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Global periodicity conditions for maps and recurrences via Normal Forms

Abstract

We face the problem of characterizing the periodic cases in parametric families of (real or complex) rational diffeomorphisms having a fixed point. Our approach relies on the Normal Form Theory, to obtain necessary conditions for the existence of a formal linearization of the map, and on the introduction of a suitable rational parametrization of the parameters of the family. Using these tools we can find a finite set of values p for which the map can be p-periodic, reducing the problem of finding the parameters for which the periodic cases appear to simple computations. We apply our results to several two and three dimensional classes of polynomial or rational maps. In particular we find the global periodic cases for several Lyness type recurrences

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Global periodicity conditions for maps and recurrences via Normal Forms

Author: Cima Mollet, Anna,Gasull Embid, Armengol,Mañosa Fernández, Víctor
Year: 2012
Source: https://upcommons.upc.edu/bitstream/2117/15947/1/1205.0923v1.pdf
a Xi :1205.0923 1 [ma h.DS] 4 May 2012
Global pe iodici y condi ions o maps and ecu ences
ia No mal Fo ms
Anna Cima(1), A mengol Gasull(1) and V´ıc o Ma˜nosa (2)
(1) Dep . de Ma em`a iques, Facul a de Ci`encies,
Uni e si a Au `onoma de Ba celona,
08193 Bella e a, Ba celona, Spain
[email p o ec ed]b.ca , ga[email p o ec ed]
(2) Dep . de Ma em`a ica Aplicada III (MA3),
Con ol, Dynamics and Applica ions G oup (CoDALab)
Uni e si a Poli `ecnica de Ca alunya (UPC)
Colom 1, 08222 Te assa, Spain
ic o [email protected]
May 7, 2012
Abs ac
We ace he p oblem o cha ac e izing he pe iodic cases in pa ame ic amilies o
a ional di eomo phisms o Kk, whe e Kis Ro C, ha ing a ixed poin . Ou app oach
elies on he No mal Fo m Theo y, o ob ain necessa y condi ions o he exis ence
o a o mal linea iza ion o he map, and on he in oduc ion o a sui able a ional
pa ame iza ion o he pa ame e s o he amily. Using hese ools we can ind a ini e
se o alues p o which he map can be p-pe iodic, educing he p oblem o inding he
pa ame e s o which he pe iodic cases appea o simple compu a ions. We apply ou
esul s o se e al wo and h ee dimensional classes o polynomial o a ional maps. In
pa icula we ind he global pe iodic cases o se e al Lyness ype ecu ences.
2000 Ma hema ics Subjec Classi ica ion: 37G05, 39A11, 39A20, 37C05
Keywo ds: Pe iodic maps; Linea iza ion; No mal Fo ms; Ra ional pa ame iza ions; Glob-
ally pe iodic ecu ences; Lyness ecu ences.
1
1 In oduc ion
A map Fsuch ha Fp(x)≡x, o some p∈Nand o all x o which Fpis well de ined,
will be called a pe iodic map. I pis he smalles posi i e in ege wi h his p ope y, hen
Fis called p-pe iodic. In his pape we ea he p oblem o cha ac e izing he p-pe iodic
cases in pa ame ic amilies o a ional maps o Kk, whe e Kis Ro C, ha ing a ixed poin .
When Fis a p-pe iodic di e en iable map ha ing a ixed poin , x0, i is well-known ha
(DF (x0))p= Id. In ac his is a simple consequence o he chain ule. As we will see in
P oposi ion 10, m=pis he smalles posi i e in ege numbe such ha (DF(x0))m= Id.
This simple esul allows o ea in a easy way he pe iodici y p oblem when a alue p
such ha (DF(x0))p= Id is known. Fo ins ance i Fhas a ixed poin x0such ha
(DF (x0))2= Id hen i Fis p-pe iodic hen pmus be 2,and no p= 2m, m ∈Nas we
could hink in p inciple, and hen we simply ha e o check whe he F2= Id o no .
In gene al, gi en a pa ame ic amily o maps Fa,a∈Km, he mos di icul p oblem
o inding he pe iodic maps is o de e mine which a e he possible alues psuch ha he e
exis s some asuch ha Fais p-pe iodic. The ools ha we will in oduce in his pape
will allow o ind a ini e se o possible alues o p o which he map can be p-pe iodic,
con e ing he p oblem o inding hese alues o ain o a compu a ional p oblem.
P oposi ion 10 as well as ou app oach o he cha ac e iza ion o p-pe iodic maps ia
No mal Fo m Theo y a e based on he Mon gome y-Bochne Theo em, see [23]. I will be
ecalled and p o ed in Sec ion 2. In a ew wo ds i says ha any p-pe iodic, C1-map wi h
a ixed poin is locally conjuga ed wi h he linea map L(x) = DF(x0)x, and so locally
linea izable. No ice ha he di e en iabili y condi ion is necessa y since i is well known
ha he e a e pe iodic in olu ions (i.e. F2= Id) gi en by homemo phisms wi h ixed poin s
which a e no linea izable, see [8].
Hence any p-pe iodic case in a gi en amily wi h ixed poin s can be locally linea ized.
Thus, he applica ion o a sui able No mal Fo m algo i hm, will gi e necessa y condi ions
o he exis ence o he linea iza ion. As we will see, hese condi ions a e some imes also
su icien .
We ema k ha his app oach does no co e he p oblem in i s ull gene ali y, because
he e a e pe iodic di eomo phisms wi hou ixed poin s in Rkwi h k≥7, see [18, 20].
I is well-known ha he No mal Fo m algo i hms o en lead o e y complica ed ex-
p essions which a e di icul o handle when dealing wi h he gi en pa ame e s o he map.
Some imes, hese obs uc ions can be signi ica i ely so ened by in oducing new pa ame-
e s a ionally depending on he old ones, and such ha he coo dina es o he ixed poin s
as well as he eigen alues o he jacobian ma ix a hese ixed poin s, depend a ionally
on hese new pa ame e s. This is he second main cha ac e is ic o ou app oach, when
2
dealing wi h conc e e applica ions.
The No mal Fo m Theo y is b ie ly ecalled in Sec ion 3. In Sec ion 4 we ob ain some
esul s o plana maps in he case ha he linea pa o Fa he ixed poin is gi en by a
ma ix diag(α, β) wi h αβ = 1, o diag(α, 1). As i s applica ions o he me hod, we ge :
Theo em 1. Conside a smoo h complex map o he o m
F(x, y) = 
αx +X
i+j≥2
i,jxiyj,1
αy+X
i+j≥2
gi,jxiyj
,(1)
whe e αis a p imi i e p- oo o uni y, p≥5. Then he condi ions P1(F) = P2(F) =
P3(F) = 0 a e necessa y o F o be p-pe iodic, whe e
P1(F) := ( 2,1+ 1,1g1,1)α4− 1,1(2 2,0−g1,1)α3+ (2g2,0 0,2− 1,1 2,0+ 1,1g1,1)α2
−( 2,1+ 1,1 2,0)α+ 1,1 2,0,
P2(F) :=g0,2g1,1α4−(g1,2+g0,2g1,1)α3+ ( 1,1g1,1+ 2g2,0 0,2−g0,2g1,1)α2
+g1,1(−2g0,2+ 1,1)α+ 1,1g1,1+g1,2,
and P3(F)is gi en in Appendix A.
In ac , condi ions P1(F) = 0 and P2(F) = 0 also wo k o p= 4.
Theo em 2. Conside a smoo h complex map o he o m
F(x, y) = 
αx +X
i+j≥2
i,jxiyj, y +X
i+j≥2
gi,jxiyj
,(2)
whe e αis a p imi i e p- oo o uni y. Then he ollowing a e necessa y condi ions o F
o be p-pe iodic:
P1(F) := 1,1= 0,
P2(F) :=g0,2= 0,
P3(F) := 1,2α−2 2,0 0,2+ 2 0,2g1,1− 1,2= 0,
P4(F) :=g0,3α−g0,3− 0,2g1,1= 0,
P5(F) := 1,3α2+ (−2 2,0 0,3+ 3 0,3g1,1+ 2g1,2 0,2−2 2,1 0,2−2 1,3)α+ 1,3+ 2 2,0 0,3
+ 2 2,1 0,2−4g2,0 2
0,2−2g1,2 0,2−3 0,3g1,1= 0,
P6(F) :=g0,4α2−( 0,3g1,1+ 2g0,4+g1,2 0,2)α+g2,0 2
0,2+ 0,3g1,1+g0,4+g1,2 0,2= 0.
