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*Corresponding Author: Rania Kammoun, Email: raniakammoun32@gmail.com
RESEARCH ARTICLE
Available Online at www.ajms.in
Asian Journal of Mathematical Sciences 2017; 1(6):230-233
Continued 𝜷-fractions with Pisot unit base in 𝑭𝒒 ((π’™βˆ’πŸ))
Rania Kammoun*
* University of Sfax, Faculty of Sciences, Department of Mathematics, Algebra Laboratory, Geometry and Spectral
Theory (AGTS) LR11ES53, BP 802, 3038 Sfax, Tunisia.
Receivedon:15/11/2017,Revisedon:01/12/2017,Acceptedon:29/12/2017
ABSTRACT
In this paper, we are interested in introducing a new theory of continued fractions based on the beta-
expansion theory in the field of Laurent series over a finite field πΉπ‘ž. We will characterize all elements
having finite continued beta-fraction where the base is a unit Pisot quadratic series.
Classification Mathematic Subject: 11R06, 37B50.
Key words: Continued 𝛽-fraction, formal power series, Pisot series, 𝛽-expansion, finite field.
INTRODUCTION
The 𝛽-numeration introduced in 1957 by RΓ©nyi [5]
is a new numeration system when we replace the
integer base b with a non-integral base. Let 𝛽 > 1, in the case of a non-integral base, one may write any
π‘₯ ∈ [0,1] as π‘₯ = βˆ‘π‘˜β‰₯1
π‘₯π‘˜
π›½π‘˜ , where π‘₯π‘˜ ∈ {0, β‹― , [𝛽]}. The sequence (π‘₯π‘˜)π‘˜β‰₯1 is called an expansion of π‘₯ in
𝛽 base. There is no expansion uniqueness but, among them, the greatest sequence for the lexicographical
order is called the 𝛽-expansion of π‘₯and it is denoted by 𝑑𝛽(π‘₯).
The 𝛽-expansion of π‘₯ is constructed by the greedy following algorithm. We consider the 𝛽-
transformation
𝑇𝛽: [0,1] β†’ [0,1], π‘₯ β†’ {𝛽π‘₯} = 𝛽π‘₯ βˆ’ [𝛽π‘₯]
and then we define
(π‘₯π‘˜)π‘˜β‰₯1 = 𝑑𝛽(π‘₯) ≔ π‘₯1π‘₯2π‘₯3 β‹―, where π‘₯π‘˜ = [𝛽𝑇𝛽
π‘˜βˆ’1
(π‘₯) ].
In the case π‘₯ β‰₯ 1, there exists a unique integer 𝑖 such that π›½π‘–βˆ’1
≀ π‘₯ < 𝛽𝑖
. So one can write
π‘₯
𝛽𝑖 = βˆ‘
π‘¦π‘˜
π›½π‘˜
π‘˜β‰₯1 ,
where (π‘¦π‘˜)π‘˜β‰₯1 is the 𝛽-expansion of
π‘₯
𝛽𝑖 . Thus, we have
π‘₯ = βˆ‘ π‘₯π‘˜π›½βˆ’π‘˜
∞
π‘˜=βˆ’π‘›
π‘ π‘’π‘β„Ž π‘‘β„Žπ‘Žπ‘‘ π‘₯π‘˜ = π‘¦π‘˜βˆ’π‘›.
The 𝛽-integer part of π‘₯ is [π‘₯]𝛽 = βˆ‘ π‘₯π‘˜π›½βˆ’π‘˜
∞
π‘˜=βˆ’π‘› and the 𝛽-fractional part of π‘₯is {π‘₯}𝛽 = βˆ‘ π‘₯π‘˜π›½βˆ’π‘˜
π‘˜>0 .
When {π‘₯}𝛽 = 0, we denote by ℀𝛽 the set of all 𝛽-integers.
Obviously, we can present an algorithm of continued fractions similarly to the classical decimal case by
consideration 𝛽 ∈ ℝ (non-integer) and then we get the so called continued 𝛽-fraction, whither the
sequence of partial quotients consists of 𝛽-integers instead of integers.
In [2]
, J. Bernat has showed that the continued πœ™-fraction of π‘₯ is finite if and only if π‘₯ ∈ β„š(πœ™). In [4]
, we
have studied the continued 𝛽-fraction with formal power series over finite fields and we have
characterize elements of π”½π‘ž((π‘₯βˆ’1
)) having finite 𝛽-fraction when the base 𝛽 is a quadratic Pisot unit.
Throughout this paper, we improve the result given [4]
by studying the case when 𝛽 is only a Pisot unit in
π”½π‘ž((π‘₯βˆ’1
)). The paper is organized as follows, Section 2, we introduce some basic definitions and results.
In Section 3, we define the continued 𝛽-fraction expansion. In Section 4, we state our main result.
Kammoun Rania et al. Continued 𝜷-fractions with Pisot unit base in 𝑭𝒒 ((π’™βˆ’πŸ
))
Β© 2017, AJMS. All Rights Reserved. 231
Fields of Formal series 𝔽𝒒((π’™βˆ’πŸ
))
Let π”½π‘ž be the field with π‘ž elements, π”½π‘ž[π‘₯] the ring of polynomials with coefficient in π”½π‘ž, π”½π‘ž(π‘₯) the field
of rational functions, π”½π‘ž(π‘₯, 𝛽) the minimal extension of π”½π‘žcontaining π‘₯ and 𝛽 and by π”½π‘ž[π‘₯, 𝛽] the
minimal ring containing π‘₯ and 𝛽. Let π”½π‘ž((π‘₯βˆ’1
)) be the field of formal power series of the form:
𝑓 = βˆ‘ π‘“π‘˜π‘₯π‘˜
𝑙
π‘˜=βˆ’βˆž
, π‘“π‘˜ ∈ π”½π‘ž,
where 𝑙 = deg(𝑓) ≔ {
max{π‘˜: π‘“π‘˜ β‰  0} for 𝑓 β‰  0;
βˆ’βˆž for 𝑓 = 0.
