arXiv:physics/0610081 v1 11 Oct 2006
S. S. Apostolov, Z. A. Mayzelis
V. N.Karazin Kharkov National University, 4 Svoboda Sq.,Kharkov 61077, Ukraine
O. V. Usatenko
∗
, V. A. Yampol'skii
A. Ya. Usikov Institute for Radiophysi s and Ele troni s
Ukrainian A ademy of S ien e, 12 Proskura Street, 61085 Kharkov, Ukraine
Twoapproa hes tostudyingthe orrelation fun tionsof thebinary Markovsequen es are on-sidered. The first of them is based onthe studyof probability of o urring differentwords in thesequen e.Theotheroneusesre urren erelationsfor orrelationfun tions.Thesemethodsare appliedfortwoimportantparti ular lassesoftheMarkov hains.These lassesin ludetheMarkov hainswithpermutative onditionalprobabilityfun tionsandtheadditiveMarkov hainswiththe smallmemoryfun tions.Theex itingpropertyoftheself-similarity(dis overedinPhys.Rev.Lett. 90, 110601(2003)fortheadditiveMarkov hainwiththestep-wisememoryfun tion)isprovedto betheintrinsi propertyofanypermutativeMarkov hain.Appli abilityofthe orrelationfun tions oftheadditiveMarkov hainswiththesmallmemoryfun tionsto al ulatingthethermodynami hara teristi softhe lassi alIsingspin hainwithlong-rangeintera tionisdis ussed.
PACSnumbers:05.40.-a,02.50.Ga,87.10.+e
I. INTRODUCTION
Theproblem of long-range orrelatedrandomsymboli systems(LRCS) hasbeen under studyfor alongtime in manyareasof ontemporaryphysi s[1,2,3,4,5,6℄,biology[7,8,9,10,11,12℄,e onomi s[8,13,14℄,linguisti s[15, 16, 17, 18, 19℄, et . Among the ways to get a orre t insight into the nature of orrelations of omplex dynami systems, theuse of themulti-step Markov hains is of great importan e be ause it enables onstru ting arandom sequen e with the pres ribed orrelated properties in the mostnatural way [19, 20, 21℄. Alsothe additive Markov hainswithsmallmemoryfun tionsareofinterestforthenon-extensivethermodynami sofIsingspin hains[22,23℄. Themulti-step binary Markov hainis hara terizedby the onditional probability of the definedsymbol
a
i
(for example,a
i
= 1
)o urring after previous symbols within thememory lengthN
, i.e., afterN
-word.We definetheL
-wordT
L
,orthewordoflengthL
,asthesetofL
sequentialsymbols.TheMarkov hain anbeeasily onstru tedby thesequentialgenerationofsymbolsusingthepres ribed onditionalprobabilityfun tion.The onditionalprobability pointstothedire tasso iationbetweenthesymbols.Atthesametime,the orrelationfun tionsdes ribetheimpli it intera tionbetween thesymbols.Correlation fun tions ofall ordersdetermine ompletely everystatisti al property ofany randomsequen e.So, theproblemof finding the orrelationfun tions ofhigh ordersis essential.The aimof thepaperistofindthe orrelationfun tionsofdifferentordersofthebinaryMarkov hainusingtwoapproa hesand toexaminetheirproperties.Thepaperisorganizedasfollows.These ondSe tiondes ribesthemethodof al ulatingstatisti al hara teristi s oftheMarkov hainviathe onditionalprobabilityfun tion.Herethepropertyoftheself-similarityofthe orrelated random sequen es is alsodis ussed. Thethird Se tion is devoted to amethod for finding the orrelation fun tions usingre urren erelationsforthem. Theappli ations oftheproposedgeneralalgorithms tosome on rete lassesof hainsarepresented.