In his las case, and in con as wi h he one ea ed in Theo em 1, i is no di icul
o ob ain addi ional pe iodici y condi ions. Two mo e pe iodici y condi ions a e gi en in
Appendix B.
3
The abo e esul s a e applied in se e al con ex s. The i s applica ion is o polynomial
maps. Pe iodic polynomial maps a e no o ious examples o in e ible polynomial ones,
which, in u n, a e he ocus o many deep open p oblems like he Jacobian conjec u e,
o he linea iza ion conjec u e. This second conjec u e says ha i F:Cn→Cnis a p-
pe iodic polynomial map, hen he e exis s a polynomial au omo phism ϕ(i.e. an in e ible
polynomial map wi h polynomial in e se) such ha ϕ◦F◦ϕ−1is a linea map. This
conjec u e is ue o n= 2 and as a as we know i is open o n≥3, see [15, Chaps. 8
and 9] and [21].
In Sec ion 5 we cha ac e ize he p-pe iodic maps in a amily o iangula maps, see
Theo em 15, and we gi e a simple and sel -con ained p oo o he linea iza ion conjec u e
o his case. As an applica ion o his esul and Theo em 1 we p o e:
P oposi ion 3. Conside a complex polynomial map
F(x, y) = 
αx +
3
X
i+j=2
i,jxiyj, y/α +
3
X
i+j=2
gi,jxiyj
,(3)
The map is p-pe iodic i and only i αis a p imi i e p- oo o he uni y, and i holds one o
he ollowing condi ions
(i) p= 1 and F(x, y) = (x, y);
(ii) p= 2,4and F(x, y) = (αx + 0,2y2, y/α)o F(x, y) = (αx, y/α +g2,0x2);
(iii) p= 3, and F(x, y) = (αx + 0,3y3, y/α)o F(x, y) = (αx, y/α +g3,0x3);
(i ) p≥5and F(x, y) = (αx+ 0,2y2+ 0,3y3, y/α)o F(x, y) = (αx, y/α+g2,0x2+g3,0x3).
Simila ly, as an applica ion o Theo em 2, we p o e:
P oposi ion 4. The only p-pe iodic cases in he amily o complex maps
F(x, y) = αx +bx2+cxy +dy2
1 + m(x2+y2),y+ x2+sxy + y2
1 + m(x2+y2),
a e, ei he F(x, y) = (x, y)when α= 1, o he ones gi en he polynomial maps F(x, y) =
(αx +dy2, y)o F(x, y) = (αx, y + x2)when αa p imi i e p- oo o he uni y wi h p > 1
and dand a bi a y complex numbe s.
In all he es o examples, gi en in Sec ions 6 and 7, he maps a e he ones associa ed
o some ecu ences. Recall ha gi en a ecu ence, au onomous o no , i is said ha
i is globally p-pe iodic i o all ini ial condi ions o which he sequence is well-de ined i
gi es ise o a p-pe iodic sequence and pis he smalles posi i e in ege numbe wi h his
4
p ope y. We will ace his ques ion s udying an associa ed map F. Wi h his poin o iew,
he ecu ence will be globally pe iodic i and only i he map Fis pe iodic.
The s udy o he global pe iodici y in di e ence equa ions is nowadays he subjec o
an ac i e esea ch, see o ins ance [1, 2, 4, 5, 6, 7, 9, 10, 11, 12, 13, 16, 22, 25, 26], and
e e ences he ein and se e al echniques ha e been used o app oach he p oblem. To he
bes o ou knowledge, his is he i s ime ha he No mal Fo m Theo y is used in his
se ing. As a second applica ion o Theo em 1, we classi y he globally pe iodic second
o de Lyness ecu ences, eob aining he esul s in [13] o his case:
P oposi ion 5. The only globally pe iodic Lyness ecu ences xn+2 =a+xn+1
xn
wi h a∈C,
a e he 5-pe iodic case wi h a= 1; and he 6-pe iodic case wi h a= 0.
Also as a di ec consequence o Theo em 1 we ge nex esul o some Gumo ski-Mi a-
ype ecu ences [17],
P oposi ion 6. The e a e no globally pe iodic cases in he amily o Gumo ski-Mi a ecu -
ences
xn+2 =−xn+xn+1
b+x2
n+1
, b ∈C.
One o he main applica ions in his se ing conce ns he 2-pe iodic Lyness ecu ence
xn+2 =an+xn+1
xn
,whe e an=(a o n= 2ℓ+ 1,
b o n= 2ℓ, (4)
and a, b ∈C. In Sec ion 6.3 we sol e he global pe iodici y p oblem o i by s udying he
amily o maps
Fb,a(x, y) = a+y
x,a+bx +y
xy ,
which as we will see desc ibes he beha io o (4).
Theo em 7. The only globally pe iodic ecu ences in (4) a e:
(i) The cases a=b= 0 (6-pe iodic) and a=b= 1 (5-pe iodic).
(ii) The cases a= (−1±i√3)/2and b=a= 1/a,10-pe iodic.
No ice ha he cases gi en in (i) co espond o he well-known au onomous globally
pe iodic Lyness ecu ences also appea ing in P oposi ion 5.
Finally, o show an applica ion in K3we ind he globally pe iodic hi d o de Lyness
ecu ences, eob aining again he esul in [13]:
P oposi ion 8. The only globally pe iodic hi d-o de Lyness ecu ence
xn+3 =a+xn+1 +xn+2
xn
, a ∈C,
co esponds o a= 1 and is 8-pe iodic.
5

2 Some consequences o he Mon gome y-Bochne Theo em
The nex e sion o Mon gome y-Bochne Theo em is a simpli ied one, adap ed o ou
in e es s. The gene al one applies in a much mo e gene al con ex , see [23].
Theo em 9 (Mon gome y-Bochne ). Le F:U → U be a p-pe iodic C1-di eomo -
phism, whe e Uis an open se o Kk. Le x0∈ U be a ixed poin o F. Then, he e exis s a
neighbou hood o x0whe e Fis conjuga ed wi h he linea map L(x) = DF(x0)x. Mo eo e
he linea iza ion is gi en by he local di eomo phism
ψ(x) = 1
p
p−1
X
i=0
(DF (x0))−iFi(x).
P oo . Since Fis p-pe iodic (DF(x0))p= Id. So (de (DF(x0))p= 1 and DF(x0) is in-
e ible. Conside ψas in he s a emen . By he in e se unc ion heo em i is clea ha
he map ψis a local di eomophism because Dψ(x0) = Id. Mo eo e , using again he
p-pe iodici y o Fwe ge ha ψ(F(x)) = L(ψ(x)), as we wan ed o p o e.
As we ha e seen in he p oo o he abo e heo em, i Fis a p-pe iodic di e en iable
map wi h a ixed poin x0, hen (DF(x0))p= Id. Nex esul ela es pwi h he minimum
posi i e msuch ha (DF(x0))m= Id.
P oposi ion 10. Le Fbe a di e en iable map ha ing a ixed poin x0. Assume ha Fis
p-pe iodic and le mbe he minimum posi i e msuch ha (DF(x0))m= Id. Then p=m.
P oo . By using he Mon gome y-Bochne Theo em we know ha Fis C1-conjuga ed o
L(x) = DF(x0)xin a neighbo hood o x0. Thus F=ψ−1◦L◦ψ, o some C1di eomo phism
ψ. Since Lm= Id i and only i Fm=ψ−1◦Lm◦ψ=ψ−1◦ψ= Id, he esul ollows.
Co olla y 11. Le Fa(x) = Lx+G(x,a),wi h x∈ U ⊂ Knand a∈Km,a smoo h amily
o maps such ha G(0,a)≡DxG(0,a)≡0 o all a∈Km. Assume ha pis he minimum
posi i e in ege numbe such ha Lp= Id. Then i Fais pe iodic o some a∈K hen i is
p-pe iodic, i.e. Fp
a= Id .
In pa icula no e ha i L= Id hen he only pe iodic case is Fa(x) = xand when
L2= Id he pe iodici y condi ions a e gi en by Fa(Fa(x)) ≡x.Fo example he ac p o ed
in [25, Ex. 2], ha he only pe iodic map o he o m F(x1, x2) = (x2+ax2
1, x1+bx1x2)
co esponds o he linea case a=b= 0, ollows easily using his app oach.
