Similarities Between Hidden Markov Models and Turing Machines, and Possible Applications Towards Bioinformatics
|
|
- Lauren Chase
- 6 years ago
- Views:
Transcription
1 Bonformatcs Fnal Proect, Fall 2000 Smlartes Between Hdden Markov Models and Turng Machnes, and Possble Applcatons Towards Bonformatcs Tyler Cheung Over the past fve or sx years, Hdden Markov Models (HMMs) have become an mportant tool for certan bonformatcal tasks, ncludng sequence and structural algnment. The advantage of an HMM s that t gves bonformatcsts, among other thngs, a rgorous mathematcal method, through probablty and combnatorcs, of algnng two or more sequences of protens and nuclec acds. However, mathematcal constructs known as "Turng Machnes" are very smlar to how HMMs are defned, and thus, we wsh to consder whether these machnes have any bonformatcal applcatons. HMMs can be brefly descrbed as a seres of states lnked by several probablstc paths. A typcal model often used for sequence algnment s descrbed n Krogh et al, 1994 (1). The states represent matches, gap nsertons, or gap deletons, and the match states also defne the probabltes for the occurrence of each amno acd. The arrangement of the states and the probabltes are often bult by a gven tranng set of amno acd sequences,.e. a known set of orthologs. If one partcular sequence n queston wants to be scored aganst the known tranng set, every possble path through the HMM that gves that sequence s determned and the total probablty, or the sum of the probabltes of all the paths, s calculated. Ths probablty then serves as the bass of the score. A dagram of the dfferent states and ther nterrelatons s gven n Eddy, 1996 (2): Page 1 of 5
2 In ths case, the M states are the match states wth the amno acd probabltes, the D states are the deleton states, and the I states are the nserton states. Each of the arrows denotng the paths also would be assgned a probablty. Ths would be a typcal HMM for a 2 or 3 amno acd sequence. A Turng Machne s smlar to ths n that t also s a set of states connected by paths. The Turng Machne was devsed by Brtsh mathematcan Alan Turng as a way of dealng wth the decdablty problem, or "Entschedungsproblem" (3). The mathematcan Kurt Gödel had shown logcally that certan mathematcal problems were unsolvable, and Turng's nventon was a practcal proof of that, but one whch also happened to be programmable and thus became the foundaton of modern computer scence (4). The machne can be loosely descrbed as a "black box" equpped wth a 1 dmensonal data tape, whch has three defned functons - read, wrte, and move. The box tself can assume any number of a fnte number of states, smlar to a Hdden Markov Model. A typcal Turng machne moves n a seres of tme steps - each step nvolves readng from the tape, assumng the state based on the read nput, movng along the tape, and wrtng. The tape tself contans an ntal set of symbols, and to whch are wrtten new symbols by the Turng Machne. The machne tself moves one slot on the tape wth each step. We can bascally defne each Turng Machne wth "quntuples," a set of fve values, statng the read nput, the current state, the new state, the drecton to move left or rght, and what to wrte. In mathematcal terms, Feynman proposed representng the quntuples as a seres of 5 varable sets, Q, S, Q, S, and D, subected to the three functons F, G, and D where Q = F(Q, S ) S = G(Q, S ) D = D(Q, S ) Q and S represent the ntal states and nput tape symbol, respectvely, whle Q and S represent the new state and the wrte symbol. D represents the drecton for the machne to move (5). A more ntutve way of dong ths s to draw a state dagram smlar to that of a Hdden Markov Model n fgure 1, as follows (5): A farly good llustraton of how a Turng Machne works s gven by Rchard Feynman n hs seres of lectures on computaton at Caltech n the 1980's (5). A verson of the machne he descrbed s shown here. Ths partcular machne checks for properly nested parentheses n a strng of arbtrary length. The state dagram s as follows: Page 2 of 5
3 We supply a tape wth the followng symbols: E ( ( ) ( ) ( ) ( ) ) ( ( ( ( ( ) ( ) ) ( ( ) ) ) ) ) ) ) E Ths s bascally a parentheses strng flanked by E symbols. We defne the machne to start at the leftmost E, and work ts way step by step to the rght, keepng the machne n the state R1. It gnores any left parentheses, "(",.e. wrtng left parentheses back nto ther orgnal slots, untl t hts a rght parenthess, ")", whereupon t replaces the ")" wth an "X", swtches nto state L1 and changes drecton back left. It replaces the frst "(" t sees wth another "X", swtches back to R1 and changes drecton back to the rght. Eventually, t wll reach ether the left E or the rght E, where we can tell whether the parentheses are properly nested by several of the followng ways: f t has ht the left E, we know that the parentheses strng s not properly nested, as ths sgnfes an unpared ")". We can replace that leftmost E wth a "0" to sgnfy "false". If t hts the rght E, then we have the machne swtch nto state L2 where t moves left. If t hts an "X," nothng happens, but f t hts a "(," t swtches nto state L3. When t hts the left E, t wrtes a 1 f n state L2, and a 0 f n state L3. Thus, we can tell f the parentheses were properly nested by lookng at the output at the leftmost E when the machne has fnshed. The fnshed state of the tape s thus: 0 X X X X X X X X X X X X X X X X X X X X X X X X X X ) ) E Turng machnes can also be used to defne varous mathematcal functons. An example of a smple adder s gven as follows: Page 3 of 5