II. DIRECT METHODFORCALCULATING STATISTICALCHARACTERISTICS OFTHE
MARKOVCHAIN
Inthisse tion,we des ribeadire t methodoffindingfollowing hara teristi sof the
N
-stepsMarkov hains:the probabilityP (T
N
)
oftheN
-wordso urring,theprobabilityP (T
L
)
ofo urringthewordsof anarbitrarylengthL
, andthehigh-order orrelationfun tions.∗
Itisknownthatallstatisti alpropertiesofMarkovsequen earedetermined ompletelybythe onditional proba-bilityfun tion.Alongwiththisfun tion,itis onvenienttoemploytheprobabilities
P (T
N
)
oftheN
-wordso urring. All other hara teristi s of the hain an be found using these probabilities. Though the al ulation ofP (T
N
)
is quite a hallenge in the general ase, we su eed in obtaining the analyti alresults for some parti ular ases (see Subse .IIC).The
N
-step Markov hain is asequen e ofrandom symbolsa
i
,i ∈ Z = {. . . , −2, −1, 0, 1, 2, . . .}
.It possessesthe followingproperty: the probability ofsymbola
i
to have a ertain value, under the ondition that thevaluesof all previous symbolsaregiven,dependsonthevaluesofN
previoussymbolsonly,P (a
i
= a| . . . , a
i−2
, a
i−1
) = P (a
i
= a|a
i−N
, . . . , a
i−2
, a
i−1
).
(1) WerefertoN
asthememory depth.Inthispaperwe onsiderbinary hainsonly,but someresults anbegeneralizedto non-binarysequen esaswell.
A. Probabilitiesof the
N
-wordso urringWestartexaminingthestatisti alpropertiesoftheMarkov hainswithsear hingtheprobabilitiesofthe
N
-words o urring.Thereare2
N
different
N
-wordsin thearbitraryMarkov hainwhi his hara terizedby2
N
probabilities ofthesewordso urring.They anbefoundusingevidentformulasoftheprobabilitytheory,
P (A) = P (A ∩ B) + P (A ∩ B),
(2)P (A ∩ B) = P (A|B)P (B).
(3)Here
A ∩ B
meansthat eventsA
andB
o ursimultaneouslyand eventB
isoppositeto theeventB
.Eqs.(2), (3) yieldthefollowingequation,P (a
1
a
2
. . . a
N
) =
X
a=0,1
P (a
N
|aa
1
. . . a
N −1
)P (aa
1
. . . a
N −1
).
(4)Thisequation,beingwrittenforallpossiblevaluesofsymbols
a
1
, . . . , a
N
,alongwiththenormalizationrequirement,X
ai=0,1
i=1,...,N
P (a
1
a
2
. . . a
N
) = 1,
(5)isinfa tthesetoflinearequations.Fromthisset,one anobtainallsoughtprobabilities
P (T
N
)
.Thoughset(4),(5) ontains2
N
+ 1
equations,ithasasinglesolutionbe auseoneofEqs.(4)isalinear ombinationofothers.
B. Probabilities ofarbitrarywords o urringand orrelationfun tions
Using Eq. (2) we an al ulate the probability
P (T
L
)
withL < N
by redu ing theN
-words to theL
-word(a
1
a
2
. . . a
s
)
,P (a
1
a
2
. . . a
L
) =
X
ai=0,1
i=L+1,...,N
P (a
1
a
2
. . . a
N
),
L < N.
(6)This equation represents the probabilityof the
L
-wordo urring asthe average of theprobabilities to have theN
-word ontainingthisL
-word.Itispossibletoredu etheN
-wordtotheshorterL
-wordbysummingoverdifferent setsofsymbolsattheleftandrightedgesoftheN
-word.Thewordoflength
L
greaterthanN
anbepresented asthe ombinationofthewordoflengthN
and(L − N)
symbolsfollowingafterit. A ordingtothedefinitionoftheMarkov hain, ea hofthese(L − N)
symbols antake ona ertainvaluewiththeprobability dependingonthe pre edentN
-word.The(L − N)
-folduseofEq. (3)yields thefollowingequation,P (a
1
a
2
. . . a
L
) = P (a
1
a
2
. . . a
N
)
L−N
Y
r=1
Letusdefinea orrelationfun tionofthe
s
thorder:K
s
(i
1
, i
2
, . . . , i
s
) = (a
i
1
− ¯a
i
1
)(a
i
2
− ¯a
i
2
) . . . (a
i
s
− ¯a
i
s
),
(8) where· · ·
isthestatisti alaverageovertheensembleof hains.We onsiderergodi hain.A ordingtotheMarkov theorem(see, e.g.,Ref.[24℄),this propertyisvalidfor thehomogenousMarkov hainsifthe onditionalprobability doesnottakeonvalues0
and1
.Inthis aseaveragingovertheensemble of hainsandoverthe hain oin ide.Formally,fun tion
K
s
dependsons
arguments(s
differentindexesofthesymbols),butwedo onsiderhomogenous Markov hains.Therefore, orrelationfun tionK
s
dependson(s−1)
arguments,i.e.,thedistan esbetweentheindexes,r
1
= i
2
− i
1
, r
2
= i
3
− i
2
, . . . , r
s−1
= i
s
− i
s−1
.Itsdefinitionis writtenasK
s
(r
1
, r
2
, . . . , r
s−1
) = (a
0
− ¯a)(a
r
1
− ¯a)(a
r
1
+r
2
− ¯a) . . . (a
r
1
+...+r
s−1
− ¯a).
