ON THE MAXIMUM OF A NORMAL STATIONARY STOCHASTIC PROCESS 1 BY HARALD CRAMER. Communicated by W. Feller, May 1, 1962

Similar documents
ON CONVERGENCE OF STOCHASTIC PROCESSES

ASYMPTOTIC DISTRIBUTION OF THE MAXIMUM CUMULATIVE SUM OF INDEPENDENT RANDOM VARIABLES

EXISTENCE OF NEUTRAL STOCHASTIC FUNCTIONAL DIFFERENTIAL EQUATIONS WITH ABSTRACT VOLTERRA OPERATORS

ON THE AVERAGE NUMBER OF REAL ROOTS OF A RANDOM ALGEBRAIC EQUATION

PRODUCTS OF INDECOMPOSABLE, APERIODIC, STOCHASTIC MATRICES1 J. WOLFOWITZ

DISTRIBUTION OF THE FIBONACCI NUMBERS MOD 2. Eliot T. Jacobson Ohio University, Athens, OH (Submitted September 1990)

J2 e-*= (27T)- 1 / 2 f V* 1 '»' 1 *»

SRI VIDYA COLLEGE OF ENGINEERING AND TECHNOLOGY UNIT 3 RANDOM PROCESS TWO MARK QUESTIONS

Krzysztof Burdzy University of Washington. = X(Y (t)), t 0}

The Equivalence of Ergodicity and Weak Mixing for Infinitely Divisible Processes1

GRONWALL'S INEQUALITY FOR SYSTEMS OF PARTIAL DIFFERENTIAL EQUATIONS IN TWO INDEPENDENT VARIABLES

GENERALIZED L2-LAPLACIANS

Characterization of Wiener Process by Symmetry and Constant Regression

ON ADDITIVE TIME-CHANGES OF FELLER PROCESSES. 1. Introduction

IEOR 6711: Stochastic Models I Fall 2013, Professor Whitt Lecture Notes, Thursday, September 5 Modes of Convergence

460 HOLGER DETTE AND WILLIAM J STUDDEN order to examine how a given design behaves in the model g` with respect to the D-optimality criterion one uses

Maxima and Minima. (a, b) of R if

ON THE REPRESENTATION OF A FUNCTION BY CERTAIN FOURIER INTEGRALS*

National Sun Yat-Sen University CSE Course: Information Theory. Maximum Entropy and Spectral Estimation

New Identities for Weak KAM Theory

A NOTE ON VOLTERRA INTEGRAL EQUATIONS AND TOPOLOGICAL DYNAMICS 1

The Hilbert Transform and Fine Continuity

THE MAXIMUM OF SUMS OF STABLE RANDOM VARIABLES

A Note on the Strong Law of Large Numbers

GAUSSIAN PROCESSES GROWTH RATE OF CERTAIN. successfully employed in dealing with certain Gaussian processes not possessing

A Connection between Controlled Markov Chains and Martingales

Arithmetic progressions in sumsets

Citation Osaka Journal of Mathematics. 41(4)

Application of Measure of Noncompactness for the System of Functional Integral Equations

ELEG 3143 Probability & Stochastic Process Ch. 6 Stochastic Process

A Criterion for the Compound Poisson Distribution to be Maximum Entropy

A New Wavelet-based Expansion of a Random Process

APPROXIMATE ISOMETRIES ON FINITE-DIMENSIONAL NORMED SPACES

E[X n ]= dn dt n M X(t). ). What is the mgf? Solution. Found this the other day in the Kernel matching exercise: 1 M X (t) =

ELEMENTS OF PROBABILITY THEORY

ASYMPTOTIC PROPERTIES OF THE MAXIMUM IN A STATIONARY GAUSSIAN PROCESS

Fundamentals of Noise

A COUNTEREXAMPLE TO AN ENDPOINT BILINEAR STRICHARTZ INEQUALITY TERENCE TAO. t L x (R R2 ) f L 2 x (R2 )

Lesson 4: Stationary stochastic processes

ASYMPTOTICALLY NONEXPANSIVE MAPPINGS IN MODULAR FUNCTION SPACES ABSTRACT

Math 328 Course Notes

SMOOTHNESS OF FUNCTIONS GENERATED BY RIESZ PRODUCTS

1 Functions of Several Variables 2019 v2

NONTRIVIAL SOLUTIONS FOR SUPERQUADRATIC NONAUTONOMOUS PERIODIC SYSTEMS. Shouchuan Hu Nikolas S. Papageorgiou. 1. Introduction

LqJ M: APR VISO. Western Management Science Institute University of California 0. Los Angeles

Spatial Ergodicity of the Harris Flows

Mi-Hwa Ko. t=1 Z t is true. j=0

(1.2) Jjexp/(z) 2 \dz\ < expj i \f'(z)\2 do(z) J (q = 1).