No ice ha using Mon gome y-Bochne Theo em a necessa y condi ion o a map o he
o m Fa(x) = Lx+G(x,a), o be pe iodic is ha Fais linea izable in a neighbou hood
o 0. The linea izable cases can be de ec ed by ollowing he well-know No mal Fo m
Theo y, which, as a as we know, has no been used o his pu pose. Some esul s use ul
o applying i will be ecalled in he nex sec ion.
6
3 Pe iodici y condi ions ia No mal Fo m Theo y
We s a in oducing some well-known issues o No mal Fo m Theo y, while e e ing he
eade o [3, Sec. 2.5], o u he de ails.
Le F:= F(1) :Kk→Kk, be a amily o smoo h maps depending on some pa ame e s
and sa is ying F(1)(0) = 0.Le
F(1)(x) = F(1)
1(x) + F(1)
2(x) + ···+F(1)
k(x) + O(|x|k+1) (5)
be he Taylo expansion o Fa 0,whe e F(1)
∈ H , he eal ec o space o maps whose
componen s a e homogeneous polynomials o deg ee .
The aim o he No mal Fo m Theo y is o cons uc a sequence o ans o ma ions Φn,
s a ing om n= 2, such ha a each s ep, Φnsimpli ies, as much as possible, he e ms o
he co esponding homogeneous pa o deg ee n. To his end, le F(1)
1(x) = DF(1)(0)x=:
Lxand suppose ha
F(n−1)(x) = Lx+F(n−1)
n(x) + O(|x|n+1), n ≥2.
Conside a ans o ma ion
x= Φn(y) := y+φn(y),
wi h φn∈ Hn,such ha i conjuga es he map F(n−1) wi h a new map F(n), ia he
conjuga ion
F(n−1)(Φn) = Φn(F(n)).
F om he abo e equa ion, i can be easily seen ha
F(n)(y) = Ly+L φn(y)−φn(Ly) + F(n−1)
n(y) + O(|y|n+1).
Clea ly, i φn(y) can be chosen in such a way ha
ML(φn(y)) := L φn(y)−φn(Ly) = −F(n−1)
n(y),(6)
hen F(n−1) is ans o med in o
F(n)(y) = Ly+F(n)
n+1(y) + O(|y|n+2) = Ly+O(|y|n+1).
The ec o ial equa ion (6) is he well-known homological equa ion associa ed wi h L=
DF(1)(0), and he exis ence o solu ions o i is he necessa y and su icien condi ion o be
able o emo e he homogeneous e ms o deg ee n.
F om now, one we will assume ha he linea map is diagonalizable, and so ha i is
L= diag(λi)k
i=1. In his case, he linea ope a o ML:= Hn→ Hn,gi en in (6), has he
7
eigen ec o s xmei, i = 1,2,...,k, wi h m= (m1, m2,...,mk)∈ Mk
n:= {m∈Nksa is ying
Pk
i=1 mi=n};xm=xm1
1xm2
2···xmk
nwhe e x= (x1, x2,...,xk)∈Kk; and whe e eiis he
i- h membe o he na u al basis o Kk.Hence
ML(xmei) = (λi−λm)xmei,(7)
whe e λm=λm1
1λm2
2···λmk
n.
Se
F(n−1)
n(x) = X
m
(n−1)
1;mxm,X
m
(n−1)
2;mxm,...,X
m
(n−1)
k;mxm!,
and
φn(x) = X
m
a1;mxm,X
m
a2;mxm,...,X
m
ak;mxm!,
whe e m∈ Mk
n.
When λi−λm6= 0 o all he sui able alues o m∈Nkand o all i= 1,2,...,k,
i is said ha he e a e no esonances. In his case he ope a o MLis in e ible, he
homological equa ion always has solu ion and so he linea iza ion p ocess can con inue. On
he con a y, i λi−λm= 0 o some m∈ Mk
nand some i∈ {1,2,...,k}, hen he ec o
λ= (λ1, λ1,...,λk) is said o be esonan o o de n. In his case, by simple inspec ion
o he homological equa ion, and using (7), we ob ain ha he he n h o de obs uc ion
equa ion associa ed o he esonance is gi en by
(λi−λm)ai;m=− (n−1)
i;m.
Howe e , he e a e some maps ha ing his esonance o which he p ocess can con inue.
This happens i he igh -hand side o his scala equa ions anish, namely (n−1)
i;m= 0, and
hese cases a e he ones candida e o be linea ized. Hence, we ha e ob ained he ollowing
esul
P oposi ion 12. I L:= diag(λi)k
i=1, hen a necessa y condi ion o he map (5) o be
pe iodic is gi en by he n h o de pe iodici y condi ion associa ed o he esonance condi ion,
λi−λm= 0, gi en by (n−1)
i;m= 0.
Rema k 13. No ice ha p-pe iodic maps wi h Ldiagonal a e such ha λp
i= 1, o all i.
The e o e o hese maps many esonances λi−λm= 0 appea .
By ollowing he No mal Fo m Algo i hm, i is s aigh o wa d (and well known) o
see ha he nume a o o (n−1)
i;mis a polynomial in he coe icien s o F(1). Thus, o each
pa icula case, he abo e equa ions gi e pe iodici y condi ions, which a e algeb aic in e ms
o he ini ial pa ame e s o he map, once exp essed in o m (5).
8
To ix he ideas we gi e a simple example. Suppose ha k= 2. Assume ha L=
diag(α, β). Se Φ2(y) := y+φ2(y), whe e
φ2(x, y) := a20x2+a11xy +a02y2
b20x2+b11xy +b02y2!.
Conside he map F(1)(x) = Lx+F(1)
2(x) + O(|y|3) wi h
F(1)
2(x, y) = 20x2+ 11xy + 02y2
g20x2+g11xy +g02y2!,
whe e o simpli y he no a ion, and om now on, i he e is no possibili y o con usion, we
will d op he supe sc ip (1) o he coe icien s o F(1).
The homological equa ion a o de 2 is L φ2(y)−φ2(Ly) = −F(1)
2(y), and gi es he
ollowing six scala equa ions:







(α−α2)a20 =− 20,(β−α2)b20 =−g20,
(α−αβ)a11 =− 11,(β−αβ)b11 =−g11,
(α−β2)a02 =− 02,(β−β2)b02 =−g02.
I no one o he six 2nd o de esonance condi ions:α2−α, αβ −α, β2−α, β2−β, αβ −β,
and α2−β, anish, he e is no obs uc ion o emo e he second o de e ms o F(1) using
he conjuga ion Φ2.
Suppose now, ha he map F(1) is such ha he esonance β−α2= 0 occu s. Then
he scala equa ion (β−α2)b20 =−g20 is an obs uc ion equa ion. Bu his obs uc ion o
he linea iza ion p ocess disappea s i g20 anishes. In summa y, i β=α2, hen g20 = 0 is
ape iodici y condi ion.
4 P oo o Theo ems 1 and 2
We keep he no a ion in oduced in he abo e sec ion, i.e., F(k)is he map ob ained a e
k−1 s eps o he no mal o m p ocedu e, F(k)(x) = Lx+F(k)
k+1(x) + O(|x|k+2),and i s
coe icien s a e (k)
i,j and g(k)
i,j . Fi s conside he case ea ed in Theo em 1:
F(k)(x, y) = 
αx +X
i+j≥k+1
(k)
i,j xiyj,1
αy+X
i+j≥k+1
g(k)
i,j xiyj
.
I is easy o check ha he scala equa ions associa ed o equa ion (6) a e
(α(1 −αn−2i−1)an−i,i =− (n−1)
n−i,i ,
α−1(1 −αn−2i+1)bn−i,i =−g(n−1)
n−i,i ,
9
We conside sepa a ely he case b= 0.In his si ua ion x0:= (√2/2,√2/2) is a ixed
poin o G0. I is easy o see ha (DG0(x0)p6= Id, o any posi i e in ege p, because he
ma ix is no diagonalizable. So G0is no a pe iodic map.
When b6= 0 we in oduce a new pa ame e λ, and w i e b=λ/(1 + λ2) wi h λ2+ 1 6= 0
and λ6= 0.No ice ha his pa ame iza ion co e s all alues o bin C {0}. We ename he
new map co esponding o Gbas gλ. The eigen alues o i s Jacobian ma ix a he o igin,
which is always a ixed poin , a e λand 1/λ. The linea map Ψ(x, y) = (x−λy, x −y/λ)
is a conjuga ion be ween Dgλ(0) and i s diagonal o m L(x, y) := (λx, y/λ). Using his
conjuga ion we conside he map Fλ:= Ψ ◦gλ◦Ψ−1. Using Theo em 1 we impose ha
P2(Fλ) = 0. We ge ha a necessa y condi ion o Fλ o be pe iodic is
λ2+ 12λ2+λ+ 1= 0.
