• No results found

Bounding the Cebysev functional for a function that is convex in absolute value and applications

N/A
N/A
Protected

Academic year: 2020

Share "Bounding the Cebysev functional for a function that is convex in absolute value and applications"

Copied!
22
0
0

Loading.... (view fulltext now)

Full text

(1)

BOUNDING THECEBYˇ SEV FUNCTIONAL FOR A FUNCTION THAT ISˇ CONVEX IN ABSOLUTE VALUE AND APPLICATIONS

Silvestru Sever Dragomir

Abstract.Some sharp bounds for theCebyˇ ˇsev functional of a function that is convex in absolute value and applications for functions of self-adjoint operators in Hilbert spaces via the spectral representation theorem are given.

Keywords: Cebyˇ sev functional, self-adjoint operator, spectral representation theorem,ˇ

integrable function, integral mean.

1. Introduction

For two Lebesgue integrable functions f,: [a,b] → C, in order to compare the integral mean of the product with the product of the integral means, we consider theCebyˇˇ sev functionaldefined by

Cf,:= 1 ba

b

a f(t)(t)dt

1 ba

b

a f(t)dt·

1 ba

b

a (t)dt.i

In 1934, G. Gr ¨uss [14] showed that

(1.1) Cf,≤ 14(M−m) (Nn),

providedm,M,n,Nare real numbers with the property that

(1.2) − ∞<mfM<∞, −∞<n≤≤N<∞ a.e. on [a,b].

The constant 1

4 is best possible in (1.1) in the sense that it cannot be replaced by a smaller one.

Another lesser known inequality forCf,was derived in 1882 byCebyˇ ˇsev [4] under the assumption that f,exist and are continuous on [a,b],and is given by

(1.3) Cf,≤ 121 f

∞∞(b−a)

2,

Received May 02, 2015; Accepted November 05, 2015

2010Mathematics Subject Classification.Primary 26D15; Secondary 47A63, 47A99

(2)

wheref

∞:=supt∈[a,b]f(t)<∞. The constant 1

12cannot be improved in general in (1.3). ˇ

Cebyˇsev’s inequality (1.3) also holds if f, : [a,b] → R are assumed to be absolutely continuous and f,L[a,b].

In 1970, A.M. Ostrowski [18] proved, amongst others, the following result that is in a sense a combination of theCebyˇ sev and Gr ¨uss results:ˇ

(1.4) Cf,≤ 1

8(b−a) (Mm)∞,

provided f is Lebesgue integrable on [a,b] and satisfying (1.2) while: [a,b]→R is absolutely continuous andL

∞[a,b].Here the constant 18is also sharp. In 1973, A. Lupas¸ [16] (see also [17, p. 210]) obtained the following result as well:

(1.5) Cf,≤ 1

π2f22(b−a), provided f,are absolutely continuous and f,L2[a,b].

Here the constant 1

π2 is the best possible as well.

In [2], P. Cerone and S.S. Dragomir proved the following inequalities:

Cf,

(1.6)

⎧ ⎪⎪⎪⎪ ⎪⎪⎪⎪ ⎪⎨ ⎪⎪⎪⎪ ⎪⎪⎪⎪ ⎪⎩

inf

γ∈R

−γ· 1

ba b

a

f(t)− 1

ba b

a f(s)ds dt,

inf

γ∈R

−γq· 1

ba b

a

f(t)− 1

ba b

a f(s)ds pdt

1 p

wherep>1, 1/p+1/q=1.

Forγ=0,we get from thefirst inequality in (1.6)

(1.7) Cf,≤·b1a

b

a

f(t)−b1a

b

a f(s)ds dt for which the constant 1 cannot be replaced by a smaller constant.

Ifm≤ ≤ Mfor a.e. x ∈ [a,b],then− m+M

2 ∞ ≤ 12(M−m) and by thefirst inequality in (1.6) we can deduce the following result obtained by Cheng and Sun [5]

(1.8) Cf,≤ 12(M−m)·b1a

b

a

f(t)−b1 a

b

a f(s)ds dt.

The constant 1

(3)

Theorem 1.1. Let f : [a,b] →Cbe of bounded variation on[a,b]and: [a,b]→Ca Lebesgue integrable function on[a,b].Then

(1.9) Cf,≤ 1

2

b

a

f· 1 ba

b

a

(t)−b−1a

b

a (s)ds dt

where

b

a

fdenotes the total variation of f on the interval[a,b].

The constant 1

2 is best possible in (1.9).

We denote thevarianceof the function f : [a,b]→CbyDfand defined as

(1.10) Df=Cf,f¯1/2

⎡ ⎢⎢⎢⎢ ⎢⎣b1a

b

a

f(t)2dtb1a

b

a f(t)dt 2⎤

⎥⎥⎥⎥ ⎥⎦

1/2

,

where ¯f denotes the complex conjugate function of f.

We have [11]:

Corollary 1.1. If the function f : [a,b]→Cis of bounded variation on[a,b],then

(1.11) Df≤ 12

b

a

f.

The constant1

2 is best possible in (1.11).

Now we can state the following result when both functions are of bounded variation [11]:

Corollary 1.2. If f,: [a,b]→Care of bounded variation on[a,b],then

(1.12) Cf,≤ 14 b

a

f

b

a

.