Define the absolute value |𝑓| = {
π‘ždeg(𝑓 )
for 𝑓 β‰  0;
0 for 𝑓 = 0.
As |. | is not Archimedean, it satisfies the strict triangle inequality
|𝑓 + 𝑔| ≀ max(|𝑓|, |𝑔|) and |𝑓 + 𝑔| = max(|𝑓|, |𝑔|) if |𝑓| β‰  |𝑔|.
Let ∈ π”½π‘ž((π‘₯βˆ’1
)) , the polynomial part of 𝑓 is [𝑓] = βˆ‘ π‘“π‘˜π‘₯π‘˜
π‘˜β‰₯0 . We know that the empty sum is always
equal zero. Therefore, the fraction part is [𝑓] ∈ π”½π‘ž[π‘₯] and {𝑓} = 𝑓 βˆ’ [𝑓] is in the unit disk 𝐷(0,1).
An element 𝛽 ∈ π”½π‘ž((π‘₯βˆ’1
)) is called a Pisot element if it is an algebraic integer over π”½π‘ž[π‘₯], [𝛽] >
1 and|𝛽𝑖| < 1 for all conjugates 𝛽. Using the coefficient of minimal polynomial, P. Batman and A.L.
Duquette [1] had characterized the Pisot elements in π”½π‘ž((π‘₯βˆ’1
)) :
Theorem 2.1.Let 𝛽 ∈ π”½π‘ž((π‘₯βˆ’1
))be an algebraic integer over π”½π‘ž[π‘₯] with the minimal polynomial 𝑃(𝑦) =
𝑦𝑛
βˆ’ 𝐴1π‘¦π‘›βˆ’1
βˆ’ β‹― βˆ’ 𝐴𝑛 , 𝐴𝑖 ∈ π”½π‘ž[π‘₯].
Then, 𝛽 is a Pisot elements if and only if |𝐴1| > max
2≀i≀n
|𝐴𝑖|.
Let 𝛽 ∈ π”½π‘ž((π‘₯βˆ’1)) with |𝛽| > 1. A 𝛽-representation of 𝑓 is an infinite sequences(𝑑𝑖)𝑖β‰₯1, where 𝑑𝑖 ∈
π”½π‘ž[π‘₯] and 𝑓 = βˆ‘
𝑑𝑖
𝛽𝑖
𝑖β‰₯1 . A 𝛽-expansion of 𝑓, denoted 𝑑𝛽(𝑓) = (𝑑𝑖)𝑖β‰₯1 , is a 𝛽-represenation of 𝑓 such
that:
𝑑𝑖 = [𝛽𝑇𝛽
π‘–βˆ’1(𝑓)] where𝑇𝛽: 𝐷(0,1) β†’ 𝐷(0,1) 𝑓 β†’ 𝛽𝑓 βˆ’ [𝛽𝑓]. (1)
The 𝛽-expansion can be computed by the following algorithm:
π‘Ÿ0 = 𝑓 and for 𝑖 β‰₯ 1 𝑑𝑖 = [π›½π‘Ÿπ‘–βˆ’1], π‘Ÿπ‘– = π›½π‘Ÿπ‘–βˆ’1 βˆ’ 𝑑𝑖.
The 𝛽-expansion𝑑𝛽(𝑓) is finite if and only if there is π‘˜ β‰₯ 0 such that 𝑑𝑖 = 0 for all 𝑖 β‰₯ π‘˜. It is called
ultimately periodic if and only if there is some smallest 𝑝 β‰₯ 0 (the pre-period length) and 𝑠 β‰₯ 1 (the
period length) for which 𝑑𝑖+𝑠 = 𝑑𝑖 for all 𝑖 β‰₯ 𝑝 + 1. Using the last notion, let:
𝐹𝑖𝑛(𝛽) = {𝑓 ∈ π”½π‘ž((π‘₯βˆ’1)): 𝑑𝛽(𝑓)is finite}
and
π‘ƒπ‘’π‘Ÿ(𝛽) = {𝑓 ∈ π”½π‘ž((π‘₯βˆ’1)): 𝑑𝛽(𝑓)is eventuallly periodic}.
When 𝑑𝛽(𝑓) = 𝑑1𝑑2 β‹― 𝑑𝑙+1 Β· 𝑑𝑙+2 β‹― π‘‘π‘š then, we denote by deg(𝑓)𝛽 = 𝑙 and ord(𝑓) = π‘š.
For |𝑓| β‰₯ 1, then there is a unique π‘˜ ∈ 𝑁 such that |𝛽|π‘˜
≀ |𝑓| ≀ |𝛽|π‘˜+1
. So we have |
𝑓
π›½π‘˜+1
| < 1 and we
can represent 𝑓 by shifting 𝑑𝛽(
𝑓
π›½π‘˜+1) by π‘˜ digits to the left. Thus, if 𝑑𝛽(𝑓) = 0. 𝑑1𝑑2 β‹― , then𝑑𝛽(𝛽𝑓) =
𝑑1. 𝑑2𝑑3 β‹―
Remark 2.1. There is no carry occurring, when we add two polynomials in π”½π‘ž[π‘₯] with degree less than
deg(𝛽). Consequently, if 𝑓, 𝑔 ∈ π”½π‘ž((π‘₯βˆ’1
)), we get 𝑑𝛽(𝑓 + 𝑔) = 𝑑𝛽(𝑓) + 𝑑𝛽(𝑔).
In [6], Scheicher has characterized the set 𝐹𝑖𝑛 (𝛽) when 𝛽 is Pisot.
Theorem 2.2.[6] 𝛽 is a Pisot series if and only if 𝐹𝑖𝑛(𝛽) = π”½π‘ž[π‘₯, π›½βˆ’1].
