Math 212-Lecture 24 13.10. Interior Critical Points of Functions of Two
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Math 327 Final Summary 20 February 2015 1. Manifold A
Math 327 Final Summary 20 February 2015 1. Manifold A subset M ⊂ Rn is Cr a manifold of dimension k if for any point p 2 M, there is an open set U ⊂ Rk and a Cr function φ : U ! Rn, such that (1) φ is injective and φ(U) ⊂ M is an open subset of M containing p; (2) φ−1 : φ(U) ! U is continuous; (3) D φ(x) has rank k for every x 2 U. Such a pair (U; φ) is called a chart of M. An atlas for M is a collection of charts f(Ui; φi)gi2I such that [ φi(Ui) = M i2I −1 (that is the images of φi cover M). (In some texts, like Spivak, the pair (φ(U); φ ) is called a chart or a coordinate system.) We shall mostly study C1 manifolds since they avoid any difficulty arising from the degree of differen- tiability. We shall also use the word smooth to mean C1. If we have an explicit atlas for a manifold then it becomes quite easy to deal with the manifold. Otherwise one can use the following theorem to find examples of manifolds. Theorem 1 (Regular value theorem). Let U ⊂ Rn be open and f : U ! Rk be a Cr function. Let a 2 Rk and −1 Ma = fx 2 U j f(x) = ag = f (a): The value a is called a regular value of f if f is a submersion on Ma; that is for any x 2 Ma, D f(x) has r rank k. -
Math 2374: Multivariable Calculus and Vector Analysis
Math 2374: Multivariable Calculus and Vector Analysis Part 25 Fall 2012 Extreme points Definition If f : U ⊂ Rn ! R is a scalar function, • a point x0 2 U is called a local minimum of f if there is a neighborhood V of x0 such that for all points x 2 V, f (x) ≥ f (x0), • a point x0 2 U is called a local maximum of f if there is a neighborhood V of x0 such that for all points x 2 V, f (x) ≤ f (x0), • a point x0 2 U is called a local, or relative, extremum of f if it is either a local minimum or a local maximum, • a point x0 2 U is called a critical point of f if either f is not differentiable at x0 or if rf (x0) = Df (x0) = 0, • a critical point that is not a local extremum is called a saddle point. First Derivative Test for Local Extremum Theorem If U ⊂ Rn is open, the function f : U ⊂ Rn ! R is differentiable, and x0 2 U is a local extremum, then Df (x0) = 0; that is, x0 is a critical point. Proof. Suppose that f achieves a local maximum at x0, then for all n h 2 R , the function g(t) = f (x0 + th) has a local maximum at t = 0. Thus from one-variable calculus g0(0) = 0. By chain rule 0 g (0) = [Df (x0)] h = 0 8h So Df (x0) = 0. Same proof for a local minimum. Examples Ex-1 Find the maxima and minima of the function f (x; y) = x2 + y 2. -
A Level-Set Method for Convex Optimization with a 2 Feasible Solution Path
1 A LEVEL-SET METHOD FOR CONVEX OPTIMIZATION WITH A 2 FEASIBLE SOLUTION PATH 3 QIHANG LIN∗, SELVAPRABU NADARAJAHy , AND NEGAR SOHEILIz 4 Abstract. Large-scale constrained convex optimization problems arise in several application 5 domains. First-order methods are good candidates to tackle such problems due to their low iteration 6 complexity and memory requirement. The level-set framework extends the applicability of first-order 7 methods to tackle problems with complicated convex objectives and constraint sets. Current methods 8 based on this framework either rely on the solution of challenging subproblems or do not guarantee a 9 feasible solution, especially if the procedure is terminated before convergence. We develop a level-set 10 method that finds an -relative optimal and feasible solution to a constrained convex optimization 11 problem with a fairly general objective function and set of constraints, maintains a feasible solution 12 at each iteration, and only relies on calls to first-order oracles. We establish the iteration complexity 13 of our approach, also accounting for the smoothness and strong convexity of the objective function 14 and constraints when these properties hold. The dependence of our complexity on is similar to 15 the analogous dependence in the unconstrained setting, which is not known to be true for level-set 16 methods in the literature. Nevertheless, ensuring feasibility is not free. The iteration complexity of 17 our method depends on a condition number, while existing level-set methods that do not guarantee 18 feasibility can avoid such dependence. We numerically validate the usefulness of ensuring a feasible 19 solution path by comparing our approach with an existing level set method on a Neyman-Pearson classification problem.20 21 Key words. -