(9) Here¯
a
istheaveragenumberofunitiesin thesequen eand notation· · ·
isthestatisti alaverageoverthe hain,f (a
r
1
, . . . , a
r
1
+...+r
s
) = lim
M→∞
1
2M + 1
M
X
i=−M
f (a
i+r
1
, . . . , a
i+r
1
+...+r
s
).
(10)Introdu ingthenotation,
R
0
= 0,
R
k
=
k
X
i=1
r
i
,
d
i
= a
i
− ¯a,
(11)werewritedefinition(9)ofthe orrelationfun tion,
K
s
(r
1
, r
2
, . . . , r
s−1
) =
X
aR
i
=0,1
i=0,...,s−1
d
R
0
d
R
1
. . . d
R
s−1
P (a
R
0
a
R
1
. . . a
R
s−1
).
(12)Nowwe an omplement theset ofsymbols
a
R
0
, a
R
1
, . . . , a
R
s−1
with thesymbolsbetween them. Finallywe have thefollowingformula,K
s
(r
1
, r
2
, . . . , r
s−1
) =
X
ai=0,1
i=0,...,Rs
−1
d
R
0
d
R
1
. . . d
R
s−1
P (a
0
a
1
. . . a
R
s−1
).
(13) HereprobabilitiesP (a
0
a
1
. . . a
R
s−1
)
should be al ulatedusingEqs.(6) or(7).C. PermutativeMarkov hains
Solvinglinearsystem(4),(5)forthegeneral aseisa hallengingproblem.Herewedemonstratetheappli ationof thedes ribed methodto a ertain lass ofthe Markov hains. Weassumethat the onditional probability fun tion of the hainunder onsiderationis independent of the order of symbols in the previous
N
-word.We refer to su h sequen esasthepermutative Markov hains.1. Probabilitiesofword o urringinthepermutativeMarkov hain
It is onvenient to introdu e a new abbreviated notation for the onditional probability fun tion
P (a
N +1
|a
1
a
2
. . . a
N
) = p
k
(a
N +1
)
. Herek = a
1
+ a
2
+ . . . + a
N
is the number of unities inN
-word(a
1
a
2
. . . a
N
)
. Besides,we definep
k
(1)
asp
k
.Nowwe seekthesolutionofsystem(4),(5)intheform
b
N
(k) = b
N
(a
1
+ a
2
+ . . . + a
N
) = P (a
1
a
2
. . . a
N
).
(14)Inotherwords,theprobabilityofthe
N
-wordo urringdependsonthenumberofunitiesinthisN
-wordonly.Then Eq.(4) anberewrittenasthefollowingre urren erelation,Thesolutionofthisequationis
b
N
(k) = b
N
(0)
k
Y
r=1
p
r−1
1 − p
r
.
(16)Hereprobability
b
N
(0)
anbeobtainedfromEq.(5) ,b
N
(0) =
X
N
k=0
C
k
N
k
Y
r=1
p
r−1
1 − p
r
−1
,
(17)C
n
k
=
n!
k!(n − k)!
=
Γ(n + 1)
Γ(k + 1)Γ(n − k + 1)
.
Theprobability
P (a
1
a
2
. . . a
N
)
,Eq.(14) ,does notdepend ontheorderofsymbolsinN
-word(a
1
a
2
. . . a
N
)
. From Eq. (6) and the above statement it followsthat theprobabilityP (T
L
)
of a short word (withL < N
)o urring is likewiseindependentoftheorderofsymbolsinthisword.Denotingthisprobabilitybyb
L
(k) = b
L
(a
1
+a
2
+. . .+a
L
) =
P (a
1
a
2
. . . a
L
)
wearrivedatthefollowingformula,b
L
(k) =
N −L
X
m=0
C
N −L
m
b
N
(k + m).