Mi Ryeong Lee and Hye Yeong Yun

Yunhi Cho and Young-One Kim

Diagonal matrix solutions of a discrete-time Lyapunov inequality

Fourier Series. 1. Review of Linear Algebra

SOLUTIONS OF SEMILINEAR WAVE EQUATION VIA STOCHASTIC CASCADES

EXISTENCE AND UNIQUENESS OF SOLUTIONS FOR A SECOND-ORDER NONLINEAR HYPERBOLIC SYSTEM

ON THE HÖLDER CONTINUITY OF MATRIX FUNCTIONS FOR NORMAL MATRICES

ON THE "BANG-BANG" CONTROL PROBLEM*

CONTINUOUS STATE BRANCHING PROCESSES

1.4 Complex random variables and processes

Complete q-moment Convergence of Moving Average Processes under ϕ-mixing Assumption

Angular Spectrum Representation for Propagation of Random Electromagnetic Beams in a Turbulent Atmosphere

A CLT FOR MULTI-DIMENSIONAL MARTINGALE DIFFERENCES IN A LEXICOGRAPHIC ORDER GUY COHEN. Dedicated to the memory of Mikhail Gordin

1.1 Limits and Continuity. Precise definition of a limit and limit laws. Squeeze Theorem. Intermediate Value Theorem. Extreme Value Theorem.

for all subintervals I J. If the same is true for the dyadic subintervals I D J only, we will write ϕ BMO d (J). In fact, the following is true

On the second smallest prime non-residue

ON THE AVERAGE NUMBER OF REAL ZEROS OF A CLASS OF RANDOM ALGEBRAIC CURVES

Sample path large deviations of a Gaussian process with stationary increments and regularily varying variance

Combinatorial Dimension in Fractional Cartesian Products

THE GAME QUANTIFIER1

International Journal of Pure and Applied Mathematics Volume 5 No ,

Jae Gil Choi and Young Seo Park

Harnack Inequalities and Applications for Stochastic Equations

THE POISSON TRANSFORM^)

P (A G) dp G P (A G)

ANOTHER CLASS OF INVERTIBLE OPERATORS WITHOUT SQUARE ROOTS

Convergence at first and second order of some approximations of stochastic integrals

Chapter 6. Random Processes

tidissomsi D DC if: RELATIVE INVARIANTS AND CLOSURE HARD COPY MICROFICHE MEMORANDUM Q*^M-4209-ARPA ßmf&t&tfa«. Richard Eeliman and John M.

Pointwise convergence rates and central limit theorems for kernel density estimators in linear processes

The Mean Value Inequality (without the Mean Value Theorem)

RESEARCH ANNOUNCEMENTS

(4) cn = f f(x)ux)dx (n = 0, 1, 2, ).

Nonparametric regression with martingale increment errors

CLASSIFICATION OF OPERATORS BY MEANS OF THE OPERATIONAL CALCULUS 1

Reliability Theory of Dynamic Loaded Structures (cont.) Calculation of Out-Crossing Frequencies Approximations to the Failure Probability.