I λis a oo o λ2+λ+1, hen i is a p imi i e 3 d- oo o he uni y. Then by Co olla y 11,
Fλshould be globally 3-pe iodic. Bu we ha e al eady disca ded his possibili y. So he
esul ollows.
6.3 Global pe iodici y in he 2-pe iodic non-au onomous Lyness ecu -
ence
In his sec ion we s udy he p oblem o he global pe iodici y o he he sequence gene a ed
by he 2-pe iodic Lyness ecu ence (4). The sequence {xn}gi en by his ecu ence can
be eob ained as
(x1, x2)Ga
−−→ (x2, x3)Gb
−→ (x3, x4)Ga
−−→ (x4, x5)Gb
−→ (x5, x6)Ga
−−→ ···
whe e Gα(x, y), wi h α∈ {a, b}, is he Lyness map gi en in (10). So he beha io o (4) is
gi en by he dynamical sys em gene a ed by he map:
Gb,a(x, y) := Gb◦Ga(x, y) = a+y
x,a+bx +y
xy .(12)
P oo o Theo em 7. As we ha e seen i su ices o s udy he pe odici y p oblem o he
map (12). I is easy o see ha Gp
a6= Id o p= 1,2,4. Mo eo e i is 3-pe iodic i and only
i a=b= 0. No ice ha his case co esponds o he globally 6-pe iodic ecu ence. We
con inue sea ching p-pe iodic maps wi h p≥5.
Following simila ideas ha in he p e ious subsec ions we in oduce a mo e sui able
a ional pa ame iza ion o aand b. We conside
a=B3λ2+ 1+λ2B3−1
B(λ+ 1)2,
b=−B+ (B2−a)2,wi h B(λ+ 1) 6= 0 and λ6= 0.
(13)
16

Using hese new pa ame e s we co e all he alues o aand bin C. Mo eo e he ixed
poin is (B, B2−a),whe e ais gi en in (13), and he eigen alues o Gb,a a his poin a e
λand 1/λ. A e a ansla ion (x, y)→(x−B, y −(B2−a)), which b ings he ixed poin
o he o igin, he map Gb,a conjuga es, using again xand yas a iables, wi h
gB,λ(x, y) = 

y−Bx
x+B,−B2(λ+ 1)2x−Bλ2+λ+ 1y+λ xy
B(λ+ 1)2y+λ(x+B)
,
wi h linea pa .
LB,λ(x, y) = −x+y
B,−B(λ+ 1)2x
λ+λ2+λ+ 1y
λ!.
The linea change o a iables Ψ(x, y) = x+y, (λ+ 1) Bx +1 + 1
λBygi es a conjuga-
ion be ween LB,λ and i s diagonal o m L(x, y) := (λx, y/λ). Using his conjuga ion we
conside he map
FB,λ(x, y) := Ψ ◦gB,λ(x, y)◦Ψ−1(x, y),
which sa is ies DFB,λ(0,0) = diag (λ, 1/λ). Fo simplici y, we omi i s explici exp ession.
Recall ha λp−16= 0 o p= 1,2,3.
By Theo em 1, when p≥5, om bo h condi ions Pi(FB,λ) = 0, i = 1,2,we ob ain he
same pe iodici y condi ion C1(B, λ) = 0, whe e
C1(B, λ) := B6λ10 + 9B6λ9+ 35B6λ8+ 80B6λ7+ 124B6λ6+ 2B3λ9+ 142B6λ5+ 8B3λ8
+124B6λ4+ 18B3λ7+ 80B6λ3+ 32B3λ6+ 35B6λ2+ 40B3λ5+ 9B6λ
+32B3λ4+λ7+B6+ 18B3λ3+ 3λ6+ 8B3λ2+ 2λ5+ 2B3λ+ 3λ4+λ3.
Using again Theo em 1, we ob ain ano he polynomial es ic ion C2(B, λ) := P3(FB,λ) =
0. The exp ession o C2(B, λ) is gi en in Appendix C. To s udy he pe iodici y o FB,λ i
su ices o deal wi h he wo condi ions
C1(B, λ) = 0, C2(B, λ) = 0.
Compu ing R(λ) := Res(C1(B, λ), C2(B, λ); B) we ge
R(λ) = λ36 (λ−1)24 (λ+ 1)72 λ2+ 16λ2+λ+ 124 S6(λ)T6(λ),
whe e S(λ) = λ4+λ3+λ2+λ+ 1 and T(λ) = 3λ4+ 15λ3+ 20λ2+ 15λ+ 3. Then, a
necessa y condi ion o FB,λ o be p-pe iodic wi h p≥4 is ha λis a p imi i e p- h o he
uni y and ha ei he S(λ) = 0 o T(λ) = 0. Le us disca d he o me possibili y.
I u ns ou ha Thas wo eal oo s and wo complex oo s o modulus one. We ha e
o p o e ha hey a e no oo s o he uni y. This can be seen, o ins ance, p o ing ha T
17
is no di isible by any cyclo omic polynomial. This holds because i i had a cyclo omic
polynomial di iso , i s deg ee should be a mos 4. The cyclo omic polynomials o deg ee
a mos 4 co espond o p∈ {1,2,3,4,5,6,8,10,12}:= D4. This is because hese a e he
cases which co espond o cyclo omic polynomials o deg ee ϕ(p)≤4, being ϕ he Eule ’s
unc ion, see o ins ance [24]. Since
Res(T(λ), λp−1; λ)6= 0, o p∈ D4,
he esul ollows.
Finally, when S(λ) = 0 no ice ha λis a p imi i e 5- h oo o he uni y. So, by
Co olla y 11 i FB,λ is p-pe iodic i should be 5-pe iodic. The e o e i su ices o s udy
whe he F5
B,λ = Id o no , o equi alen ly whe he G5
b,a = Id. Compu ing he nume a o o
he i s componen o G5
b,a(x, y)−(x, y) we ge ha i w i es as a4b(1 −ab)x+O(2), whe e
as usual O(m) deno es e ms o deg ee a leas min xand y. Hence only h ee possibili ies
o Gb,a o be 5-pe iodic appea : ei he a= 0 o b= 0 o ab = 1.
The i s wo cases can easily disca ded. I holds ha G5
0,a 6= Id and G5
b,06= Id. On he
o he hand, when b= 1/a, a 6= 0 he nume a o o he i s componen o G5
1/a,a(x, y)−(x, y)
w i es as −a(a−1)2(a2+a+ 1)2x2y+O(3). Since his las unc ion has o anish we ge
h ee candida es o be 5-pe iodic: a= 1 and a= (−1±i√3)/2 wi h b= 1/a =a. I is easy
see ha all hem gi e ise o 5-pe iodic maps Gb,a. The las wo co espond o he globally
10-pe iodic ecu ence.
Rema k 17. The cha ac e iza ion o he globally pe iodic di e ence equa ions ea ed in
his sec ion can also be ob ained ollowing he app oach de eloped in [27] ha gi es all he
pe iodic QRT-maps. This esul also appea s in [14, p. 165] and [19].
7 The hi d o de Lyness ecu ence
We s a p o ing a gene al esul which will use ul o sol ing he pe iodici y p oblem o
he Lyness ecu ence.
P oposi ion 18. Conside he smoo h amily o maps
F(x, y, z) = αx +X
m
mxm, βy +X
m
gmxm, γz +X
m
hmxm!,
wi h m∈ {(i, j, k)such ha i+j+k≥2}, and whe e xm=xiyjzk. When α=±1,βγ = 1,
and β6= 1, γ 6= 1,some necessa y condi ions o i o be pe iodic a e
(2)
3,0,0= (2)
1,1,1=g(2)
2,1,0=g(2)
0,2,1=h(2)
2,0,1=h(2)
0,1,2= 0,
18
whe e (2)
i,j,k and g(2)
i,j,k a e he exp essions gi en in he second s ep o he no mal o m p oce-
du e desc ibed in Sec ion 3.
