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A NOTE ON UNIFORM MATRIX SUMMABILITY

Shyam Lal

1

, Mradul Veer Singh

2

and Saurabh Porwal

3*

1

Department of Mathematics, Faculty of Science, Banaras Hindu University, Varanasi, (U.P.) - INDIA E-mail: [email protected]

2

Department of Mathematics, Lovely Professional University, (Punjab), INDIA E-mail: [email protected]

3

Department of Mathematics, UIET, CSJM University, Kanpur-208024, (U.P.), INDIA E-mail: [email protected]

(Received on: 07-12-11; Accepted on: 23-12-11)

________________________________________________________________________________________________ ABSTRACT

T

he purpose of the present paper is to establish a new result concerning uniform matrix summability of conjugate series of a Fourier series. Relevant connections of the results presented herewith various known results are briefly indicated.

Key Words: Uniform triangular matrix summability, Conjugate series of Fourier series, Fourier coefficients, Nörlund summability.

AMS 2010 Mathematics Subject Classification: 42A24, 40C05.

________________________________________________________________________________________________

1. INTRODUCTION AND PRELIMINARIES:

Let

f

be

2

π

periodic, Lebesgue integrable function with Fourier series given by

=

+

+

1

0

(

cos

sin

)

2

1

)

(

n

nx

n

b

nx

n

a

a

x

f

. (1.1)

The conjugate series of series (1.1) is given by

1 1

( sin

n n

cos )

n

( )

n n

a

nt

b

nt

B t

∞ ∞

= =

=

. (1.2)

Let

T

=

(

a

n,k

)

be an infinite lower triangular matrix satisfying Silverman-Töeplitz [9] conditions of regularity i.e.

(i)

=

as n

a

n

k

n,k

1

0

(ii)

a

n,k

=

0

for k

>

n

and

(iii)

=

n

k

n,k

M

a

0

where M is finite constant.

Let

=0

)

(

n

n

x

u

be an infinite series defined in

[

a

,

b

]

[

π

,

π

]

. The

n

th partial sum of the series

=0

)

(

n

n

x

u

is

given by

(

)

(

)

[

,

]

0

b

a

x

x

u

x

S

n

n

=

=

ν

ν .

(2)

© 2012, IJMA. All Rights Reserved 234

If there exists a bounded function

S

(

x

)

such that

{

}

0

( )

n

( )

( )

n n,k k

k

t x

a S x

S x

=

=

,

=

o

(1),

as n

→ ∞

,

uniformly

x

[

a

,

b

]

then we say that the series

∞ =0

)

(

n n

x

u

is summable (T) uniformly in

a

x

b

to the

sum

S

(

x

)

.

Particular Cases:

Several authors such as ([1]-[4]), (see also [5]) studied the matrix summability method and obtained many interesting results.

The important particular cases of the triangular matrix means are:

(i) Cesàro mean of order 1 or (C, 1) mean if ,

1

1

n k

a

k

n

=

+

.

(ii) Harmonic means when ,

1

=

(

1) log

n k

a

n k

− +

n

.

(iii) (C, ) means when ,

1

1

n k

n

k

a

n

δ

δ

δ

δ

− + −

=

+

.

(iv) (H, p) means when

1

, 1

0

1

log (

1)

(log)

(

1)

p q

n k p

q

a

k

n

− −

=

=

+

+

.

(v) Nörlund means when , n k n k

n

p

a

P

=

, where

=

=

0 k

k

n

p

P

,

P

n

0

.

(vi) Riesz means

(

N

,

p

n

)

when , k n k

n

p

a

P

=

,

P

n

0

.

(vii) Generalised Nörlund Means (N, p, q) when , n k k n k

n

p

q

a

R

=

. where

=

=

0 k

k n k

n

p

q

R

,

R

n

0

.

We denote

S

n

(

x

)

, the nth partial sum of the series (1.2).