(18)Theprobabilityofthelong
L
-word(withL > N
)o urringdoesdependontheorderofthesymbolsinthisword. UsingEq.(7)we haveP (a
1
a
2
. . . a
L
) = b
N
(q
0
)
L−N
Y
r=1
p
q
r−1
(a
N +r
).
(19)Here
q
i
= a
i+1
+ a
i+2
+ . . . + a
i+N
. Equations(16)-(18)are thegeneralizationof resultsearlier obtainedin [21,25℄ fortheadditivebinaryMarkov hainwiththestep-wisememoryfun tion.2. Correlationfun tions
Herewepresentanalyti alresultsfrom the al ulationofthe orrelationfun tionsofarguments
r
1
, . . . , r
s−1
satis-fyingthe onditionr
1
+ . . . + r
s−1
< N
.Forthispurposeweexpressthefra tionofunitiesinthe hainusingEq.(18),a = b
1
(1) =
N
X
k=1
b
N
(k)C
N −1
k−1
.
(20)Forthepermutative Markov hainsunder onsideration,the orrelationfun tion ofarguments
r
1
, . . . , r
s−1
depends ontheirnumbers
only.Equation(13)yieldsK
s
(r
1
, r
2
, . . . , r
s−1
) = K
s
=
N
X
k=0
b
N
(k)S
N
(k, s, a),
(21)S
N
(k, s, ¯
a) =
min{s,k}
X
j=0
(−¯a)
s−j
C
N −j
k−j
C
s
j
.
(22)Inparti ular,thebinary orrelationfun tion
K
2
(r)
ofanypermutative hainis onstantforthevaluesofarguments lessthanthememorydepth:K
2
(r) = K
2
,
r < N
.IfweapplyallderivedformulastotheadditiveMarkov hainwiththestep-wisememoryfun tion,
p
k
=
1
2
− ν + µ
2k
N
− 1
,
(23)wegetthe orrelationfun tionsoforder
s
,K
s
=
Γ(n
1
+ n
2
)
Γ(n
1
)
s
X
k=0
(−¯a)
s−k
C
s
k
Γ(n
1
+ k)
Γ(n
1
+ n
2
+ k)
.
(24) Here¯
a =
n
1
n
1
+ n
2
,
n
1
=
N (1 − 2(µ + ν))
4µ
,
n
2
=
N (1 − 2(µ − ν))
4µ
.
(25)For
s = 2
we re overtheresultspreviouslyobtainedin[21, 25℄forthebinary orrelationfun tionK
2
.D. Self-similarity ofthe permutativeMarkov hain
In this subse tion we point out an interesting property of the permutative Markov hains, namely, their self-similarity.Thedis ussionofthisissueforthestep-likememoryfun tionispresentedin paper[25℄.
Letusredu e the
N
-stepMarkovsequen eby regularly(orrandomly)removingsomesymbolsand introdu ethe de imationparameterλ = N
∗
/N, 1/N < λ < 1
,whi h representsthefra tionofsymbols keptinthe hain.
Due to approa hmentof symbols in thesequen e afterthe de imation pro edure,the binary orrelation fun tion
K
2
(r)
transformsintoK
∗
2
(r) =
(1 − {r/λ})K
2
([r/λ]) + {r/λ}K
2
([r/λ] + 1),
regularde imation,∞
P
l=0
K
2
(r + l)C
l+r−1
l
(1 − λ)
l
λ
r
,
randomde imation, (26)where
[x]
isthemaximalintegernumberlessthanx
and{x} = x − [x]
.The orrelation fun tion
K
2
(r)
of the permutative Markov hain is equalto onstant valueK
2
with argumentsr 6 N − 1
.A ordingto Eq.(26)(regularde imation),thevaluesofthe orrelationfun tionK
∗
2
(r)
atr 6 λ(N − 1)
takeon thesamevalueK
2
.In the aseofthe randomde imation wehave onlyan exponentiallysmall (atN ≫ 1
) differen ebetweenthe orrelationfun tionK
∗
2
(r)
andvalueK
2
,|K
2
∗
(r) − K
2
| 6
√
A
¯
λN
exp − a(¯λ, λ)N
,
r = ¯
λN,
¯
λ < λ.