P oo . By inspec ion o he 3 d o de esonance condi ions, we obse e ha when α=±1
and βγ = 1 he e appea he esonances α3−α,αβγ −α,α2β−β,β2γ−β,α2γ−γand
β2γ−γwhich a e associa ed o he coe icien s (2)
3,0,0, (2)
1,1,1,g(2)
2,1,0,g(2)
0,2,1,h(2)
2,0,1and h(2)
0,2,1
espec i ely. So all hem mus anish o ha e a pe iodic map.
P oo o P oposi ion 8. The dynamics o he hi d-o de Lyness’ equa ion can be s udied
h ough he Lyness maps
Ga(x, y, z) = y, z, a+y+z
x.
I is easy o see ha Gp
a6= Id o p= 1,2. We con inue sea ching p-pe iodic maps wi h
p≥3.I has always some ixed poin (x0, x0, x0) wi h x2
0−2x0−a= 0 and x06= 0.
Mo eo e he eigen alues λo he Jacobian ma ix a his poin s a e gi en by he ze oes
o −(λ+ 1)(λ2−(1 + 1/x0)λ+ 1) = 0. These wo equa ions sugges us o in oduce he
a ional pa ame iza ion o aas
a=−λ2λ2−3λ+ 2
(λ2−λ+ 1)2,wi h λ2−λ+ 1 6= 0 and λ6= 0,
which co e s all alues o a∈C.Then he ixed poin is (x0, x0, x0) wi h x0=λ/(λ2−λ+1)
and he eigen alues o DGaa his poin a e −1, λ, 1/λ. No ice ha since p≥3, we can
assume λ6= 1. To apply P oposi ion 18 we pe o m he ansla ion (x, y, z)→(x−x0, y −
x0, z −x0), which b ings he ixed poin o he o igin, ob aining
gλ(x, y, z) := y, z, −λx +λ2−λ+ 1y+λ2−λ+ 1z
(λ2−λ+ 1) x+λ!,
wi h linea pa
Lλ(x, y) = y, z, −x+λ2−λ+ 1y
λ+λ2−λ+ 1z
λ!.
The linea change o a iables Ψ(x, y, z) = (x+y+λ2z, −x+λ y +λ z, x +λ2y+z)
gi es a conjuga ion be ween Lλand i s diagonal o m L(x, y, z) := (−x, λy, z/λ). Using he
conjuga ion Ψ, we inally ob ain a map wi h diagonal linea pa Fλ:= Ψ ◦gλ◦Ψ−1, which
is unde he assump ions o P oposi ion 18.
Applying his p oposi ion and he No mal Fo m Algo i hm o Fλwe can compu e g(2)
2,1,0.
F om he equa ion g(2)
2,1,0= 0 we ob ain ha
λ2−λ+ 13(λ4+ 1) = 0.
19
Thus λhas o be a p imi i e 8- h oo o he uni y. All hese alues o λco espond o he
same alue a= 1, which gi es a globally 8-pe iodic ecu ence. So he esul ollows
Acknowledgemen s
GSD-UAB and CoDALab G oups a e suppo ed by he Go e nmen o Ca alonia h ough
he SGR p og am. The i s and second au ho s a e also suppo ed by MCYT h ough
g an s MTM2008-03437 and he hi d au ho by he g an DPI2011-25822.
Appendix A. Exp ession o P3(F) when αβ = 1
Conside he map (1), applying he No mal Fo m Algo i hm one ge s ha he pe iodici y
condi ion associa ed o (4)
3,2is gi en by
P3(F) := 1,1g0,2g2
1,1α17 + (2g2
1,1 1,1g0,2− 3,1g0,2− 1,1g1,1g1,2− 1,1g0,2g2,1)α16
+ ( 3,2+ 3g2
1,1 1,1g0,2+ 3 1,1g0,2 3,0−3 1,1g0,2g2,1+ 2 1,1 2,0g0,2g1,1+ 2 2
1,1g0,2g2,0
−2 3,1g0,2+ 2 2,1 2,0g0,2+g2
1,1 1,2+ 2 2,2g1,1+ 1,1g2,2+ 2 0,2 1,1g1,1g2,0− 1,1g1,1g1,2
+g2
1,1 2
1,1)α15 + (3g2
1,1 1,1g0,2+ 6 1,1g0,2 3,0−6 0,2 3,0g1,1−4 1,2 2,0g1,1−3 1,1g1,1 2,1
+ 2 1,2g2,1−3 1,2 3,0+ 5g2
1,1 1,2+ 2g2
1,1 2
1,1+ 2 0,2 1,1g1,1g2,0−2 2,2 2,0−2 2
1,1g2,1
−3 3,1g0,2−2 1,1g2
0,2g2,0+ 3 1,1 2,0g0,2g1,1+ 4 2,1 2,0g0,2−3 0,2 1,1g3,0−2 1,2g0,2g2,0
+ 4 2,2g1,1+ 3,2+ 2g3
1,1 0,2+ 2 0,2g1,1g2,1−4 1,1 2
2,0g0,2−4 1,1g0,2g2,1+ 6 2
1,1g0,2g2,0
−3 1,1 3,1−2 1,1 2,0g1,2−2 1,1 1,2g2,0−4 4,0 0,2−2g2
1,1 0,2 2,0+ 2 1,1g2,2)α14
+ (4 1,1 2,0 2,1+ 4g2
1,1 1,1g0,2+ 11 1,1g0,2 3,0−12 0,2 3,0g1,1+ 6 2
1,1 2,0g1,1
−10 1,2 2,0g1,1−8 1,1g1,1 2,1+ 2 1,2g2,1−3 1,2 3,0+ 4 1,2 2
2,0+ 3 3
1,1g2,0+ 10g2
1,1 1,2
+g2
1,1 2
1,1+ 6 2
1,1 3,0−4 0,2 1,1g1,1g2,0−2 2,2 2,0−7 2
1,1g2,1+ 12 3,0 2,0 0,2
+ 4 0,2 2,0g0,2g2,0− 3,1g0,2−2 0,2g0,2g3,0−6 1,1g2
0,2g2,0+ 8 0,2 1,1 2,0g2,0+ 6 2,1 2,0g0,2
−6 0,2 1,1g3,0−4 1,2g0,2g2,0+ 6 2,2g1,1+ 3,2+ 6g3
1,1 0,2+ 3 1,1g0,3g2,0+ 6 0,2g1,1g2,1
+ 6 0,3g1,1g2,0−8 1,1 2
2,0g0,2−3 1,1g0,2g2,1+ 5 1,1g1,1g1,2+ 8 0,2 2
2,0g1,1+ 11 2
1,1g0,2g2,0
−5 1,1 3,1−5 1,1 2,0g1,2+ 3 1,3g2,0−8 1,1 1,2g2,0−4 4,0 0,2−12g2
1,1 0,2 2,0+ 2 0,2g3,1
−4 0,2 2,0g2,1+ 3 1,1g2,2)α13 + (6 1,1 2,0 2,1+ 9g2
1,1 1,1g0,2+ 7 1,1g0,2 3,0−24 0,2 3,0g1,1
+ 19 2
1,1 2,0g1,1−16 1,2 2,0g1,1−15 1,1g1,1 2,1+ 4 1,2g2,1−5 1,2 3,0−8 0,2 3
2,0+ 4 1,2 2
2,0
+ 12 3
1,1g2,0+ 15g2
1,1 1,2−5g2
1,1 2