Let

1

1

( )

( )cot

2

2

n

n n

t

f

f x

t

dt

π

ψ

π

=

= −

, (1.3)

f

(

x

)

=

∞ →

n

lim

f

n

(

x

)

, (1.4)

ψ

(

t

)

=

f

(

x

+

t

)

f

(

x

t

)

, (1.5)

Ψ

=

t

du

u

t

0

)

(

)

(

ψ

, (1.6)

− = =

=

=

n

n k

k n o

k

k n n

n

a

a

A

τ τ

τ , ,

, , (1.7)

where

=

=

t

1

τ

integral part of

t

1

(3)

and

=

+

=

n

k t

k n n

t

k

a

t

K

0 2

2 1 ,

sin

)

cos(

2

1

)

(

π

, (1.9)

Saxena [6] discussed the uniform harmonic summability of conjugate series of a Fourier series in the following form:

Theorem: 1.1 If

Ψ

=

=

t t

t

o

du

u

t

1

0

log

)

(

)

(

ψ

, uniformly in a set E, as

t

+

0

, then the series (1.2) is

summable by harmonic means uniformly in E to the sum

f

(

x

)

, provided the limit (1.4) exists uniformly in E.

Tripathi and Singh [8] extended the above result to the case of uniform Nörlund summability in the following form:

Theorem: 1.2 If the sequence

{ }

q

n is real, non-negative and monotonic non-increasing sequence of coefficients such

that

Q

n

as

n

and the function

λ

(

t

)

,

β

(

t

)

and

)

(

)

(

t

t

t

β

λ

increase monotonically with

t

and

)]

(

[

)

(

n

Q

n

O

β

Q

n

λ

=

as

n

, then if

Ψ

=

=

( )

)

(

)

(

)

(

1

0 τ

τ

β

λ

ψ

Q

q

o

du

u

t

t

t

,

uniformly in a set E, as

t

+

0

, then the series (1.2) is summable

(

N

,

q

n

)

uniformly in E to the sum

f

(

x

)

, at the point

t

=

x

, provided the limit (1.4) exists uniformly in E.

2 MAIN THEOREM:

The purpose of this paper is to generalize the result of Saxena [6] and Tripathi and Singh [8] for uniform matrix summability method. In fact, we prove the following interesting result.

Theorem: 2.1 Let

T

=

(

a

n,k

)

be an infinite triangular matrix such that the elements

(

a

n,k

)

are non-negative and non-decreasing with

k

n

and if

1 1 0

( )

( )

( )

=

log( )

t

t

t

t

t

ψ

u

du o

β

Ψ

=

, (2.1)

as

t

+

0

, uniformly in a set

E

=

[ , ]

a b

, where

β

(

t

)

is a positive function of t such that

0

log

)

(

n

n

β

as

n

→ ∞

, then the conjugate series of a Fourier series (1.2) is summable (T) uniformly in E to

0

1

( )

( )cot

2

2

t

f x

t

dt

π

ψ

π

= −

provided the limit (1.4) exist uniformly in

E

=

[ , ]

a b

.

To prove our main theorem we require the following lemmas.

3. LEMMAS:

Lemma: 3.1 If

(

a

n,k

)

is a non-negative and non-decreasing with

k

n

, then

)

(

)

cos(

,

0 2

1

, nτ

n

k k

n

k

t

O

A

a

+

=

=

for

<

t

<

δ

<

π

n

1

0

.

Proof:

− = −

= =

+

+

+

+

n

n k

k n n

k k n n

k k

n

k

t

a

k

t

a

k

t

a

τ τ

)

cos(

)

cos(

)

cos(

21

,

0 2

1 ,

0 2

1

(4)

© 2012, IJMA. All Rights Reserved 236

− = =

− ≤ ≤ ≤

+

+

+

n

n k

k n r

k n r k n

n

k

t

a

k

t

a

τ τ

τ

max

cos(

)

cos(

)

2

21

, 0

2 1 0

, ,

(by Abel’s Lemma)

τ ,τ 2

2 ,

sin

)

1

sin(

2

n

t t

n

n

A

r

a

+

+

=

+

n

k k

n

k

t

a

0 2

1

,

cos(

)

τ

τ

, ,

2

n n

n

A

t

a

+

− . (3.1)

Now

− = =

=

=

n

n k

k n k

k n n

n

a

a

A

τ τ

τ ,

0 , ,

=

a

n,nτ

+

a

n,nτ+1

+

...

+

a

n,n

(

τ

+

1

)

a

n,nτ

t

a

nnτ

, ( since

τ

=

[ ]

1t ).

Therefore n,nτ

O

(

A

n,τ

)

t

a

=

. (3.2)

By (3.1) and (3.2), we have

cos(

)

(

,

)

0 2

1

, nτ

n

k k

n

k

t

O

A

a

+

=

=

.