(27)Herethenewfun tion
a(¯
λ, λ)
and onstantA
areintrodu ed,a(¯
λ, λ) = ¯
λ ln
¯
λ
λ
+ (1 − ¯λ) ln
1 − ¯λ
1 − λ
> 0,
A =
√
e
π
|K
2
| + max
r>N
|K
2
(r)|
.
(28)Thus, the orrelation fun tion of the de imated sequen e is onstant (or asymptoti ally onstant) at the region
r < N
∗
.Thispropertyisreferredtoastheself-similarity.Theself-similarity is the intrinsi propertyof the permutative Markov hains.It is possible to showthat, in the general ase, the onditional probability fun tion of the de imated
N
-step Markovsequen e is of infinite memory depth. This is be auseits onditional probabilityis blurred by the de imation pro edureand be omes dependent onallprevioussymbols.So,the self-similarity istheproperty of thebinary orrelationfun tion onlyand inheresin allrandomsequen es witha onstantbinary orrelationfun tion
K
2
(r)
atr < N
,K
2
(r) = K
2
, 1 6 r < N ⇒
Self-similarity. (29)III. CORRELATION FUNCTIONS ANDCHARACTERISTICEQUATIONS
InthisSe tion,wedealwiththere urren erelationstofindthe orrelationfun tions.InSubse tionAweshowthat theserelationsyieldtheexpli itexpressionforthe orrelationfun tionsviatherootsofthe hara teristi equations. Subse tion B is devoted to appli ations of this method. The last Subse tion ontains some generalizations of the above-mentionedre urren erelations.
The pro edure of finding the orrelation fun tions
K
s
is based on the mathemati al indu tion method. In other words,we supposethat all orrelationfun tionsK
l
oftheorderslessthans
arefound.Forthe onvenien esake,we admitthatK
0
= 1
andK
1
= 0
.A. High-order orrelation fun tionsofthe additive Markov hain
Considerthe
N
-stepMarkov hainwiththeadditive onditionalprobabilityfun tion,P (a
i
= 1|a
i−N
. . . a
i−1
) = ¯
a +
N
X
r=1
F (r)(a
i−r
− ¯a).
(30)Herefun tion
F (r)
,r = 1, . . . , N
,isreferredtoasthememory fun tion and¯
a
isthefra tionof unitiesintheabove sequen e(fordetailsseeRef. [26℄).Letusfindthere urren erelationsforthe orrelationfun tionsof
N
-stepadditiveMarkov hain.Forthispurpose, wefirst al ulateexpli itlytheaverageoversymbola
r
1
+...+r
s−1
inEq.(9).UsingthenotationofSe .IIBandEq.(30), and takingintoa ountequationP (a
R
s−1
= 1|·) + P (a
R
s−1
= 0|·) = 1
,we anrewriteEq. (9)forarbitraryr
i
> 0
,i = 1, . . . , s − 1
,intheform,(a
R
0
− ¯a) . . . (a
R
s−1
− ¯a) =
= (a
0
− ¯a) . . . (a
R
s−2
− ¯a)((1 − ¯a)P (a
R
s−1
= 1|T
N,R
s−1
) − ¯aP (a
R
s−1
= 0|T
N,R
s−1
)) =
(31)= (a
0
− ¯a) . . . (a
R
s−2
− ¯a)
N
X
r=1
F (r)(a
R
s−1
−r
− ¯a).
HereT
N,R
s−1
isthesetofsymbols(a
R
s−1
−N
, . . . , a
R
s−1
−1
)
.Inthatway,weobtainthefundamentalre urren erelation onne tingthe orrelationfun tions ofdifferentorderss
,K
s
(r
1
, . . . , r
s−1
) =
N
X
r=1
F (r)K
s
(r
1
, . . . , r
s−1
− r).