4 Intal tape: A B C D The machne would move rght untl t ht a B, move left, and replace the dgt mmedately to the left wth another B and change nto a one of 2 states (R2, R3) representng the dgt t ust replaced, move rght untl t ht the C, and replace the dgt to the left wth a C, and assume one of three states representng the sum of that dgt and the one represented by the correspondng dgt of B (0, 1, 0 + carry - states R4, R5, and R6, respectvely). It moves rght, and wrtes that sum dgt nto the space drectly to the rght of the last C whle shftng exstng dgts to the rght of C further rght by 1 slot. It then moves left to the leftmost B to deal wth the next dgts. If t needs to carry a dgt, t assumes an alternate leftward state to sgnfy ths. Each new dgt sum s nserted nto the space drectly to the rght of the last C. We would, n theory, end up wth the tape A B B B B B C C C C C D The Turng Machne model s partcularly powerful, as once the basc mathematcal operatons are defned, one can do a varety of tasks wth them. In lght of ths, we can assume that Turng Machnes can be appled to certan common bonformatcs tasks. One possble use would be to mplement a smple Needleman-Wunsch scorng algorthm (6) by ncorporatng the addng machne descrbed above. In comparng two sample proten sequences, say ALWE and ALPN, we could have a tape as follows: X 0 A L W E X 1 A L P N X 2 X 3 X 4 A Turng Machne shuttlng back and forth could easly match up the dfferent pars of amno acds, and wrte the rows, n sequental order, of a Needleman-Wunsch smlarty matrx between X 2 and X 3. It could then sum up the smlarty matrx and wrte the resultng rows between X and X. If the rows are separated by a placeholder, you could even have the 3 4 machne zp back and forth among the rows n X and X, fnd the maxma of each row, and 3 4 wrte down possble algnment paths through the Needleman-Wunsch matrx on the tape after X. Another applcaton would be to smulate ndvdual paths through a HMM, wth 4 probablstc Turng Machnes descrbed n Leeuw et al (7). Such machnes have the functons F, G, or D of the quntuples set to generate a random values from the fnte set of possble Turng machne states or outputs. We could set up a generc nput tape to such a machne, such as X 1 X 2 X 3... X 20 for a random 20 amno acd sequence from a gven HMM confguraton, mnus any gaps that Page 4 of 5
5 mght be nserted, and run t through a Turng Machne wth a state dagram and quntuple functons defned to be equvalent to the HMM. The 1 letter abbrevaton for each amno acd, or a placeholder for gaps, could be nserted as the Turng machne steps over each X slot, thus generatng on the tape a random sequence from the HMM. Or, we could have a gven amno acd sequence on a tape,.e. T Y N G A A V X1 and we could somehow have a Turng Machne defned wth a HMM state dagram step through the sequence, evaluate all the possble paths through the state dagram, and calculate the sum of the probabltes, gvng the score. All ths leads to the obvous queston - what advantages do Turng Machnes offer over current sequence algnment technques? Wth the computers currently n use, a Turng Machne s a "vrtual" or emulated mplementaton wrtten on top of the exstng natve language of the computer. Thus, t s often a slower way of dong thngs rather than encodng programs wth smple logc nstructons wth assembly language, or wth languages such as C or perl. As noted above, however, ther smlarty wth HMMs could mean that t would be easy to couple them wth a HMM based algnment or proflng scheme. Also, the smularty of turng machnes wth natural bologcal obects that handle bts of nformaton s strkng - both usually operate on a 1-dmensonal nformaton storage system. What s a RNA polymerase but a Turng Machne defned as a coper wth separate read and wrte tapes? What s a rbosome but a translatng Turng Machne? The use of nuclec acd based Turng Machnes have already been touched on n Adleman, 1994 (8), and Shapro, 2000 (9). As the felds of bocomputng, proten desgn, proten engneerng, and structure predcton mprove, we may be able to desgn molecular Turng machnes able to perform sequence algnments drectly n the test tubes, or perhaps even n vvo sequence analyss or structure predcton. In other words, there may be a potental n bologcal systems for a natve or "hard" Turng Machne. Also, gven the nature of the unversal Turng Machne and the relatvely free-form nature of the machne, there are probably a multtude of bonformatcs applcatons overlooked n ths report and are ust watng to be dscovered. Works Cted 1. Krogh, A., Brown, B., Man, I.S., Solander, K., Haussler, D. (1994). "Hdden Markov Models n Computatonal Bology: Applcatons to Proten Modelng." J. Mol. Bol. 235: Eddy, S.R. (1996). "Hdden Markov Models." Curr. Opn. Struc. Bol. 6, Turng, A.M. "On the Computablty of Numbers, Wth an Applcaton to The Entschedungsproblem." Proc. of the London Mathematcal Socety Hopcraft, J.E. (1984). "Turng Machnes." Sc. Am Feynman, R.P. (1996). Feynman Lectures on Computaton. Eds. T. Hey and R. W. Allen. New York: Addson-Wesley. 