The Binary Space Partitioning-Tree Process Supplementary Material
|
|
- Paula Hensley
- 6 years ago
- Views:
Transcription
1 The inary Space Partitioning-Tree Process Suppementary Materia Xuhui Fan in Li Scott. Sisson Schoo of omputer Science Fudan University Schoo of Mathematics and Statistics University of New South Waes Schoo of Mathematics and Statistics University of New South Waes Justification on the accumuated cut cost Let = sup x,x { x x } denotes the diameter of the poygon. θ, it is obviousy that the ength of the newy generated cut ine L(θ, u) is smaer or equa to, i.e., L(θ, u). Thus, we have the resut for the sum of perimeters in the -th partitioning resut as: k= P ( τ ) P ( ) + ( ) () h $ h θ # $ θ # w$ w # ccording to the Fatou s emma, we get im inf im inf k= P ( τ ) k= P ( τ ) [P ( )] + ( ) im inf < () k= which eads to im inf P ( τ ) surey. Since surey, we get = surey. k= P ( τ < amost ) is increasing for amost [ k= P ( τ )] = amost Mathematica formuation of the three-restrictions on the measure invariance. transation t: ( θ ) = λ t v t v ( θ ), where t v (x) = x + v, v R ;. rotation r: = λ rθ r θ, where r θ (x) = [ ] cos θ sin θ sin θ cos θ x refers to rotate the point x in an ange of θ ; Figure : The design of a set of divisions in Lemma. Red dashed ines denote the rough divisions, whie green dashed ines denote the grained divisions based on each consecutive rough divisions. 3. restriction ψ: ( θ ) = λ ψ ψ ( θ ), where refers to a sub-domain of ; ψ = {x x }, and θ refers to the set of cut ines for a the potentia cuts crossing through. Proof of Proposition Lemma. ssume two convex poygons and have the same ength on the ine segment (θ). There exists a set of countabe divisions passing through (θ) in the direction of θ + π. ach ine sub-segment of (θ) cut by consecutive divisions is covered by the intersection of the,, whie, can move in the direction of θ + π/. Proof. The set of divisions (a in the direction of θ + π ) can be designed into two stages. Stage, a set of rough divisions that pass through each vertices of the two poygons. Stage, sets of grained divisions based on the each consecutive rough divisions. Let denotes the distance between two seected consecutive divisions, w (w ) denotes
2 Running heading tite breaks the ine the maximum width of poygon ( ) between these two rough divisions and θ (θ ) is the smaest ange between the edge of poygon ( ) and division. We proceed the grained division in the foowing way. In the case of min{w tan θ, w tan θ }, there is no need to do further grained division; otherwise, et (θ, d ) = arg θ,d min{d tan θ, d tan θ }, the first grained division is paced in the position of d tan θ (see h in Figure ). The second grained division woud design based on the first one and proceed in a simiar way. Given the condition of d tan θ <, we can do the partition at the positions of: { d tan θ ( d tan θ ) } = where = d tan θ ( ) d tan θ =. Proposition. The famiy of partition probabiity measure ( θ ) keeps invariant under the operations of transation, rotation and restriction if and ony if we have a constant such that ( θ ) = (θ), R+. Proof. The reverse case is fuy discussed as in the main part of the paper. On the other hand, assume we have two sets of cut ines θ, θ with (θ ) = (θ). Given that the measure ( θ ) is invariant under the operations of transation, rotation and restriction, we need to prove the foowing equity: (3) ( θ ) = ( θ ) (4) To compete this, we first do rotation and transation operations on, which is := r θ t v, in a way that and project into the same image (θ). ased on Lemma, we divide and into countabe parts, where the intersection of these pair parts projects to the same images. That is: θ, θ = k,, = k (5) Y =,, (θ) Y, k N (6) = {L(θ, u) crossing, θ is fixed, u ies on (θ)} = {L(θ, u) crossing θ is fixed,, u ies on (θ)} (7) The additivity of measures indicates that: ( θ ) = k ( θ ) = k, ( θ,) ( θ ) q. (4) is correct if we can prove the foowing, ( θ, ) = ( θ ), k N (8) From the measure invariance under rotation and transation, we get ( θ ) = λ tv(r θ ( ))(t v (r θ ( θ ))). We aso get Thus, we get λ tvr θ, Π Y π = {Y } = Π Y t (ρπ) (9) Π Y θ, ( θ,) restriction = Π Y θ = λ ΠY t vr θ, q.(9) = λ ΠY, q.() restriction = λ ΠY = Proof of Proposition ( θ ) () (Π Y θ,) (Π Y θ,) (Π Y θ ) () Our partition woud resut in convex poygon. We have the integration resuts for the convex poygon. Lemma. The integration of the intersection ine in a triange over [, π] equas to the triange s perimeter. Proof. We first consider the acute triange (Top row of Figure ) case. Let {,, 3 } being the engths of the triange s edges and {,, } being the corresponding anges. ccording to the aw of sines, we have = sin = sin = 3 sin () where we use to denote the ratio between the ength and its corresponding ange. W..o.g., we are cutting the bock in the direction within. The projection scaar of is cacuated as =