Lemma: 3.2 If

(

a

n,k

)

is non-negative and non-decreasing with

k

n

and

K

n

(

t

)

is given by (1.9) then

=

t

A

O

t

K

n

(

)

n,τ for

<

t

<

δ

<

π

n

1

0

.

Proof: Since for

<

t

<

δ

<

π

n

1

0

,

π

t

t

sin

,

We have

=

+

=

n

k t

k n n

t

k

a

t

K

0 2

2 1 ,

sin

)

cos(

2

1

)

(

π

+

=

t

k

a

n

k k n

t

cos(

)

sin

2

1

2 1

0 , 2

π

.

2

[

(

)

]

2

1

π

π

t

O

A

n

from Lemma 3.1

=

t

A

O

t

K

n

(

)

n,τ .

Hence the lemma is proved.

4. PROOF OF THE MAIN THEOREM:

It is well known that the integral formula for the kthpartial sum of conjugate series of a Fourier series (1.2) is given by, (see [7]):

S

x

t

k

t

t

dt

t

k

+

=

π

ψ

π

0 2

2 2

1

sin

cos

)

cos(

)

(

2

(5)

S

k

x

f

x

t

k

t

t

dt

+

=

π

ψ

π

0 2

2 1

sin

)

cos(

)

(

2

1

)

(

)

(

Now

a

{

S

x

f

x

}

t

a

k

t

t

dt

n

k

k n k

n

k

k n

+

=

= =

π

ψ

π

0 2

2 1

0 , 0

,

sin

)

cos(

)

(

2

1

)

(

)

(

t

a

k

t

dt

t n

k

k n

+

=

=

π

π

ψ

0 2

2 1

0 ,

sin

)

cos(

2

1

).

(

=

t

K

n

t

dt

π

ψ

0

)

(

)

(

(4.1)

So in order to prove our main theorem, we have to show that

(

)

(

)

(

1

)

0

o

dt

t

K

t

n

=

π

ψ

, uniformly in E. (4.2)

We set

dt

t

K

t

dt

t

K

t

dt

t

K

t

dt

t

K

t

n n n n

n n

+

+

=

π

δ δ

π

ψ

ψ

ψ

ψ

(

)

(

)

(

)

(

)

(

)

(

)

(

)

(

)

1 1

0 0

=

I

1

+

I

2

+

I

3, say (4.3)

Since limit (1.4) exists uniformly in E so

(

)

(

)

(

1

)

2

1

1

0

o

dt

t

K

t

n

n

=

ψ

π

, uniformly in E. (4.4)

Also, for

n

t

1

0

<

<

,

=

+

n

k t

t

k n

t

k

a

0 2

2 2

1

,

sin

cos

)

cos(

2

1

π

=

+

=

n

k t

t t

k n

k

k

a

0 2

2 2 ,

sin

sin

)

1

sin(

2

2

1

π

=

+

n

k t

t t

k n

k

k

a

0 2

2 2

,

sin

sin

.

sin

)

1

(

1

π

(Since

sin

kt

k

sin

t

for

0

<

t

<

n1 )

=

+

=

n

k k

n

k

k

t

a

O

0

,

.

(

1

)

=

=

n

k k n

a

t

n

O

0 , 2

(6)

© 2012, IJMA. All Rights Reserved 238 Hence 1 1 0

( )

( )

n n

I

=

ψ

t K

t dt

= =

+

+

=

n n

dt

t

a

dt

t

k

a

t

t n k k n t t n k k n 1 1 0 2 0 , 0 2 2 2 1 0

,

(

)

cot

2

1

sin

cos

)

cos(

2

1

)

(

ψ

π

π

ψ

I

t

O

n

t

dt

n

)

(

.

)

(

2 0 1 1

ψ

+

o

(

1

)

, uniformly in E, (using (4.4) and (4.5))

O

n

t

dt

n

1 0

)

(

).

(

ψ

+

o

(

1

)

, uniformly in E,

(

1

)

log

)

(

).

(

o

n

n

n

o

n

O

+

β

, uniformly in E, (by condition (2.1))

(

1

)

log

)

(

o

n

n

o

+

β

, uniformly in E,

=

o

(

1

)

, as

n

, uniformly in E (by hypothesis of theorem) (4.6)

Now

I

t

K

t

dt

n n

=

δ

ψ

1

)

(

)

(

2

t

dt

t

A

O

I

n n

=

δ τ

ψ

1

)

(

.