The constant1

4 is best possible in (1.12).

Remark 1.1. We can consider the following quantity associated with a complex valued functionf: [a,b]→C,

Ef:=Cf,f1/2=

1

ba

b

a f 2(t)dt

1

ba

b

a f(t)dt

2

(4)

Utilising the above results we can state that

E2f 1 2

b

a

f· 1 ba

b a

f(t)− 1

ba

b a f(s)ds

dt (1.13) ≤1 2 b a

fDf≤ 1 4 ⎡ ⎢⎢⎢⎢ ⎢⎣ b a f ⎤ ⎥⎥⎥⎥ ⎥⎦ 2 .

If we consider

Gf:=Cf,f1/2

=b1a

b

a f(t)

f(t)dtb1a

b

a f(t)dt· 1

ba

b

a

f(t)dt

1/2 ,

then we also have

(1.14)

G2f 1

2 b

a

f· 1

ba

b

a

f(t)− 1 ba

b

a

f(s)dsdt

≤ 12 b

a

fDf≤14 b a f b a f

≤ 14

⎡ ⎢⎢⎢⎢ ⎢⎣ b a f ⎤ ⎥⎥⎥⎥ ⎥⎦ 2 and (1.15)

G2f 1

2 b

a

f

·b1a

b

a

f(t)−b1a

b

a f(s)ds

dt

≤ 12 b

a

f

Df≤14 b a f b a f

≤14

⎡ ⎢⎢⎢⎢ ⎢⎣ b a f ⎤ ⎥⎥⎥⎥ ⎥⎦ 2 .

For recent related results see [1] and [9]-[13].

Motivated by the results presented above, we establish in this paper some new bounds for the magnitude ofCf,in the case when one of the complex valued function, say f, is convex in absolute value while the other is Lebesgue integrable on [a,b].Applications for functions of self-adjoint operators in Hilbert spaces via the spectral representation theorem are also given.

2. New Results forCebyˇ ˇsev Functional

Recall that a function: [a,b]→Risconvex(strictly convex) on the interval [a,b],if

(1−t)x+ty≤(<) (1−t)(x)+ty for anyx,y∈[a,b]xyandt∈[0,1] ((0,1)).

We observe that theconstant function k(t)=k,t∈[a,b] and theidentity function e(t) =t,t ∈[a,b] can then be interpreted as convex functions. However, they are not strictly convex functions on [a,b].

(5)

Theorem 2.1. Let f : [a,b]→Cbe a measurable function such thatfis convex on[a,b] and: [a,b]→Cis a Lebesgue integrable function on[a,b].Then

(2.1) Cf,≤maxf(a),f(b) 1

ba

b

a

(t)−b1a

b

a (s)ds dt.

The inequality (2.1) is sharp.

Proof. We use Sonin’s identity

(2.2) Cf,= 1 ba

b

a

f(t)λ(t) 1 ba

b

a (s)ds

dt,

forλ=0 to get

(2.3) Cf,= b1 a

b

a f(t)

(t)−b1a

b

a (s)ds

dt.

Taking the modulus and utilizing the convexity offon [a,b] we have

Cf, ≤ 1

ba b

a f(t)

(t)− 1

ba b

a (s)ds dt (2.4)

≤ 1

ba b

a (

bt)|f(a)|+(ta)|f(b)|

ba

×(t)− 1

ba b

a (s)ds dt If we denote the right side of (2.4) byI,then we have

I≤ sup

t∈[a,b] ⎡ ⎢⎢⎢⎢ ⎣(b−t)

f(a)+(t−a)f(b)

ba

⎤ ⎥⎥⎥⎥ ⎦

×b1a

b

a

(t)−b1a

b

a (s)ds dt

=maxf(a),f(b) 1

ba

b

a

(t)−b1a

b

a (s)ds dt and by (2.4) we get (2.1).

Assume that the inequality (2.1) holds with a constantK>0,namely

(2.5) Cf,≤Kmaxf(a),f(b) 1

ba

b

a

(t)−b−1a

b

a (s)ds dt.

Consider the functions f,: [a,b]→Rdefined by

f(t) := ⎧ ⎪⎪⎪⎪ ⎨ ⎪⎪⎪⎪ ⎩

−1,ta,a+b

2

1, ta+b

(6)

and: [a,b]→R,(t)=ta+b

2 .

We havef=1, which satisfy the convexity condition with equality and

Cf,= b1a

b

a

ta+2b

dt= b4a,

maxf(a),f(b)=1

and 1 ba

b

a

(t)−b1a

b

a (s)ds

dt= b1a b

a

ta+2b

dt= b4 a

and by (2.5) we have

ba 4 ≤K

ba 4 , which shows thatK≥1.

With the notations from the introduction we have:

Corollary 2.1. Let f : [a,b] → Cbe a measurable function such thatfis convex on [a,b].Then

D2f,E2f (2.6)

≤maxf(a),f(b) 1

ba b

a

f(t)− 1

ba b

a f(s)ds dt,

and

(2.7) G2fmaxf(a),f(b) 1 ba

b

a

f(t)− b−1a

b

a

f(s)dsdt.

We recall thep-logarithmic meandefined by

Lpp(m,n) := m

p+1np+1

p+1(M−m), mn wherep−1,0 andm,n>0.

