• Nem Talált Eredményt

SOME INEQUALITIES REGARDING A GENERALIZATION OF EULER’S CONSTANT

N/A
N/A
Protected

Academic year: 2022

Ossza meg "SOME INEQUALITIES REGARDING A GENERALIZATION OF EULER’S CONSTANT"

Copied!
15
0
0

Teljes szövegt

(1)

Generalization of Euler’s Constant Alina Sînt ˘am ˘arian vol. 9, iss. 2, art. 46, 2008

Title Page

Contents

JJ II

J I

Page1of 15 Go Back Full Screen

Close

SOME INEQUALITIES REGARDING A GENERALIZATION OF EULER’S CONSTANT

ALINA SÎ NT ˘AM ˘ARIAN

Department of Mathematics Technical University of Cluj-Napoca Str. C. Daicoviciu nr. 15

400020 Cluj-Napoca, Romania.

EMail:Alina.Sintamarian@math.utcluj.ro

Received: 28 November, 2007

Accepted: 20 March, 2008

Communicated by: L. Tóth 2000 AMS Sub. Class.: 11Y60, 40A05.

Key words: Sequence, Convergence, Euler’s constant, Approximation, Estimate, Series.

Abstract: The purpose of this paper is to evaluate the limitγ(a)of the sequence

1

a + 1

a+ 1+· · ·+ 1

a+n1lna+n1 a

n∈N

,

wherea(0,+∞). We give some lower and upper estimates for 1

a+ 1

a+ 1+· · ·+ 1

a+n1lna+n1

a γ(a), nN.

(2)

Generalization of Euler’s Constant Alina Sînt ˘am ˘arian vol. 9, iss. 2, art. 46, 2008

Title Page Contents

JJ II

J I

Page2of 15 Go Back Full Screen

Close

Contents

1 Introduction 3

2 The Numberγ(a) 4

3 Proving Some Estimates foryn−γ(a)using the Logarithmic Derivative

of the Gamma Function 6

(3)

Generalization of Euler’s Constant Alina Sînt ˘am ˘arian vol. 9, iss. 2, art. 46, 2008

Title Page Contents

JJ II

J I

Page3of 15 Go Back Full Screen

Close

1. Introduction

Let (Dn)n∈N be the sequence defined by Dn = 1 + 12 +· · ·+ n1 −lnn, for each n ∈ N. It is well-known that the sequence (Dn)n∈N is convergent and its limit, usually denoted byγ, is called Euler’s constant.

ForDn−γ, n ∈ N, many lower and upper estimates have been obtained in the literature. We recall some of them:

2(n+1)1 < Dn−γ < 2(n−1)1 , for eachn∈N\ {1}([14]);

2(n+1)1 < Dn−γ < 2n1 , for eachn∈N([8], [19]);

2n+11 < Dn−γ < 2n1 , for eachn∈N([17]);

2n+1 2 5

< Dn−γ < 2n+1 1 3

, for eachn ∈N([15], [16]);

1

2n+2γ−11−γ ≤Dn−γ < 1

2n+13, for eachn∈N([16, Editorial comment], [2], [3]).

In Section 2 we present a generalization of Euler’s constant as the limit of the sequence

1 a + 1

a+ 1 +· · ·+ 1

a+n−1−lna+n−1 a

n∈N

, a∈(0,+∞), and we denote this limit byγ(a).

In Section3we give some lower and upper estimates for 1

a + 1

a+ 1 +· · ·+ 1

a+n−1 −lna+n−1

a −γ(a), n∈N.

(4)

Generalization of Euler’s Constant Alina Sînt ˘am ˘arian vol. 9, iss. 2, art. 46, 2008

Title Page Contents

JJ II

J I

Page4of 15 Go Back Full Screen

Close

2. The Number γ(a)

It is known that the sequence 1

a + 1

a+ 1 +· · ·+ 1

a+n−1−lna+n−1 a

n∈N

, a∈(0,+∞), is convergent (see for example [5, p. 453], [7], where problems in this sense were proposed; [6]; [13]).

The results contained in the following theorem were given in [10].

Theorem 2.1. Leta ∈ (0,+∞). We consider the sequences (xn)n∈N and(yn)n∈N

defined by

xn = 1 a + 1

a+ 1 +· · ·+ 1

a+n−1 −lna+n a and

yn= 1 a + 1

a+ 1 +· · ·+ 1

a+n−1−lna+n−1

a ,

for eachn ∈N. Then:

(i) the sequences(xn)n∈Nand(yn)n∈Nare convergent to the same number, which we denote byγ(a), and satisfy the inequalitiesxn < xn+1 < γ(a)< yn+1 < yn, for eachn∈N;

(ii) 0< a1 −ln 1 + 1a

< γ(a)< 1a; (iii) lim

n→∞n(γ(a)−xn) = 12 and lim

n→∞n(yn−γ(a)) = 12.

(5)

Generalization of Euler’s Constant Alina Sînt ˘am ˘arian vol. 9, iss. 2, art. 46, 2008

Title Page Contents

JJ II

J I

Page5of 15 Go Back Full Screen

Close

Remark 1. The sequence (yn)n∈N from Theorem 2.1, for a = 1, becomes the se- quence(Dn)n∈N, soγ(1) =γ.

The following theorem was given by the author in [12, Theorem 2.3].

Theorem 2.2. Let a ∈ (0,+∞). We consider the sequence (un)n∈N defined by un = yn2(a+n−1)+1 1

3

, for each n ∈ N, where (yn)n∈N is the sequence from the statement of Theorem 2.1. Also, we specify that γ(a) is the limit of the sequence (yn)n∈N.