Lecture 9. d N(0, 1). Now we fix n and think of a SRW on [0,1]. We take the k th step at time k n. and our increments are ± 1

On the intersections between the trajectories of a normal stationary stochastic process and a high level. By HARALD CRkMER

Chapter 2 Event-Triggered Sampling

DIFFERENTIAL CRITERIA FOR POSITIVE DEFINITENESS

Computability of Koch Curve and Koch Island

FUNCTIONALS OF FINITE DEGREE AND THE CONVERGENCE OF THEIR FOURIER-HERMITE DEVELOPMENTS

UNIFORM INTEGRABILITY AND THE POINTWTSE ERGODIC THEOREM

x i y i f(y) dy, x y m+1

Duality and dynamics in Hamilton-Jacobi theory for fully convex problems of control

Probability and Statistics for Final Year Engineering Students

Asymptotic results for empirical measures of weighted sums of independent random variables

Large Sample Properties of Estimators in the Classical Linear Regression Model

ON DIVISION ALGEBRAS*

On the Regularized Trace of a Fourth Order. Regular Differential Equation

On the N-tuple Wave Solutions of the Korteweg-de Vnes Equation

Gaussian Processes. 1. Basic Notions

Transcription:

ON THE MAXIMUM OF A NORMAL STATIONARY STOCHASTIC PROCESS 1 BY HARALD CRAMER Communicated by W. Feller, May 1, 1962 1. Let x(t) with oo </ < + be the variables of a real, separable, normal and stationary stochastic process, such that [#($)] = () and E[x 2 (f)] = 1. Let the covariance function of the process be I cos \tf(\)d\, 0 and assume that the spectral density (X) is of bounded variation in ( oo, oo ) and satisfies the condition i 0 X 2 (log(l + \)) f(\)d\ < oo for some a>l. Then it is known (Hunt [5], Belayev [l]) that the sample functions x(t) will almost certainly be everywhere continuous and have continuous first derivatives x'(t). Consequently for every fixed t>0 the maximum max %(u) will be a random variable defined but for equivalence. For the sake of typographical convenience, we write in the sequel simply maxx(w), omitting the subscript 0Su^*t, and similarly in respect of min x(u). The object of this note is to prove the relation (1) lim P \ I max x(u) - (2 log 0 1/2 1 < g g 1 = 1. r-oo L' ' (log/) 1/2 J The notation P[ ] denotes here, as throughout the sequel, the probability of the relation between the brackets. A similar relation was recently given for the case of a normal stationary sequence x n with» = 0, ±1, by Berman [2]. 2. We shall first prove that 1 Research work done (Tech. Report No. 1) partially under Contract NASw-334, National Aeronautics and Space Administration. 512

A NORMAL STATIONARY STOCHASTIC PROCESS 513 (2) P [max x(u) g (2 log /) 1/2 - g g H -> 0 L * (log/) 1 ' 2 J as * oo. Let c>0 be given, and define a random variable y(u) by writing for any real u (1 if x(u) > c, \0 if *(») ^ c. Then y(w) will define a stationary process such that 4>(x)dx, where E[y(u)y(v)] = P[x(u) > c y x(v) > c] /» J *(*, y; r)dxdy, 1 / x 2 \ 1 / x 2 2rxy + y 2 \ < (#, y;r) = expl ), " 2TT(1 - r 2 ) 1 ' 2 F \ 2(1 - r 2 ) / r = r(w v). It follows (cf. e.g. Loève [6, pp. 472, 520]) that the integral z(l) = y{% / I y(u)du J o is defined both in quadratic mean and as a sample function integral, and that the two integrals coincide, but for equivalence. Then z(t) will, with probability 1, be equal to the Lebesgue measure of the set of points u in [0, t] such that x(u) >c. Thus z(t) èo with probability 1, and (3) P[z(t) = 0] = P[m2ixx(u) ^ c]. For all sufficiently large c we have (Loève, I.e.) and further J t / c 2 \ 4>(x)dx> expf-yj,

514 HARALD CRAMÉR [September» t / t /» /» I dudv I I 4>(x, y; r)dxdy 0 J O J c J o with r = r(w v). For any fixed r in ( 1, 1) we have the identity /» I < (#, ;y; r)dxdy c * W *y + 2W 0 exp \ l + w/(l - w*)w ' (For r = 0 the identity is obvious, and some calculation will show that the derivatives of both sides with respect to r are equal.) It then follows that the variance of 0(0 is Var[z(0] I f f ' fr(u-v) / c2 v OW - s Jo Jo dudv Jo exp v~ r^jö^^ï (5) < I I I r(u - v) expf - * -j)dudv. From our assumptions concerning the spectral density (X), it follows that there exist positive constants k and m such that I r (0 I < TT for a11 *' KO â 1 -m 2 / 2 for t â 2*. (The latter inequality is easily proved by means of Cramer [4, Lemma l].) Dividing the domain of integration in (5) into two parts, defined respectively by \u v\ >2k and w 1; ^2fe, and using in each part the appropriate inequality for r(u v), we obtain from (5) by some straightforward estimation r. / 2C 2 \ 27T 1 ' 2 t / C 2 \ (6) Va.r[z(i)\ < 2kt log t expi ) - exp( ). \ 3/ m c \ 2 / Now the Tchebychev inequality gives Taking.Var [z{t)\ P[z(t) = 0] ^ ±-^+

