subexponential size, we only prove a superpolynomial lower bound on the size of the circuits, but now the depth I. INTRODUCTION is no more constant. More precisely, we show the following Both in Boolean and algebraic complexity, the permanent theorem. has proven to be a central problem and showing lower Theorem 1: The permanent does not have DLOGTIME- bounds on its complexity has become a major challenge. uniform polynomial-size threshold circuits of depth This central position certainly comes, among others, from its o(log log n). ]P-completeness [15], its VNP-completeness [14], and from It seems to be the first superpolynomial lower bound on Toda’s theorem stating that the permanent is as powerful the size of non-constant-depth threshold circuits for the as the whole polynomial hierarchy [13]. -
ECC 2015 English
© Springer-Verlag 2015 SpringerMedizin.at/memo_inoncology SpringerMedizin.at 2/15 /memo_inoncology memo – inOncology SPECIAL ISSUE Congress Report ECC 2015 A GLOBAL CONGRESS DIGEST ON NSCLC Report from the 18th ECCO- 40th ESMO European Cancer Congress, Vienna 25th–29th September 2015 Editorial Board: Alex A. Adjei, MD, PhD, FACP, Roswell Park, Cancer Institute, New York, USA Wolfgang Hilbe, MD, Departement of Oncology, Hematology and Palliative Care, Wilhelminenspital, Vienna, Austria Massimo Di Maio, MD, National Institute of Tumor Research and Th erapy, Foundation G. Pascale, Napoli, Italy Barbara Melosky, MD, FRCPC, University of British Columbia and British Columbia Cancer Agency, Vancouver, Canada Robert Pirker, MD, Medical University of Vienna, Vienna, Austria Yu Shyr, PhD, Department of Biostatistics, Biomedical Informatics, Cancer Biology, and Health Policy, Nashville, TN, USA Yi-Long Wu, MD, FACS, Guangdong Lung Cancer Institute, Guangzhou, PR China Riyaz Shah, PhD, FRCP, Kent Oncology Centre, Maidstone Hospital, Maidstone, UK Filippo de Marinis, MD, PhD, Director of the Th oracic Oncology Division at the European Institute of Oncology (IEO), Milan, Italy Supported by Boehringer Ingelheim in the form of an unrestricted grant IMPRESSUM/PUBLISHER Medieninhaber und Verleger: Springer-Verlag GmbH, Professional Media, Prinz-Eugen-Straße 8–10, 1040 Wien, Austria, Tel.: 01/330 24 15-0, Fax: 01/330 24 26-260, Internet: www.springer.at, www.SpringerMedizin.at. Eigentümer und Copyright: © 2015 Springer-Verlag/Wien. Springer ist Teil von Springer Science + Business Media, springer.at. Leitung Professional Media: Dr. Alois Sillaber. Fachredaktion Medizin: Dr. Judith Moser. Corporate Publishing: Elise Haidenthaller. Layout: Katharina Bruckner. Erscheinungsort: Wien. Verlagsort: Wien. Herstellungsort: Linz. Druck: Friedrich VDV, Vereinigte Druckereien- und Verlags-GmbH & CO KG, 4020 Linz; Die Herausgeber der memo, magazine of european medical oncology, übernehmen keine Verantwortung für diese Beilage. -
Lecture 10: Logspace Division and Its Consequences 1. Overview
IAS/PCMI Summer Session 2000 Clay Mathematics Undergraduate Program Advanced Course on Computational Complexity Lecture 10: Logspace Division and Its Consequences David Mix Barrington and Alexis Maciel July 28, 2000 1. Overview Building on the last two lectures, we complete the proof that DIVISION is in FOMP (first-order with majority quantifiers, BIT, and powering modulo short numbers) and thus in both L-uniform TC0 and L itself. We then examine the prospects for improving this result by putting DIVISION in FOM or truly uniform TC0, and look at some consequences of the L-uniform result for complexity classes with sublogarithmic space. We showed last time that we can divide a long number by a nice long number, • that is, a product of short powers of distinct primes. We also showed that given any Y , we can find a nice number D such that Y=2 D Y . We finish the proof by finding an approximation N=A for D=Y , where≤ A ≤is nice, that is good enough so that XN=AD is within one of X=Y . b c We review exactly how DIVISION, ITERATED MULTIPLICATION, and • POWERING of long integers (poly-many bits) are placed in FOMP by this argument. We review the complexity of powering modulo a short integer, and consider • how this affects the prospects of placing DIVISION and the related problems in FOM. Finally, we take a look at sublogarithmic space classes, in particular problems • solvable in space O(log log n). These classes are sensitive to the definition of the model. We argue that the more interesting classes are obtained by marking the space bound in the memory before the machine starts. -
Discrete Differential Geometry: an Applied Introduction