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[version: January 7, 2014] Ann. Sc. Norm. Super. Pisa Cl. Sci. (5) vol. 12 (2013), no. 4, 863{902 DOI 10.2422/2036-2145.201107 006 Structure of level sets and Sard-type properties of Lipschitz maps Giovanni Alberti, Stefano Bianchini, Gianluca Crippa 2 d d−1 Abstract. We consider certain properties of maps of class C from R to R that are strictly related to Sard's theorem, and show that some of them can be extended to Lipschitz maps, while others still require some additional regularity. We also give examples showing that, in term of regularity, our results are optimal. Keywords: Lipschitz maps, level sets, critical set, Sard's theorem, weak Sard property, distri- butional divergence. MSC (2010): 26B35, 26B10, 26B05, 49Q15, 58C25. 1. Introduction In this paper we study three problems which are strictly interconnected and ultimately related to Sard's theorem: structure of the level sets of maps from d d−1 2 R to R , weak Sard property of functions from R to R, and locality of the divergence operator. Some of the questions we consider originated from a PDE problem studied in the companion paper [1]; they are however interesting in their own right, and this paper is in fact largely independent of [1]. d d−1 2 Structure of level sets. In case of maps f : R ! R of class C , Sard's theorem (see [17], [12, Chapter 3, Theorem 1.3])1 states that the set of critical values of f, namely the image according to f of the critical set S := x : rank(rf(x)) < d − 1 ; (1.1) has (Lebesgue) measure zero. -
A Stability Boundary Based Method for Finding Saddle Points on Potential Energy Surfaces
JOURNAL OF COMPUTATIONAL BIOLOGY Volume 13, Number 3, 2006 © Mary Ann Liebert, Inc. Pp. 745–766 A Stability Boundary Based Method for Finding Saddle Points on Potential Energy Surfaces CHANDAN K. REDDY and HSIAO-DONG CHIANG ABSTRACT The task of finding saddle points on potential energy surfaces plays a crucial role in under- standing the dynamics of a micromolecule as well as in studying the folding pathways of macromolecules like proteins. The problem of finding the saddle points on a high dimen- sional potential energy surface is transformed into the problem of finding decomposition points of its corresponding nonlinear dynamical system. This paper introduces a new method based on TRUST-TECH (TRansformation Under STability reTained Equilibria CHaracter- ization) to compute saddle points on potential energy surfaces using stability boundaries. Our method explores the dynamic and geometric characteristics of stability boundaries of a nonlinear dynamical system. A novel trajectory adjustment procedure is used to trace the stability boundary. Our method was successful in finding the saddle points on different potential energy surfaces of various dimensions. A simplified version of the algorithm has also been used to find the saddle points of symmetric systems with the help of some analyt- ical knowledge. The main advantages and effectiveness of the method are clearly illustrated with some examples. Promising results of our method are shown on various problems with varied degrees of freedom. Key words: potential energy surfaces, saddle points, stability boundary, minimum gradient point, computational chemistry. I. INTRODUCTION ecently, there has been a lot of interest across various disciplines to understand a wide Rvariety of problems related to bioinformatics. -
3.2 Sources, Sinks, Saddles, and Spirals
3.2. Sources, Sinks, Saddles, and Spirals 161 3.2 Sources, Sinks, Saddles, and Spirals The pictures in this section show solutions to Ay00 By0 Cy 0. These are linear equations with constant coefficients A; B; and C .C The graphsC showD solutions y on the horizontal axis and their slopes y0 dy=dt on the vertical axis. These pairs .y.t/;y0.t// depend on time, but time is not inD the pictures. The paths show where the solution goes, but they don’t show when. Each specific solution starts at a particular point .y.0/;y0.0// given by the initial conditions. The point moves along its path as the time t moves forward from t 0. D We know that the solutions to Ay00 By0 Cy 0 depend on the two solutions to 2 C C D As Bs C 0 (an ordinary quadratic equation for s). When we find the roots s1 and C C D s2, we have found all possible solutions : s1t s2t s1t s2t y c1e c2e y c1s1e c2s2e (1) D C 0 D C The numbers s1 and s2 tell us which picture we are in. Then the numbers c1 and c2 tell us which path we are on. Since s1 and s2 determine the picture for each equation, it is essential to see the six possibilities. We write all six here in one place, to compare them. Later they will appear in six different places, one with each figure. The first three have real solutions s1 and s2. The last three have complex pairs s a i!. -
Lecture 8: Maxima and Minima