Kammoun Rania et al. Continued 𝜷-fractions with Pisot unit base in 𝑭𝒒 ((π’™βˆ’πŸ
))
Β© 2017, AJMS. All Rights Reserved. 232
Let 𝑓 ∈ π”½π‘ž((π‘₯βˆ’1)), the 𝛽-polynomial part of 𝑓 is [𝑓]𝛽 = βˆ‘ π‘‘π‘–π›½π‘™βˆ’π‘–+1
𝑙+1
𝑖=1 and the 𝛽-fractional part is
{𝑓}𝛽 = 𝑓 βˆ’ [𝑓]𝛽 = βˆ‘ π‘‘π‘–π›½π‘™βˆ’π‘–+1
𝑖>𝑙+1 . We define the set of 𝛽-polynomials as follows:
π”½π‘ž[π‘₯]𝛽 = {𝑓 ∈ π”½π‘ž((π‘₯βˆ’1)); {𝑓}𝛽 = 0}.
Then, clearly π”½π‘ž[π‘₯]𝛽 βŠ† π”½π‘ž[π‘₯, 𝛽]. Furthermore, we introduce the following set
(π”½π‘ž[π‘₯])
β€²
= {𝑃 ∈ π”½π‘ž[π‘₯]𝜷, deg(𝑃) ≀ deg(𝛽) βˆ’ 1} = {𝑃 ∈ π”½π‘ž[π‘₯]𝜷, 𝑑𝑒𝑔𝛽(𝑃) = 0}.
The set of power series that can be written as a fraction of two 𝛽-polynomials denoted by π”½π‘ž(π‘₯)𝛽. Then,
clearly π”½π‘ž[π‘₯]𝛽 βŠ† π”½π‘ž(π‘₯, 𝛽). In [3], the authors studied the quantity πΏβŠ™ and they define as follows:
πΏβŠ™ = min{𝑛 ∈ β„•: βˆ€ 𝑃1, 𝑃2 ∈ π”½π‘ž[π‘₯]𝛽; 𝑃1𝑃2 ∈ 𝐹𝑖𝑛(𝛽) β‡’ 𝛽𝑛(𝑃1𝑃2) ∈ π”½π‘ž[π‘₯]𝛽 }.
Theorem 2.3.[3] Let 𝛽be a quadratic Pisot unit series. Then πΏβŠ™ = 1.
Continued 𝜷-fraction algorithm
We begin by introduce a generalization of the algorithm of the expansion in continued fraction in the
field of formal power series in base 𝛽 ∈ π”½π‘ž((π‘₯βˆ’1)) with |𝛽| > 1.When 𝛽 = π‘₯, this theory is seems to be
similar to the classical case of continued fractions.
We define the 𝛽-transformation 𝑇𝛽
β€²
by:
𝑇𝛽
β€²
: 𝐷(0,1) β†’ 𝐷(0,1)
𝑓 β†’
1
𝑓
βˆ’ [
1
𝑓
]
𝛽
.
when |𝑓| < 1, we obtain
𝑓 =
1
𝐴1 +
1
𝐴2 +
1
β‹±
= [0,𝐴1, 𝐴2, β‹― ]𝛽
whither (π΄π‘˜)π‘˜β‰₯1 ∈ π”½π‘ž[π‘₯]𝛽and there are defined by π΄π‘˜ = [
1
𝑇′
𝛽
π‘˜βˆ’1
(𝑓)
]
𝛽
, βˆ€ π‘˜ β‰₯ 1.
For 𝑓 ∈ π”½π‘ž((π‘₯βˆ’1)) and 𝐴0 = [𝑓]𝛽, we get
𝑓 = 𝐴0 +
1
𝐴1 +
1
𝐴2 +
1
β‹±
= [𝐴0, 𝐴1, 𝐴2, β‹― ]𝛽.
The last bracket is called continued 𝛽-fraction expansion of 𝑓. The sequence (π΄π‘˜)π‘˜β‰₯0 is called the
sequence of partial 𝛽-quotients of 𝑓. We define the π‘›π‘‘β„Ž
𝛽-complete quotient of 𝑓 by 𝑓
𝑛 =
[𝐴0, 𝐴1, 𝐴2, β‹― , 𝑓
𝑛]𝛽. We remark that all (π΄π‘˜)π‘˜β‰₯1are not in π”½π‘ž.
Main Results
Our main result is an improvement of Theorem 4.1 in [4]
.
Theorem 4.1. Let 𝛽 be a quadratic Pisot unit formal power series over the finite field π”½π‘ž such that
deg(𝛽) = π‘š. Let 𝛽 ∈ π”½π‘ž(π‘₯, 𝛽) such that the continued 𝛽-fraction of 𝑓 is given by 𝑓 =
[𝐴0, 𝐴1, 𝐴2, β‹― , 𝐴𝑛, β‹― ]. If 𝑓 ∈ π”½π‘ž(π‘₯, 𝛽) then {𝐴𝑖/ deg𝛽(𝐴𝑖) > 0} is finite.
So as to prove the above Theorem, first we need to recall some results given in [4]
and we use the
following Lemmas and Propositions.
Lemma 4.2. [4] Let 𝛽 be a unit Pisot series. Then π”½π‘ž(π‘₯, 𝛽) = π”½π‘ž(π‘₯)𝛽.
Now, we define two sequences (𝑃
𝑛)π‘›βˆˆβ„• and (𝑄𝑛)π‘›βˆˆβ„• in π”½π‘ž[π‘₯, 𝛽] by
{
𝑃0 = π‘Ž0, 𝑃1 = π‘Ž0π‘Ž1 + 1
𝑄0 = 1 , 𝑄1 = π‘Ž1
and {
𝑃
𝑛 = π‘Žπ‘›π‘ƒπ‘›βˆ’1 + π‘ƒπ‘›βˆ’2
𝑄𝑛 = π‘Žπ‘›π‘„π‘›βˆ’1 + π‘„π‘›βˆ’2, βˆ€π‘› β‰₯ 2
The pair (𝑃𝑛, 𝑄𝑛) is called reduced 𝛽-fractionary expansion of 𝑓 for all 𝑛 β‰₯ 0.