The case ofp-norm of the deviation

fb−1a

b

a f(s)ds

(7)

Theorem 2.2. Let f : [a,b]→Cbe a measurable function such thatfis convex on[a,b] and, for p>1,: [a,b]→Cis in the Lebesgue space Lp[a,b].Then

(2.8) Cf,≤Lqf(a),f(b) ⎡⎢⎢⎢⎢b1a b

a

(t)−b−1a

b

a (s)ds p

dt

⎤ ⎥⎥⎥⎥ ⎦

1/p ,

where q>1and 1

p+1q =1.

The inequality (2.8) is sharp.

Proof. Making use of H¨older’s inequality, we have

(b−a)I =ab(bt)|f(a)b|+a(ta)|f(b)| (t)− 1

ba b

a (s)ds dt (2.9)

ab(bt)|f(a)b|+(ata)|f(b)| qdt1/q

×ab(t)− 1

ba b

a (s)ds pdt1/p.

Observe that, by changing the variableu= ta

bawe have b

a (

bt)|f(a)|+(ta)|f(b)|

ba

q

dt

=(b−a)01uf(b)+(1−u)f(a)qdu.

Changing the variable again

v=uf(b)+(1−u)f(a)

we have forf(a)f(b)

(b−a)

1

0

uf(b)+(1−u)f(a)qdu= ba f(b)−f(a)

1

0 v

qdu

=(b−a)Lqqf(a),f(b)

.

Forf(a)=f(b)we also have

(b−a)

1

0

uf(b)+(1−u)f(a)qdu=(b−a)f(a)q

=(b−a)Lqqf(a),f(b)

.

Therefore

(b−a)I ≤(b−a)Lqqf(a),f(b) 1/qb

a

(t)− 1

ba b

a (s)ds pdt1/p

=(b−a)1/qL

qf(a),f(b) ab(t)− b1a b

(8)

which implies

ILqf(a),f(b) ⎛⎜⎜⎜⎜b1a b

a

(t)−b−1a

b

a (s)ds p

dt

⎞ ⎟⎟⎟⎟ ⎠

1/p .

Making use of (2.9) we get the desired result (2.8). Assume that

Cf, ≤KLqf(a),f(b)

(2.10)

× 1

ba b

a

(t)− 1

ba b

a (s)ds pdt1/p,

holds with a constantK>0 for anyp>1 and f,as above. Consider the functions f,: [a,b]→Rdefined by

f(t) := ⎧ ⎪⎪⎪⎪ ⎨ ⎪⎪⎪⎪ ⎩

−1,ta,a+b

2

,

1, ta+b

2 ,b

and: [a,b]→R,(t)=ta+b

2 .

We havef=1, which satisfies the convexity condition with equality and

Cf,= b1a

b

a

ta+2b

dt= b4a.

We also haveLqf(a),f(b)

=1 and

1

ba b

a

(t)− 1

ba b

a (s)ds pdt1/p

= 1

ba b

a ta+2b

p

dt1/p= 2

ba b

a+b 2

ta+b

2 p

dt1/p

=

2

ba(

b−a 2)

p+1

p+1 1/p

= ba

2(p+1)1/p.

If we replace these values in (2.10) we get

(2.11) b4aK(b−a)

2p+11/p for anyp>1.

Now, if we let p → 1+ in (2.11) we get K ≥ 1, which proves the desired sharpness.

(9)

Corollary 2.2. Let f : [a,b] → Cbe a measurable function such thatfis convex on [a,b]and: [a,b]→Cis in the Lebesgue space L2[a,b].Then

(2.12) Cf,≤

⎛ ⎜⎜⎜⎜ ⎜⎜⎝

f(a)2+f(a)f(b)+f(b)2

3

⎞ ⎟⎟⎟⎟ ⎟⎟⎠

1/2

D.

The following particular cases are of interest as well:

Corollary 2.3. Let f : [a,b] → Cbe a measurable function such thatfis convex on [a,b].Then

(2.13)

D2f,E2fL

qf(a),f(b)

×

⎡ ⎢⎢⎢⎢ ⎣b1a

b

a

f(t)−b1a

b

a f(s)ds p

dt

⎤ ⎥⎥⎥⎥ ⎦

1/p ,

and

(2.14)

G2fL

qf(a),f(b)

×

⎡ ⎢⎢⎢⎢ ⎣b1a

b

a

f(t)−b−1 a

b

a f(s)ds

p

dt

⎤ ⎥⎥⎥⎥ ⎦

1/p ,

where p,q>1and 1

p +1q =1.

In particular, we have

(2.15) D2f,E2f ⎛ ⎜⎜⎜⎜ ⎜⎜⎝

f(a)2+f(a)f(b)+f(b)2

3

⎞ ⎟⎟⎟⎟ ⎟⎟⎠

1/2

Df,

and

(2.16) G2f ⎛ ⎜⎜⎜⎜ ⎜⎜⎝

f(a)2+f(a)f(b)+f(b)2

3

⎞ ⎟⎟⎟⎟ ⎟⎟⎠

1/2

Df.

Thefirst inequality in (2.15) is equivalent to

(2.17) Df

⎛ ⎜⎜⎜⎜ ⎜⎜⎝

f(a)2+f(a)f(b)+f(b)2

3

⎞ ⎟⎟⎟⎟ ⎟⎟⎠

1/2

.