Maxima and minima Lecture 8: Maxima and Minima Rafikul Alam Department of Mathematics IIT Guwahati Rafikul Alam IITG: MA-102 (2013) Maxima and minima Local extremum of f : Rn ! R Let f : U ⊂ Rn ! R be continuous, where U is open. Then • f has a local maximum at p if there exists r > 0 such that f (x) ≤ f (p) for x 2 B(p; r): • f has a local minimum at a if there exists > 0 such that f (x) ≥ f (p) for x 2 B(p; ): A local maximum or a local minimum is called a local extremum. Rafikul Alam IITG: MA-102 (2013) Maxima and minima Figure: Local extremum of z = f (x; y) Rafikul Alam IITG: MA-102 (2013) Maxima and minima Necessary condition for extremum of Rn ! R Critical point: A point p 2 U is a critical point of f if rf (p) = 0: Thus, when f is differentiable, the tangent plane to z = f (x) at (p; f (p)) is horizontal. Theorem: Suppose that f has a local extremum at p and that rf (p) exists. Then p is a critical point of f , i.e, rf (p) = 0: 2 2 Example: Consider f (x; y) = x − y : Then fx = 2x = 0 and fy = −2y = 0 show that (0; 0) is the only critical point of f : But (0; 0) is not a local extremum of f : Rafikul Alam IITG: MA-102 (2013) Maxima and minima Saddle point Saddle point: A critical point of f that is not a local extremum is called a saddle point of f : Examples: 2 2 • The point (0; 0) is a saddle point of f (x; y) = x − y : 2 2 2 • Consider f (x; y) = x y + y x: Then fx = 2xy + y = 0 2 and fy = 2xy + x = 0 show that (0; 0) is the only critical point of f : But (0; 0) is a saddle point. -
An Improved Level Set Algorithm Based on Prior Information for Left Ventricular MRI Segmentation
electronics Article An Improved Level Set Algorithm Based on Prior Information for Left Ventricular MRI Segmentation Lei Xu * , Yuhao Zhang , Haima Yang and Xuedian Zhang School of Optical-Electrical and Computer Engineering, University of Shanghai for Science and Technology, Shanghai 200093, China; [email protected] (Y.Z.); [email protected] (H.Y.); [email protected] (X.Z.) * Correspondence: [email protected] Abstract: This paper proposes a new level set algorithm for left ventricular segmentation based on prior information. First, the improved U-Net network is used for coarse segmentation to obtain pixel-level prior position information. Then, the segmentation result is used as the initial contour of level set for fine segmentation. In the process of curve evolution, based on the shape of the left ventricle, we improve the energy function of the level set and add shape constraints to solve the “burr” and “sag” problems during curve evolution. The proposed algorithm was successfully evaluated on the MICCAI 2009: the mean dice score of the epicardium and endocardium are 92.95% and 94.43%. It is proved that the improved level set algorithm obtains better segmentation results than the original algorithm. Keywords: left ventricular segmentation; prior information; level set algorithm; shape constraints Citation: Xu, L.; Zhang, Y.; Yang, H.; Zhang, X. An Improved Level Set Algorithm Based on Prior 1. Introduction Information for Left Ventricular MRI Uremic cardiomyopathy is the most common complication also the cause of death with Segmentation. Electronics 2021, 10, chronic kidney disease and left ventricular hypertrophy is the most significant pathological 707. -
Calculus and Differential Equations II
Calculus and Differential Equations II MATH 250 B Linear systems of differential equations Linear systems of differential equations Calculus and Differential Equations II Second order autonomous linear systems We are mostly interested with2 × 2 first order autonomous systems of the form x0 = a x + b y y 0 = c x + d y where x and y are functions of t and a, b, c, and d are real constants. Such a system may be re-written in matrix form as d x x a b = M ; M = : dt y y c d The purpose of this section is to classify the dynamics of the solutions of the above system, in terms of the properties of the matrix M. Linear systems of differential equations Calculus and Differential Equations II Existence and uniqueness (general statement) Consider a linear system of the form dY = M(t)Y + F (t); dt where Y and F (t) are n × 1 column vectors, and M(t) is an n × n matrix whose entries may depend on t. Existence and uniqueness theorem: If the entries of the matrix M(t) and of the vector F (t) are continuous on some open interval I containing t0, then the initial value problem dY = M(t)Y + F (t); Y (t ) = Y dt 0 0 has a unique solution on I . In particular, this means that trajectories in the phase space do not cross. Linear systems of differential equations Calculus and Differential Equations II General solution The general solution to Y 0 = M(t)Y + F (t) reads Y (t) = C1 Y1(t) + C2 Y2(t) + ··· + Cn Yn(t) + Yp(t); = U(t) C + Yp(t); where 0 Yp(t) is a particular solution to Y = M(t)Y + F (t). -
Maxima, Minima, and Saddle Points