3 Xuhui Fan, in Li, Scott. Sisson Here the nd equation hods due to the aw of Sines. The case of right triange (Midde row of Figure ) is straight forward. We can get 3 I = cos + cos + cos + 3 cos = = P ( ) (5) On the case of obtuse triange (ottom row of Figure ) 3 I = cos 3 cos + cos cos + 3 cos + cos = = P ( ) (6) Lemma 3. The integration of the ength of the bock s projected image in the direction of θ over (, π] equas to the perimeter of the bock, which is π (θ) dθ = P ( ). 3 F Figure : Top: cute Triange; Midde: Right Triange; ottom: Obtuse Triange. cos θ(θ = ). Whie θ is ranging from to, the integration of is dθ = cos θdθ = sin θ = cos( ) (3) y using the simiar routines, we can get the integration of a the projection ines I as: I = cos + cos + cos + cos + 3 cos + 3 cos = sin cos + sin cos + sin cos + sin cos + sin cos + sin cos = sin( + ) + sin( + ) + sin( + ) = sin + sin + sin = = P ( ) (4) Figure 3: From convex poygon with n vertices to convex poygon with n vertices. Proof. onvex poygon with n vertices can be divided into n trianges. Since we have the resut for the case of trianges, mathematica induction is used to get the concusion for any convex poygons. ssume we have the resut for convex poygon with n vertices, the additiona part for its transformation to convex poygon with n vertices is the triange. orrespondingy, the increase in the scaar projection is composed of two parts: L increase = sin θdθ = cos = (7)
4 Running heading tite breaks the ine where θ = F and L increase refers to the integration of F in the ange of. L increase = sin θdθ = cos = (8) Thus, the tota add amount is L increase = + ( + ) = +. This is exacty the increase of perimeter from the convex poygon with n vertices to convex poygon with n vertices. Thus, we can get the resut for a the convex poygons. Proposition is a direct resut of Lemma 3. onsistency Some notations are firsty defined for convenient reference. We use and to denote a domain and its subdomain, which is. M τ and N τ are individuay defined as the SP-Tree processes on and respectivey. The restriction is denoted as Π, in which we have Π M τ = N τ. so, we et c( ) denote the measure over the bock, which is c( ) = θ ω(θ) (θ) dθ and et O n denote the partition after n-th cut on the convex poygon. xtending partition from to For the SP-Tree process N τ, we et Z and {σ } N denotes the reated Markov chain and the corresponding time stops. For t, define m t to be the index such that t [σ mt, σ mt+ ], N t = Z mt. To extend N τ from to, et τ = and Y =. For n N, we define τ n+ and Y n+ inductivey as: τ n+ := min{σ mτn +, τ n + ξ n c(y n ) c(z mτn ) } (9) where ξ n is generated from the exponentia distribution with mean. { iftyn, (Z Y n+ = ), τ mτn n+ = σ mτn + ; gencut (Y n ), otherwise. () where ift Yn, (Z mτn ) denotes extending the existing cut to the arger domain and gencut (Y n ) refers to the case that there wi be a new cut generated in that does not cross into. ccording to the resuts of Proposition V.6 of chapter VI in [], the defined process {Y n, τ n } are we-defined. Prove the correctness t >, the waiting time for the next cut in X is: ζ t = τ n+ t () ccording to τ n+ s definition (q. (9)), ζ t foows the exponentia distribution with the rate being c(y nt ). What is more, the probabiity of the event τ n+ = σ mτn + occurs with probabiity c(o n )/c(o n ). For the newy extended case {Y n } n, whie Y n crosses through, the probabiity measure on θ is in proportion to ω(θ) (θ) and u ocates ony on (θ). Thus, we get P = c(o n ) c(o n ) = ω(θ) c(o n ) ω(θ) (θ) θ ω(θ) (θ) dθ (θ) () whie Y n does not cross through,, the probabiity measure on θ \ is in proportion to ω(θ)( (θ) (θ) ) and u ocates ony on \ (θ) (with the ength (θ) (θ) ). Thus, we get P = c(o n ) c(on ) ω(θ)( (θ) (θ) ) c(on ) θ ω(θ)( (θ) (θ) )dθ (θ) (θ) = ω(θ) (3) c(on ) q. () and q. (3) show that the probabiity measure of Y n equas to the one that directy generated in the domain of. Therefore, the partition constructed by q. (9) and q. () is a reaization of SP-Tree process in. ccording the transfer theorem (Theorem V.3 of chapter VI in []), the partition distribution is consistent from to. F MM for the SP-RM gorithm dispays an MM soution for the SP-RM. gorithm MM for SP-RM Input: Training data X, udget τ, Number of partices Output: reaization of the SP-Tree process; coordinates {(ξ i, η i )} n i= of X : Initiaize the partition and nodes coordinates : for t = : T do 3: Use -SM agorithm to update the partition structure, according to gorithm ; 4: Update nodes coordinates {ξ i, η i } n i= according to q. (4). 5: end for F. Updating nodes coordinates (ξ i, η i ) n i= (ξ i, η i ) s updating is impemented through the Metropois- Hastings agorithm. We propose the new vaues of ξ i, η i
5 Xuhui Fan, in Li, Scott. Sisson Figure 4: Toy ata Partition Visuaization (ase ). with the uniform distribution in [, ] and the acceptance ratio min(, α) is as foows: α(ξ i, ξ i ) = α(η j, η j ) = j = P (e ij ξ i, ξ \i, η j, θ) j = P (e ij ξ i, ξ \i, η j, θ) ; i = P (e i j η j, η \j, ξ i, θ) i = P (e i j η j, η \j, ξ i, θ) (4) G Visuaization of ase Figure 4 shows the visuaization of ase. References [] anie M. Roy. omputabiity, Inference and Modeing in Probabiistic Programming. Ph thesis, MIT,.