(10)

Theorem 2.3. Let f : [a,b]→Cbe a measurable function such thatfis convex on[a,b] and: [a,b]→Cis essentially bounded on[a,b].Then

(2.18) Cf,≤ 12f(a)+f(b) sup

t∈[a,b]

(t)− b1a

b

a (s)ds .

The inequality (2.18) is sharp.

Proof. We have

Ib1a

b

a ⎡ ⎢⎢⎢⎢ ⎣(b−t)

f(a)+(t−a)f(b)

ba

⎤ ⎥⎥⎥⎥ ⎦

×(t)−b1 a

b

a (s)ds dt

esssup

t∈[a,b]

(t)− b−1a

b

a (s)ds

×b1a

b

a ⎡ ⎢⎢⎢⎢ ⎣(b−t)

f(a)+(t−a)f(b)

ba

⎤ ⎥⎥⎥⎥ ⎦dt

=

f(a)+f(b)

2 esstsup∈[a,b]

(t)− b−1a

b

a (s)ds

and by (2.4) and (2.19) we get the desired result (2.18).

Assume that the inequality (2.18) holds with a constantD>0

(2.19) Cf,≤Df(a)+f(b)sup

t∈[a,b]

(t)−b−1a

b

a (s)ds .

Consider the functions f,: [a,b]→Rdefined by

f(t)=(t) := ⎧ ⎪⎪⎪⎪ ⎨ ⎪⎪⎪⎪ ⎩

−1, ta,a+b

2

,

1, ta+b

2 ,b

.

We havef=1, which satisfies the convexity condition with equality and

Cf,:= b1a b

a dt=1,

f(a)=f(b)=1

while

sup

t∈[a,b]

(t)−b−1a

b

a (s)ds =1.

(11)

Corollary 2.4. Let f : [a,b] → Cbe a measurable function such thatfis convex on [a,b].Then

(2.20) D2f,E2f1

2f(a)+f(b)

sup

t∈[a,b]

f(t)−b1a

b

a f(s)ds

and

(2.21) G2f 1

2f(a)+f(b)

sup

t∈[a,b]

f(t)−b−1a

b

a

f(s)ds.

3. Application for Riemann-Stieltjes Integral

The following representation is of interest in itself. The result wasfirstly obtained in [6] (see also [7]). For the sake a completeness we give here a short proof as well.

Lemma 3.1. If v : [a,b] → C is continuous (of bounded variation) on [a,b]and h : [a,b]→Cis of bounded variation (continuous) on[a,b], then we have the identity

v(b)ab(ta)dh(t)+v(a)ab(bt)dh(t)

ba

b

a v(t)dh(t)

(3.1)

=abh(t)dv(t)−v(bb)−av(a)abh(t)dt.

Proof. Integrating by parts in the Riemann-Stieltjes integral we have

v(b)ab(ta)dh(t)+v(a)ab(bt)dh(t)

ba

b

a v(t)dh(t)

(3.2)

=abv(b)(tab)+va(a)(bt) −v(t)dh(t)

= (ta)v(bb)+(abt)v(a)−v(t)h(t)b

aabh(t)d(ta)v(bb)+(abt)v(a) −v(t) =[v(b)−v(b)]h(b)−[v(a)−v(a)]h(a)

abh(t)v(bb)−av(a)dtdv(t) =abh(t)dv(t)−v(bb)va(a)abh(t)dt

and the identity is proven.

We can provide now the following application for Riemann-Stieltjes integral:

(12)

the inequalities

v(b)

b

a(ta)dh(t)+v(a)

b a(bt)dh(t)

ba

b

a v(t)dh(t)

(3.3)

⎧ ⎪⎪⎪⎪ ⎪⎪⎪⎪ ⎪⎪⎪⎪ ⎪⎪⎨ ⎪⎪⎪⎪ ⎪⎪⎪⎪ ⎪⎪⎪⎪ ⎪⎪⎩

max{|v(a)|,|v(b)|}b

a

h(t)− 1

ba b

a h(s)ds dt,

(b−a)Lq(|v(a)|,|v(b)|)

1

ba b

a

h(t)− 1

ba b

a h(s)ds pdt1/p where q>1and 1

p+1q =1,

1

2(b−a) [|v(a)|+|v(b)|] supt∈[a,b]

h(t)− 1

ba b

a h(s)ds .

Proof. From (3.1) we have

v(b)ab(ta)dh(t)+v(a)ab(bt)dh(t)

ba

b

a v(t)dh(t)

(3.4)

=abh(t)v(t)dtv(b)−v(a)

ba b

a h(t)dt=(b−a)C(v,h).

Since|v|is convex on [a,b],then by applying Theorem2.1-Theorem2.3for f =v

and=hwe deduce the desired result (3.3).

Remark 3.1. Ifp=q=2, then by (3.3) we get

v(b)

b

a(ta)dh(t)+v(a)

b a(bt)dh(t)

ba

b

a v(t)dh(t)

(3.5)

≤(ba)

|v(a)|2

+|v(a)v(b)|+|v(b)|2 3

1/2

× 1 ba

b a

h(t)− 1

ba

b a h(s)ds

2dt1/2,

provided that|v|is convex on [a,b] andh: [a,b]Cis integrable on [a,b].