1962] A NORMAL STATIONARY STOCHASTIC PROCESS 515 log log t c= (21og0 1/2 - > (log0 1/2 we then obtain from (3), (4) and (6) P[max*(i0 S c] < A((logt)H- 1 '*+ (log t) 1^2' 12 ) where A is independent of t. Since the second member obviously tends to zero as t > <*>, (2) is proved. 3. It now remains to prove that (7) P ["max x(u) ^ (2 log t) 1 ' 2 + g g H -> 0 L * (log0 1/2 J as / > oo. For any c>0 we evidently have P[max x(u) ^c] = P[min x(u) ^ c ^ max #(w)] + P[min x(u) > c] = Pi + P 2. Pi is, for any continuous sample function x(u), the probability of at least one "crossing" with the level c within [0, /], i.e., the probability that there is at least one point u in [0, /] such that x(u) =c. Let N denote the total number of such points, and write p n = P[N=n\ for w = 0, 1,. Then (8) Pi = p x + p 2 + S Pi + 2p 2 + = E[N]. However, it is known (Bulinskaya [3]) that under the present conditions r i M 172 / C 2 \ (9) E[N] = where X2 denotes the second moment of/(x). Further P 2 = P[min x(u) > c] ^ P[x(0) > c] K -^ texp{-jy Taking now log log t <- (21 s,), " + 5 ^ ' it follows from (8), (9) and (10) that Pi and P 2 both tend to zero as / >, so that (7) is proved. Finally, the result (1) follows from (2) and (7).

516 RICHARD BELLMAN AND WILLIAM KARUSH [September REFERENCES 1. Yu. K. Belayev, Continuity and Holder's conditions for sample functions of stationary Gaussian processes, Proc. Fourth Berkeley Symp., Vol. 2, pp. 23-33, 1961. 2. S. M. Berman, A law of large numbers for the maximum in a stationary Gaussian sequence, Ann. Math. Statist. 33 (1962), 93-97. 3. E. V. Bulinskaya, On the mean number of crossings of a level by a stationary Gaussian process, Teor. Verojatnost. i Primenen. 6 (1961), 474-477. 4. H. Cramer, Random variables and probability distributions, Cambridge Tracts in Mathematics, Vol. 36, Cambridge University Press, Cambridge, 1937. 2nd ed. to appear in 1962. 5. G. A. Hunt, Random Fourier transforms, Trans. Amer. Math. Soc. 71 (1951), 38-69. 6. M. Loève, Probability theory, 2nd éd., Van Nostrand, Princeton, N. J., I960. RESEARCH TRIANGLE INSTITUTE ON THE MAXIMUM TRANSFORM AND SEMIGROUPS OF TRANSFORMATIONS BY RICHARD BELLMAN AND WILLIAM KARUSH Communicated by Peter D. Lax, April 27, 1962 1. Introduction. The problem of determining the maximum of the function (1.1) F(x h x 2y, x N ) = X &(*<) over the domain DN denned by / ^ x 0, is one with various ramifications and applications. Analytic solutions and computational algorithms have been obtained in a number of ways; see Karush [7], Bellman [2], Bellman and Karush [3], Let us now discuss a new way of generating solutions of (1.1). Let g(x, a) be a scalar function of the scalar variable x and the M-dimensional vector a with the group property that (1.2) max [g(x h a) + g(x 2, b)] = g(x, h(a, b)) (x h x 2 à 0), where h(a, b) is a known function of a and b. It follows inductively that (1.3) maxt J2 «(**, a^)! = g(*> K* {1 \ <* (2),, *<*>)), DN L fc-i J where DN is as above, and A(a (1), a (2 \, a m ) is obtained from