• 検索結果がありません。

THE EXPECTED VARIATION OF RANDOM BOUNDED INTEGER SEQUENCES OF FINITE LENGTH

N/A
N/A
Protected

Academic year: 2022

シェア "THE EXPECTED VARIATION OF RANDOM BOUNDED INTEGER SEQUENCES OF FINITE LENGTH"

Copied!
10
0
0

読み込み中.... (全文を見る)

全文

(1)

THE EXPECTED VARIATION OF RANDOM BOUNDED INTEGER SEQUENCES OF FINITE LENGTH

RUDOLFO ANGELES, DON RAWLINGS, LAWRENCE SZE, AND MARK TIEFENBRUCK

Received 24 November 2004 and in revised form 15 June 2005

From the enumerative generating function of an abstract adjacency statistic, we deduce the mean and variance of the variation on random permutations, rearrangements, com- positions, and bounded integer sequences of finite length.

1. Introduction

When the finite sequence of integersw=1, 3, 2, 2, 4, 3 is sketched as below,

w=

4

3 3

2 2

1

(1.1)

its most compelling aspect is its verticalvariation, that is, the sum of the vertical distances between its adjacent terms. Denoted by varw, the vertical variation of the sequence in (1.1) is varw=2 + 1 + 0 + 2 + 1=6. Our purpose here is to compute the mean and vari- ance of var on four classical sets of combinatorial sequences.

To formalize matters and place our problem in the context of other work, let [m]n denote the set of sequencesw=x1x2···xnof lengthnwith eachxi∈ {1, 2,...,m}. For a real-valued function f on [m]2, the f-adjacency numberofw=x1x2···xn[m]n is defined to be

adfw=

n1 k=1

fxkxk+1

. (1.2)

Copyright©2005 Hindawi Publishing Corporation

International Journal of Mathematics and Mathematical Sciences 2005:14 (2005) 2277–2285 DOI:10.1155/IJMMS.2005.2277

(2)

Table 1.1

Sequences Expected value of var Variance of var

Sn n21

3

(n2)(n+ 1)(4n7) 90

[m]n (n1)(m21)

3m

(m21)(6m2n+ 6n7m22) 90m2

Rn(i) 2

n

1≤x<y≤m

(yx)ixiy See (3.10)

Cn(m) 2(n1) (m1)n−1

m/2

x=1

(m2x)n−1 See (3.18)

Some specializations of thef-adjacency number have been considered elsewhere. For in- stance, iff(xy) is 1 whenx < yand 0 otherwise, then adfwis known as therise numberof w[1,3,4]. For the selection f(xy)= |yx|, adfw=varw. In a sorting problem of com- puter science, Levcopoulos and Petersson [5] introduced the related notion of oscillation (varwn+ 1) as a measure of the presortedness of a sequence ofndistinct numbers.

In [6], compositions were enumerated by theirascent variation, the f-adjacency statis- tic induced by f(xy)=yx ifx < yand 0 otherwise. For the case f(xy)=h(|yx|) wherehis a linear, convex, or concave increasing real-valued function, Chao and Liang [2] described the arrangements ofndistinct integers for which adf achieves its extreme values.

Besides considering the distribution of var on the set [m]n, we also consider it on the set of rearrangementsRn(i1,i2,...,im) consisting of sequences of lengthn=i1+i2+

···+imwhich containlexactlyil times, on the set of permutationsSn=Rn(1, 1,..., 1) of{1, 2,...,n}, and on the set of compositions ofmintonpartsCn(m)= {x1x2···xn [m]n:x1+x2+···+xn=m}. For m,n2,Table 1.1 displays the mean and variance of var on these four sets. Thekth falling factorial ofn isnk=n(n1)···(nk+ 1), i=(i1,i2,...,im), and, forra real number,r denotes the greatest integer less than or equal tor. The results inTable 1.1are new. David and Barton [3, Chapter 10] present the distributions of several statistics (some f-adjacency numbers, some not) primarily on permutations. We also note that Tiefenbruck [7] derived a generating function for compositions with bounded parts by a close relative of var. We leave open questions con- cerning the asymptotic behavior of var.