4. Applications for Self-adjoint Operators

We denote byB(H) the Banach algebra of all bounded linear operators on a complex Hilbert space (H; ·,·).LetA∈ B(H) be self-adjoint and letϕλ be defined for all

λ∈Ras follows

ϕλ(s) := ⎧ ⎪⎪⎪⎨

⎪⎪⎪⎩ 10,, forforλ <− ∞s<<s+λ,.

Then for everyλ∈Rthe operator

(13)

is a projection which reducesA.

The properties of these projections are collected in the following fundamental result concerning the spectral representation of bounded self-adjoint operators in Hilbert spaces, see for instance [15, p. 256]:

Theorem 4.1.Spectral Representation Theorem Let A be a bonded self-adjoint op-erator on the Hilbert space H and let m = minλλ∈Sp(A) =: minSp(A) and M=maxλλ∈Sp(A)=: maxSp(A).Then there exists a family of projections{Eλ}λ∈R, called the spectral family of A,with the following properties

a) Eλ≤Eλforλ≤λ;

b) Em−0=0,EM=I and Eλ+0=Eλfor allλ∈R;

c) We have the representation

(4.2) A=

M

m−0λdEλ.

More generally, for every continuous complex-valued functionϕdefined onRand for everyε >0there exists aδ >0such that

(4.3)

ϕ(A)−

n '

k=1

ϕλ

k (

EλkEλk−1

) ≤ε

whenever

(4.4)

⎧ ⎪⎪⎪⎪ ⎪⎪⎪⎨ ⎪⎪⎪⎪ ⎪⎪⎪⎩

λ0<m=λ1 < ... < λn−1< λn=M,

λk−λk−1≤δfor1≤kn,

λ

k∈[λk−1, λk] for1≤kn

this means that

(4.5) ϕ(A)=

M

m−0ϕ(λ)dEλ,

where the integral is of Riemann-Stieltjes type.

Corollary 4.1. With the assumptions of Theorem4.1for A,Eλandϕwe have the

repre-sentations

(4.6) ϕ(A)x=

M

(14)

and

(4.7) *ϕ(A)x,y+=

M

m−0ϕ(λ)d *

Eλx,y+ for all x,yH.

In particular,

(4.8) *ϕ(A)x,x+=

M

m−0ϕ(λ)d Eλx,x for all xH. Moreover, we have the equality

(4.9) ϕ(A)x2=

M

m−0

ϕ(λ)2dEλx2 for all xH.

The next result shows that it is legitimate to talk about ”the” spectral family of the bounded self-adjoint operator A since it is uniquely determined by the requirements a), b) and c) in Theorem4.1, see for instance [15, p. 258]:

Theorem 4.2. Let A be a bonded self-adjoint operator on the Hilbert space H and let m=minSp(A)and M=maxSp(A).If{Fλ}λ∈Ris a family of projections satisfying the requirements a), b) and c) in Theorem4.1, then Fλ =Eλfor allλ∈Rwhere Eλis defined

by (4.1).

By the above two theorems, the spectral family {Eλ}λ∈R uniquely determines and in turn is uniquely determined by the bounded self-adjoint operatorA.

We can state now the following generalized trapezoid inequality for functions of self-adjoint operators:

Theorem 4.3. Let A be a bonded self-adjoint operator on the Hilbert space H and let m =minλλ∈Sp(A) =: minSp(A)and M = maxλλ∈Sp(A)=: maxSp(A).

Consider also the spectral family{Eλ}λ∈Rof A.

If f :I→Cis dierentiable on the interior of the interval I,denotedI and˚ [m,M]I˚,

fis convex on[m,M], then we have the inequalities

,f(m)(M1HA)+f(M)(Am1H)

Mm

x,y-−*f(A)x,y+ (4.10)

≤ 1

2f(m)+f(M)

(M−m)

×supt[m,M]

⎡ ⎢⎢⎢⎢ ⎢⎣Mt−−mm

t

m−0 ,

E(·)x,y

-+ Mt Mm

M

t ,

E(·)x,y -⎤⎥⎥⎥⎥

⎥⎦

≤ 1

2f(m)+f(M)

(M−m)

M

m−0 ,

E(·)x,y

-≤ 1

2f(m)+f(M)

(M−m)xy

(15)

Proof. Let x,yHand considerh : R → C,h(t) := *Etx,y+.If we use the third

inequality in (3.3) for the interval [m−ε,M] with smallε >0,we have

f(M)

M

m−ε(tm+ε)d Etx,y+f(m−ε)

M

m−ε(Mt)d Etx,y

Mm

(4.11)

mMε f(t)d*Etx,y+

≤ 1

2f(M)+f(m−ε)

(M−m+ε)

×supt[mε,M]*Etx,y+−M1m+ε M

m−ε *

Esx,y+ds.

Taking the limit overε →0+and using the Spectral representation theorem, we have

,f(m)(M1HA)+f(M)(Am1H)

Mm

x,y-−*f(A)x,y+

(4.12)

≤ 1

2f(m)+f(M)

(M−m)

×supt[m,M]*Etx,y+−M1m M

m−0 *E

sx,y+ds

for anyx,yH.