1,1+ 12 2
1,1 3,0+ 3 0,3g3,0−33 0,2 1,1g1,1g2,0−2 2,2 2,0
−13 2
1,1g2,1+ 12 3,0 2,0 0,2+ 12 0,2 2,0g0,2g2,0+ 2 3,1g0,2−4 0,2g0,2g3,0−8 1,1g2
0,2g2,0
−6 0,2 2,1g2,0−8 1,1g2
0,2g2,0−6 0,2 2,1g2,0+ 26 0,2 1,1 2,0g2,0−14 1,1 2,0g0,2g1,1
+ 2 2,1 2,0g0,2−15 0,2 1,1g3,0−2 1,2g0,2g2,0−8 1,1g2
0,2g2,0−6 0,2 2,1g2,0+ 2 2,1 2,0g0,2
+ 26 0,2 1,1 2,0g2,0−14 1,1 2,0g0,2g1,1−15 0,2 1,1g3,0−2 1,2g0,2g2,0+ 2 2,2g1,1−2 3,2
+ 16g3
1,1 0,2+ 6 1,1g0,3g2,0+ 14 0,2g1,1g2,1+ 12 0,3g1,1g2,0−14 1,1 2
2,0g0,2+ 3 1,1g0,2g2,1
20
+ 9 1,1g1,1g1,2+ 20 0,2 2
2,0g1,1−6 2
1,1 2
2,0+ 10 2
1,1g0,2g2,0−7 1,1 3,1−9 1,1 2,0g1,2
+ 3 1,3g2,0−19 1,1 1,2g2,0−6 0,3 2,0g2,0−4 4,0 0,2−30g2
1,1 0,2 2,0+ 2 0,2g3,1
−8 0,2 2,0g2,1+ 4 0,2g0,2g1,1g2,0+ 1,1g2,2)α12 + (8 1,1 2,0 2,1+ 15g2
1,1 1,1g0,2
+ 2 1,1g0,2 3,0−18 0,2 3,0g1,1+ 40 2
1,1 2,0g1,1−12 1,2 2,0g1,1−15 1,1g1,1 2,1−2 1,2g2,1
+ 4 1,2 3,0−8 0,2 3
2,0+ 6 1,2 2
2,0+ 29 3
1,1g2,0+ 11g2
1,1 1,2−16g2
1,1 2
1,1+ 21 2
1,1 3,0
+ 3 0,3g3,0−74 0,2 1,1g1,1g2,0+ 4 2,2 2,0−16 2
1,1g2,1+ 16 3,0 2,0 0,2+ 12 0,2 2,0g0,2g2,0
+ 5 3,1g0,2−6 0,2g0,2g3,0−8 1,1g2
0,2g2,0−6 0,2 2,1g2,0+ 70 0,2 1,1 2,0g2,0
−35 1,1 2,0g0,2g1,1−4 2,1 2,0g0,2−19 0,2 1,1g3,0−4 2,2g1,1+ 4g1,2 0,2g2,0−3 3,2
+ 24g3
1,1 0,2+ 9 1,1g0,3g2,0+ 14 0,2g1,1g2,1+ 18 0,3g1,1g2,0−8 1,1 2
2,0g0,2+ 6 1,1g0,2g2,1
+ 10 1,1g1,1g1,2+ 40 0,2 2
2,0g1,1−10 2
1,1 2
2,0−3 2
1,1g0,2g2,0−8 1,1 2,0g1,2+ 3 1,3g2,0
−25 1,1 1,2g2,0−12 0,3 2,0g2,0+ 4 4,0 0,2−54g2
1,1 0,2 2,0+ 2 0,2g3,1−12 0,2 2,0g2,1
+ 10 0,2g0,2g1,1g2,0−2 1,1g2,2)α11 + (−2 1,1 2,0 2,1+ 22g2
1,1 1,1g0,2−9 1,1g0,2 3,0
−10 0,2 3,0g1,1+ 54 2
1,1 2,0g1,1+ 2 1,2 2,0g1,1−8 1,1g1,1 2,1−2 1,2g2,1+ 5 1,2 3,0
−12 0,2 3
2,0−6 1,2 2
2,0+ 46 3
1,1g2,0+ 4g2
1,1 1,2−25g2
1,1 2
1,1+ 13 2
1,1 3,0+ 3 0,3g3,0
−115 0,2 1,1g1,1g2,0+ 6 2,2 2,0−9 2
1,1g2,1−8 3,0 2,0 0,2+ 4 0,2 2,0g0,2g2,0+ 5 3,1g0,2
+ 2 0,2g0,2g3,0−6 0,2 2,1g2,0+ 98 0,2 1,1 2,0g2,0−52 1,1 2,0g0,2g1,1−10 2,1 2,0g0,2
−17 0,2 1,1g3,0+ 8 1,2g0,2g2,0−10 2,2g1,1+ 4g1,2 0,2g2,0−3 3,2+ 32g3
1,1 0,2
+ 6 1,1g0,3g2,0+ 12 0,2g1,1g2,1−8 2
0,2g2
2,0+ 15 0,3g1,1g2,0+ 9 1,1g0,2g2,1
+ 5 1,1g1,1g1,2+ 40 0,2 2
2,0g1,1−16 2
1,1 2
2,0−20 2
1,1g0,2g2,0+ 7 1,1 3,1−3 1,1 2,0g1,2
−3 1,3g2,0−19 1,1 1,2g2,0−12 0,3 2,0g2,0+ 8 4,0 0,2−62g2
1,1 0,2 2,0−2 0,2g3,1
−4 0,2 2,0g2,1+ 24 0,2g0,2g1,1g2,0−5 1,1g2,2)α10 + (−10 1,1 2,0 2,1+ 21g2
1,1 1,1g0,2
−11 1,1g0,2 3,0+ 14 0,2 3,0g1,1+ 53 2
1,1 2,0g1,1+ 16 1,2 2,0g1,1+ 5 1,1g1,1 2,1
−8 1,2g2,1+ 11 1,2 3,0+ 4 0,2 3
2,0−8 1,2 2
2,0+ 53 3
1,1g2,0−9g2
1,1 1,2−29g2
1,1 2
1,1
+ 2 2
1,1 3,0−6 0,3g3,0−130 0,2 1,1g1,1g2,0+ 6 2,2 2,0+ 2
1,1g2,1−16 3,0 2,0 0,2
−24 0,2 2,0g0,2g2,0+ 2 3,1g0,2+ 6 0,2g0,2g3,0+ 4 1,1g2
0,2g2,0+ 98 0,2 1,1 2,0g2,0
−56 1,1 2,0g0,2g1,1−10 2,1 2,0g0,2−3 0,2 1,1g3,0+ 4 1,2g0,2g2,0−10 2,2g1,1
+ 4g1,2 0,2g2,0+ 28g3
1,1 0,2−4 0,2g1,1g2,1−8 2
0,2g2
2,0+ 3 0,3g1,1g2,0+ 14 1,1 2
2,0g0,2
+ 3 1,1g0,2g2,1−3 1,1g1,1g1,2+ 28 0,2 2
2,0g1,1−4 2
1,1 2
2,0−38 2
1,1g0,2g2,0+ 13 1,1 3,1
+ 5 1,1 2,0g1,2−6 1,3g2,0− 1,1 1,2g2,0+ 8 4,0 0,2−56g2
1,1 0,2 2,0−4 0,2g3,1
+ 4 0,2 2,0g2,1+ 26 0,2g0,2g1,1g2,0−5 1,1g2,2)α9+ (−16 1,1 2,0 2,1+ 17g2
1,1 1,1g0,2
−10 1,1g0,2 3,0+ 22 0,2 3,0g1,1+ 36 2
1,1 2,0g1,1+ 24 1,2 2,0g1,1+ 15 1,1g1,1 2,1
−2 1,2g2,1+ 2 1,2 3,0+ 8 0,2 3
2,0−14 1,2 2
2,0+ 45 3
1,1g2,0−13g2
1,1 1,2−22g2
1,1 2
1,1
−17 2
1,1 3,0−6 0,3g3,0−103 0,2 1,1g1,1g2,0+ 14 2
1,1g2,1−24 3,0 2,0 0,2− 3,1g0,2
−28 0,2 2,0g0,2g2,0+ 10 0,2g0,2g3,0+ 10 1,1g2
0,2g2,0+ 6 0,2 2,1g2,0+ 58 0,2 1,1 2,0g2,0
−41 1,1 2,0g0,2g1,1−4 2,1 2,0g0,2+ 16 0,2 1,1g3,0+ 6 1,2g0,2g2,0−4 2,2g1,1+ 3 3,2
+ 22g3
1,1 0,2−6 1,1g0,3g2,0−10 0,2g1,1g2,1−8 2
0,2g2
2,0−9 0,3g1,1g2,0+ 16 1,1 2
2,0g0,2
21

−8 1,1g1,1g1,2−4 0,2 2
2,0g1,1+ 6 2
1,1 2
2,0−36 2
1,1g0,2g2,0+ 10 1,1 3,1+ 10 1,1 2,0g1,2
−6 1,3g2,0+ 20 1,1 1,2g2,0+ 18 0,3 2,0g2,0+ 4 4,0 0,2−26g2
1,1 0,2 2,0−4 0,2g3,1
+ 16 0,2 2,0g2,1+ 36 0,2g0,2g1,1g2,0−2 1,1g2,2)α8+ (−10 1,1 2,0 2,1+ 8g2
1,1 1,1g0,2