THE THREE POINT STEINER PROBLEM ON THE FLAT TORUS: THE MINIMAL LUNE CASE
THE THREE POINT STEINER PROBLEM ON THE FLAT TORUS: THE MINIMAL LUNE CASE KATIE L. MAY AND MELISSA A. MITCHELL Abstract. We show how to identify the minima path network connecting three fixed points on
More informationMath 124B January 31, 2012
Math 124B January 31, 212 Viktor Grigoryan 7 Inhomogeneous boundary vaue probems Having studied the theory of Fourier series, with which we successfuy soved boundary vaue probems for the homogeneous heat
More informationSUPPLEMENTARY MATERIAL TO INNOVATED SCALABLE EFFICIENT ESTIMATION IN ULTRA-LARGE GAUSSIAN GRAPHICAL MODELS
ISEE 1 SUPPLEMENTARY MATERIAL TO INNOVATED SCALABLE EFFICIENT ESTIMATION IN ULTRA-LARGE GAUSSIAN GRAPHICAL MODELS By Yingying Fan and Jinchi Lv University of Southern Caifornia This Suppementary Materia
More informationV.B The Cluster Expansion
V.B The Custer Expansion For short range interactions, speciay with a hard core, it is much better to repace the expansion parameter V( q ) by f(q ) = exp ( βv( q )) 1, which is obtained by summing over
More informationDYNAMIC RESPONSE OF CIRCULAR FOOTINGS ON SATURATED POROELASTIC HALFSPACE
3 th Word Conference on Earthquake Engineering Vancouver, B.C., Canada August -6, 4 Paper No. 38 DYNAMIC RESPONSE OF CIRCULAR FOOTINGS ON SATURATED POROELASTIC HALFSPACE Bo JIN SUMMARY The dynamic responses
More informationBASIC NOTIONS AND RESULTS IN TOPOLOGY. 1. Metric spaces. Sets with finite diameter are called bounded sets. For x X and r > 0 the set
BASIC NOTIONS AND RESULTS IN TOPOLOGY 1. Metric spaces A metric on a set X is a map d : X X R + with the properties: d(x, y) 0 and d(x, y) = 0 x = y, d(x, y) = d(y, x), d(x, y) d(x, z) + d(z, y), for a
More informationSome Measures for Asymmetry of Distributions
Some Measures for Asymmetry of Distributions Georgi N. Boshnakov First version: 31 January 2006 Research Report No. 5, 2006, Probabiity and Statistics Group Schoo of Mathematics, The University of Manchester
More informationPhysics Dynamics: Springs
F A C U L T Y O F E D U C A T I O N Department of Curricuum and Pedagogy Physics Dynamics: Springs Science and Mathematics Education Research Group Supported by UBC Teaching and Learning Enhancement Fund
More informationA Brief Introduction to Markov Chains and Hidden Markov Models
A Brief Introduction to Markov Chains and Hidden Markov Modes Aen B MacKenzie Notes for December 1, 3, &8, 2015 Discrete-Time Markov Chains You may reca that when we first introduced random processes,
More informationExpectation-Maximization for Estimating Parameters for a Mixture of Poissons
Expectation-Maximization for Estimating Parameters for a Mixture of Poissons Brandon Maone Department of Computer Science University of Hesini February 18, 2014 Abstract This document derives, in excrutiating
More informationV.B The Cluster Expansion
V.B The Custer Expansion For short range interactions, speciay with a hard core, it is much better to repace the expansion parameter V( q ) by f( q ) = exp ( βv( q )), which is obtained by summing over
More informationAn Extension of Almost Sure Central Limit Theorem for Order Statistics
An Extension of Amost Sure Centra Limit Theorem for Order Statistics T. Bin, P. Zuoxiang & S. Nadarajah First version: 6 December 2007 Research Report No. 9, 2007, Probabiity Statistics Group Schoo of
More informationXSAT of linear CNF formulas
XSAT of inear CN formuas Bernd R. Schuh Dr. Bernd Schuh, D-50968 Kön, Germany; bernd.schuh@netcoogne.de eywords: compexity, XSAT, exact inear formua, -reguarity, -uniformity, NPcompeteness Abstract. Open
More informationPhysics 235 Chapter 8. Chapter 8 Central-Force Motion
Physics 35 Chapter 8 Chapter 8 Centra-Force Motion In this Chapter we wi use the theory we have discussed in Chapter 6 and 7 and appy it to very important probems in physics, in which we study the motion
More informationIntegrating Factor Methods as Exponential Integrators
Integrating Factor Methods as Exponentia Integrators Borisav V. Minchev Department of Mathematica Science, NTNU, 7491 Trondheim, Norway Borko.Minchev@ii.uib.no Abstract. Recenty a ot of effort has been
More informationThe Sorting Problem. Inf 2B: Sorting, MergeSort and Divide-and-Conquer. What is important? Insertion Sort
The Sorting Probem Inf 2B: Sorting, MergeSort and Divide-and-Conquer Lecture 7 of DS thread Kyriaos Kaoroti Input: Tas: rray of items with comparabe eys. Sort the items in by increasing eys. Schoo of Informatics
More informationA. Distribution of the test statistic
A. Distribution of the test statistic In the sequentia test, we first compute the test statistic from a mini-batch of size m. If a decision cannot be made with this statistic, we keep increasing the mini-batch
More informationHomework 5 Solutions
Stat 310B/Math 230B Theory of Probabiity Homework 5 Soutions Andrea Montanari Due on 2/19/2014 Exercise [5.3.20] 1. We caim that n 2 [ E[h F n ] = 2 n i=1 A i,n h(u)du ] I Ai,n (t). (1) Indeed, integrabiity
More informationRestricted weak type on maximal linear and multilinear integral maps.