Real Analysis III (MAT312β) Department of Mathematics University of Ruhuna A.W.L. Pubudu Thilan Department of Mathematics University of Ruhuna | Real Analysis III(MAT312β) 1/80 Chapter 12 Maxima, Minima, and Saddle Points Department of Mathematics University of Ruhuna | Real Analysis III(MAT312β) 2/80 Introduction A scientist or engineer will be interested in the ups and downs of a function, its maximum and minimum values, its turning points. For instance, locating extreme values is the basic objective of optimization. In the simplest case, an optimization problem consists of maximizing or minimizing a real function by systematically choosing input values from within an allowed set and computing the value of the function. Department of Mathematics University of Ruhuna | Real Analysis III(MAT312β) 3/80 Introduction Cont... Drawing a graph of a function using a computer graph plotting package will reveal behavior of the function. But if we want to know the precise location of maximum and minimum points, we need to turn to algebra and differential calculus. In this Chapter we look at how we can find maximum and minimum points in this way. Department of Mathematics University of Ruhuna | Real Analysis III(MAT312β) 4/80 Chapter 12 Section 12.1 Single Variable Functions Department of Mathematics University of Ruhuna | Real Analysis III(MAT312β) 5/80 Local maximum and local minimum The local maximum and local minimum (plural: maxima and minima) of a function, are the largest and smallest value that the function takes at a point within a given interval. It may not be the minimum or maximum for the whole function, but locally it is. -
Analysis of Asymptotic Escape of Strict Saddle Sets in Manifold Optimization
Analysis of Asymptotic Escape of Strict Saddle Sets in Manifold Optimization Thomas Y. Hou∗ , Zhenzhen Li y , and Ziyun Zhang z Abstract. In this paper, we provide some analysis on the asymptotic escape of strict saddles in manifold optimization using the projected gradient descent (PGD) algorithm. One of our main contributions is that we extend the current analysis to include non-isolated and possibly continuous saddle sets with complicated geometry. We prove that the PGD is able to escape strict critical submanifolds under certain conditions on the geometry and the distribution of the saddle point sets. We also show that the PGD may fail to escape strict saddles under weaker assumptions even if the saddle point set has zero measure and there is a uniform escape direction. We provide a counterexample to illustrate this important point. We apply this saddle analysis to the phase retrieval problem on the low-rank matrix manifold, prove that there are only a finite number of saddles, and they are strict saddles with high probability. We also show the potential application of our analysis for a broader range of manifold optimization problems. Key words. Manifold optimization, projected gradient descent, strict saddles, stable manifold theorem, phase retrieval AMS subject classifications. 58D17, 37D10, 65F10, 90C26 1. Introduction. Manifold optimization has long been studied in mathematics. From signal and imaging science [38][7][36], to computer vision [47][48] and quantum informa- tion [40][16][29], it finds applications in various disciplines. -
Instability Analysis of Saddle Points by a Local Minimax Method
INSTABILITY ANALYSIS OF SADDLE POINTS BY A LOCAL MINIMAX METHOD JIANXIN ZHOU Abstract. The objective of this work is to develop some tools for local insta- bility analysis of multiple critical points, which can be computationally carried out. The Morse index can be used to measure local instability of a nondegen- erate saddle point. However, it is very expensive to compute numerically and is ineffective for degenerate critical points. A local (weak) linking index can also be defined to measure local instability of a (degenerate) saddle point. But it is still too difficult to compute. In this paper, a local instability index, called a local minimax index, is defined by using a local minimax method. This new instability index is known beforehand and can help in finding a saddle point numerically. Relations between the local minimax index and other local insta- bility indices are established. Those relations also provide ways to numerically compute the Morse, local linking indices. In particular, the local minimax index can be used to define a local instability index of a saddle point relative to a reference (trivial) critical point even in a Banach space while others failed to do so. 1. Introduction Multiple solutions with different performance, maneuverability and instability in- dices exist in many nonlinear problems in natural or social sciences [1,7, 9,24,29,31, 33,35]. When cases are variational, the problems reduce to solving the Euler- Lagrange equation (1.1) J 0(u) = 0; where J is a C1 generic energy functional on a Banach space H and J 0 its Frechet derivative.