Proposition 4.1. Let 𝑓 ∈ π”½π‘ž(π‘₯, 𝛽) such that 𝑓 = [𝐴0, 𝐴1, 𝐴2, β‹― , 𝐴𝑛, β‹― ]. Then |𝑓 βˆ’
𝑃𝑛
𝑄𝑛
| <
1
|𝑄𝑛|2.
Proof. Similarly to the classical case.
Kammoun Rania et al. Continued 𝜷-fractions with Pisot unit base in 𝑭𝒒 ((π’™βˆ’πŸ
))
Β© 2017, AJMS. All Rights Reserved. 233
Proposition 4.2. Let 𝛽 be a quadratic Pisot unit power formal series such that deg(𝛽) = π‘š and
𝑃1, 𝑃2, β‹― , π‘ƒπ‘š ∈ π”½π‘ž[π‘₯]𝛽. Then, π›½π‘šβˆ’1
𝑃1𝑃2 β‹― π‘ƒπ‘š ∈ π”½π‘ž[π‘₯]𝛽.
The proof of the last proposition is an immediate consequence of Thoerem 2.3.
Corollary 4.3. Let 𝑃1, 𝑃2, β‹― , 𝑃
π‘š ∈ π”½π‘ž[π‘₯]𝛽. Then we have, for all positive integer
𝑛, 𝛽
(π‘šβˆ’1)𝑛
π‘š 𝑃1𝑃2 β‹― π‘ƒπ‘š ∈ π”½π‘ž[π‘₯]𝛽.
Corollary 4.4.Let (𝑃𝑛, 𝑄𝑛)𝑛β‰₯0 the reduced 𝛽-fractionary expansion of 𝑓 . Then 𝛽
(π‘šβˆ’1)𝑛
π‘š 𝑃
𝑛 ∈ π”½π‘ž[π‘₯]𝛽 and
𝛽
(π‘šβˆ’1)𝑛
π‘š 𝑄𝑛 ∈ π”½π‘ž[π‘₯]𝛽.
For 𝑃 = π‘Žπ‘ π›½π‘ 
+ β‹― + π‘Ž0 ∈ π”½π‘ž[π‘₯]𝛽. We denote by 𝛾(𝑃) = π‘š deg𝛽(𝑃) + deg𝑠(π‘Žπ‘ ) = 2π‘š +
deg(π‘Žπ‘ ).
Lemma 4.5. [4] Let 𝐴, 𝐡 ∈ π”½π‘ž[π‘₯]𝛽 with 𝛾(𝐴) > 𝛾(𝐡). Then there exists 𝐢, 𝐴1 and 𝐡1in π”½π‘ž[π‘₯]𝛽, such
that
𝐴
𝐡
= 𝐢 +
1
𝐴1
𝐡1
with 𝛾(𝐴1) > 𝛾(𝐡1).
Proof of Theorem 4.1
It is equivalent to prove that there exist 𝑛0 β‰₯ 1, 𝐴𝑛 ∈ (π”½π‘ž[π‘₯]𝛽) β€². By Lemma 4.2, we obtain 𝑓 =
𝑃
𝑄
∈
π”½π‘ž(π‘₯)𝛽 such as 𝑃, 𝑄 ∈ π”½π‘ž[π‘₯]𝛽 and (𝑃
𝑛, 𝑄𝑛) the reduced 𝛽-fractionary expansion of 𝑓.
By proposition 4.1, |
𝑃
𝑄
βˆ’
𝑃𝑛
𝑄𝑛
| <
1
|𝑄𝑛|2 . According to Corollary 4.3 and Lemma 4.5, we have
(𝛽
(π‘šβˆ’1)
π‘š
(𝑛+1)
(𝑃𝑄𝑛 βˆ’ 𝑄𝑃
𝑛)) inπ”½π‘ž[π‘₯]𝛽 .So, we obtain
1
|𝑄|
< |𝛽|(π‘šβˆ’1)(𝑛+1)/π‘š
|
𝑃𝑄𝑛 βˆ’ 𝑄𝑃
𝑛
𝑄
| <
|𝛽|
(π‘šβˆ’1)(𝑛+1)
π‘š
|𝑄𝑛|
which implies that deg(𝑄𝑛) ≀ deg(𝑄) + (π‘š βˆ’ 1)(𝑛 + 1), where
deg(𝑄𝑛) = βˆ‘ deg(𝐴𝑖)
𝑛
𝑖=1
≀ deg(𝑄) + (π‘š βˆ’ 1)(𝑛 + 1).
Thus βˆ‘ (deg(𝐴𝑖) βˆ’ (π‘š βˆ’ 1)) ≀ deg(𝑄) + (π‘š βˆ’ 1)
𝑛
𝑖=1 . Finally there exists 𝑛0 β‰₯ 1, such that, for
deg(𝐴𝑖) βˆ’ (π‘š βˆ’ 1) ≀ 0, for all 𝑖 β‰₯ 𝑛0 and the desired result is reached.
REFERENCES
1. P. Bateman and L. Duquette. The analogue of Pisot- Vijayaraghvan numbers in fields of power
series, Ill. J. Math, 6, (1962), 594-606.
2. J. Bernat. Continued fractions and numeration in the Fibonacci base, Discrete Mathematics, 22,
(2006), 2828-2850.
3. R. Ghorbel, M. Hbaib and S. Zouari. Arithmetics on beta-expansions with Pisot bases over
πΉπ‘ž((π‘₯βˆ’1
)), Bull. Belg. Math. Soc. Simon Stevin, 21, (2014), 241-251.
4. M. Hbaib, R. Kammoun. Continued beta-fractions with formal power series over finite fields,
Ramaujan J Math, (2015), DOI 10.1007/s11139-015-9725-5.
5. A. RΓ©nyi. Representations for real numbers and their ergodic properties, Acta Math. Acad. Sci.
Hung, 8, (1957), 477-493.