Restricted weak type on maxima inear and mutiinear integra maps. Oscar Basco Abstract It is shown that mutiinear operators of the form T (f 1,..., f k )(x) = R K(x, y n 1,..., y k )f 1 (y 1 )...f k (y
More informationSEMINAR 2. PENDULUMS. V = mgl cos θ. (2) L = T V = 1 2 ml2 θ2 + mgl cos θ, (3) d dt ml2 θ2 + mgl sin θ = 0, (4) θ + g l
Probem 7. Simpe Penduum SEMINAR. PENDULUMS A simpe penduum means a mass m suspended by a string weightess rigid rod of ength so that it can swing in a pane. The y-axis is directed down, x-axis is directed
More information14-6 The Equation of Continuity
14-6 The Equation of Continuity 14-6 The Equation of Continuity Motion of rea fuids is compicated and poory understood (e.g., turbuence) We discuss motion of an idea fuid 1. Steady fow: Laminar fow, the
More informationExplicit overall risk minimization transductive bound
1 Expicit overa risk minimization transductive bound Sergio Decherchi, Paoo Gastado, Sandro Ridea, Rodofo Zunino Dept. of Biophysica and Eectronic Engineering (DIBE), Genoa University Via Opera Pia 11a,
More informationMARKOV CHAINS AND MARKOV DECISION THEORY. Contents
MARKOV CHAINS AND MARKOV DECISION THEORY ARINDRIMA DATTA Abstract. In this paper, we begin with a forma introduction to probabiity and expain the concept of random variabes and stochastic processes. After
More informationCS229 Lecture notes. Andrew Ng
CS229 Lecture notes Andrew Ng Part IX The EM agorithm In the previous set of notes, we taked about the EM agorithm as appied to fitting a mixture of Gaussians. In this set of notes, we give a broader view
More informationAdd Math (4044/02) (+) x (+) 2. Find the coordinates of the points of intersection of the curve xy 2 the line 2y 1 x 0. [5]
Add Math (444/) Requirement : Answer a questions Tota mars : 7 Duration : hour 45 minutes. Sove the inequaity 5 and represent the soution set on the number ine. [4] 5 4 From the setch on number ine, we
More informationGauss Law. 2. Gauss s Law: connects charge and field 3. Applications of Gauss s Law
Gauss Law 1. Review on 1) Couomb s Law (charge and force) 2) Eectric Fied (fied and force) 2. Gauss s Law: connects charge and fied 3. Appications of Gauss s Law Couomb s Law and Eectric Fied Couomb s
More information1D Heat Propagation Problems
Chapter 1 1D Heat Propagation Probems If the ambient space of the heat conduction has ony one dimension, the Fourier equation reduces to the foowing for an homogeneous body cρ T t = T λ 2 + Q, 1.1) x2
More informationMore Scattering: the Partial Wave Expansion
More Scattering: the Partia Wave Expansion Michae Fower /7/8 Pane Waves and Partia Waves We are considering the soution to Schrödinger s equation for scattering of an incoming pane wave in the z-direction
More informationMath 124B January 17, 2012
Math 124B January 17, 212 Viktor Grigoryan 3 Fu Fourier series We saw in previous ectures how the Dirichet and Neumann boundary conditions ead to respectivey sine and cosine Fourier series of the initia
More informationAnalysis of Emerson s Multiple Model Interpolation Estimation Algorithms: The MIMO Case
Technica Report PC-04-00 Anaysis of Emerson s Mutipe Mode Interpoation Estimation Agorithms: The MIMO Case João P. Hespanha Dae E. Seborg University of Caifornia, Santa Barbara February 0, 004 Anaysis
More informationSTA 216 Project: Spline Approach to Discrete Survival Analysis
: Spine Approach to Discrete Surviva Anaysis November 4, 005 1 Introduction Athough continuous surviva anaysis differs much from the discrete surviva anaysis, there is certain ink between the two modeing
More informationDiscovery of Non-Euclidean Geometry
iscovery of Non-Eucidean Geometry pri 24, 2013 1 Hyperboic geometry János oyai (1802-1860), ar Friedrich Gauss (1777-1855), and Nikoai Ivanovich Lobachevsky (1792-1856) are three founders of non-eucidean
More informationBohr s atomic model. 1 Ze 2 = mv2. n 2 Z
Bohr s atomic mode Another interesting success of the so-caed od quantum theory is expaining atomic spectra of hydrogen and hydrogen-ike atoms. The eectromagnetic radiation emitted by free atoms is concentrated
More informationMATH 172: MOTIVATION FOR FOURIER SERIES: SEPARATION OF VARIABLES
MATH 172: MOTIVATION FOR FOURIER SERIES: SEPARATION OF VARIABLES Separation of variabes is a method to sove certain PDEs which have a warped product structure. First, on R n, a inear PDE of order m is
More informationAPPENDIX C FLEXING OF LENGTH BARS
Fexing of ength bars 83 APPENDIX C FLEXING OF LENGTH BARS C.1 FLEXING OF A LENGTH BAR DUE TO ITS OWN WEIGHT Any object ying in a horizonta pane wi sag under its own weight uness it is infinitey stiff or
More information12.2. Maxima and Minima. Introduction. Prerequisites. Learning Outcomes
Maima and Minima 1. Introduction In this Section we anayse curves in the oca neighbourhood of a stationary point and, from this anaysis, deduce necessary conditions satisfied by oca maima and oca minima.