6. Needleman, S. B. and Wunsch, C. D. (1971). "A general method applcable to the search for smlartes n the amno acd sequence of two protens." J. Mol. Bol. 48: Leeuw, K. de, Moore, E.F., Shannon, C.E., and Shapro, N. (1956). "Computablty by Probablstc Machnes." Annals of Mathematcal Studes (Automata Studes). 34: Adleman, L. (1994). "Molecular Computaton of Solutons to Combnatoral Problems." Scence. 266: Shapro, E. (2000). "A Mechancal Turng Machne: Blueprnt for a Bomolecular Computer." < Page 5 of 5
Turing Machines (intro)
CHAPTER 3 The Church-Turng Thess Contents Turng Machnes defntons, examples, Turng-recognzable and Turng-decdable languages Varants of Turng Machne Multtape Turng machnes, non-determnstc Turng Machnes,
More informationNote on EM-training of IBM-model 1
Note on EM-tranng of IBM-model INF58 Language Technologcal Applcatons, Fall The sldes on ths subject (nf58 6.pdf) ncludng the example seem nsuffcent to gve a good grasp of what s gong on. Hence here are
More informationModule 9. Lecture 6. Duality in Assignment Problems
Module 9 1 Lecture 6 Dualty n Assgnment Problems In ths lecture we attempt to answer few other mportant questons posed n earler lecture for (AP) and see how some of them can be explaned through the concept
More informationC/CS/Phy191 Problem Set 3 Solutions Out: Oct 1, 2008., where ( 00. ), so the overall state of the system is ) ( ( ( ( 00 ± 11 ), Φ ± = 1
C/CS/Phy9 Problem Set 3 Solutons Out: Oct, 8 Suppose you have two qubts n some arbtrary entangled state ψ You apply the teleportaton protocol to each of the qubts separately What s the resultng state obtaned
More informationCHAPTER 14 GENERAL PERTURBATION THEORY
CHAPTER 4 GENERAL PERTURBATION THEORY 4 Introducton A partcle n orbt around a pont mass or a sphercally symmetrc mass dstrbuton s movng n a gravtatonal potental of the form GM / r In ths potental t moves
More informationThe Feynman path integral
The Feynman path ntegral Aprl 3, 205 Hesenberg and Schrödnger pctures The Schrödnger wave functon places the tme dependence of a physcal system n the state, ψ, t, where the state s a vector n Hlbert space
More informationBasic Regular Expressions. Introduction. Introduction to Computability. Theory. Motivation. Lecture4: Regular Expressions
Introducton to Computablty Theory Lecture: egular Expressons Prof Amos Israel Motvaton If one wants to descrbe a regular language, La, she can use the a DFA, Dor an NFA N, such L ( D = La that that Ths
More informationDifference Equations
Dfference Equatons c Jan Vrbk 1 Bascs Suppose a sequence of numbers, say a 0,a 1,a,a 3,... s defned by a certan general relatonshp between, say, three consecutve values of the sequence, e.g. a + +3a +1
More informationDEMO #8 - GAUSSIAN ELIMINATION USING MATHEMATICA. 1. Matrices in Mathematica
demo8.nb 1 DEMO #8 - GAUSSIAN ELIMINATION USING MATHEMATICA Obectves: - defne matrces n Mathematca - format the output of matrces - appl lnear algebra to solve a real problem - Use Mathematca to perform
More informationStructure and Drive Paul A. Jensen Copyright July 20, 2003
Structure and Drve Paul A. Jensen Copyrght July 20, 2003 A system s made up of several operatons wth flow passng between them. The structure of the system descrbes the flow paths from nputs to outputs.
More informationA Bayes Algorithm for the Multitask Pattern Recognition Problem Direct Approach
A Bayes Algorthm for the Multtask Pattern Recognton Problem Drect Approach Edward Puchala Wroclaw Unversty of Technology, Char of Systems and Computer etworks, Wybrzeze Wyspanskego 7, 50-370 Wroclaw, Poland
More informationIntroduction to Vapor/Liquid Equilibrium, part 2. Raoult s Law:
CE304, Sprng 2004 Lecture 4 Introducton to Vapor/Lqud Equlbrum, part 2 Raoult s Law: The smplest model that allows us do VLE calculatons s obtaned when we assume that the vapor phase s an deal gas, and
More informationIntroduction to Algorithms
Introducton to Algorthms 6.046J/8.40J Lecture 7 Prof. Potr Indyk Data Structures Role of data structures: Encapsulate data Support certan operatons (e.g., INSERT, DELETE, SEARCH) Our focus: effcency of
More informationSplit alignment. Martin C. Frith April 13, 2012
Splt algnment Martn C. Frth Aprl 13, 2012 1 Introducton Ths document s about algnng a query sequence to a genome, allowng dfferent parts of the query to match dfferent parts of the genome. Here are some
More informationDesign and Analysis of Algorithms
Desgn and Analyss of Algorthms CSE 53 Lecture 4 Dynamc Programmng Junzhou Huang, Ph.D. Department of Computer Scence and Engneerng CSE53 Desgn and Analyss of Algorthms The General Dynamc Programmng Technque
More information} Often, when learning, we deal with uncertainty:
Uncertanty and Learnng } Often, when learnng, we deal wth uncertanty: } Incomplete data sets, wth mssng nformaton } Nosy data sets, wth unrelable nformaton } Stochastcty: causes and effects related non-determnstcally
More informationGrover s Algorithm + Quantum Zeno Effect + Vaidman
Grover s Algorthm + Quantum Zeno Effect + Vadman CS 294-2 Bomb 10/12/04 Fall 2004 Lecture 11 Grover s algorthm Recall that Grover s algorthm for searchng over a space of sze wors as follows: consder the
More information12. The Hamilton-Jacobi Equation Michael Fowler
1. The Hamlton-Jacob Equaton Mchael Fowler Back to Confguraton Space We ve establshed that the acton, regarded as a functon of ts coordnate endponts and tme, satsfes ( ) ( ) S q, t / t+ H qpt,, = 0, and
More informationModule 3 LOSSY IMAGE COMPRESSION SYSTEMS. Version 2 ECE IIT, Kharagpur
Module 3 LOSSY IMAGE COMPRESSION SYSTEMS Verson ECE IIT, Kharagpur Lesson 6 Theory of Quantzaton Verson ECE IIT, Kharagpur Instructonal Objectves At the end of ths lesson, the students should be able to:
More informationOnline Classification: Perceptron and Winnow
E0 370 Statstcal Learnng Theory Lecture 18 Nov 8, 011 Onlne Classfcaton: Perceptron and Wnnow Lecturer: Shvan Agarwal Scrbe: Shvan Agarwal 1 Introducton In ths lecture we wll start to study the onlne learnng
More information= z 20 z n. (k 20) + 4 z k = 4
Problem Set #7 solutons 7.2.. (a Fnd the coeffcent of z k n (z + z 5 + z 6 + z 7 + 5, k 20. We use the known seres expanson ( n+l ( z l l z n below: (z + z 5 + z 6 + z 7 + 5 (z 5 ( + z + z 2 + z + 5 5
More informationSupporting Information
Supportng Informaton The neural network f n Eq. 1 s gven by: f x l = ReLU W atom x l + b atom, 2 where ReLU s the element-wse rectfed lnear unt, 21.e., ReLUx = max0, x, W atom R d d s the weght matrx to
More informationLecture Notes on Linear Regression
Lecture Notes on Lnear Regresson Feng L fl@sdueducn Shandong Unversty, Chna Lnear Regresson Problem In regresson problem, we am at predct a contnuous target value gven an nput feature vector We assume
More informationHidden Markov Models
CM229S: Machne Learnng for Bonformatcs Lecture 12-05/05/2016 Hdden Markov Models Lecturer: Srram Sankararaman Scrbe: Akshay Dattatray Shnde Edted by: TBD 1 Introducton For a drected graph G we can wrte
More informationComputational Biology Lecture 8: Substitution matrices Saad Mneimneh
Computatonal Bology Lecture 8: Substtuton matrces Saad Mnemneh As we have ntroduced last tme, smple scorng schemes lke + or a match, - or a msmatch and -2 or a gap are not justable bologcally, especally
More informationProf. Dr. I. Nasser Phys 630, T Aug-15 One_dimensional_Ising_Model
EXACT OE-DIMESIOAL ISIG MODEL The one-dmensonal Isng model conssts of a chan of spns, each spn nteractng only wth ts two nearest neghbors. The smple Isng problem n one dmenson can be solved drectly n several
More informationInner Product. Euclidean Space. Orthonormal Basis. Orthogonal
Inner Product Defnton 1 () A Eucldean space s a fnte-dmensonal vector space over the reals R, wth an nner product,. Defnton 2 (Inner Product) An nner product, on a real vector space X s a symmetrc, blnear,
More informationMAE140 - Linear Circuits - Winter 16 Final, March 16, 2016
ME140 - Lnear rcuts - Wnter 16 Fnal, March 16, 2016 Instructons () The exam s open book. You may use your class notes and textbook. You may use a hand calculator wth no communcaton capabltes. () You have
More informationIntroduction to Algorithms
Introducton to Algorthms 6.046J/18.401J Lecture 7 Prof. Potr Indyk Data Structures Role of data structures: Encapsulate data Support certan operatons (e.g., INSERT, DELETE, SEARCH) What data structures
More informationEEE 241: Linear Systems
EEE : Lnear Systems Summary #: Backpropagaton BACKPROPAGATION The perceptron rule as well as the Wdrow Hoff learnng were desgned to tran sngle layer networks. They suffer from the same dsadvantage: they
More informationAn Experiment/Some Intuition (Fall 2006): Lecture 18 The EM Algorithm heads coin 1 tails coin 2 Overview Maximum Likelihood Estimation
An Experment/Some Intuton I have three cons n my pocket, 6.864 (Fall 2006): Lecture 18 The EM Algorthm Con 0 has probablty λ of heads; Con 1 has probablty p 1 of heads; Con 2 has probablty p 2 of heads
More informationHopfield networks and Boltzmann machines. Geoffrey Hinton et al. Presented by Tambet Matiisen
Hopfeld networks and Boltzmann machnes Geoffrey Hnton et al. Presented by Tambet Matsen 18.11.2014 Hopfeld network Bnary unts Symmetrcal connectons http://www.nnwj.de/hopfeld-net.html Energy functon The
More informationComparative Studies of Law of Conservation of Energy. and Law Clusters of Conservation of Generalized Energy
Comparatve Studes of Law of Conservaton of Energy and Law Clusters of Conservaton of Generalzed Energy No.3 of Comparatve Physcs Seres Papers Fu Yuhua (CNOOC Research Insttute, E-mal:fuyh1945@sna.com)
More informationCSci 6974 and ECSE 6966 Math. Tech. for Vision, Graphics and Robotics Lecture 21, April 17, 2006 Estimating A Plane Homography
CSc 6974 and ECSE 6966 Math. Tech. for Vson, Graphcs and Robotcs Lecture 21, Aprl 17, 2006 Estmatng A Plane Homography Overvew We contnue wth a dscusson of the major ssues, usng estmaton of plane projectve