−3 1,1g0,2 3,0+ 24 0,2 3,0g1,1+ 12 2
1,1 2,0g1,1+ 14 1,2 2,0g1,1+ 16 1,1g1,1 2,1
−2 1,2g2,1− 1,2 3,0+ 16 0,2 3
2,0−2 1,2 2
2,0+ 25 3
1,1g2,0−14g2
1,1 1,2−13g2
1,1 2
1,1
−21 2
1,1 3,0−6 0,3g3,0−62 0,2 1,1g1,1g2,0−6 2,2 2,0+ 15 2
1,1g2,1−12 3,0 2,0 0,2
−28 0,2 2,0g0,2g2,0−3 3,1g0,2+ 6 1,1g2
0,2g2,0+ 6 0,2 2,1g2,0−22 1,1 2,0g0,2g1,1
+ 2 2,1 2,0g0,2+ 21 0,2 1,1g3,0−4 1,2g0,2g2,0+ 2 2,2g1,1−4g1,2 0,2g2,0+ 3 3,2
+ 10g3
1,1 0,2−9 1,1g0,3g2,0−18 0,2g1,1g2,1−8 2
0,2g2
2,0−21 0,3g1,1g2,0+ 12 1,1 2
2,0g0,2
−5 1,1g0,2g2,1−9 1,1g1,1g1,2−24 0,2 2
2,0g1,1+ 20 1,12 2
2,0−29 2
1,1g0,2g2,0+ 1,1 3,1
+ 9 1,1 2,0g1,2−3 1,3g2,0+ 26 1,1 1,2g2,0+ 18 0,3 2,0g2,0−4 4,0 0,2−4g2
1,1 0,2 2,0
−2 0,2g3,1+ 12 0,2 2,0g2,1+ 22 0,2g0,2g1,1g2,0+ 1,1g2,2)α7+ (2 1,1 2,0 2,1
+ 3g2
1,1 1,1g0,2+ 1,1g0,2 3,0+ 12 0,2 3,0g1,1− 2
1,1 2,0g1,1+ 4 1,2 2,0g1,1
+ 11 1,1g1,1 2,1+ 4 1,2g2,1−7 1,2 3,0+ 8 0,2 3
2,0+ 4 1,2 2
2,0+ 8 3
1,1g2,0−7g2
1,1 1,2
−3g2
1,1 2
1,1−16 2
1,1 3,0+ 3 0,3g3,0−14 0,2 1,1g1,1g2,0−6 2,2 2,0+ 13 2
1,1g2,1
+ 4 3,0 2,0 0,2−2 3,1g0,2−2 0,2g0,2g3,0+ 4 1,1g2
0,2g2,0+ 6 0,2 2,1g2,0
−22 0,2 1,1 2,0g2,0+ 6 2,1 2,0g0,2+ 20 0,2 1,1g3,0−2 1,2g0,2g2,0+ 6 2,2g1,1
+ 2 3,2+ 4g3
1,1 0,2−6 1,1g0,3g2,0−10 0,2g1,1g2,1−15 0,3g1,1g2,0+ 2 1,1 2
2,0g0,2
−4 1,1 2,0g0,2g1,1−4g1,2 0,2g2,0−3 1,1g0,2g2,1−5 1,1g1,1g1,2−28 0,2 2
2,0g1,1
+ 16 2
1,1 2
2,0−10 2
1,1g0,2g2,0−5 1,1 3,1+ 5 1,1 2,0g1,2+ 3 1,3g2,0+ 23 1,1 1,2g2,0
+ 12 0,3 2,0g2,0−4 4,0 0,2+ 14g2
1,1 0,2 2,0+ 2 0,2g3,1+ 8 0,2 2,0g2,1+ 3 1,1g2,2
+ 16 0,2g0,2g1,1g2,0)α6+ (8 1,1 2,0 2,1+ 2 1,1g0,2 3,0+ 2 0,2 3,0g1,1−6 2
1,1 2,0g1,1
−8 1,2 2,0g1,1+ 3 1,1g1,1 2,1+ 2 1,2g2,1−4 1,2 3,0+ 10 1,2 2
2,0−3 3
1,1g2,0
−3g2
1,1 1,2−5 2
1,1 3,0+ 3 0,3g3,0−4 2,2 2,0+ 4 2
1,1g2,1+ 8 3,0 2,0 0,2− 3,1g0,2
+ 4 0,2 2,0g0,2g2,0−4 0,2g0,2g3,0−30 0,2 1,1 2,0g2,0+ 1,1 2,0g0,2g1,1+ 4 2,1 2,0g0,2
+ 6 0,2 1,1g3,0−4 1,2g0,2g2,0+ 4 2,2g1,1−4g1,2 0,2g2,0− 3,2−3 1,1g0,3g2,0
−6 0,2g1,1g2,1−9 0,3g1,1g2,0−4 1,1 2
2,0g0,2−2 1,1g0,2g2,1−2 1,1g1,1g1,2+ 6 2
1,1 2
2,0
−16 0,2 2
2,0g1,1−3 2
1,1g0,2g2,0−8 1,1 3,1+ 3 1,3g2,0+ 7 1,1 1,2g2,0−6 0,3 2,0g2,0
−4 4,0 0,2+ 10g2
1,1 0,2 2,0+ 2 0,2g3,1−4 0,2 2,0g2,1+ 2 1,1g2,2)α5+ (10 1,1 2,0 2,1
+ 1,1g0,2 3,0−2 0,2 3,0g1,1−6 1,2 2,0g1,1+ 2 1,2g2,1− 1,2 3,0−4 0,2 3
2,0
+ 6 1,2 2
2,0−2 3
1,1g2,0+g2
1,1 2
1,1+ 3 2
1,1 3,0+ 3 0,3g3,0+ 6 0,2 1,1g1,1g2,0+ 2 2,2 2,0
+ 2
1,1g2,1+ 8 3,0 2,0 0,2+ 8 0,2 2,0g0,2g2,0−4 0,2 1,1 2,0g2,0+ 2 1,1 2,0g0,2g1,1
+ 2 2,1 2,0g0,2+ 2 0,2 1,1g3,0+ 2 2,2g1,1− 3,2−4 1,1 2
2,0g0,2−4 2
1,1 2
2,0+ 2 2
1,1g0,2g2,0
−3 1,1 3,1− 1,1 2,0g1,2+ 3 1,3g2,0+ 1,1 1,2g2,0−6 0,3 2,0g2,0+ 6g2
1,1 0,2 2,0
+ 2 0,2g3,1−4 0,2 2,0g2,1+ 1,1g2,2)α4+ (− 3
1,1g2,0+ 4 0,2 2
2,0g1,1− 1,1 2,0g1,2
−8 2
1,1 2
2,0−2 1,1 2
2,0g0,2−2 0,2 1,1g3,0+ 1,2 3,0−4 1,2 2,0g1,1+ 2 2,2 2,0
22
− 1,1g1,1 2,1+ 2 2
1,1 3,0+ 2
1,1 2,0g1,1− 3,2− 2
1,1g2,1−6 0,3 2,0g2,0−4 0,2 2,0g2,1
−3 1,1 1,2g2,0−2 0,2 3,0g1,1−4 0,2 3
2,0− 1,1 3,1+ 2 1,1 2,0 2,1)α3+ (−2 2
1,1 2
2,0
+ 4 0,2 2
2,0g1,1+ 1,2 3,0+ 3
1,1g2,0+ 2
1,1 3,0+ 4 0,2 1,1 2,0g2,0+ 2 2,2 2,0+ 1,1 3,1
−2 1,2 2
2,0+ 2 2
1,1 2,0g1,1)α2+ (−2 1,2 2
2,0−2 1,1 2,0 2,1− 2
1,1 3,0)α+ 2 2
1,1 2
2,0.
Appendix B. Exp ession o P7(F) and P8(F) when β= 1
Applying he No mal Fo m Algo i hm o he map (2) we ge ha , when α36= 1, hen
(4)
1,4=P7(F)/(α3−1) and g(4)
0,5=P8(F)/(α3−1) whe e
P7(F) := 1,4α3+ (3 0,3g1,2−3 1,4−2 0,3 2,1−2 2,0 0,4+ 2g1,3 0,2−2 2,2 0,2
+ 4 0,4g1,1)α2+ (−4g1,3 0,2+ 4 0,3 2,1−8 0,4g1,1−6 0,3g1,2−4g2,1 2
0,2
−10 0,3 0,2g2,0+ 3 1,4+ 3 3,0 2
0,2+ 4 2,0 0,4+ 4 2,2 0,2)α− 1,4−2 2,2 0,2
+ 2g1,3 0,2+ 4g2,1 2
0,2−2 2,0 0,4+ 2 2,02 0,22−3 3,0 2
0,2−8g1,1 2,0 2
0,2
+ 8 2
0,2g2
1,1+ 4 0,4g1,1+ 3 0,3g1,2+ 10 0,3 0,2g2,0−2 0,3 2,1,
P8(F) := g0,5α3+ (−3g0,5− 0,4g1,1−g1,3 0,2− 0,3g1,2)α2+ (2 0,3g1,2+ 2 0,4g1,1
+g2,1 2
0,2+ 2 0,3 0,2g2,0+ 2g1,3 0,2+ 3g0,5)α− 0,3g1,2−g0,5−2 0,3 0,2g2,0
− 0,4g1,1+g1,1 2,0 2
0,2−g1,3 0,2−g2,1 2
0,2−2 2
0,2g2
1,1.