More information2M2. Fourier Series Prof Bill Lionheart
M. Fourier Series Prof Bi Lionheart 1. The Fourier series of the periodic function f(x) with period has the form f(x) = a 0 + ( a n cos πnx + b n sin πnx ). Here the rea numbers a n, b n are caed the Fourier
More informationSeparation of Variables and a Spherical Shell with Surface Charge
Separation of Variabes and a Spherica She with Surface Charge In cass we worked out the eectrostatic potentia due to a spherica she of radius R with a surface charge density σθ = σ cos θ. This cacuation
More informationThe Group Structure on a Smooth Tropical Cubic
The Group Structure on a Smooth Tropica Cubic Ethan Lake Apri 20, 2015 Abstract Just as in in cassica agebraic geometry, it is possibe to define a group aw on a smooth tropica cubic curve. In this note,
More informationarxiv: v1 [math.co] 17 Dec 2018
On the Extrema Maximum Agreement Subtree Probem arxiv:1812.06951v1 [math.o] 17 Dec 2018 Aexey Markin Department of omputer Science, Iowa State University, USA amarkin@iastate.edu Abstract Given two phyogenetic
More informationLecture 8 February 18, 2010
Sources of Eectromagnetic Fieds Lecture 8 February 18, 2010 We now start to discuss radiation in free space. We wi reorder the materia of Chapter 9, bringing sections 6 7 up front. We wi aso cover some
More informationVersion 2.2 NE03 - Faraday's Law of Induction
Definition Version. Laboratory Manua Department of Physics he University of Hong Kong Aims o demonstrate various properties of Faraday s Law such as: 1. Verify the aw.. Demonstrate the ighty damped osciation
More information6.434J/16.391J Statistics for Engineers and Scientists May 4 MIT, Spring 2006 Handout #17. Solution 7
6.434J/16.391J Statistics for Engineers and Scientists May 4 MIT, Spring 2006 Handout #17 Soution 7 Probem 1: Generating Random Variabes Each part of this probem requires impementation in MATLAB. For the
More informationTheory and implementation behind: Universal surface creation - smallest unitcell
Teory and impementation beind: Universa surface creation - smaest unitce Bjare Brin Buus, Jaob Howat & Tomas Bigaard September 15, 218 1 Construction of surface sabs Te aim for tis part of te project is
More informationWeek 6 Lectures, Math 6451, Tanveer
Fourier Series Week 6 Lectures, Math 645, Tanveer In the context of separation of variabe to find soutions of PDEs, we encountered or and in other cases f(x = f(x = a 0 + f(x = a 0 + b n sin nπx { a n
More informationIn-plane shear stiffness of bare steel deck through shell finite element models. G. Bian, B.W. Schafer. June 2017
In-pane shear stiffness of bare stee deck through she finite eement modes G. Bian, B.W. Schafer June 7 COLD-FORMED STEEL RESEARCH CONSORTIUM REPORT SERIES CFSRC R-7- SDII Stee Diaphragm Innovation Initiative
More informationJoel Broida UCSD Fall 2009 Phys 130B QM II. Homework Set 2 DO ALL WORK BY HAND IN OTHER WORDS, DON T USE MATHEMAT- ICA OR ANY CALCULATORS.
Joe Broida UCSD Fa 009 Phys 30B QM II Homework Set DO ALL WORK BY HAND IN OTHER WORDS, DON T USE MATHEMAT- ICA OR ANY CALCULATORS. You may need to use one or more of these: Y 0 0 = 4π Y 0 = 3 4π cos Y
More informationBourgain s Theorem. Computational and Metric Geometry. Instructor: Yury Makarychev. d(s 1, s 2 ).