More informationThe Order Relation and Trace Inequalities for. Hermitian Operators
Internatonal Mathematcal Forum, Vol 3, 08, no, 507-57 HIKARI Ltd, wwwm-hkarcom https://doorg/0988/mf088055 The Order Relaton and Trace Inequaltes for Hermtan Operators Y Huang School of Informaton Scence
More information1 The Mistake Bound Model
5-850: Advanced Algorthms CMU, Sprng 07 Lecture #: Onlne Learnng and Multplcatve Weghts February 7, 07 Lecturer: Anupam Gupta Scrbe: Bryan Lee,Albert Gu, Eugene Cho he Mstake Bound Model Suppose there
More informationCHALMERS, GÖTEBORGS UNIVERSITET. SOLUTIONS to RE-EXAM for ARTIFICIAL NEURAL NETWORKS. COURSE CODES: FFR 135, FIM 720 GU, PhD
CHALMERS, GÖTEBORGS UNIVERSITET SOLUTIONS to RE-EXAM for ARTIFICIAL NEURAL NETWORKS COURSE CODES: FFR 35, FIM 72 GU, PhD Tme: Place: Teachers: Allowed materal: Not allowed: January 2, 28, at 8 3 2 3 SB
More informationFoundations of Arithmetic
Foundatons of Arthmetc Notaton We shall denote the sum and product of numbers n the usual notaton as a 2 + a 2 + a 3 + + a = a, a 1 a 2 a 3 a = a The notaton a b means a dvdes b,.e. ac = b where c s an
More informationLecture Space-Bounded Derandomization
Notes on Complexty Theory Last updated: October, 2008 Jonathan Katz Lecture Space-Bounded Derandomzaton 1 Space-Bounded Derandomzaton We now dscuss derandomzaton of space-bounded algorthms. Here non-trval
More informationCourse organization. Part II: Algorithms for Network Biology (Week 12-16)
Course organzaton Introducton Week 1-2) Course ntroducton A bref ntroducton to molecular bology A bref ntroducton to sequence comparson Part I: Algorthms for Sequence Analyss Week 3-11) Chapter 1-3 Models
More informationNumerical Heat and Mass Transfer
Master degree n Mechancal Engneerng Numercal Heat and Mass Transfer 06-Fnte-Dfference Method (One-dmensonal, steady state heat conducton) Fausto Arpno f.arpno@uncas.t Introducton Why we use models and
More informationMarkov Chain Monte Carlo Lecture 6
where (x 1,..., x N ) X N, N s called the populaton sze, f(x) f (x) for at least one {1, 2,..., N}, and those dfferent from f(x) are called the tral dstrbutons n terms of mportance samplng. Dfferent ways
More informationCOMPARISON OF SOME RELIABILITY CHARACTERISTICS BETWEEN REDUNDANT SYSTEMS REQUIRING SUPPORTING UNITS FOR THEIR OPERATIONS
Avalable onlne at http://sck.org J. Math. Comput. Sc. 3 (3), No., 6-3 ISSN: 97-537 COMPARISON OF SOME RELIABILITY CHARACTERISTICS BETWEEN REDUNDANT SYSTEMS REQUIRING SUPPORTING UNITS FOR THEIR OPERATIONS
More informationA particle in a state of uniform motion remain in that state of motion unless acted upon by external force.
The fundamental prncples of classcal mechancs were lad down by Galleo and Newton n the 16th and 17th centures. In 1686, Newton wrote the Prncpa where he gave us three laws of moton, one law of gravty,
More informationLinear Feature Engineering 11
Lnear Feature Engneerng 11 2 Least-Squares 2.1 Smple least-squares Consder the followng dataset. We have a bunch of nputs x and correspondng outputs y. The partcular values n ths dataset are x y 0.23 0.19
More informationMessage modification, neutral bits and boomerangs
Message modfcaton, neutral bts and boomerangs From whch round should we start countng n SHA? Antone Joux DGA and Unversty of Versalles St-Quentn-en-Yvelnes France Jont work wth Thomas Peyrn 1 Dfferental
More information10-701/ Machine Learning, Fall 2005 Homework 3
10-701/15-781 Machne Learnng, Fall 2005 Homework 3 Out: 10/20/05 Due: begnnng of the class 11/01/05 Instructons Contact questons-10701@autonlaborg for queston Problem 1 Regresson and Cross-valdaton [40
More informationCS286r Assign One. Answer Key
CS286r Assgn One Answer Key 1 Game theory 1.1 1.1.1 Let off-equlbrum strateges also be that people contnue to play n Nash equlbrum. Devatng from any Nash equlbrum s a weakly domnated strategy. That s,
More informationChapter 5. Solution of System of Linear Equations. Module No. 6. Solution of Inconsistent and Ill Conditioned Systems
Numercal Analyss by Dr. Anta Pal Assstant Professor Department of Mathematcs Natonal Insttute of Technology Durgapur Durgapur-713209 emal: anta.bue@gmal.com 1 . Chapter 5 Soluton of System of Lnear Equatons
More informationErrors for Linear Systems
Errors for Lnear Systems When we solve a lnear system Ax b we often do not know A and b exactly, but have only approxmatons  and ˆb avalable. Then the best thng we can do s to solve ˆx ˆb exactly whch
More informationIntroduction to information theory and data compression
Introducton to nformaton theory and data compresson Adel Magra, Emma Gouné, Irène Woo March 8, 207 Ths s the augmented transcrpt of a lecture gven by Luc Devroye on March 9th 207 for a Data Structures
More informationLinear Approximation with Regularization and Moving Least Squares
Lnear Approxmaton wth Regularzaton and Movng Least Squares Igor Grešovn May 007 Revson 4.6 (Revson : March 004). 5 4 3 0.5 3 3.5 4 Contents: Lnear Fttng...4. Weghted Least Squares n Functon Approxmaton...