6. K. Scheicher. Beta-expansions in algebraic function fields over finite fields, finite fields and their
Applications, (2007), 394-410.

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5. Rania.pdf

  • 1. *Corresponding Author: Rania Kammoun, Email: raniakammoun32@gmail.com RESEARCH ARTICLE Available Online at www.ajms.in Asian Journal of Mathematical Sciences 2017; 1(6):230-233 Continued 𝜷-fractions with Pisot unit base in 𝑭𝒒 ((π’™βˆ’πŸ)) Rania Kammoun* * University of Sfax, Faculty of Sciences, Department of Mathematics, Algebra Laboratory, Geometry and Spectral Theory (AGTS) LR11ES53, BP 802, 3038 Sfax, Tunisia. Receivedon:15/11/2017,Revisedon:01/12/2017,Acceptedon:29/12/2017 ABSTRACT In this paper, we are interested in introducing a new theory of continued fractions based on the beta- expansion theory in the field of Laurent series over a finite field πΉπ‘ž. We will characterize all elements having finite continued beta-fraction where the base is a unit Pisot quadratic series. Classification Mathematic Subject: 11R06, 37B50. Key words: Continued 𝛽-fraction, formal power series, Pisot series, 𝛽-expansion, finite field. INTRODUCTION The 𝛽-numeration introduced in 1957 by RΓ©nyi [5] is a new numeration system when we replace the integer base b with a non-integral base. Let 𝛽 > 1, in the case of a non-integral base, one may write any π‘₯ ∈ [0,1] as π‘₯ = βˆ‘π‘˜β‰₯1 π‘₯π‘˜ π›½π‘˜ , where π‘₯π‘˜ ∈ {0, β‹― , [𝛽]}. The sequence (π‘₯π‘˜)π‘˜β‰₯1 is called an expansion of π‘₯ in 𝛽 base. There is no expansion uniqueness but, among them, the greatest sequence for the lexicographical order is called the 𝛽-expansion of π‘₯and it is denoted by 𝑑𝛽(π‘₯). The 𝛽-expansion of π‘₯ is constructed by the greedy following algorithm. We consider the 𝛽- transformation 𝑇𝛽: [0,1] β†’ [0,1], π‘₯ β†’ {𝛽π‘₯} = 𝛽π‘₯ βˆ’ [𝛽π‘₯] and then we define (π‘₯π‘˜)π‘˜β‰₯1 = 𝑑𝛽(π‘₯) ≔ π‘₯1π‘₯2π‘₯3 β‹―, where π‘₯π‘˜ = [𝛽𝑇𝛽 π‘˜βˆ’1 (π‘₯) ]. In the case π‘₯ β‰₯ 1, there exists a unique integer 𝑖 such that π›½π‘–βˆ’1 ≀ π‘₯ < 𝛽𝑖 . So one can write π‘₯ 𝛽𝑖 = βˆ‘ π‘¦π‘˜ π›½π‘˜ π‘˜β‰₯1 , where (π‘¦π‘˜)π‘˜β‰₯1 is the 𝛽-expansion of π‘₯ 𝛽𝑖 . Thus, we have π‘₯ = βˆ‘ π‘₯π‘˜π›½βˆ’π‘˜ ∞ π‘˜=βˆ’π‘› π‘ π‘’π‘β„Ž π‘‘β„Žπ‘Žπ‘‘ π‘₯π‘˜ = π‘¦π‘˜βˆ’π‘›. The 𝛽-integer part of π‘₯ is [π‘₯]𝛽 = βˆ‘ π‘₯π‘˜π›½βˆ’π‘˜ ∞ π‘˜=βˆ’π‘› and the 𝛽-fractional part of π‘₯is {π‘₯}𝛽 = βˆ‘ π‘₯π‘˜π›½βˆ’π‘˜ π‘˜>0 . When {π‘₯}𝛽 = 0, we denote by ℀𝛽 the set of all 𝛽-integers. Obviously, we can present an algorithm of continued fractions similarly to the classical decimal case by consideration 𝛽 ∈ ℝ (non-integer) and then we get the so called continued 𝛽-fraction, whither the sequence of partial quotients consists of 𝛽-integers instead of integers. In [2] , J. Bernat has showed that the continued πœ™-fraction of π‘₯ is finite if and only if π‘₯ ∈ β„š(πœ™). In [4] , we have studied the continued 𝛽-fraction with formal power series over finite fields and we have characterize elements of π”½π‘ž((π‘₯βˆ’1 )) having finite 𝛽-fraction when the base 𝛽 is a quadratic Pisot unit. Throughout this paper, we improve the result given [4] by studying the case when 𝛽 is only a Pisot unit in π”½π‘ž((π‘₯βˆ’1 )). The paper is organized as follows, Section 2, we introduce some basic definitions and results. In Section 3, we define the continued 𝛽-fraction expansion. In Section 4, we state our main result.