(32)Intheparti ular ase
s = 2
,this equation,K
2
(r
1
) =
N
X
r=1
F (r)K
2
(r
1
− r),
(33)was obtained and dis ussed in [26℄. Re urren e relation (32) is orre t for
r
i
> 0
,i = 1, . . . , s − 1
. Provided thatr
s−1
6
N
,thelastargument ofthe orrelationfun tionin theright-handsideofEq.(32)isnegativeorzeroandone shouldinterpretitinthefollowingmanner,whi hisreferredtoas ollating.Ifthe orrelationfun tionhasnegative arguments,we mustreorganizeita ordingtodefinition(9).Forexample,K
4
(2, 2, −3) =
(a
0
− ¯a)(a
2
− ¯a)(a
4
− ¯a)(a
1
− ¯a)
=
=
(a
0
− ¯a)(a
1
− ¯a)(a
2
− ¯a)(a
4
− ¯a)
= K
4
(1, 1, 2).
(34)Ifthe orrelationfun tion haszeroarguments(indexes
i
andk
oftwomultipliers(a
i
− ¯a)
and(a
k
− ¯a)
oin ide)one shouldemploythepropertyofthebinary hain:a
2
i
= a
i
,a
i
= {0, 1}
.Thus, wehave(a
i
− ¯a)
2
= (1 − 2¯a)(a
i
− ¯a) + ¯a(1 − ¯a).
With this property we an write the useful relations for the orrelation fun tion ontaining zero arguments in differentpositionsamongallargumentsof
K
s
,K
s
(0, r
2
, . . . , r
s−1
) = (1 − 2¯a)K
s−1
(r
2
, . . . , r
s−1
) + ¯
a(1 − ¯a)K
s−2
(r
3
, . . . , r
s−1
),
K
s
(r
1
, . . . , r
k−1
, 0, r
k+1
, . . . , r
s−1
) = (1 − 2¯a)K
s−1
(r
1
, . . . , r
k−1
, r
k+1
, . . . , r
s−1
)+
+¯
a(1 − ¯a)K
s−2
(r
1
, . . . , r
k−1
+ r
k+1
, . . . , r
s
),
k 6= 1, s,
K
s
(r
1
, . . . , r
s−2
, 0) = (1 − 2¯a)K
s−1
(r
1
, . . . , r
s−2
) + ¯
a(1 − ¯a)K
s−2
(r
1
, . . . , r
s−3
).
ThegeneralsolutionofEq.(32) an berepresentedasalinear ombination,
K
s
(r
1
, . . . , r
s−1
) =
N
X
j=1
L
j
(r
1
, . . . , r
s−2
)ξ
j
r
s−1
, r
i
> 0 (i = 1, . . . , s − 1),
(36)ofpowersoftheroots
ξ
j
,j = 1, . . . , N
, ofthe hara teristi equation,ξ
N
−
N
X
j=1
F (j)ξ
N −j
= 0.
(37)Newfun tions
L
j
(r
1
, . . . , r
s−2
)
, i.e. oeffi ients oflinearform Eq.(36) , intheirturn, should bedefined. All one has todoistosubstituteEq.(36)into ollatedEq.(32)for0 < r
s−1
< N
.Finally,thispro edureyieldsthere urren e relationsforthesoughtfun tionsL
j
.Thegeneralsolutionofthisre urren erelationisredu edtotheform,
L
i
(r
1
, . . . , r
s−2
) =
N (N −1)/2
X
k=1
M
ik
(r
1
, . . . , r
s−3
)η
k
r
s−2
,
(38)where
η
k
,k = 1, . . . , N (N − 1)/2
,aretherootsofthenew hara teristi equationdet Υ(η) = 0,
(39)Υ
ij
(η) = (η/ξ
j
)
i−1
− ξ
j
i−1
+ δ
1i
,
i, j = 1, . . . , N.
(40) Fromthe ollating pro edurewe anfindthenextre urren erelationsforfun tionsM
ij
et .Using thisalgorithm we anfind,in prin iple,the orrelationfun tionsofallorders.B. Appli ation ofthe algorithm
All results obtainedin this subse tionare orre tfor the additiveMarkov hain, but someof them arevalid for thenon-additive hainaswell.
Thefirstsimpleresultisthatthe orrelationfun tionsofalloddordersarezerofortheadditiveMarkov hainwith
¯
a = 1/2
.ThisresultsfromEq. (35):fun tionK
2m+1
(·)
isexpressedonlyin termofK
2m−1
(·)
andK
1
= 0
.The orrelationfun tion ofthese ondorder
K
2
(·)
(the binary orrelationfun tion) foranadditiveMarkov hain anbefoundfrom Eq.(32):K
2
(r) =
N
X
j=1
L
j
ξ
j
r
,
r > −N,
(41)where
ξ
j
,j = 1, . . . , N
, are therootsof the hara teristi equation (37) .Coeffi ientsL
j
should beobtainedby the ollating:K
2
(0) = ¯
a(1 − ¯a);
K
2
(−r) = K
2
(r),
0 < r < N.