2. Enumerative factorial moments for f-adjacencies

Before working specifically with var, we discuss the enumerative generating function for adf on sequences as developed by F´edou and Rawlings [4]. Let [m]denote the set of sequences of 1, 2,...,mof finite length (including the empty sequence of length 0). For w=x1x2···xn[m], we defineZw=zx1zx2···zxn. The enumerative generating func- tion for adf over [m]is then defined to beG(p)=

w[m]padfwZw.

By manipulatingG(p), we will obtain all of the information inTable 1.1(and more).

As a brief outline of our approach, note that the coefficient ofpkz1i1z2i2···zimm inG(p) is

(3)

just the number of rearrangementswinRn(i) with adfw=k. Thus, by dividing the coeffi- cient ofzi11zi22···zmiminG(1) by the cardinality ofRn(i), we will obtain the mean of adf. So, in general, we compute thedthenumerative factorial momentG(d)(1)=

w[m](adfw)d Zw.

From the work of F´edou and Rawlings [4], it follows that

G(p)= 1

D(p), (2.1)

where

D(p)=1

n1

x1···xn[m]n

Zx1···xn

n1 k=1

pf(xkxk+1)1. (2.2)

Examples are presented in [4,6] for whichDhas a closed form. We do not know a closed form forDwhen adf=var (that is, when f(x,y)= |yx|). Nevertheless, (2.1) is still useful in computing the mean and variance of var.

Although the formula for taking thed-fold derivative with respect to pof a function of the form in (2.1) is known, we provide a short derivation. To avoid the quotient and chain rules, rewrite (2.1) asGD=1. Differentiating the latterdtimes,d1, and dividing byd! gives

d j=0

G(dj) (dj)!

D(j)

j! =0. (2.3)

To solve forG(d), consider the system G(d)

d!

D(0)

0! + G(d1) (d1)!

D(1)

1! + G(d2) (d2)!

D(2)

2! +···+G(0) 0!

D(d) d! =0, G(d1)

(d1)!

D(0)

0! + G(d2) (d2)!

D(1)

1! +···+G(0) 0!

D(d1) (d1)!=0,

... G(1)

1!

D(0) 0! +G(0)

0!

D(1) 1! =0, G(0)

0!

D(0) 0! =1,

(2.4)

where the topdequations arise from repeated application of (2.3). Cramer’s rule applied

(4)

to the above system yields

G(d) d! =

(1)d Dd+1

D(1) 1!

D(2) 2!

D(3)

3! ···

D(d) d!

D(0) 0!

D(1) 1!

D(2) 2!

D(d1) (d1)!

0 D(0) 0!

D(1) 1!

D(d2) (d2)!

... ...

0 ··· 0 D(0)

0!

D(1) 1!

(2.5)

which, when expanded, implies that G(d)=d

ν=1

(1)ν Dν+1

j1+···+jν=d jk1

d j1···jν

D(j1)···D(jν). (2.6)

To determine the enumerative factorial momentG(d)(1), we see from (2.2) that D(j)(1)= −

j+1

r=2

D(rj), (2.7)

where

D(rj)=

x1···xr[m]r

Zx1···xr

l1+···+lr1=j lk1

j l1···lr1

r1

k=1

fxkxk+1

lk

. (2.8)

For instance,

D2=

xy[m]2

f(xy)zxzy, D2 =

xy[m]2

f(xy)2zxzy, D3=2

vxy[m]3

f(vx)f(xy)zvzxzy. (2.9)

Further settingj=(j1,...,jν),s(j)=j1+···+jν, d

j

= d

j1···jν

, and D(µj)=

r1+···+rν=µ rk2

D(r1j1)···D(rνjν), (2.10)

it follows from (2.6) and (2.7) that G(d)(1)=d

ν=1

1 Dν+1(1)

s(j)=d jk1

d j

d+ν

µ=2ν

D(µj). (2.11)

(5)

