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Some Properties on the Error-Sum Function of

Alternating Sylvester Series

Huiping Jing, Luming Shen*

Science College of Hunan Agricultural University, Changsha, China Email: [email protected], *[email protected]

Received July 11, 2012; revised September 21, 2012; acceptedSeptember 29, 2012

ABSTRACT

The error-sum function of alternating Sylvester series is introduced. Some elementary properties of this function are studied. Also, the hausdorff dimension of the graph of such function is determined.

Keywords: Alternating Sylvester Series; Error-Sum Function; Hausdorff Dimension

1. Introduction

 

 

For any x

0,1

, let d1:d1

 

xN and

  

: x  0,1

T T be defined as

 

 

 

x T,

 

0 : 0.

x

      

1

1

1 , : 1

d x x

x d

  (1)

where

denote the integer part. And we define the sequence

dn

 

x ,n2

as follows:

 

1

1 ,

n

d Tx

n

T T T

0Id0,1

 

n

d x  (2)

where denotes the nth iterate of .

It is well known that from the algorithm (1), all

0,1 x

 

can be developped uniquely into an infinite or finite series

 

 

1 1 1

where

i i

i i

x

x d

  

   

1

1 ,

1 .

i

i

d x

x d x

 

 

, ,d x ,

  

(3)

In the literature [2], (3) is called the Alternating

Balkema-Oppenheim expansion of x and denoted by

n

  for short. From the algorithm,

one can see that T maps irrational element into irrational element, and the series is infinite. While for rational numbers, in fact, we have

 

1 xd x

0,1 x

 

1 , ,

d x

is rational if and

only if its sequence of digits is terminate or

periodic, see [1-3].

For any x 0,1

and n1, define

 

 

i

 

1i 1 1

 

.

n i

p x

q x d x

 

=1

n n

From the algorithm of (1), it is clear that

 

1n

 

n n

n p x

x T x .

q x

   (4)

For any x 0,1 , let x=d1

 

x , , dn

 

x , be

its Alternating Sylvester expansion, then we have

 

   

1 1

j j j

d xd x d x  for any j1. On the other

hand, any

dj,j1

of integer sequence satisfying

 

   

1

dj1 xdj x dj x  for all j1 is a Sylvester

admissible sequence, that is, there exists a unique

0,1

 

=

x such that j j

The behaviors of the sequence n are of interest and the metric and ergodic properties of the sequence

d x d j1

 

d x

for all , see [9].

dn

 

x ,n1

and T have been investigated by a

number of authors, see [1-3].

0,1 x

 

 

 

, define For any

1

: n ,

n n

p x

S x x

q x

 

 

   

 

(5)

and we call S x

 

 

the error-sum function of Alternating

Sylvester series. By (4), since n1 n

n

 

for all , then

1 d xd x d x  1

nS x

 

1 and S x is well defined.

In this paper, we shall discuss some basic nature of

 

 

S x , also the Hausdorff dimension of the graph of

 

S x

 

is determined.

S

2. Some Basic Properties of

x

1 n

In what follows, we shall often make use of the symbolic space.

For any , let

1, 2, , : 1 1

for all1 .

n

n n k k k

D N

k n

     

   

 

Define

(2)

0

, : .

n D

  

, , ,n

Dn

  

0

n

D D

 

For any  1 2 , write

 

1 1

1 n ,

n

1 2

1 1

A

  

  

   (6)

 

1 1

1

1 n

n B

  

     

1 2

1 1

. (7)

We use J to denote the following subset of (0,1],

 

 

2 2

0,1 : , ,

J x d

d x

  

 

1 1,

.

n n

x

d x

 

  (8)

From theorem 4.14 of [8], we have J

A B,

when is even, and

n J

B,A

when is odd.

Finally, define

n

D nn, 1.

, ,

IA B  (9)

Lemma 1. For any n1 and x 0,1

0 0;

 

,

1) limS x

 

(10)

x

2) 17S x

 

0;

 

30 (11)

3)

 

   

1

 

.

n

n n

p x

S T x

 

 

   

1 1

j j

dxd x d x

1

d x

1

2 2

1 2 ,

n

d

1 2 2

2 2

1

> n 1 n .

d

 

 

2

1

 

 

2

> n n

d a x 1

i

i i

S x x

q x

   

 

(12)

Proof. 1) Since j and

, so when , we can get

 

1 n3

> >

n n

d d

accordingly

2 1

n

d d d

 

 

2

 

a x d x d x

we write 1 1 , so

.