(42)Paper[21℄ ontainsananalysisofthisequationsinthe aseoftheadditiveMarkov hainwiththestep-wisememory fun tion.Belowwe presenttheresultsof al ulationforthe orrelationfun tion ofaweakly orrelated hain,
|P (a
i
= 1|a
i−N
. . . a
i−1
) − ¯a| ≪ 1.
(43)This aseisveryimportantfromthephysi alpointofviewbe ausethestatisti alpropertiesoftheequilibrium long-range orrelatedIsing hains anberepresentedand onsideredastheMarkov hains.Spe ifi ally,theMarkov hain withthesmallmemoryfun tionisstatisti allyequivalent totheweakly orrelatedIsing hain(seeRefs.[22, 23℄).
Forthe orrelationfun tion ofevenorderof theunbiased (
a = 1/2
¯
)additive hainwehaveK
2
(r) ≈
1
4
F (r),
0 < r < N,
K(0) =
1
4
,
(44)K
2s
(r
1
, . . . , r
2s−1
) =
s
Y
j=1
K
2
(r
2j−1
),
r
j
> 0, j = 1, . . . , 2s − 1.
(45)Thelatter equation is orre t forthe non-additivesequen e aswell. Inthe ase ofone-step Markov hain,
N = 1
, thisequationis exa t.ButifN > 1
oneshould interpretitastheasymptoti alequality.AtN = 2
,theexa t result forthe orrelationfun tionK
4
(·)
oftheadditive hainis,K
4
(r
1
, r
2
, r
3
) = K
2
(r
1
)K
2
(r
3
) + (−ξ
1
ξ
2
)
r
2
1
4
K
2
(r
1
+ r
3
) − K
2
(r
1
)K
2
(r
3
)
.
(46)Here
ξ
1
andξ
2
aretherootsofthe hara teristi equation,ξ
2
− F (1)ξ − F (2) = 0.
(47)Andfinally,Eq.(32)allowsustoexpressthememoryfun tionintermsthepres ribed orrelationfun tions
K
s
.In Ref. [26℄,themethodof onstru tingthe orrelatedbinarysequen e withpres ribedbinary orrelationfun tionK
2
wasearlierdis ussed.C. Generalized algorithm offindingthe orrelationfun tions
Herewe generalizethealgorithmproposedin Subse .IIIAfortheadditiveMarkov hainsto thearbitrarybinary multi-stepMarkov hains.
The onditionalprobabilityfun tionofthe
N
-stepbinaryMarkov hain anbewrittenasP (a
i
= 1|a
i−N
. . . a
i−1
) =
X
lj =0,1
j=1,...,N
F (l
1
, l
2
, . . . , l
N
)
N
Y
r=1
(a
i−r
− ¯a)
l
r
.
(48)It is a general form for the arbitrary binary fun tion, be ause
P (·|·)
an be thought of a linear fun tion of ea h argumenta
j
.Werefertofun tionF (l
1
, l
2
, . . . , l
N
)
asthegeneralized memoryfun tion.Equation(48) anbeapplied totheadditiveMarkov haindes ribedbyEq.(30),namely,
F (0, 0, . . . , 0) = ¯
a,
F (0, . . . , 0
| {z }
r−1
, 1, 0, . . . , 0
| {z }
N −r
) = F (r),
r = 1, 2, . . . , N,
(49)F (l
1
, l
2
, . . . , l
N
) = 0,
l
1
+ l
2
+ . . . + l
N
> 1.