AsD(1)=1(z1+···+zm), extracting the contributions made by allw[m]n from both sides of (2.11) gives thedth enumerative factorial moment of adf over [m]nas

w[m]n

(adfw)dZw= d ν=1

s(j)=d jk1

d j

d+ν

µ=2ν

n+νµ ν

m

i=1

zi

nµ

D(µj) (2.12)

valid ford1. Whend=1, 2, (2.9) and (2.12) imply that

w[m]n

adfw Zw=(n1) m

i=1

zi n2

xy[m]2

f(xy)zxzy (2.13)

and that

w[m]n

(adfw)2Zw=(n1) m

i=1

zi n2

xy[m]2

f(xy)2zxzy

+ 2(n2) m

i=1

zi n3

vxy[m]3

f(vx)f(xy)zvzxzy

+ (n2)(n3) m

i=1

zi

n4

xy[m]2

f(xy)zxzy 2

.

(2.14)

3. Discussion ofTable 1.1

The entries inTable 1.1are consequences of (2.13) and (2.14) with f(xy)= |yx|and with appropriate substitutions for Z. For the mean and variance of var on the set of bounded sequences [m]n, putzi=1 for 1im. Noting that

xy[m]2

|yx| =

1x<ym

2(yx)=2 m+ 1

3

, (3.1)

it follows from (2.13) that the mean of var on [m]nis 1

mn

w[m]n

varw=2(n1)mn2 mn

m+ 1 3

=(n1)m21

3m . (3.2)

As

xy[m]2

|yx|2=4 m+ 1

4

(3.3)

(6)

and as

vxy[m]n

|xv||yx| =

1v<x<ym

2(xv)(yx)

+

1x<yvm

4(vx)(yx)

1x<ym

2(yx)2

=7m28 10

m+ 1 3

,

(3.4)

(2.14) implies that 1 mn

w[m]n

(varw)2=4(n1) m2

m+ 1 4

+(n2)7m28 5m3

m+ 1 3

+4(n2)(n3) m4

m+ 1 3

2

.

(3.5)

Then, subbing the last result into 1

mn

w[m]n

(varw)2+(n1)m21

3m

(n1)m21 3m

2

(3.6) and simplifying gives the variance of var as recorded inTable 1.1.

ForRn(i), extracting the coefficient ofzi11zi22,···,zmimfrom (2.13) leads to

wRn(i)

varw=2(n1)

1x<ym

(yx)

n2

i1···ix1···iy1···im

. (3.7)

As the cardinality ofRn(i) is

n i1i2···im

= n

i

, (3.8)

it follows that the mean of var onRn(i) is n

i 1

wRn(i)

varw=2 n

1x<ym

(yx)ixiy. (3.9)

Leti\r=(i1,...,ir1,...,in). For example, (3, 2, 1, 4)\3\2\3=(3, 1,1, 4). The variance on Rn(i) is then

n i

1

wRn(i)

varw2+2 n

1x<ym

(yx)ixiy 2

n

1x<ym

(yx)ixiy 2

, (3.10)

(7)

where, upon extraction of the coefficient ofzi11zi22,...,zmimfrom (2.14), we have

wRn(i)

(varw)2=(n1)

1x,ym

|yx|2 n2

i\x\y

+ 2(n2)

1v,x,ym

|xv||yx| n3

i\v\x\y

+ (n2)(n3)

1u,v,x,ym

|vu||yx|

n4 i\u\v\x\y

.

(3.11)

The permutation entries inTable 1.1follow from (3.9) and (3.10). Selectingm=nand ik=1 for 1knin (3.9) reveals the mean of var onSnas

1 n!

wSn

varw=2 n

1x<yn

(yx)=2 n

n+ 1 3

=n21

3 . (3.12)

From (3.11), withm=nandik=1 for 1kn,

wSn

(varw)2=(n1)!

1x,yn

|yx|2 + 2(n2)!

1v,x,yn

|xv||yx| + (n2)!