More informationGlobal Sensitivity. Tuesday 20 th February, 2018
Global Senstvty Tuesday 2 th February, 28 ) Local Senstvty Most senstvty analyses [] are based on local estmates of senstvty, typcally by expandng the response n a Taylor seres about some specfc values
More informationMore metrics on cartesian products
More metrcs on cartesan products If (X, d ) are metrc spaces for 1 n, then n Secton II4 of the lecture notes we defned three metrcs on X whose underlyng topologes are the product topology The purpose of
More informationSome Consequences. Example of Extended Euclidean Algorithm. The Fundamental Theorem of Arithmetic, II. Characterizing the GCD and LCM
Example of Extended Eucldean Algorthm Recall that gcd(84, 33) = gcd(33, 18) = gcd(18, 15) = gcd(15, 3) = gcd(3, 0) = 3 We work backwards to wrte 3 as a lnear combnaton of 84 and 33: 3 = 18 15 [Now 3 s
More informationVapnik-Chervonenkis theory
Vapnk-Chervonenks theory Rs Kondor June 13, 2008 For the purposes of ths lecture, we restrct ourselves to the bnary supervsed batch learnng settng. We assume that we have an nput space X, and an unknown
More informationPoisson brackets and canonical transformations
rof O B Wrght Mechancs Notes osson brackets and canoncal transformatons osson Brackets Consder an arbtrary functon f f ( qp t) df f f f q p q p t But q p p where ( qp ) pq q df f f f p q q p t In order
More informationIntroduction ( Week 1-2) Course introduction A brief introduction to molecular biology A brief introduction to sequence comparison Part I: Algorithms
Course organzaton 1 Introducton Week 1-2) Course ntroducton A bref ntroducton to molecular bology A bref ntroducton to sequence comparson Part I: Algorthms for Sequence Analyss Week 3-8) Chapter 1-3 Models
More informationChapter Newton s Method
Chapter 9. Newton s Method After readng ths chapter, you should be able to:. Understand how Newton s method s dfferent from the Golden Secton Search method. Understand how Newton s method works 3. Solve
More informationLecture 7: Boltzmann distribution & Thermodynamics of mixing
Prof. Tbbtt Lecture 7 etworks & Gels Lecture 7: Boltzmann dstrbuton & Thermodynamcs of mxng 1 Suggested readng Prof. Mark W. Tbbtt ETH Zürch 13 März 018 Molecular Drvng Forces Dll and Bromberg: Chapters
More informationMMA and GCMMA two methods for nonlinear optimization
MMA and GCMMA two methods for nonlnear optmzaton Krster Svanberg Optmzaton and Systems Theory, KTH, Stockholm, Sweden. krlle@math.kth.se Ths note descrbes the algorthms used n the author s 2007 mplementatons
More informationfind (x): given element x, return the canonical element of the set containing x;
COS 43 Sprng, 009 Dsjont Set Unon Problem: Mantan a collecton of dsjont sets. Two operatons: fnd the set contanng a gven element; unte two sets nto one (destructvely). Approach: Canoncal element method:
More informationCompilers. Spring term. Alfonso Ortega: Enrique Alfonseca: Chapter 4: Syntactic analysis
Complers Sprng term Alfonso Ortega: alfonso.ortega@uam.es nrque Alfonseca: enrque.alfonseca@uam.es Chapter : Syntactc analyss. Introducton. Bottom-up Analyss Syntax Analyser Concepts It analyses the context-ndependent
More informationWeek 5: Neural Networks
Week 5: Neural Networks Instructor: Sergey Levne Neural Networks Summary In the prevous lecture, we saw how we can construct neural networks by extendng logstc regresson. Neural networks consst of multple
More informationWeek3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity
Week3, Chapter 4 Moton n Two Dmensons Lecture Quz A partcle confned to moton along the x axs moves wth constant acceleraton from x =.0 m to x = 8.0 m durng a 1-s tme nterval. The velocty of the partcle
More informationEPR Paradox and the Physical Meaning of an Experiment in Quantum Mechanics. Vesselin C. Noninski
EPR Paradox and the Physcal Meanng of an Experment n Quantum Mechancs Vesseln C Nonnsk vesselnnonnsk@verzonnet Abstract It s shown that there s one purely determnstc outcome when measurement s made on
More informationLecture 4: November 17, Part 1 Single Buffer Management
Lecturer: Ad Rosén Algorthms for the anagement of Networs Fall 2003-2004 Lecture 4: November 7, 2003 Scrbe: Guy Grebla Part Sngle Buffer anagement In the prevous lecture we taled about the Combned Input
More informationn α j x j = 0 j=1 has a nontrivial solution. Here A is the n k matrix whose jth column is the vector for all t j=0