Appendix C. Exp ession o C2(B, λ) in he p oo o Theo em 7
C2(B, λ) := 8B12λ25 + 125B12λ24 + 912B12λ23 + 4140B12λ22 + 13091B12λ21 + 23B9λ24
+30388B12λ20 + 264B9λ23 + 52493B12λ19 + 1457B9λ22 + 64792B12λ18
+5130B9λ21 + 44963B12λ17 + 12792B9λ20 + 17B6λ23 −22114B12λ16
+23399B9λ19 + 152B6λ22 −126694B12λ15 + 30518B9λ18 + 685B6λ21
−230443B12λ14 + 23012B9λ17 + 2027B6λ20 −285544B12λ13 −7945B9λ16
+4241B6λ19 −265465B12λ12 −59005B9λ15 + 6222B6λ18 + 23B3λ21
−182980B12λ11 −111409B9λ14 + 5530B6λ17 + 126B3λ20 −80299B12λ10
−140407B9λ13 −138B6λ16 + 356B3λ19 −280B12λ9−131599B9λ12
−10552B6λ15 + 644B3λ18 + 37544B12λ8−90967B9λ11 −21809B6λ14
+723B3λ17 + 40086B12λ7−40111B9λ10 −28180B6λ13 + 253B3λ16 + 8λ19
+26571B12λ6−883B9λ9−26229B6λ12 −844B3λ15 + 29λ18 + 12701B12λ5
+17318B9λ8−17474B6λ11 −2101B3λ14 + 36λ17 + 4481B12λ4+ 18449B9λ7
−6870B6λ10 −2804B3λ13 + 34λ16 + 1143B12λ3+ 12036B9λ6+ 902B6λ9
−2563B3λ12 −33λ15 + 199B12λ2+ 5561B9λ5+ 4012B6λ8−1532B3λ11 −71λ14
+21B12λ+ 1827B9λ4+ 3635B6λ7−364B3λ10 −137λ13 +B12 + 404B9λ3
+2079B6λ6+ 335B3λ9−92λ12 + 53B9λ2+ 839B6λ5+ 493B3λ8−56λ11
+3B9λ+ 232B6λ4+ 348B3λ7+ 8λ10 + 37B6λ3+ 149B3λ6+ 29λ9+ 2B6λ2
+35B3λ5+ 25λ8+ 3B3λ4+ 9λ7+λ6.
23
Re e ences
[1] R.M. Abu-Sa is. A sel -in e ibili y condi ion o global pe iodici y o di e ence equa-
ions. Appl. Ma h. Le . 19 (2006), 1078–1082
[2] R.M. Abu-Sa is, Q.M. Al-Hassan. On global pe iodici y o di e ence equa ions. J. Ma h.
Anal. Appl. 283 (2003), 468–477.
[3] D.K. A owsmi h, C.M. Place. An in oduc ion o dynamical sys ems. Camb idge Uni-
e si y P ess, Camb idge 1990.
[4] F. Balib ea, A. Line o. Some new esul s and open p oblems on pe iodici y o di e ence
equa ions. G aze Ma h. Be . 350 (2006), 15-38.
[5] F. Balib ea, A. Line o. On he global pe iodici y o some di e ence equa ions o hi d
o de . J. Di e ence Equ. Appl. 13 (2007), 1011-1027.
[6] I. Bajo, E. Liz. Pe iodici y on disc e e dynamical sys ems gene a ed by a class o a ional
mappings. J. Di e ence Equ. Appl. 12 (2006), no. 12, 1201-1212.
[7] L. Be g, S. S e i´c. Pe iodici y o some classes o holomo phic di e ence equa ions. J.
Di e ence Equa ions and Appl. 12 (2006), 827–835.
[8] R.H. Bing. A homeomo phism be ween he 3-sphe e and he sum o wo solid ho ned
sphe es. Annals o Ma hema ics. 56 (1952). 354-362.
[9] A. Ca o, A. Line o. Exis ence and uniqueness o p-cycles o second and hi d o de . J.
Di e ence Equ. Appl. 15 (2009), 489-500.
[10] A. Ca o, A. Line o. Gene al cycles o po en ial o m. In e na . J. Bi u . Chaos Appl.
Sci. Eng g. 20 (2010), 2735-2749.
[11] A. Cima, A. Gasull, F. Ma˜nosas. On pe iodic a ional di e ence equa ions o o de k.
J. Di e ence Equ. Appl. 10 (2004), 549–559.
[12] A. Cima, A. Gasull, F. Ma˜nosas. Global linea iza ion o pe iodic di e ence equa ions.
Disc e e Con in. Dynam. Sys ems A 32 (2012), 1575–1595.
[13] M. Cs¨o nyei, M. Laczko ich. Some pe iodic and non-pe iodic ecu sions. Mona sh.
Ma h. 132 (2001), 215-236.
[14] J. J. Duis e maa . “Disc e e In eg able Sys ems: QRT Maps and Ellip ic Su aces”.
Sp inge Monog aphs in Ma hema ics. Sp inge , New Yo k, 2010.
24
[15] A. an den Essen. “Polynomial Au omo phisms and he Jacobian Conjec u e”. P og ess
in Ma hema ics 190, Bi kh¨ause Ve lag, Basel, 2000.
[16] E.A. G o e, G. Ladas. “Pe iodici ies in Nonlinea Di e ence Equa ions Equa ions”.
Ad ances in disc e e Ma h. and Appl, ol. 4. Chapman & Hall/CRC P ess, Boca Ra on
FL, 2005.
[17] I. Gumo ski, Ch. Mi a. “Recu ences and disc e e dynamic sys ems”. Lec u e No es
in Ma hema ics 809. Sp inge Ve lag, Be lin, 1980.
[18] R. Haynes, S. Kwasik, J. Mas , R. Schul z. Pe iodic maps R7wi hou ixed poin s.
Ma h. P oc. Camb idge Philos. Soc. 132 (2002), 131-136.
[19] D. Jogia, J.A.G. Robe s, F. Vi aldi. An algeb aic geome ic app oach o in eg able
maps o he plane. J. Phys. A 39 (2006), 1133-1149.
[20] J.M. Kis e . Di e en iable pe iodic ac ions on E8wi hou ixed poin s. Ame . J. Ma h.
85 (1963), 316-319.
[21] S. Maubach. “Polynomial Endomo phisms and Ke nels o De i a ions”. Ph. D. Theses
Uni e si y o Nijemegen, Nijmegen, 2003.
[22] B.D. Mes el. On globally pe iodic solu ions o he di e ence equa ion xn+1 =
(xn)/xn−1. J. Di e ence Equ. Appl. 9 (2003), 201–209.
[23] D. Mon gome y, L. Zippin. “Topological T ans o ma ion G oups”. In e science, New
Yo k, 1955.
[24] I. Ni en, H.S. Zuke man, H.L. Mon gome y. “An In oduc ion o he Theo y o Num-
be s”. Fi h edi ion, John Wiley & Sons, Inc., New Yo k, 1991.
[25] J. Rubi´o-Masseg´u. On he global pe iodici y o disc e e dynamical sys ems and appli-
ca ion o a ional di e ence equa ions. J. Ma h. Anal. Appl. 343 (2008), 182-189.
[26] J. Rubi´o-Masseg´u, V. Ma˜nosa. No mal o ms o a ional di e ence equa ions wi h
applica ions o he global pe iodici y p oblem. J. Ma h. Anal. Appl. 332 (2007), 896-
918.
[27] T. Tsuda. In eg able mappings ia a ional ellip ic su aces. J. Phys. A: Ma h. Gen.
37 (2004), 2721–2730.
25