1u,v,x,ym {u,v}∩{x,y}=∅

|vu||yx|

= 4 15

(n2)!10n2+ 14n27 n+ 1

4

.

(3.13)

So the variance of var onSnis 1

n!

wSn

varw2+n21

3

n21 3

2

=(n2)(n+ 1)(4n7)

90 . (3.14)

For w=x1···xn[m]n, let w =x1+···+xn. For the composition results in Table 1.1, setzk=qkfor 1km. Then (2.13) implies that

w[m]n

varw qw=(n1)qn2 1qm 1q

n2

1x,ym

|yx|qx+y (3.15)

(8)

and (2.14) leads to

w[m]n

(varw)2qw=(n1)qn2 1qm 1q

n2

1x,ym

|yx|2qx+y + 2(n2)qn3 1qm

1q

n3

1v,x,ym

|xv||yx|qv+x+y + (n2)(n3)qn4 1qm

1q

n4

1u,v,x,ym

|vu||yx|qu+v+x+y. (3.16) Extracting the coefficient ofqmfrom (3.15) to obtain

wCn(m)

varw=2(n1)

1x<ym

(yx)

m1xy n3

=2(n1)

1xm/2

m2x n1

(3.17)

and then dividing by the cardinalitymn11

ofCn(m) gives the mean of var as stated in Table 1.1. The variance is

m1 n1

1

wCn(m)

varw2+ 2(n1) (m1)n1

1xm/2

(m2x)n1

2(n1) (m1)n1

1xm/2

(m2x)n1 2

,

(3.18)

where, pulling the coefficient ofqmfrom (3.16), we have

wCn(m)

(varw)2=(n1)

1x,ym

|yx|2

m1xy n3

+ 2(n2)

1v,x,ym

|xv||yx|

m1vxy n4

+ (n2)(n3)

1u,v,x,ym

|vu||yx|

m1uvxy n5

. (3.19) The sums in (3.19) are marginally simplified. For instance,

1x,ym

|yx|2

m1xy n3

=4

1xm/2

m2x n

. (3.20)

(9)

As a part of the second sum on the right-hand side of (3.19), we note that

1v<x<ym

(xv)(yx)

m1vxy n4

=

2x(m+1)/2

m3x+ 1 n

m2x+ 1 n

+x

m2x n1

.

(3.21)

The four-fold sums arising in the last sum in (3.19) reduce to double sums.

Acknowledgment

This work is based on work supported by the National Science Foundation under Grant no. 0097392.

References

[1] L. Carlitz,Enumeration of compositions by rises, falls and levels, Math. Nachr.77(1977), 361–

371.

[2] C.-C. Chao and W.-Q. Liang,Arrangingndistinct numbers on a line or a circle to reach extreme total variations, European J. Combin.13(1992), no. 5, 325–334.

[3] F. N. David and D. E. Barton,Combinatorial Chance, Hafner, New York, 1962.

[4] J.-M. F´edou and D. P. Rawlings,Adjacencies in words, Adv. in Appl. Math.16(1995), no. 2, 206–218.

[5] C. Levcopoulos and O. Petersson,Heapsort—adapted for presorted files, Algorithms and Data Structures (Ottawa, ON, 1989), Lecture Notes in Comput. Sci., vol. 382, Springer, Berlin, 1989, pp. 499–509.

[6] D. P. Rawlings,Restricted words by adjacencies, Discrete Math.220(2000), no. 1-3, 183–200.

[7] M. Tiefenbruck,Enumerating compositions with bounded parts by variation, REU report, Cali- fornia Polytechnic State University, California, 2003.