MODULE 2 Topcs: Lnear ndependence, bass and dmenson We have seen that f n a set of vectors one vector s a lnear combnaton of the remanng vectors n the set then the span of the set s unchanged f that vector
More informationPARTICIPATION FACTOR IN MODAL ANALYSIS OF POWER SYSTEMS STABILITY
POZNAN UNIVE RSITY OF TE CHNOLOGY ACADE MIC JOURNALS No 86 Electrcal Engneerng 6 Volodymyr KONOVAL* Roman PRYTULA** PARTICIPATION FACTOR IN MODAL ANALYSIS OF POWER SYSTEMS STABILITY Ths paper provdes a
More informationNodal analysis of finite square resistive grids and the teaching effectiveness of students projects
2 nd World Conference on Technology and Engneerng Educaton 2 WIETE Lublana Slovena 5-8 September 2 Nodal analyss of fnte square resstve grds and the teachng effectveness of students proects P. Zegarmstrz
More informationarxiv:quant-ph/ Jul 2002
Lnear optcs mplementaton of general two-photon proectve measurement Andrze Grudka* and Anton Wóck** Faculty of Physcs, Adam Mckewcz Unversty, arxv:quant-ph/ 9 Jul PXOWRZVNDR]QDRODQG Abstract We wll present
More informationCHAPTER-5 INFORMATION MEASURE OF FUZZY MATRIX AND FUZZY BINARY RELATION
CAPTER- INFORMATION MEASURE OF FUZZY MATRI AN FUZZY BINARY RELATION Introducton The basc concept of the fuzz matr theor s ver smple and can be appled to socal and natural stuatons A branch of fuzz matr
More informationThe optimal delay of the second test is therefore approximately 210 hours earlier than =2.
THE IEC 61508 FORMULAS 223 The optmal delay of the second test s therefore approxmately 210 hours earler than =2. 8.4 The IEC 61508 Formulas IEC 61508-6 provdes approxmaton formulas for the PF for smple
More informationISQS 6348 Final Open notes, no books. Points out of 100 in parentheses. Y 1 ε 2
ISQS 6348 Fnal Open notes, no books. Ponts out of 100 n parentheses. 1. The followng path dagram s gven: ε 1 Y 1 ε F Y 1.A. (10) Wrte down the usual model and assumptons that are mpled by ths dagram. Soluton:
More informationHMMT February 2016 February 20, 2016
HMMT February 016 February 0, 016 Combnatorcs 1. For postve ntegers n, let S n be the set of ntegers x such that n dstnct lnes, no three concurrent, can dvde a plane nto x regons (for example, S = {3,
More informationQuadratic speedup for unstructured search - Grover s Al-
Quadratc speedup for unstructured search - Grover s Al- CS 94- gorthm /8/07 Sprng 007 Lecture 11 001 Unstructured Search Here s the problem: You are gven a boolean functon f : {1,,} {0,1}, and are promsed
More informationLecture 10: May 6, 2013
TTIC/CMSC 31150 Mathematcal Toolkt Sprng 013 Madhur Tulsan Lecture 10: May 6, 013 Scrbe: Wenje Luo In today s lecture, we manly talked about random walk on graphs and ntroduce the concept of graph expander,
More informationE Tail Inequalities. E.1 Markov s Inequality. Non-Lecture E: Tail Inequalities
Algorthms Non-Lecture E: Tal Inequaltes If you hold a cat by the tal you learn thngs you cannot learn any other way. Mar Twan E Tal Inequaltes The smple recursve structure of sp lsts made t relatvely easy
More informationHidden Markov Model Cheat Sheet
Hdden Markov Model Cheat Sheet (GIT ID: dc2f391536d67ed5847290d5250d4baae103487e) Ths document s a cheat sheet on Hdden Markov Models (HMMs). It resembles lecture notes, excet that t cuts to the chase
More informationMath 261 Exercise sheet 2
Math 261 Exercse sheet 2 http://staff.aub.edu.lb/~nm116/teachng/2017/math261/ndex.html Verson: September 25, 2017 Answers are due for Monday 25 September, 11AM. The use of calculators s allowed. Exercse
More informationSearch sequence databases 2 10/25/2016
Search sequence databases 2 10/25/2016 The BLAST algorthms Ø BLAST fnds local matches between two sequences, called hgh scorng segment pars (HSPs). Step 1: Break down the query sequence and the database
More informationGeneral Tips on How to Do Well in Physics Exams. 1. Establish a good habit in keeping track of your steps. For example, when you use the equation
General Tps on How to Do Well n Physcs Exams 1. Establsh a good habt n keepng track o your steps. For example when you use the equaton 1 1 1 + = d d to solve or d o you should rst rewrte t as 1 1 1 = d
More informationFinding Primitive Roots Pseudo-Deterministically
Electronc Colloquum on Computatonal Complexty, Report No 207 (205) Fndng Prmtve Roots Pseudo-Determnstcally Ofer Grossman December 22, 205 Abstract Pseudo-determnstc algorthms are randomzed search algorthms
More informationIntroduction to Information Theory, Data Compression,