  • 2. Kammoun Rania et al. Continued 𝜷-fractions with Pisot unit base in 𝑭𝒒 ((π’™βˆ’πŸ )) Β© 2017, AJMS. All Rights Reserved. 231 Fields of Formal series 𝔽𝒒((π’™βˆ’πŸ )) Let π”½π‘ž be the field with π‘ž elements, π”½π‘ž[π‘₯] the ring of polynomials with coefficient in π”½π‘ž, π”½π‘ž(π‘₯) the field of rational functions, π”½π‘ž(π‘₯, 𝛽) the minimal extension of π”½π‘žcontaining π‘₯ and 𝛽 and by π”½π‘ž[π‘₯, 𝛽] the minimal ring containing π‘₯ and 𝛽. Let π”½π‘ž((π‘₯βˆ’1 )) be the field of formal power series of the form: 𝑓 = βˆ‘ π‘“π‘˜π‘₯π‘˜ 𝑙 π‘˜=βˆ’βˆž , π‘“π‘˜ ∈ π”½π‘ž, where 𝑙 = deg(𝑓) ≔ { max{π‘˜: π‘“π‘˜ β‰  0} for 𝑓 β‰  0; βˆ’βˆž for 𝑓 = 0. Define the absolute value |𝑓| = { π‘ždeg(𝑓 ) for 𝑓 β‰  0; 0 for 𝑓 = 0. As |. | is not Archimedean, it satisfies the strict triangle inequality |𝑓 + 𝑔| ≀ max(|𝑓|, |𝑔|) and |𝑓 + 𝑔| = max(|𝑓|, |𝑔|) if |𝑓| β‰  |𝑔|. Let ∈ π”½π‘ž((π‘₯βˆ’1 )) , the polynomial part of 𝑓 is [𝑓] = βˆ‘ π‘“π‘˜π‘₯π‘˜ π‘˜β‰₯0 . We know that the empty sum is always equal zero. Therefore, the fraction part is [𝑓] ∈ π”½π‘ž[π‘₯] and {𝑓} = 𝑓 βˆ’ [𝑓] is in the unit disk 𝐷(0,1). An element 𝛽 ∈ π”½π‘ž((π‘₯βˆ’1 )) is called a Pisot element if it is an algebraic integer over π”½π‘ž[π‘₯], [𝛽] > 1 and|𝛽𝑖| < 1 for all conjugates 𝛽. Using the coefficient of minimal polynomial, P. Batman and A.L. Duquette [1] had characterized the Pisot elements in π”½π‘ž((π‘₯βˆ’1 )) : Theorem 2.1.Let 𝛽 ∈ π”½π‘ž((π‘₯βˆ’1 ))be an algebraic integer over π”½π‘ž[π‘₯] with the minimal polynomial 𝑃(𝑦) = 𝑦𝑛 βˆ’ 𝐴1π‘¦π‘›βˆ’1 βˆ’ β‹― βˆ’ 𝐴𝑛 , 𝐴𝑖 ∈ π”½π‘ž[π‘₯]. Then, 𝛽 is a Pisot elements if and only if |𝐴1| > max 2≀i≀n |𝐴𝑖|. Let 𝛽 ∈ π”½π‘ž((π‘₯βˆ’1)) with |𝛽| > 1. A 𝛽-representation of 𝑓 is an infinite sequences(𝑑𝑖)𝑖β‰₯1, where 𝑑𝑖 ∈ π”½π‘ž[π‘₯] and 𝑓 = βˆ‘ 𝑑𝑖 𝛽𝑖 𝑖β‰₯1 . A 𝛽-expansion of 𝑓, denoted 𝑑𝛽(𝑓) = (𝑑𝑖)𝑖β‰₯1 , is a 𝛽-represenation of 𝑓 such that: 𝑑𝑖 = [𝛽𝑇𝛽 π‘–βˆ’1(𝑓)] where𝑇𝛽: 𝐷(0,1) β†’ 𝐷(0,1) 𝑓 β†’ 𝛽𝑓 βˆ’ [𝛽𝑓]. (1) The 𝛽-expansion can be computed by the following algorithm: π‘Ÿ0 = 𝑓 and for 𝑖 β‰₯ 1 𝑑𝑖 = [π›½π‘Ÿπ‘–βˆ’1], π‘Ÿπ‘– = π›½π‘Ÿπ‘–βˆ’1 βˆ’ 𝑑𝑖. The 𝛽-expansion𝑑𝛽(𝑓) is finite if and only if there is π‘˜ β‰₯ 0 such that 𝑑𝑖 = 0 for all 𝑖 β‰₯ π‘˜. It is called ultimately periodic if and only if there is some smallest 𝑝 β‰₯ 0 (the pre-period length) and 𝑠 β‰₯ 1 (the period length) for which 𝑑𝑖+𝑠 = 𝑑𝑖 for all 𝑖 β‰₯ 𝑝 + 1. Using the last notion, let: 𝐹𝑖𝑛(𝛽) = {𝑓 ∈ π”½π‘ž((π‘₯βˆ’1)): 𝑑𝛽(𝑓)is finite} and π‘ƒπ‘’π‘Ÿ(𝛽) = {𝑓 ∈ π”½π‘ž((π‘₯βˆ’1)): 𝑑𝛽(𝑓)is eventuallly periodic}. When 𝑑𝛽(𝑓) = 𝑑1𝑑2 β‹― 𝑑𝑙+1 Β· 𝑑𝑙+2 β‹― π‘‘π‘š then, we denote by deg(𝑓)𝛽 = 𝑙 and ord(𝑓) = π‘š. For |𝑓| β‰₯ 1, then there is a unique π‘˜ ∈ 𝑁 such that |𝛽|π‘˜ ≀ |𝑓| ≀ |𝛽|π‘˜+1 . So we have | 𝑓 π›½π‘˜+1 | < 1 and we can represent 𝑓 by shifting 𝑑𝛽( 𝑓 π›½π‘˜+1) by π‘˜ digits to the left. Thus, if 𝑑𝛽(𝑓) = 0. 𝑑1𝑑2 β‹― , then𝑑𝛽(𝛽𝑓) = 𝑑1. 𝑑2𝑑3 β‹― Remark 2.1. There is no carry occurring, when we add two polynomials in π”½π‘ž[π‘₯] with degree less than deg(𝛽). Consequently, if 𝑓, 𝑔 ∈ π”½π‘ž((π‘₯βˆ’1 )), we get 𝑑𝛽(𝑓 + 𝑔) = 𝑑𝛽(𝑓) + 𝑑𝛽(𝑔). In [6], Scheicher has characterized the set 𝐹𝑖𝑛 (𝛽) when 𝛽 is Pisot. Theorem 2.2.[6] 𝛽 is a Pisot series if and only if 𝐹𝑖𝑛(𝛽) = π”½π‘ž[π‘₯, π›½βˆ’1].