DISCRETE DIFFERENTIAL GEOMETRY: AN APPLIED INTRODUCTION Keenan Crane Last updated: April 13, 2020 Contents Chapter 1. Introduction 3 1.1. Disclaimer 6 1.2. Copyright 6 1.3. Acknowledgements 6 Chapter 2. Combinatorial Surfaces 7 2.1. Abstract Simplicial Complex 8 2.2. Anatomy of a Simplicial Complex: Star, Closure, and Link 10 2.3. Simplicial Surfaces 14 2.4. Adjacency Matrices 16 2.5. Halfedge Mesh 17 2.6. Written Exercises 21 2.7. Coding Exercises 26 Chapter 3. A Quick and Dirty Introduction to Differential Geometry 28 3.1. The Geometry of Surfaces 28 3.2. Derivatives and Tangent Vectors 31 3.3. The Geometry of Curves 34 3.4. Curvature of Surfaces 37 3.5. Geometry in Coordinates 41 Chapter 4. A Quick and Dirty Introduction to Exterior Calculus 45 4.1. Exterior Algebra 46 4.2. Examples of Wedge and Star in Rn 52 4.3. Vectors and 1-Forms 54 4.4. Differential Forms and the Wedge Product 58 4.5. Hodge Duality 62 4.6. Differential Operators 67 4.7. Integration and Stokes’ Theorem 73 4.8. Discrete Exterior Calculus 77 Chapter 5. Curvature of Discrete Surfaces 84 5.1. Vector Area 84 5.2. Area Gradient 87 5.3. Volume Gradient 89 5.4. Other Definitions 91 5.5. Gauss-Bonnet 94 5.6. Numerical Tests and Convergence 95 Chapter 6. The Laplacian 100 6.1. Basic Properties 100 6.2. Discretization via FEM 103 6.3. Discretization via DEC 107 1 CONTENTS 2 6.4. Meshes and Matrices 110 6.5. The Poisson Equation 112 6.6. -
LANDSCAPE of COMPUTATIONAL COMPLEXITY Spring 2008 State University of New York at Buffalo Department of Computer Science & Engineering Mustafa M
LANDSCAPE OF COMPUTATIONAL COMPLEXITY Spring 2008 State University of New York at Buffalo Department of Computer Science & Engineering Mustafa M. Faramawi, MBA Dr. Kenneth W. Regan A complete language for EXPSPACE: PIM, “Polynomial Ideal Arithmetical Hierarchy (AH) Membership”—the simplest natural completeness level that is known PIM not to have polynomial‐size circuits. TOT = {M : M is total, K(2) TOT e e ∑n Πn i.e. halts for all inputs} EXPSPACE Succinct 3SAT Unknown ∑2 Π2 but Commonly Believed: RECRE L ≠ NL …………………….. L ≠ PH NEXP co‐NEXP = ∃∀.REC = ∀∃.REC P ≠ NP ∩ co‐NP ……… P ≠ PSPACE nxn Chess p p K D NP ≠ ∑ 2 ∩Π 2 ……… NP ≠ EXP D = {Turing machines M : EXP e Best Known Separations: Me does not accept e} = RE co‐RE the complement of K. AC0 ⊂ ACC0 ⊂ PP, also TC0 ⊂ PP QBF REC (“Diagonal Language”) For any fixed k, NC1 ⊂ PSPACE, …, NL ⊂ PSPACE = ∃.REC = ∀.REC there is a PSPACE problem in this P ⊂ EXP, NP ⊂ NEXP BQP: Bounded‐Error Quantum intersection that PSPACE ⊂ EXPSPACE Polynomial Time. Believed larger can NOT be Polynomial Hierarchy (PH) than P since it has FACTORING, solved by circuits p p k but not believed to contain NP. of size O(n ) ∑ 2 Π 2 L WS5 p p ∑ 2 Π 2 The levels of AH and poly. poly. BPP: Bounded‐Error Probabilistic TAUT = ∃∀ P = ∀∃ P SAT Polynomial Time. Many believe BPP = P. NC1 PH are analogous, NLIN except that we believe NP co‐NP 0 NP ∩ co‐NP ≠ P and NTIME [n2] TC QBF PARITY ∑p ∩Πp NP PP Probabilistic NP FACT 2 2 ≠ P , which NP ACC0 stand in contrast to P PSPACE Polynomial Time MAJ‐SAT CVP RE ∩ co‐RE = REC and 0 AC RE P P ∑2 ∩Π2 = REC GAP NP co‐NP REG NL poly 0 0 ∃ . -
Arxiv:1111.4304V1 [Math.NA] 18 Nov 2011 3.3
MIMETIC FRAMEWORK ON CURVILINEAR QUADRILATERALS OF ARBITRARY ORDER JASPER KREEFT, ARTUR PALHA, AND MARC GERRITSMA Abstract. In this paper higher order mimetic discretizations are introduced which are firmly rooted in the geometry in which the variables are defined. The paper shows how basic constructs in differential geometry have a discrete counterpart in algebraic topology. Generic maps which switch between the continuous differential forms and discrete cochains will be discussed and finally a realization of these ideas in terms of mimetic spectral elements is presented, based on projections for which operations at the finite dimensional level commute with operations at the continuous level. The two types of orientation (inner- and outer-orientation) will be introduced at the continu- ous level, the discrete level and the preservation of orientation will be demonstrated for the new mimetic operators. The one-to-one correspondence between the continuous formulation and the discrete algebraic topological setting, provides a characterization of the oriented discrete bound- ary of the domain. The Hodge decomposition at the continuous, discrete and finite dimensional level will be presented. It appears to be a main ingredient of the structure in this framework. Contents 1. Introduction 3 1.1. Motivation 3 1.2. Prior and related work 5 1.3. Scope and outline of this paper 5 2. Differential Geometric Concepts 8 2.1. Manifolds 8 2.2. Differential forms 13 2.3. Differential forms under mappings 14 2.4. Exterior derivative 16 2.5. Hodge-? operator 18 2.6. Hodge decomposition 21 2.7. Hilbert spaces 22 3. An introduction to Algebraic Topology 24 3.1.