Introducton to Informaton Theory, Data Compresson, Codng Mehd Ibm Brahm, Laura Mnkova Aprl 5, 208 Ths s the augmented transcrpt of a lecture gven by Luc Devroye on the 3th of March 208 for a Data Structures
More information11 Tail Inequalities Markov s Inequality. Lecture 11: Tail Inequalities [Fa 13]
Algorthms Lecture 11: Tal Inequaltes [Fa 13] If you hold a cat by the tal you learn thngs you cannot learn any other way. Mark Twan 11 Tal Inequaltes The smple recursve structure of skp lsts made t relatvely
More informationELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM
ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM An elastc wave s a deformaton of the body that travels throughout the body n all drectons. We can examne the deformaton over a perod of tme by fxng our look
More informationNote 10. Modeling and Simulation of Dynamic Systems
Lecture Notes of ME 475: Introducton to Mechatroncs Note 0 Modelng and Smulaton of Dynamc Systems Department of Mechancal Engneerng, Unversty Of Saskatchewan, 57 Campus Drve, Saskatoon, SK S7N 5A9, Canada
More informationNOTES FOR QUANTUM GROUPS, CRYSTAL BASES AND REALIZATION OF ŝl(n)-modules
NOTES FOR QUANTUM GROUPS, CRYSTAL BASES AND REALIZATION OF ŝl(n)-modules EVAN WILSON Quantum groups Consder the Le algebra sl(n), whch s the Le algebra over C of n n trace matrces together wth the commutator
More informationGeneralized Linear Methods
Generalzed Lnear Methods 1 Introducton In the Ensemble Methods the general dea s that usng a combnaton of several weak learner one could make a better learner. More formally, assume that we have a set
More informationChapter 11: Simple Linear Regression and Correlation
Chapter 11: Smple Lnear Regresson and Correlaton 11-1 Emprcal Models 11-2 Smple Lnear Regresson 11-3 Propertes of the Least Squares Estmators 11-4 Hypothess Test n Smple Lnear Regresson 11-4.1 Use of t-tests
More informationbe the i th symbol in x and
2 Parwse Algnment We represent sequences b strngs of alphetc letters. If we recognze a sgnfcant smlart between a new sequence and a sequence out whch somethng s alread know, we can transfer nformaton out
More informationThis column is a continuation of our previous column
Comparson of Goodness of Ft Statstcs for Lnear Regresson, Part II The authors contnue ther dscusson of the correlaton coeffcent n developng a calbraton for quanttatve analyss. Jerome Workman Jr. and Howard
More informationLecture 12: Discrete Laplacian
Lecture 12: Dscrete Laplacan Scrbe: Tanye Lu Our goal s to come up wth a dscrete verson of Laplacan operator for trangulated surfaces, so that we can use t n practce to solve related problems We are mostly
More informationExpectation Maximization Mixture Models HMMs
-755 Machne Learnng for Sgnal Processng Mture Models HMMs Class 9. 2 Sep 200 Learnng Dstrbutons for Data Problem: Gven a collecton of eamples from some data, estmate ts dstrbuton Basc deas of Mamum Lelhood
More information3.1 Expectation of Functions of Several Random Variables. )' be a k-dimensional discrete or continuous random vector, with joint PMF p (, E X E X1 E X
Statstcs 1: Probablty Theory II 37 3 EPECTATION OF SEVERAL RANDOM VARIABLES As n Probablty Theory I, the nterest n most stuatons les not on the actual dstrbuton of a random vector, but rather on a number
More informationAssortment Optimization under MNL
Assortment Optmzaton under MNL Haotan Song Aprl 30, 2017 1 Introducton The assortment optmzaton problem ams to fnd the revenue-maxmzng assortment of products to offer when the prces of products are fxed.
More informationMultilayer Perceptron (MLP)
Multlayer Perceptron (MLP) Seungjn Cho Department of Computer Scence and Engneerng Pohang Unversty of Scence and Technology 77 Cheongam-ro, Nam-gu, Pohang 37673, Korea seungjn@postech.ac.kr 1 / 20 Outlne
More informationx = , so that calculated
Stat 4, secton Sngle Factor ANOVA notes by Tm Plachowsk n chapter 8 we conducted hypothess tests n whch we compared a sngle sample s mean or proporton to some hypotheszed value Chapter 9 expanded ths to
More informationLecture 3 January 31, 2017
CS 224: Advanced Algorthms Sprng 207 Prof. Jelan Nelson Lecture 3 January 3, 207 Scrbe: Saketh Rama Overvew In the last lecture we covered Y-fast tres and Fuson Trees. In ths lecture we start our dscusson
More informationDiscussion 11 Summary 11/20/2018
Dscusson 11 Summary 11/20/2018 1 Quz 8 1. Prove for any sets A, B that A = A B ff B A. Soluton: There are two drectons we need to prove: (a) A = A B B A, (b) B A A = A B. (a) Frst, we prove A = A B B A.
More information