  • 3. Kammoun Rania et al. Continued 𝜷-fractions with Pisot unit base in 𝑭𝒒 ((π’™βˆ’πŸ )) Β© 2017, AJMS. All Rights Reserved. 232 Let 𝑓 ∈ π”½π‘ž((π‘₯βˆ’1)), the 𝛽-polynomial part of 𝑓 is [𝑓]𝛽 = βˆ‘ π‘‘π‘–π›½π‘™βˆ’π‘–+1 𝑙+1 𝑖=1 and the 𝛽-fractional part is {𝑓}𝛽 = 𝑓 βˆ’ [𝑓]𝛽 = βˆ‘ π‘‘π‘–π›½π‘™βˆ’π‘–+1 𝑖>𝑙+1 . We define the set of 𝛽-polynomials as follows: π”½π‘ž[π‘₯]𝛽 = {𝑓 ∈ π”½π‘ž((π‘₯βˆ’1)); {𝑓}𝛽 = 0}. Then, clearly π”½π‘ž[π‘₯]𝛽 βŠ† π”½π‘ž[π‘₯, 𝛽]. Furthermore, we introduce the following set (π”½π‘ž[π‘₯]) β€² = {𝑃 ∈ π”½π‘ž[π‘₯]𝜷, deg(𝑃) ≀ deg(𝛽) βˆ’ 1} = {𝑃 ∈ π”½π‘ž[π‘₯]𝜷, 𝑑𝑒𝑔𝛽(𝑃) = 0}. The set of power series that can be written as a fraction of two 𝛽-polynomials denoted by π”½π‘ž(π‘₯)𝛽. Then, clearly π”½π‘ž[π‘₯]𝛽 βŠ† π”½π‘ž(π‘₯, 𝛽). In [3], the authors studied the quantity πΏβŠ™ and they define as follows: πΏβŠ™ = min{𝑛 ∈ β„•: βˆ€ 𝑃1, 𝑃2 ∈ π”½π‘ž[π‘₯]𝛽; 𝑃1𝑃2 ∈ 𝐹𝑖𝑛(𝛽) β‡’ 𝛽𝑛(𝑃1𝑃2) ∈ π”½π‘ž[π‘₯]𝛽 }. Theorem 2.3.[3] Let 𝛽be a quadratic Pisot unit series. Then πΏβŠ™ = 1. Continued 𝜷-fraction algorithm We begin by introduce a generalization of the algorithm of the expansion in continued fraction in the field of formal power series in base 𝛽 ∈ π”½π‘ž((π‘₯βˆ’1)) with |𝛽| > 1.When 𝛽 = π‘₯, this theory is seems to be similar to the classical case of continued fractions. We define the 𝛽-transformation 𝑇𝛽 β€² by: 𝑇𝛽 β€² : 𝐷(0,1) β†’ 𝐷(0,1) 𝑓 β†’ 1 𝑓 βˆ’ [ 1 𝑓 ] 𝛽 . when |𝑓| < 1, we obtain 𝑓 = 1 𝐴1 + 1 𝐴2 + 1 β‹± = [0,𝐴1, 𝐴2, β‹― ]𝛽 whither (π΄π‘˜)π‘˜β‰₯1 ∈ π”½π‘ž[π‘₯]𝛽and there are defined by π΄π‘˜ = [ 1 𝑇′ 𝛽 π‘˜βˆ’1 (𝑓) ] 𝛽 , βˆ€ π‘˜ β‰₯ 1. For 𝑓 ∈ π”½π‘ž((π‘₯βˆ’1)) and 𝐴0 = [𝑓]𝛽, we get 𝑓 = 𝐴0 + 1 𝐴1 + 1 𝐴2 + 1 β‹± = [𝐴0, 𝐴1, 𝐴2, β‹― ]𝛽. The last bracket is called continued 𝛽-fraction expansion of 𝑓. The sequence (π΄π‘˜)π‘˜β‰₯0 is called the sequence of partial 𝛽-quotients of 𝑓. We define the π‘›π‘‘β„Ž 𝛽-complete quotient of 𝑓 by 𝑓 𝑛 = [𝐴0, 𝐴1, 𝐴2, β‹― , 𝑓 𝑛]𝛽. We remark that all (π΄π‘˜)π‘˜β‰₯1are not in π”½π‘ž. Main Results Our main result is an improvement of Theorem 4.1 in [4] . Theorem 4.1. Let 𝛽 be a quadratic Pisot unit formal power series over the finite field π”½π‘ž such that deg(𝛽) = π‘š. Let 𝛽 ∈ π”½π‘ž(π‘₯, 𝛽) such that the continued 𝛽-fraction of 𝑓 is given by 𝑓 = [𝐴0, 𝐴1, 𝐴2, β‹― , 𝐴𝑛, β‹― ]. If 𝑓 ∈ π”½π‘ž(π‘₯, 𝛽) then {𝐴𝑖/ deg𝛽(𝐴𝑖) > 0} is finite. So as to prove the above Theorem, first we need to recall some results given in [4] and we use the following Lemmas and Propositions. Lemma 4.2. [4] Let 𝛽 be a unit Pisot series. Then π”½π‘ž(π‘₯, 𝛽) = π”½π‘ž(π‘₯)𝛽. Now, we define two sequences (𝑃 𝑛)π‘›βˆˆβ„• and (𝑄𝑛)π‘›βˆˆβ„• in π”½π‘ž[π‘₯, 𝛽] by { 𝑃0 = π‘Ž0, 𝑃1 = π‘Ž0π‘Ž1 + 1 𝑄0 = 1 , 𝑄1 = π‘Ž1 and { 𝑃 𝑛 = π‘Žπ‘›π‘ƒπ‘›βˆ’1 + π‘ƒπ‘›βˆ’2 𝑄𝑛 = π‘Žπ‘›π‘„π‘›βˆ’1 + π‘„π‘›βˆ’2, βˆ€π‘› β‰₯ 2 The pair (𝑃𝑛, 𝑄𝑛) is called reduced 𝛽-fractionary expansion of 𝑓 for all 𝑛 β‰₯ 0. Proposition 4.1. Let 𝑓 ∈ π”½π‘ž(π‘₯, 𝛽) such that 𝑓 = [𝐴0, 𝐴1, 𝐴2, β‹― , 𝐴𝑛, β‹― ]. Then |𝑓 βˆ’ 𝑃𝑛 𝑄𝑛 | < 1 |𝑄𝑛|2. Proof. Similarly to the classical case.