It is well known that ifp: [a,b]→Cis a bounded function,v: [a,b]→Cis of bounded variation and the Riemann-Stieltjes integralabp(t)dv(t) exists, then the following inequality holds

(4.13)

b

a p(t)dv(t)

tsup[a,b]p(t) b

a

(v),

where

b

a

(v) denotes the total variation ofvon [a,b].

Now, a simple integration by parts in the Riemann-Stieltjes integral reveals the following equality of interest

*

Etx,y+− M1m M

m−0 *

Esx,y+ds

(4.14)

= 1

Mm t

m−0(s−m)d *

Esx,y++ M

t (s−M)d *

Esx,y+

that holds for anyt∈[m,M] and for anyx,yH.

(16)

x,yH,then on applying the inequality (4.13), we get

*Etx,y+−M1m M

m−0 *E

sx,y+ds

(4.15)

≤ 1

Mm t

m−0(s−m)d *E

sx,y++ M

t (s−M)d *E

sx,y+

tm Mm

t

m−0 ,

E(·)x,y

-+ Mt Mm

M

t ,

E(·)x,y

-≤maxtm

Mm,MM−−mt

M

m−0 ,

E(·)x,y

-=1 2+

tm+2M

Mm

M

m−0 ,

E(·)x,y

-that holds for anyt∈[m,M] and for anyx,yH.

This implies that

supt[m,M]*Etx,y+− M1m M

m−0 *E

sx,y+ds

(4.16)

≤supt[m,M]

⎡ ⎢⎢⎢⎢ ⎢⎣Mt−−mm

t

m−0 ,

E(·)x,y

-+ Mt Mm

M

t ,

E(·)x,y -⎤⎥⎥⎥⎥

⎥⎦

≤supt∈[m,M]

1 2+

tm+2M

Mm

M

m−0 ,

E(·)x,y

-=

M

m−0 ,

E(·)x,y

-for anyx,yH.

The proof of the inequality

M

m−0 ,

E(·)x,y

-≤ xy

for anyx,yH,can be found in [13, p. 9]. We also have:

Theorem 4.4. Let A be a bonded self-adjoint operator on the Hilbert space H and let m =minλλ∈Sp(A) =: minSp(A)and M = maxλλ∈Sp(A)=: maxSp(A).

Consider also the spectral family{Eλ}λ∈Rof A.

If f :I → Cis dierentiable onI,˚ [m,M]I and˚ fis convex on[m,M], then we

have the inequalities

,f(m)(M1HA)+f(M)(Am1H)

Mm

x,y-−*f(A)x,y+ (4.17)

≤maxf(m),f(M) M

m−0

*Etx,y+−M1m M

m−0 *

Esx,y+dsdt

≤ 1

2maxf(m),f(M)

(17)

for any x,yH.

Proof. Let x,yH and considerh : R → C, h(t) := *Etx,y+.If we use the first

inequality in (3.3) for the interval [m−ε,M] with smallε >0,we have

f(M)

M

m−ε(tm+ε)d Etx,y+f(m−ε)

M

m−ε(Mt)d Etx,y

Mm

(4.18)

mMε f(t)d*Etx,y+

≤maxf(M),f(mε)(Mm+ε)

× 1

MmM

m−ε

*Etx,y+−M1m+ε M

m−ε *E

sx,y+dsdt.

Taking the limit overε →0+and using the Spectral representation theorem, we have

,f(m)(M1HA)+f(M)(Am1H)

Mm

x,y-−*f(A)x,y+ (4.19)

≤maxf(m),f(M) M

m−0

*Etx,y+−M1m M

m−0 *

Esx,y+dsdt

for anyx,yH.

By the Schwarz inequality inHwe have that

M m−0

*Etx,y+−M1m M

m−0 *

Esx,y+dsdt

(4.20)

=mM0.EtxM1m M

m−0Esxds ,y/dt

ymM0EtxM1m M

m−0Esxds dt for anyx,yH.

On utilizing the Cauchy-Buniakovski-Schwarz integral inequality we may state that

M m−0

EtxM1m M

m−0Esxds dt (4.21)

≤(M−m)1/2mM0EtxM1m M

m−0Esxds 2dt1/2

for anyxH.

Observe that the following equalities of interest hold and they can be easily proved by direct calculations

1

Mm M

m−0

EtxM1m M

m−0Esxds 2dt (4.22)

= 1

Mm M

m−0Etx2dt

1

Mm M

(18)

and

1

Mm M

m−0Etx2dt

1

Mm M

m−0Esxds 2

(4.23)

= 1

Mm M

m−0 .

EtxM1m M

m−0Esxds,Etx−12x /

dt

for anyxH.

By (4.21), (4.22) and (4.23) we get

M m−0

EtxM1m M

m−0Esxds dt (4.24)

≤(M−m)1/2mM0.EtxM1m M

m−0Esxds,Etx−12x /

dt1/2

for anyxH.

On making use of the Schwarz inequality inHwe also have

M m−0

.

EtxM1m M

m−0Esxds,Etx− 12x /

dt (4.25)

mM0EtxM1m M

m−0Esxds

Etx− 12xdt

=1 2x

M m−0

EtxM1m M

m−0Esxds dt,

where we used the fact thatEtare projectors, and in this case we have

Etx−12x 2

=Etx2− Etx,x+ 14x2= 14x2

for anyt∈[m,M] for anyxH.