Bourgain s Theorem Computationa and Metric Geometry Instructor: Yury Makarychev 1 Notation Given a metric space (X, d) and S X, the distance from x X to S equas d(x, S) = inf d(x, s). s S The distance
More informationStrauss PDEs 2e: Section Exercise 1 Page 1 of 7
Strauss PDEs 2e: Section 4.3 - Exercise 1 Page 1 of 7 Exercise 1 Find the eigenvaues graphicay for the boundary conditions X(0) = 0, X () + ax() = 0. Assume that a 0. Soution The aim here is to determine
More informationTwo Birds With One Stone: An Efficient Hierarchical Framework for Top-k and Threshold-based String Similarity Search
Two Birds With One Stone: An Efficient Hierarchica Framework for Top-k and Threshod-based String Simiarity Search Jin Wang Guoiang Li Dong Deng Yong Zhang Jianhua Feng Department of Computer Science and
More informationLECTURE 10. The world of pendula
LECTURE 0 The word of pendua For the next few ectures we are going to ook at the word of the pane penduum (Figure 0.). In a previous probem set we showed that we coud use the Euer- Lagrange method to derive
More information$, (2.1) n="# #. (2.2)
Chapter. Eectrostatic II Notes: Most of the materia presented in this chapter is taken from Jackson, Chap.,, and 4, and Di Bartoo, Chap... Mathematica Considerations.. The Fourier series and the Fourier
More informationApproximate Bandwidth Allocation for Fixed-Priority-Scheduled Periodic Resources (WSU-CS Technical Report Version)
Approximate Bandwidth Aocation for Fixed-Priority-Schedued Periodic Resources WSU-CS Technica Report Version) Farhana Dewan Nathan Fisher Abstract Recent research in compositiona rea-time systems has focused
More informationApproximation and Fast Calculation of Non-local Boundary Conditions for the Time-dependent Schrödinger Equation
Approximation and Fast Cacuation of Non-oca Boundary Conditions for the Time-dependent Schrödinger Equation Anton Arnod, Matthias Ehrhardt 2, and Ivan Sofronov 3 Universität Münster, Institut für Numerische
More informationVI.G Exact free energy of the Square Lattice Ising model
VI.G Exact free energy of the Square Lattice Ising mode As indicated in eq.(vi.35), the Ising partition function is reated to a sum S, over coections of paths on the attice. The aowed graphs for a square
More informationIterative Decoding Performance Bounds for LDPC Codes on Noisy Channels
Iterative Decoding Performance Bounds for LDPC Codes on Noisy Channes arxiv:cs/060700v1 [cs.it] 6 Ju 006 Chun-Hao Hsu and Achieas Anastasopouos Eectrica Engineering and Computer Science Department University
More informationEfficient Generation of Random Bits from Finite State Markov Chains
Efficient Generation of Random Bits from Finite State Markov Chains Hongchao Zhou and Jehoshua Bruck, Feow, IEEE Abstract The probem of random number generation from an uncorreated random source (of unknown
More informationAppendix of the Paper The Role of No-Arbitrage on Forecasting: Lessons from a Parametric Term Structure Model
Appendix of the Paper The Roe of No-Arbitrage on Forecasting: Lessons from a Parametric Term Structure Mode Caio Ameida cameida@fgv.br José Vicente jose.vaentim@bcb.gov.br June 008 1 Introduction In this
More informationAALBORG UNIVERSITY. The distribution of communication cost for a mobile service scenario. Jesper Møller and Man Lung Yiu. R June 2009
AALBORG UNIVERSITY The distribution of communication cost for a mobie service scenario by Jesper Møer and Man Lung Yiu R-29-11 June 29 Department of Mathematica Sciences Aaborg University Fredrik Bajers
More informationASummaryofGaussianProcesses Coryn A.L. Bailer-Jones
ASummaryofGaussianProcesses Coryn A.L. Baier-Jones Cavendish Laboratory University of Cambridge caj@mrao.cam.ac.uk Introduction A genera prediction probem can be posed as foows. We consider that the variabe
More informationCandidate Number. General Certificate of Education Advanced Level Examination January 2012
entre Number andidate Number Surname Other Names andidate Signature Genera ertificate of Education dvanced Leve Examination January 212 Physics PHY4/1 Unit 4 Fieds and Further Mechanics Section Tuesday
More information1.2 Partial Wave Analysis
February, 205 Lecture X.2 Partia Wave Anaysis We have described scattering in terms of an incoming pane wave, a momentum eigenet, and and outgoing spherica wave, aso with definite momentum. We now consider
More informationThe distribution of the number of nodes in the relative interior of the typical I-segment in homogeneous planar anisotropic STIT Tessellations
Comment.Math.Univ.Caroin. 51,3(21) 53 512 53 The distribution of the number of nodes in the reative interior of the typica I-segment in homogeneous panar anisotropic STIT Tesseations Christoph Thäe Abstract.