).

1

(

,

2 (by using Lemma 3.2)

=

Ψ

Ψ

t

dt

t

A

dt

d

t

t

A

O

n n n n δ τ δ τ 1 1

)

(

.

)

(

.

).

1

(

, ,

=

+

+

δ τ δ τ δ

τ

β

β

β

n n n n t t t t n t t n

A

d

t

t

dt

t

t

A

t

t

A

o

1 1 1

)

(

)

log(

)

(

.

1

)

log(

)

(

.

)

log(

)

(

.

).

1

(

, 1 1 1 1 2 , 1 1 ,

[ ]

[ ]

[ ]

+

+

+

=

n u n n u n n n n

A

d

u

u

o

du

u

u

u

A

o

n

n

A

o

A

o

δ δ

δ

β

β

β

β

δ δ 1 1 1

)

(

log

)

(

log

)

(

log

)

(

log

, , , 1 1 ,

( )

( )

[ ]

[ ]

[ ]

+

[ ]

+

+

+

=

+ = + = n k k n n k k n n n

a

n

n

o

a

o

n

n

A

o

o

o

1 , 1 , 1 1 , 1 1

.

log

)

(

.

log

log

)

(

1

1

δ δ

β

β

β

δ δ

(Applying the Mean Value Theorem for integrals)

( )

( )

( )

1

(

1

)

log

)

(

).

1

(

1

1

o

o

n

n

o

O

o

o

+

+

+

+

=

β

(7)

Also by the virtue of Riemann Lebesgue theorem and regularity of method of summation, we have

I

3

=

o

( )

1

, as

n

, (4.8)

Thus from (4.1), (4.3), (4.6), (4.7) and (4.8), we have

{

(

)

(

)

}

(

1

)

0

,

S

x

f

x

o

a

k

n

k

k

n

=

=

, as

n

, uniformly in E.

This completes the proof of the theorem.

Remark: 1 If we put

n

k

n

a

nk

log

)

1

(

1

,

+

=

,

β

(

t

)

=

1

t

,

[ , ]

a b

=

E

then we obtain the corresponding

result of Saxena [6].

Remark: 2 The result of Tripathi and Singh [8] is a particular case of our theorem if

n k n k n

Q

q

a

,

=

− ,

=

=

n

k k

n

q

Q

0

,

)

(

log

)

(

)

(

t

Q

t

q

t

t

t

t

α

λ

β

=

and

[ , ]

a b

=

E

.

REFERENCES:

[1] Shyam Lal, On the degree of approximation of conjugate of a function belonging to weighted

W L

(

P

,

ξ

( )

t

)

class by matrix summability means of conjugate series of a Fourier series, Tamkang J. Math., 11 (2000), 7-16.

[2] Shyam Lal and J.K. Kushwaha, Approximation of conjugate of functions belonging to the generalized Lipschitz class by lower triangular matrix means, Int. J. Math. Anal., 3 (2009), 21, 1031-1041.

[3] Shyam Lal and Purnima Yadav, Matrix Summability of the conjugate series of derived Fourier series, Tamkang J. Math., 33 (1) (2002), 35-43.

[4] M.L. Mittal and R. Kumar, On matrix summability of Fourier series and its conjugate Series, Bull. Cal. Math. Soc., 82 (1990), 363-368.

[5] K. Qureshi, On the degree of approximation of a periodic function by almost Nörlund means of its Fourier series, Tamkang J. Math., 12 (1), (1981), 35-38.

[6] Ashok Saxena, On uniform harmonic summability of Fourier series and its conjugate series, Proc. Nat. Inst. Sci. India Part A, 31(1965), 303-310.

[7] E. C. Titchmarsh, Theory of Functions, Second edition, Oxford Press, (1939).

[8] L. M. Tripathi and K. N. Singh, On the uniform Nörlund summability of Fourier Series and its conjugate series, Bull. Cal. Math. Soc., 72(1980), 233-239.

[9] O.Töeplitz,Überallagemeiene lineare Mittel bildunger, P.M.F., 22(1913), 113-119.

[10] A. Zygmund, Trigonometric series, Cambridge University Press, (1977).

References

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