From (4.24) and (4.25) we get

M m−0

EtxM1m M

m−0Esxds dt (4.26)

≤(M−m)1/21 2x

M m−0

EtxM1m M

m−0Esxds dt1/2,

which is clearly equivalent with the following inequality of interest in itself

(4.27)

M

m−0

EtxM1m

M

m−0Esxds

dt≤ 12x(M−m) for anyxH.

From (4.20) we then get 1

Mm

M

m−0

*Etx,y+−M1m

M

m−0 *E

sx,y+ds

(19)

Finally, we also have:

Theorem 4.5. Let A be a bonded self-adjoint operator on the Hilbert space H and let m =minλλ∈Sp(A) =: minSp(A)and M = maxλλ∈Sp(A)=: maxSp(A).

Consider also the spectral family{Eλ}λ∈Rof A.

If f :I → Cis dierentiable onI,˚ [m,M]I and˚ fis convex on[m,M], then we

have the inequalities

,f(m)(M1HA)+f(M)(Am1H)

Mm

x,y-−*f(A)x,y+ (4.28)

≤|f(M)|2+|f(M3)f(m)|+|f(m)|21/2(M−m)

× 1

Mm M

m−0

*Etx,y+− M1m M

m−0 *

Esx,y+ds

2 dt1/2

≤ 1

2 |f(M)|2

+|f(M)f(m)|+|f(m)|2 3

1/2

(M−m)xy

for any x,yH.

Proof. Utilising the inequality (3.5) we can prove in a similar manner as above the first inequality in (4.28).

By the Schwarz inequality inHwe have that

1

Mm M

m−0

*Etx,y+− M1m M

m−0 *

Esx,y+ds

2 dt (4.29)

= 1

Mm M

m−0 .

EtxM1m M

m−0Esxds ,y/ 2

dt

y2 1

Mm M

m−0

EtxM1m M

m−0Esxds 2dt for anyx,yH.

As in the proof of Theorem4.4we also have

1

Mm M

m−0

EtxM1m M

m−0Esxds 2dt (4.30)

≤ 1

2xM1−m M

m−0

EtxM1m M

m−0Esxds dt≤1

4x2.

By (4.29) and (4.30) we then get

1 Mm

M

m−0

*Etx,y+−M1m

M

m−0 *

Esx,y+ds 2

dt≤ 1

4x2y 2

,

namely

⎡ ⎢⎢⎢⎢ ⎢⎣M1m

M

m−0

*Etx,y+−M1m

M

m−0 *

Esx,y+ds 2

dt

⎤ ⎥⎥⎥⎥ ⎥⎦

1/2

(20)

for anyx,yH.

This proves the last part of (4.28).

Example 4.1. a) LetAbe a bonded self-adjoint operator on the Hilbert spaceHand let

m = minλλ∈Sp(A) =: minSp(A) ≥ 0 and M = maxλλ∈Sp(A) =: maxSp(A).

Consider also the spectral family{Eλ}λ∈RofA.Then by Theorem4.3-4.5we have forf(t)=tp,

p≥2 that

,mp(M1H−A)+Mp(Am1H)

Mm

x,y-−*Apx,y+ (4.31)

≤1 2p

mp−1+Mp−1(Mm)

×supt∈[m,M]

⎡ ⎢⎢⎢⎢ ⎢⎣Mt−−mm

t

m−0

*

E(·)x,y++MM−−mt M

t

*

E(·)x,y+

⎤ ⎥⎥⎥⎥ ⎥⎦

≤ 1 2p

mp−1+Mp−1(Mm) M

m−0

*E(

·)x,y+

≤1 2p

mp−1+Mp−1(Mm)xy,

,mp(M1H−A)+Mp(Am1H)

Mm

x,y-−*Apx,y+ (4.32)

pMp−1M m−0

*Etx,y+−M1−m

M

m−0

*E

sx,y+dsdt

≤ 1

2pMp−1(Mm)xy

and

,mp(M1H−A)+Mp(Am1H)

Mm

x,y-−*Apx,y+ (4.33)

pM2(p−1)+(Mm3)p−1+m2(p−1)1/2(Mm)

× 1 Mm

M

m−0

*Etx,y+−M1m

M

m−0

*E

sx,y+ds 2

dt1/2

≤1 2

M2(p−1)+(Mm)p−1+m2(p−1) 3

1/2

(Mm)xy

for anyx,yH.

b) With the assumptions of a) and ifm>0,then by Theorem4.3-4.5we have forf(t)=lnt,

that

,lnm(M1H−A)+lnM(Am1H)

Mm

x,y-−*lnAx,y+ (4.34)

m+M

2mM(Mm)

×supt∈[m,M]

⎡ ⎢⎢⎢⎢ ⎢⎣Mt−−mm

t

m−0

*

E(·)x,y++MM−−mt M

t

*

E(·)x,y+

⎤ ⎥⎥⎥⎥ ⎥⎦

m+M

2mM(Mm) M

m−0

*

(21)

lnm(M1H−A)+lnM(Am1H)

Mm x,y

*

lnAx,y+ (4.35)

≤ 1 m

M

m−0

*Etx,y+−M1m

M

m−0

*E

sx,y+dsdt

≤ 1

2mxy(Mm)

and

,lnm(M1H−A)+lnM(Am1H)

Mm

x,y-−*lnAx,y+ (4.36)

M2+mM+m2 3m2M2

1/2

(Mm)

× 1 Mm

M

m−0

*Etx,y+−M1−m

M

m−0

*

Esx,y+ds 2

dt1/2

≤ 1 2mM

M2+mM+m2 3

1/2

(Mm)xy

for anyx,yH.