More informationA Laplace type problem for a regular lattice with six obstacles
Reent Advanes in Appied & Biomedia Informatis and Computationa Engineering in Systems Appiations A Lapae type probem for a reguar attie with six obstaes D. Baria, G. Caristi, A. Pugisi University of Messina
More informationLecture 17 - The Secrets we have Swept Under the Rug
Lecture 17 - The Secrets we have Swept Under the Rug Today s ectures examines some of the uirky features of eectrostatics that we have negected up unti this point A Puzze... Let s go back to the basics
More informationPROCEEDINGS OF THE YEREVAN STATE UNIVERSITY GEOMETRIC PROBABILITY CALCULATION FOR A TRIANGLE
PROCEEDINGS OF THE YEREVAN STATE UNIVERSITY Physica and Mathematica Sciences 07, 5(3, p. 6 M a t h e m a t i c s GEOMETRIC PROBABILITY CALCULATION FOR A TRIANGLE N. G. AHARONYAN, H. O. HARUTYUNYAN Chair
More informationMinimizing Total Weighted Completion Time on Uniform Machines with Unbounded Batch
The Eighth Internationa Symposium on Operations Research and Its Appications (ISORA 09) Zhangiaie, China, September 20 22, 2009 Copyright 2009 ORSC & APORC, pp. 402 408 Minimizing Tota Weighted Competion
More informationChemical Kinetics Part 2
Integrated Rate Laws Chemica Kinetics Part 2 The rate aw we have discussed thus far is the differentia rate aw. Let us consider the very simpe reaction: a A à products The differentia rate reates the rate
More informationBackward Monte Carlo Simulations in Radiative Heat Transfer
Backward Monte Caro Simuations in Radiative Heat Transfer Michae F. Modest Department of Mechanica and Nucear Engineering Penn State University University Park, PA 82 emai: mfm@psu.edu August 29, 2 Abstract
More informationLobontiu: System Dynamics for Engineering Students Website Chapter 3 1. z b z
Chapter W3 Mechanica Systems II Introduction This companion website chapter anayzes the foowing topics in connection to the printed-book Chapter 3: Lumped-parameter inertia fractions of basic compiant
More informationEffect of transport ratio on source term in determination of surface emission coefficient
Internationa Journa of heoretica & Appied Sciences, (): 74-78(9) ISSN : 975-78 Effect of transport ratio on source term in determination of surface emission coefficient Sanjeev Kumar and Apna Mishra epartment
More informationPhysicsAndMathsTutor.com
. Two points A and B ie on a smooth horizonta tabe with AB = a. One end of a ight eastic spring, of natura ength a and moduus of easticity mg, is attached to A. The other end of the spring is attached
More informationOn some problems of synthesis of spatial five-bar hinged mechanisms with two degrees of freedom
Internationa Journa of Mechanica Engineering and Appications 014 (6): 104-110 Puished onine ecemer 18, 014 (http://www.sciencepuishinggroup.com/j/ijmea) doi: 10.11648/j.ijmea.014006.14 ISSN: 330-03X (Print)
More information#A48 INTEGERS 12 (2012) ON A COMBINATORIAL CONJECTURE OF TU AND DENG
#A48 INTEGERS 12 (2012) ON A COMBINATORIAL CONJECTURE OF TU AND DENG Guixin Deng Schoo of Mathematica Sciences, Guangxi Teachers Education University, Nanning, P.R.China dengguixin@ive.com Pingzhi Yuan
More informationMinimum Enclosing Circle of a Set of Fixed Points and a Mobile Point
Minimum Encosing Circe of a Set of Fixed Points and a Mobie Point Aritra Banik 1, Bhaswar B. Bhattacharya 2, and Sandip Das 1 1 Advanced Computing and Microeectronics Unit, Indian Statistica Institute,
More information<C 2 2. λ 2 l. λ 1 l 1 < C 1
Teecommunication Network Contro and Management (EE E694) Prof. A. A. Lazar Notes for the ecture of 7/Feb/95 by Huayan Wang (this document was ast LaT E X-ed on May 9,995) Queueing Primer for Muticass Optima
More informationElements of Kinetic Theory
Eements of Kinetic Theory Diffusion Mean free path rownian motion Diffusion against a density gradient Drift in a fied Einstein equation aance between diffusion and drift Einstein reation Constancy of
More informationSchedulability Analysis of Deferrable Scheduling Algorithms for Maintaining Real-Time Data Freshness
1 Scheduabiity Anaysis of Deferrabe Scheduing Agorithms for Maintaining Rea-Time Data Freshness Song Han, Deji Chen, Ming Xiong, Kam-yiu Lam, Aoysius K. Mok, Krithi Ramamritham UT Austin, Emerson Process
More informationHigh Efficiency Development of a Reciprocating Compressor by Clarification of Loss Generation in Bearings
Purdue University Purdue e-pubs Internationa Compressor Engineering Conference Schoo of Mechanica Engineering 2010 High Efficiency Deveopment of a Reciprocating Compressor by Carification of Loss Generation
More informationGeneralized Bell polynomials and the combinatorics of Poisson central moments
Generaized Be poynomias and the combinatorics of Poisson centra moments Nicoas Privaut Division of Mathematica Sciences Schoo of Physica and Mathematica Sciences Nanyang Technoogica University SPMS-MAS-05-43,
More informationCombining reaction kinetics to the multi-phase Gibbs energy calculation
7 th European Symposium on Computer Aided Process Engineering ESCAPE7 V. Pesu and P.S. Agachi (Editors) 2007 Esevier B.V. A rights reserved. Combining reaction inetics to the muti-phase Gibbs energy cacuation
More informationDavid Eigen. MA112 Final Paper. May 10, 2002
David Eigen MA112 Fina Paper May 1, 22 The Schrodinger equation describes the position of an eectron as a wave. The wave function Ψ(t, x is interpreted as a probabiity density for the position of the eectron.