Now

 

 

1

n

d x n1 T x

       

 implies

 

 

 

1 1

nn

1 n 1 ,

d x

  0Tn

 

x 1.

 

1 T x

d x  for

Thus

 

 

 

 

 

 

 

 

 

 

2 1

2 2

1 2

1

n n n

n

n n

T x

a x

 



1 1

2 2

2

1 1

1 1

1

1 1

, 1

n n

n

S x T x

d x d x

a x a x

 



 

0

x  d1

 

x   a x

 

 

   

      

let , we have and ,

thus

 

0

S x

1

2 2

1 > > 2 ,

n

n n

d dd

2) From 1) we know that

from the definition of d xi

we also know that d11,

so d2 d d1

1 1

2,

1

2 1

1 2 4 ,

n n

n

d d   

 

 

 

thus

2 2

1 2 2

1 1 1 17

1 .

2 4n 30

n n n

S x

d x

 

 

   

 

nm

 

 

3) Since as ,

 

 

 

 

 

1 .

m n m m

n m

m

n m n m

p T x

p x p x

q x q x q T x

 

  

 

Thus

 

 

 

 

 

 

 

 

 

 

     

 

 

 

 

 

   

 

 

 

1

1 1

1 1

1 1

1 1

1

i

i i

n

i n n i

i i i n n n i

n n

i n

n n

i n

n

i i i n i n

n n

i n

i n

n

i i i i

p x

S x x

q x

p x p x p x p x

x x

q x q x q x q x

p T x

p x

x T x

q x q T x

p T x p x

x T x

q x q T x

 

  

  

 

 

   

 

   

        

   

 

 

 

      

 

 

 

 

 

     

 

 

 

 

 

 

1

1 .

n

n

i n

i i

p x

x S T x

q x

 

  

 

 

 

 

= \ 1 . II

Let

I

 , if

Proposition 2. For any x

 

, ,

 

1 2k 1

xd xd x

 

 

, then S x is left continuous but not right continuous. If x d1 x , , d2k

 

x , then

 

S x

1

nD

is right continuous but not left continuous. Proof. For any and   n, write x1A ,

2

xB, where A, B are given by (6) and (7).

= 2 1

n k

Case I,  , then

1

1 2 2 1

1 1 1

k x

  

    (13)

2

1 2 2 1

1 1 1

1

k x

      

 (14)

and J = B,A . For any x1 J , since when

2k 1= 2k 2k 1 ,

(3)

   

 

 

1 2 2

1 2 2

1 2 2

1 1 1

1 1 1

1 1 1

k

        

   

   

    

2 1

2 2

1

1 1

. 1 k k

k k k

  

 

2 2

> 1

k k k

2This situation is included in Case II, so we can take 1    and

2k1 2k1 .

1 1

1 for some

x x  

   

i.e.

1 1, ,

x  2k,2k1, 

   

 

 

 

 

 

 

 

 

2 1

1 1 1

1 2 1

1

1 1

2 2

2 1

k

i k

i

i i

p x

S x S x x x

q x

p x

x S

q x

k

T x

 

 

        

 

 

 

1 2 2 1

1

1 2 2 1

2 2

1 1

2 2

1 1

i k

i k

k

k k

p x

q x

T x

S T x

  

 

    

 

 

    

 

   

 

By (2),

 

n

 

 

0Tn

 

x 1,

1 1

1 1

, for

1 1

n n

T x

d x   d x

which implies

 

 

 

 

 

 

 

1

1 1

1 1

1 1

1

1

n n

n n

n n

T x T x

d x d x

d x d x

 

 

 

1

1 1

n

dx

 

 

and

 

2 2 1

k

Tx 1

0 .

1

 

 

Let   2 2

 

1 0

k  

 

2 2

1 0

k

x

 

1 1 ,

 

S x 1

, we get T x and

, thus

S T

 

m S x S x

1 1

li

xx

and this implies is left continuous at x .