Rudolfo Angeles: Department of Mathematics, College of Science and Mathematics, California, Polytechnic State University, San Luis Obispo, CA 93407, USA

Current address: Department of Statistics, Stanford University, Palo Alto, CA 94305-4065, USA E-mail address:[email protected]

Don Rawlings: Department of Mathematics, College of Science and Mathematics, California Polytechnic State University, San Luis Obispo, CA 93407, USA

E-mail address:[email protected]

Lawrence Sze: Department of Mathematics, College of Science and Mathematics, California, Poly- technic State University, San Luis Obispo, CA 93407, USA

E-mail address:[email protected]

Mark Tiefenbruck: Department of Mathematics, College of Science and Mathematics, California Polytechnic State University, San Luis Obispo, CA 93407, USA

Current address: 8989 Jasmine Lane Street, Cottage Grove, MN 55016-3436, USA E-mail address:[email protected]

(10)

Special Issue on

Modeling Experimental Nonlinear Dynamics and Chaotic Scenarios

Call for Papers

Thinking about nonlinearity in engineering areas, up to the 70s, was focused on intentionally built nonlinear parts in order to improve the operational characteristics of a device or system. Keying, saturation, hysteretic phenomena, and dead zones were added to existing devices increasing their behavior diversity and precision. In this context, an intrinsic nonlinearity was treated just as a linear approximation, around equilibrium points.

Inspired on the rediscovering of the richness of nonlinear and chaotic phenomena, engineers started using analytical tools from “Qualitative Theory of Differential Equations,”

allowing more precise analysis and synthesis, in order to produce new vital products and services. Bifurcation theory, dynamical systems and chaos started to be part of the mandatory set of tools for design engineers.

This proposed special edition of the Mathematical Prob- lems in Engineering aims to provide a picture of the impor- tance of the bifurcation theory, relating it with nonlinear and chaotic dynamics for natural and engineered systems.

Ideas of how this dynamics can be captured through precisely tailored real and numerical experiments and understanding by the combination of specific tools that associate dynamical system theory and geometric tools in a very clever, sophis- ticated, and at the same time simple and unique analytical environment are the subject of this issue, allowing new methods to design high-precision devices and equipment.

Authors should follow the Mathematical Problems in Engineering manuscript format described at http://www .hindawi.com/journals/mpe/. Prospective authors should submit an electronic copy of their complete manuscript through the journal Manuscript Tracking System athttp://

mts.hindawi.com/according to the following timetable:

Manuscript Due December 1, 2008 First Round of Reviews March 1, 2009 Publication Date June 1, 2009

Guest Editors

José Roberto Castilho Piqueira,Telecommunication and Control Engineering Department, Polytechnic School, The University of São Paulo, 05508-970 São Paulo, Brazil;

[email protected]

Elbert E. Neher Macau,Laboratório Associado de Matemática Aplicada e Computação (LAC), Instituto Nacional de Pesquisas Espaciais (INPE), São Josè dos Campos, 12227-010 São Paulo, Brazil ; [email protected] Celso Grebogi,Center for Applied Dynamics Research, King’s College, University of Aberdeen, Aberdeen AB24 3UE, UK; [email protected]

Hindawi Publishing Corporation http://www.hindawi.com

参照

関連したドキュメント

Faculty of Mathematics Department of Applied Physics University of Bielefeld Tokyo Institute of

Lenbury: Department of Mathematics, Faculty of Science, Mahidol University, 272 Rama 6 Road, Bangkok 10400, Thailand. E-mail

The repeated homogeneous balance method is used to construct new exact traveling wave solutions of the (2+1) dimensional Zakharov- Kuznetsov (ZK) equation, in which the

Now s is the least overlap-free sequence beginning with w if and only if 1001y is the least overlap- free sequence beginning with 1001 (assertion 2 (b) in Lemma 2). And 1001y is

(1 Department of Mathematics, Hefei, Teacher’s College, Hefei Anhui Province, 236032, PR China 2 College of Science, University of Shanghai for Science and Technology, Shanghai,

˙Ibrahim C¸anak: Department of Mathematics, Adnan Menderes University, 09010 Aydın, Turkey Email address: [email protected]. Umit Totur: Department of Mathematics, Adnan

a College of Mathematics, Inner Mongolia University for Nationalities, Tongliao City, Inner Mongolia Autonomous Region, 028043, China.. b Department of Mathematics, College of

Mathematics Department, Faculty of Science, Cairo University, Beni- Suef, Egypt E-mail