More informationEfficiently Generating Random Bits from Finite State Markov Chains
1 Efficienty Generating Random Bits from Finite State Markov Chains Hongchao Zhou and Jehoshua Bruck, Feow, IEEE Abstract The probem of random number generation from an uncorreated random source (of unknown
More informationModel Solutions (week 4)
CIV-E16 (17) Engineering Computation and Simuation 1 Home Exercise 6.3 Mode Soutions (week 4) Construct the inear Lagrange basis functions (noda vaues as degrees of freedom) of the ine segment reference
More informationA Branch and Cut Algorithm to Design. LDPC Codes without Small Cycles in. Communication Systems
A Branch and Cut Agorithm to Design LDPC Codes without Sma Cyces in Communication Systems arxiv:1709.09936v1 [cs.it] 28 Sep 2017 Banu Kabakuak 1, Z. Caner Taşkın 1, and Ai Emre Pusane 2 1 Department of
More informationParallel-Axis Theorem
Parae-Axis Theorem In the previous exampes, the axis of rotation coincided with the axis of symmetry of the object For an arbitrary axis, the paraeaxis theorem often simpifies cacuations The theorem states
More informationORTHOGONAL MULTI-WAVELETS FROM MATRIX FACTORIZATION
J. Korean Math. Soc. 46 2009, No. 2, pp. 281 294 ORHOGONAL MLI-WAVELES FROM MARIX FACORIZAION Hongying Xiao Abstract. Accuracy of the scaing function is very crucia in waveet theory, or correspondingy,
More informationXI PHYSICS. M. Affan Khan LECTURER PHYSICS, AKHSS, K. https://promotephysics.wordpress.com
XI PHYSICS M. Affan Khan LECTURER PHYSICS, AKHSS, K affan_414@ive.com https://promotephysics.wordpress.com [TORQUE, ANGULAR MOMENTUM & EQUILIBRIUM] CHAPTER NO. 5 Okay here we are going to discuss Rotationa
More informationPHYS 110B - HW #1 Fall 2005, Solutions by David Pace Equations referenced as Eq. # are from Griffiths Problem statements are paraphrased
PHYS 110B - HW #1 Fa 2005, Soutions by David Pace Equations referenced as Eq. # are from Griffiths Probem statements are paraphrased [1.] Probem 6.8 from Griffiths A ong cyinder has radius R and a magnetization
More information17 Lecture 17: Recombination and Dark Matter Production
PYS 652: Astrophysics 88 17 Lecture 17: Recombination and Dark Matter Production New ideas pass through three periods: It can t be done. It probaby can be done, but it s not worth doing. I knew it was
More informationDo Schools Matter for High Math Achievement? Evidence from the American Mathematics Competitions Glenn Ellison and Ashley Swanson Online Appendix
VOL. NO. DO SCHOOLS MATTER FOR HIGH MATH ACHIEVEMENT? 43 Do Schoos Matter for High Math Achievement? Evidence from the American Mathematics Competitions Genn Eison and Ashey Swanson Onine Appendix Appendix
More informationLecture 11. Fourier transform
Lecture. Fourier transform Definition and main resuts Let f L 2 (R). The Fourier transform of a function f is a function f(α) = f(x)t iαx dx () The normaized Fourier transform of f is a function R ˆf =
More informationProblem Set 6: Solutions
University of Aabama Department of Physics and Astronomy PH 102 / LeCair Summer II 2010 Probem Set 6: Soutions 1. A conducting rectanguar oop of mass M, resistance R, and dimensions w by fas from rest
More informationChemical Kinetics Part 2. Chapter 16
Chemica Kinetics Part 2 Chapter 16 Integrated Rate Laws The rate aw we have discussed thus far is the differentia rate aw. Let us consider the very simpe reaction: a A à products The differentia rate reates
More informationPublished in: Proceedings of the Twenty Second Nordic Seminar on Computational Mechanics
Aaborg Universitet An Efficient Formuation of the Easto-pastic Constitutive Matrix on Yied Surface Corners Causen, Johan Christian; Andersen, Lars Vabbersgaard; Damkide, Lars Pubished in: Proceedings of
More informationGOYAL BROTHERS PRAKASHAN
Assignments in Mathematics Cass IX (Term 2) 14. STATISTICS IMPORTANT TERMS, DEFINITIONS AND RESULTS The facts or figures, which are numerica or otherwise, coected with a definite purpose are caed data.
More informationNOISE-INDUCED STABILIZATION OF STOCHASTIC DIFFERENTIAL EQUATIONS
NOISE-INDUCED STABILIZATION OF STOCHASTIC DIFFERENTIAL EQUATIONS TONY ALLEN, EMILY GEBHARDT, AND ADAM KLUBALL 3 ADVISOR: DR. TIFFANY KOLBA 4 Abstract. The phenomenon of noise-induced stabiization occurs
More informationFRIEZE GROUPS IN R 2
FRIEZE GROUPS IN R 2 MAXWELL STOLARSKI Abstract. Focusing on the Eucidean pane under the Pythagorean Metric, our goa is to cassify the frieze groups, discrete subgroups of the set of isometries of the
More informationc 2016 Georgios Rovatsos
c 2016 Georgios Rovatsos QUICKEST CHANGE DETECTION WITH APPLICATIONS TO LINE OUTAGE DETECTION BY GEORGIOS ROVATSOS THESIS Submitted in partia fufiment of the requirements for the degree of Master of Science
More informationExtensions of Laplace Type Problems in the Euclidean Space
Internationa Mathematica Forum, Vo. 9, 214, no. 26, 1253-1259 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/1.12988/imf.214.46112 Extensions of Lapace Type Probems in the Eucidean Space Giuseppe Caristi
More information