Let

1 1

2 1 2 1 2 1

1for som

k k

x x

  

  

 

2 1

e

1 k 1 k 1 ,

 

1 1 2 2 1 2 1

. , , k, k 1, k

i e        12k1,  ,,

then

 

 

 

 

 

 

 

 

 

 

 

1 1

2

1 2 1 1

1 11

1 1 2 1 1

2 2 1 2 3 1 2 3

1 1 1

2 2 1 2 3 1

2

1 2 1 1

1 1

1 1 2 1 1

k

i k

i i k

k k k

k k

k

i k

i i k

S x S x

p x p x

x x

q x q x

p x p x

x x S T x

q x q x

p x p x

x x

q x q x

 

  

 

 

 

     

 

      

   

     

  

     

   

   

       

   

 

2 3 1

2 3 1

2 1 2 1

2 2 1 .

1

k k

k k

k

T x S T x

   

 

 

 

 

   

Let  

 

  

, we have

1 1

1 1

2 1 2 1

1 lim

1

x x

k k

S x S x

 

   

 

S x is not right continuous at 1

and this implies x .

For

2

1 2 2 1

1 1 1

, 1

k x

  

    

 

 

(15)

following the same line as above, we have

2 2

2 2

2 1 2 1

1

lim .

1

x x

k k

S x S x

 

    

2

nk

Case II Let

1

1 2 2

1 1 1

k y

  

    (16)

2

1 2 2

1 1 1

1

k y

  

    

 

  

(17)

Following the same line as above, we have

1 1 1 1 2 2

1

lim ,

1

y y

k k

S y S y

 

    

 

 

2 2

2 1

2 2

1

lim ,

1

y y

k k

S y S y

 

     

   

,

S y S y

1

nD

and 1 2

Corollary 3. For any and n

is right continuous.

, write



1 max A B, 

  , 2 min

A B,

. Then for any xJ, if n= 2k1, then

 

 

 

*

2 1 ,

S  S xS

 

 

where *

2 2

2 1 2

1 1

k k

SS

 

n

D

.

From the corollary, for any 

   

 

,

sup

1

x y J

n n

n

S x S y n J

    

(4)

here

 

J J

w  is the Lebesgue measure of  .

Theorem 4. S x

 

is continuous on

0,1 \

I. Proof: For any x

0,1 \

I and x1,

x x r at y

let

 

n ing vester

n

n d

 

d1 x , ,d ,

   be its Alte S l

1

 , it

n

 

d x1 , ,

 

ex

 pansion. For anyn . By (Corollary 3), for any e

 n

y J

 , we have

   

wr

 

x

 

 

 n 0, as .

S yJ

   

S x n

 

0

Write IC , where

1 2

 

 

2 1

1 1 1

k C

 

 

Theorem 5. If a < <S b

 

, then t S c

 

y.

0 < < < 1,a b S there exists c

 

a b, \

 

I0 , such tha

 

y

Proof. Set g x

 

S xy, then g x

 

has the same

continuity as S x

 

. Write

 

 

0, ,

, sup .

Ex g xxa b x0E

trivially, aE, then the set is well defined.

If

 1, 2, ,2k1

, then by the left continuity of

ve

x

1> 0 b

ha

 

S b , we

lim

x b

g

g b

 

0,

As a result, there exists a  ch that for any

, ,b

.

su

 

> 0

g x

1

x b

If b

 1, 2, ,2k

, since g b

 

en 2

is not left con- tinuous, th  > 0 such that for any x 

b 2,b

,

 

0

g x  , that is x0b

sam .

Following the e line as above, we can prove

0> x a.

Now we shall prove that g x

 

0 0. We can choose

n

xE such that xnx0, if 0

1 2 2k 1

th

m 0,

 

, , , x     ,

en

0

n x

g x0

li g x

n

x

if x0

 1, 2, ,2k

, then

  

0

 

m 0

n

n x x

k k

g x g x

 

  

 

0 0

g x  . Following the sam line as

 

0 0

g x  , and

0

2 2

1

li 1

In both case above, we can

e prove

0  1, 2, ,

Therefore, there e 

 

a b, \

 

I0 , such that

 

= .

S c y

2 1 xists

k

x .

c

Theorem 6.

 

 

 

2 1

0 0

9 π

d d ,

S x x

x 

11

1 k k 6

k S x



0.1250.

Proof.