  • 4. Kammoun Rania et al. Continued 𝜷-fractions with Pisot unit base in 𝑭𝒒 ((π’™βˆ’πŸ )) Β© 2017, AJMS. All Rights Reserved. 233 Proposition 4.2. Let 𝛽 be a quadratic Pisot unit power formal series such that deg(𝛽) = π‘š and 𝑃1, 𝑃2, β‹― , π‘ƒπ‘š ∈ π”½π‘ž[π‘₯]𝛽. Then, π›½π‘šβˆ’1 𝑃1𝑃2 β‹― π‘ƒπ‘š ∈ π”½π‘ž[π‘₯]𝛽. The proof of the last proposition is an immediate consequence of Thoerem 2.3. Corollary 4.3. Let 𝑃1, 𝑃2, β‹― , 𝑃 π‘š ∈ π”½π‘ž[π‘₯]𝛽. Then we have, for all positive integer 𝑛, 𝛽 (π‘šβˆ’1)𝑛 π‘š 𝑃1𝑃2 β‹― π‘ƒπ‘š ∈ π”½π‘ž[π‘₯]𝛽. Corollary 4.4.Let (𝑃𝑛, 𝑄𝑛)𝑛β‰₯0 the reduced 𝛽-fractionary expansion of 𝑓 . Then 𝛽 (π‘šβˆ’1)𝑛 π‘š 𝑃 𝑛 ∈ π”½π‘ž[π‘₯]𝛽 and 𝛽 (π‘šβˆ’1)𝑛 π‘š 𝑄𝑛 ∈ π”½π‘ž[π‘₯]𝛽. For 𝑃 = π‘Žπ‘ π›½π‘  + β‹― + π‘Ž0 ∈ π”½π‘ž[π‘₯]𝛽. We denote by 𝛾(𝑃) = π‘š deg𝛽(𝑃) + deg𝑠(π‘Žπ‘ ) = 2π‘š + deg(π‘Žπ‘ ). Lemma 4.5. [4] Let 𝐴, 𝐡 ∈ π”½π‘ž[π‘₯]𝛽 with 𝛾(𝐴) > 𝛾(𝐡). Then there exists 𝐢, 𝐴1 and 𝐡1in π”½π‘ž[π‘₯]𝛽, such that 𝐴 𝐡 = 𝐢 + 1 𝐴1 𝐡1 with 𝛾(𝐴1) > 𝛾(𝐡1). Proof of Theorem 4.1 It is equivalent to prove that there exist 𝑛0 β‰₯ 1, 𝐴𝑛 ∈ (π”½π‘ž[π‘₯]𝛽) β€². By Lemma 4.2, we obtain 𝑓 = 𝑃 𝑄 ∈ π”½π‘ž(π‘₯)𝛽 such as 𝑃, 𝑄 ∈ π”½π‘ž[π‘₯]𝛽 and (𝑃 𝑛, 𝑄𝑛) the reduced 𝛽-fractionary expansion of 𝑓. By proposition 4.1, | 𝑃 𝑄 βˆ’ 𝑃𝑛 𝑄𝑛 | < 1 |𝑄𝑛|2 . According to Corollary 4.3 and Lemma 4.5, we have (𝛽 (π‘šβˆ’1) π‘š (𝑛+1) (𝑃𝑄𝑛 βˆ’ 𝑄𝑃 𝑛)) inπ”½π‘ž[π‘₯]𝛽 .So, we obtain 1 |𝑄| < |𝛽|(π‘šβˆ’1)(𝑛+1)/π‘š | 𝑃𝑄𝑛 βˆ’ 𝑄𝑃 𝑛 𝑄 | < |𝛽| (π‘šβˆ’1)(𝑛+1) π‘š |𝑄𝑛| which implies that deg(𝑄𝑛) ≀ deg(𝑄) + (π‘š βˆ’ 1)(𝑛 + 1), where deg(𝑄𝑛) = βˆ‘ deg(𝐴𝑖) 𝑛 𝑖=1 ≀ deg(𝑄) + (π‘š βˆ’ 1)(𝑛 + 1). Thus βˆ‘ (deg(𝐴𝑖) βˆ’ (π‘š βˆ’ 1)) ≀ deg(𝑄) + (π‘š βˆ’ 1) 𝑛 𝑖=1 . Finally there exists 𝑛0 β‰₯ 1, such that, for deg(𝐴𝑖) βˆ’ (π‘š βˆ’ 1) ≀ 0, for all 𝑖 β‰₯ 𝑛0 and the desired result is reached. REFERENCES 1. P. Bateman and L. Duquette. The analogue of Pisot- Vijayaraghvan numbers in fields of power series, Ill. J. Math, 6, (1962), 594-606. 2. J. Bernat. Continued fractions and numeration in the Fibonacci base, Discrete Mathematics, 22, (2006), 2828-2850. 3. R. Ghorbel, M. Hbaib and S. Zouari. Arithmetics on beta-expansions with Pisot bases over πΉπ‘ž((π‘₯βˆ’1 )), Bull. Belg. Math. Soc. Simon Stevin, 21, (2014), 241-251. 4. M. Hbaib, R. Kammoun. Continued beta-fractions with formal power series over finite fields, Ramaujan J Math, (2015), DOI 10.1007/s11139-015-9725-5. 5. A. RΓ©nyi. Representations for real numbers and their ergodic properties, Acta Math. Acad. Sci. Hung, 8, (1957), 477-493. 6. K. Scheicher. Beta-expansions in algebraic function fields over finite fields, finite fields and their Applications, (2007), 394-410.