Acknowledgement.The author would like to thank the anonymous referee for valuable suggestions that have been implemented in thefinal version of the paper.

R E F E R E N C E S

1. W. Alomari: NewCebyˇ ˇsev type inequalities and qpplications for functions of self-adjoint operators on complex Hilbert spaces, Chinese Journal of Mathematics, 2014(2014), Article ID 363050, 10 pages, http://dx.doi.org/10.1155/2014/363050

2. P. Cerone andS. S. Dragomir: New bounds for theCebyˇ ˇsev functional, Appl. Math.

Lett.,18(2005), 603–611.

3. P. Cerone andS. S. Dragomir: A refinement of the Gr¨uss inequality and applications,

Tamkang J. Math.38(2007), No. 1, 37–49. Preprint available at RGMIA Res. Rep. Coll.,5(2) (2002), Art. 14.

4. P. L. Chebyshev: Sur les expressions approximatives des int`egrals d`efinis par les outres prises entre les mˆeme limites,Proc. Math. Soc. Charkov,2(1882), 93–98.

5. X.-L. Cheng andJ. Sun: Note on the perturbed trapezoid inequality,J. Inequal. Pure

Appl. Math.,3(2) (2002), Art. 29.

6. S. S. Dragomir: Inequalities of Gr¨uss type for the Stieltjes integral and applications,

Kragujevac J. Math.,26(2004), 89–112.

7. S. S. Dragomir: Inequalities for Stieltjes integrals with convex integrators and applica-tions, Appl. Math. Lett.,20(2007), 123–130.

8. S. S. Dragomir: Cebyˇ ˇsev’s type inequalities for functions of selfadjoint operators in Hilbert spaces,Preprint RGMIA Res. Rep. Coll.,11(e) (2008), Art. 9.

9. S. S. Dragomir:,Gr¨uss’ type inequalities for functions of selfadjoint operators in Hilbert spaces,Preprint RGMIA Res. Rep. Coll.,11(e) (2008), Art. 11.

(22)

11. S. S. Dragomir: New Gr¨uss’ type inequalities for functions of bounded variation and applications.Appl. Math. Lett.25(2012), no. 10, 1475–1479.

12. S. S. Dragomir: Operator Inequalities of the Jensen,Cebyˇ ˇsev and Gr¨uss Type. Springer

Briefs in Mathematics. Springer, New York, 2012. xii+121 pp. ISBN: 978-1-4614-1520-6

13. S. S. Dragomir:Operator Inequalities of Ostrowski and Trapezoidal Type. Springer Briefs

in Mathematics. Springer, New York, 2012. x+112 pp. ISBN: 978-1-4614-1778-1 14. G. Gruss¨ : ¨Uber das maximum des absoluten Betrages von 1

ba

b

a f(x)(x)dx− 1

(ba)2

b a f(x)dx·

b

a (x)dx,, Math. Z.,39(1934), 215–226.

15. G. Helmberg:Introduction to Spectral Theory in Hilbert Space, John Wiley & Sons, Inc.

-New York, 1969.

16. A. Lupas¸;The best constant in an integral inequalityMathematica (Cluj),15(38) (1973),

No. 2, 219–222.

17. D. S. Mitrinovic´, J. E. Pecariˇ I´c andA. M. Fink: Classical and New Inequalities in Analysis,Kluwer Academic Publishers, Dordrecht, 1993.

18. A. M. Ostrowski: On an integral inequality, Aequationes Math.,4(1970), 358–373.

Sever S. Dragomir

College of Engineering and Science Department of Mathematics Ballarat Road, Footscray Park Melbourne, Australia

References

Related documents

Anhand von Temperaturanalysen wurde nachgewiesen, dass Patienten, die nach der Therapie über einen längeren Zeitraum eine lokale Tumorkontrolle aufwiesen,

Cheatgrass had greater (P&lt;O.O5) plant height, leaf area, total shoot dry weight, primary root length, number and order of branching of the second group of seminal roots, order

Survival of willow cuttings in the bareground sites was about twice that of the tufted hairgrass/ Nebraska sedge community type even though soil moisture and

To make the resulting system of nonlinear equations solvable, we select the collisions in a way keeping the algebraic degree of equations low (it does not exceed 2) and the number

Broiler male feed intake as affected by age and addition of β-glucanase to ground crumble grower diets following a common starter fed to 14 d of age in Experiment 2. 2 NC+DG2:

Repellent activity test for cream formulation showed 89.87%, 87.5% and 90% protection and smoke toxicity test for incense log showed 66.25%, 70% and 67.5% protection against

In this way, it was possible to separate and distinguish effects of unc-2 on serotonin response by the postsynaptic cell (the vulval muscle) from possible effects

The downward movement of NO 3 - in agricultural and non-agricultural soils is studied using glass column method, The Effect of Ca hardness of extractant, irrigation water