 

 

and 1

 

0S x dx 

 

 

1 1 1 1

1

1 1 1

1 1 1 1 1 1

1 1

1

1 1

1 1

1 1 1

1

1 1 1

1 1 1

1 1 1 1 1 1 1

d d

1

d

1

d d d

d d d

d d d

d d d

d d d d d d

S x x S x

x S T x x

d

0 x

x x x S T x x

d



 



  

     

       

 

 

  

 

Let

 

1

1

Tx u x

d x

   , then du dx thus

 

 

1

1 1

1 1

1 1 1

2 2

1

1 1

2 0

1 1 1 1 1 1

1 1

d

2 1

1 1 d

1

d

d d

d d d

x

d d

S u u d d

d

 

  

  

 

 

 

 

  



thus,

 

 

1 0

1

S x

 

1

2 1

1

1

2 0

1 1 1

3 1 9 π

d d .

2 6

k k

k d

S x x S x x

d

 

 

 

 

Through the MATLAB program we can get the de- finite integration

1

3. Hausdorff Dimension of Graph for

0

 

0S x dx 0.1250.

 

S x

Write

 

,

 

,

0,1 .

Gr Sx S x x

Theorem 7. dimHGr S

1.

Proof. For any n1,

JS J

 

 ,Dn

is a

covering of Gr S

 

. From (Cor 3), JS J

can be

covered by n squares with side f length o 

 

J . For

any > 0,

 

 

 

 

 

1

1 1

1

liminf 2 2 2

liminf 2 2 0.

n

n n

D n n

S

n n

n

 

1

1 liminf 2

n

n D

HGr n J





 

Thus,

 



 

dimHGr S 1

Since

,

 

,

 

,

 

,( ,

 

Proj x S xProj y S yd x S x y S y ,

th

en

 

 

1 1 1

1 0,1 H 0,1 H Proj G SrG Sr ,

 

mHGr S 1

di .

(5)
[image:5.595.60.290.83.273.2]

Figure 1. The graph of S(x).

4. Acknowledgements

This work is s ion De

[1] S. Kalpazidou, A. Knopfmacher and J. Knopfmacher, “Lü roth-Type Alt entations for Real Numbers,” Ac , No. 4, 1990, pp.

No. 3, 1991, pp. 319-325.

p. 311-

ol. 8, No. 2, 1996, pp. 331-346. B44, 1992, pp. 17-28.

[3] S. Kalpazidou, A. Knopfmacher and J. Knopfmacher, “Me- tric Properties of Alternating Lüroth Series,” Potugaliae Mathematica, Vol. 48,

[4] J. Barrionuevo, M. Burton-Robert, Dajani-Karma and C. Kraaikamp, “Ergodic Properties of Generalized Lüroth Series,” Acta Arithmetica, Vol. 74, No. 4, 1996, p

327.

[5] K. Dajani and C. Kraaikamp, “On Approximation by Lü- roth Series,” Journal de Théorie des Nombres de Borde- aux, V

doi:10.5802/jtnb.172

[6] K. J. Falconer, “Fractal Geometry, Mathematical Founda- tions and Applications,” Wiley, Hoboken, 1990.

06, pp. 223-232. [7] K. J. Falconer, “Techniques in Fractal Geometry,” Wiley,

Hoboken, 1997.

[8] J. Galambos, “Reprentations of Real Numbers by Infinite Series,” Lecture Notes in Math, Springer, Berlin, 1976. [9] L. M. Shen and J. Wu, “On the Error-Sum Function of

Lüroth Series,” Mathematics Analysis and Applications,

Vol. 329, No. 2, 2007, pp. 1440-1445.

upported by the Hunan Educat part-

ment Fund (11C671).

[10] L. M. Shen, C. Ma and J. H. Zhang, “On the Error-Sum Function of Alternating Lüroth Series,” Analysis in The- ory and Applications, Vol. 22, No. 3, 20

REFERENCES

doi:10.1007/s10496-006-0223-x

[11] T. Sálat and S. Znám, “On the Sums of Prime Powers,”

Acta Universitatis Palackianae Olomucensisof Mathema-tica, Vol. 21, 1968, pp. 21-25.

- ernating Series Repres

ta Arithmetica, Vol. 55

311-322.

doi:10.5802/jtnb doi:10.1007/s10496-006-0223-x

Figure

Figure 1. The graph of S(x).

References

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