Nowweobtainthere urren erelationforthe orrelationfun tionwiththe oeffi ientsexpressedviathegeneralized memoryfun tion.a ordingtothepro edureperformedinSubse tionIIIA,wesubstitutethelastsymbol
a
r
1
+...+r
s−1
in Eq.(9) (forr
j
> 0
,j = 1, . . . , s − 1
)for its onditionalprobabilityP (·|·)
in theform ofEq. (48).Asaresultone gets,K
s
(r
1
, . . . , r
s−1
) = (F (0, 0, . . . , 0) − ¯a)K
s−1
(r
1
, . . . , r
s−2
)+
(50)+
X
l
j
=0,1
j=1,...,N
F (l
1
, l
2
, . . . , l
N
)K
s+k−1
(r
1
, . . . , r
s−2
, r
s−1
− ρ
k
, ρ
k
− ρ
k−1
, . . . , ρ
2
− ρ
1
),
where
k = l
1
+ . . . + l
N
6= 0
.Thein reasingnumbersρ
j
,j = 1, . . . , k
aretheindexes,forwhi hl
ρ
j
6= 0
.Note that somesummands in Eq. (50) an have non-positivearguments if
r
s−1
6
N
. For this ase, one should applythe ollating pro eduretothisequation.Thus,thealgorithmforfindingofthe orrelationfun tions anbeformulatedasfollows:
1.To obtain the orrelation fun tion
K
s
(r
1
, r
2
, . . . , r
s−1
)
atr
i
> 0
,i = 1, 2, . . . , s − 1
, we should use Eq. (50) and exe ute the ollating pro edure.We find that fun tionK
s
(r
1
, . . . , r
s−1
)
is expressed viathe orrelation fun tions withthesumoftheirargumentslessthaninitial sumr
1
+ . . . + r
s−1
.2.Using Eq. (50) and performing the ollating pro edure
m
times with respe t to the obtained orrelation fun tions,wederivearelationbetweenfun tionK
s
(r
1
, . . . , r
s−1
)
andsomeother orrelationfun tions.(a) If all of them have the order less than
s
, we obtainthe re urren e relation for the orrelation fun tion ofthes
th order.This relation anbesolved bythemethodof hara teristi equationswithoutexe uting item3.(Asimilar asetakespla efortheadditiveMarkov hain.)(b) In the opposite ase, for
m > r
1
+ r
2
+ . . . + r
s−1
− N
, fun tionK
s
(r
1
, . . . , r
s−1
)
is expressed via the orrelation fun tions with the sums of their arguments less thanN
. Some of these fun tions are of the ordergreaterthans
.Thenwe shouldgotothenextitemofthealgorithm.3.All orrelationfun tionswiththesumofargumentslessthan
N
shouldbefoundfromasetoflinearequations. To thisendwe writeEq.(50)foreverysu h orrelationfun tion.Afterexe utingthe ollating pro edurewe obtainthesetof2
N −1
− 1
linearequationsfor
2
N −1
− 1
sought valuesofthe orrelationfun tions. Insomeparti ular ases,itis onvenientto define
K
s
(·)
in Eq.(9) andP (·|·)
inEq. (48)usinganarbitraryfixed value˜
a
(forexample,a = 1/2
˜
)insteadoftheaverage¯
a
.Inthisin ident everyreasoningremainvalidprovidedthat thevalueof¯
a
is hanged to˜
a
in Eqs.(50)and(35),andK
1
= 0
is hanged toK
1
= ˜
a − ¯a
. Toobtainaverage¯
a
we should addEq.(50),written forK
1
, totheset ofequationsin item3ofthealgorithm.Then wearriveat theset of2
N −1
linearequationsand2
N −1
− 1
sought values ofthe orrelation fun tionsand one ofthe averagea
¯
. Besides, one anuse˜
a
insteadof¯
a
in thedifferentphysi alproblems,whi hare relevanttotheMarkov hain. Forinstan e, theenergyin theIsingmodelismore onvenientto expressintermsorfun tionK
2
(r) = (a
i
− 1/2)(a
i+r
− 1/2)
.IV. CONCLUSION
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N
-wordso urring anbeeasilyfound.The orrelationfun tions ofdifferentorders an beexpressedviatheseprobabilities.Theexamplesofthese hainsis thepermutative Markov sequen es. The se ond approa h allows one to find the orrelation fun tions dire tly from the re urren erelations onne tingthem with thememoryfun tion.Inthe general ase,these relations ontain the orrelationfun tions of differentordersand,hen e,theyarediffi ulttosolve.Inthe aseofadditive hains,thisrelationsaresimplifiedand theirusehelpstofindthesolutions.[1℄ U.Balu ani,M. H.Lee,V.Tognetti,Phys.Rep.373,409(2003). [2℄ I.M.Sokolov,Phys.Rev.Lett.90,080601(2003).
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