Then:

(i) un < un+1 < γ(a), for eachn∈N\ {1}, and lim

n→∞n3(γ(a)−un) = 721; (ii) 2(a+n−1)+1 11

28

< yn−γ(a)< 2(a+n−1)+1 1 3

, for eachn∈N\ {1}.

Remark 2. The lower estimate from part(ii)of Theorem2.2holds forn= 1as well.

Remark 3. The second limit from part(iii)of Theorem 2.1also follows from part (ii)of Theorem2.2.

(6)

Generalization of Euler’s Constant Alina Sînt ˘am ˘arian vol. 9, iss. 2, art. 46, 2008

Title Page Contents

JJ II

J I

Page6of 15 Go Back Full Screen

Close

3. Proving Some Estimates for y

n

− γ(a) using the Logarithmic Derivative of the Gamma Function

As we already mentioned in Section1, it is known that ([16, Editorial comment], [2, Theorem 3], [3, Theorem 1.1])

1

2n+ 2γ−11−γ ≤Dn−γ < 1 2n+13,

for eachn∈N, the constants 2γ−11−γ and 13 being the best possible with this property.

Let a ∈ (0,+∞). In a similar way as in the proof given by H. Alzer in [2, Theorem 3], we shall obtain lower and upper estimates foryn−γ(a)(n∈N), where (yn)n∈N is the sequence from the statement of Theorem2.1, the limit of which we denoted byγ(a). In order to do this we shall prove, in a similar way as in [3, Lemma 2.1], some finer inequalities than those used by H. Alzer in [2, Theorem 3].

Lemma 3.1. We have:

(i) ψ(x+ 1)−lnx > 2x112x12 +120x1 4252x1 6, for eachx∈(0,+∞);

(ii) 1x −ψ0(x+ 1)< 2x126x13 + 30x1542x17 + 30x19, for eachx∈(0,+∞).

We specify that the functionψ is the logarithmic derivative of the gamma function, i.e.ψ(x) = ΓΓ(x)0(x), for eachx∈(0,+∞).

Proof. (i)It is known (see, for example, [18, p. 116]) thatlnx=R 0

e−t−e−xt t dt, for eachx∈(0,+∞). Also, we shall need the formula

ψ(x) = Z

0

e−t

t − e−xt 1−e−t

dt,

(7)

Generalization of Euler’s Constant Alina Sînt ˘am ˘arian vol. 9, iss. 2, art. 46, 2008

Title Page Contents

JJ II

J I

Page7of 15 Go Back Full Screen

Close

which holds for each x ∈ (0,+∞), known as Gauss’ expression of ψ(x) as an infinite integral (see, for example, [18, p. 247]). Having in view the above relations, we are able to write that

ψ(x+ 1)−lnx= Z

0

1

t − 1 et−1

e−xtdt,

for eachx∈(0,+∞).

It is not difficult to verify that Z

0

tne−xtdt = n!

xn+1, for eachn∈N∪ {0}, anyx∈(0,+∞).

Then we have ψ(x+ 1)−lnx− 1

2x + 1

12x2 − 1

120x4 + 1 252x6

= Z

0

1

t − 1

et−1 − 1 2+ t

12− t3

720 + t5 30240

e−xtdt

= Z

0

1

30240t(et−1)[30240(et−1)−30240t−15120t(et−1) + 2520t2(et−1)

−42t4(et−1) +t6(et−1)]e−xtdt

= Z

0

1 30240t(et−1)

"

30240

X

n=2

tn

n!−15120

X

n=1

tn+1

n! + 2520

X

n=1

tn+2 n!

−42

X

n=1

tn+4 n! +

X

n=1

tn+6 n!

#

e−xtdt

(8)

Generalization of Euler’s Constant Alina Sînt ˘am ˘arian vol. 9, iss. 2, art. 46, 2008

Title Page Contents

JJ II

J I

Page8of 15 Go Back Full Screen

Close

= Z

0

P

n=9

(n−3)(n−5)(n−7)(n−8)(n2+8n+36)

n! tn

30240t(et−1) ·e−xtdt >0, for eachx∈(0,+∞).

(ii)In part(i)we obtained that lnx−ψ(x+ 1) =

Z

0

1

et−1− 1 t

e−xtdt,

for eachx∈(0,+∞). Differentiating here we get that 1

x−ψ0(x+ 1) = Z

0

1− t et−1

e−xtdt,

for eachx∈(0,+∞).

Then we have 1

x−ψ0(x+ 1)− 1

2x2 + 1

6x3 − 1

30x5 + 1

42x7 − 1 30x9

= Z

0

1− t

et−1− t 2 + t2

12− t4

720 + t6

30240− t8 1209600

e−xtdt

= Z

0

1

1209600(et−1)[1209600(et−1)−1209600t−604800t(et−1)

+ 100800t2(et−1)−1680t4(et−1) + 40t6(et−1)−t8(et−1)]e−xtdt

(9)

Generalization of Euler’s Constant Alina Sînt ˘am ˘arian vol. 9, iss. 2, art. 46, 2008

Title Page Contents

JJ II

J I

Page9of 15 Go Back Full Screen

Close

= Z

0

1

1209600(et−1)

"

1209600

X

n=2

tn

n!−604800

X

n=1

tn+1 n!

+100800

X

n=1

tn+2

n! −1680

X

n=1

tn+4 n! + 40

X

n=1

tn+6 n! −

X

n=1

tn+8 n!

#

e−xtdt

=− Z

0

P n=11

(n−3)(n−5)(n−7)(n−9)(n−10)(n+4)(n2+2n+32)

n! tn

1209600(et−1) ·e−xtdt <0, for eachx∈(0,+∞).

Remark 4. In fact, these inequalities from Lemma 3.1 come from the asymptotic formulae (see, for example, [1, pp. 259, 260])

ψ(x)∼lnx− 1 2x −

X

n=1

B2n 2nx2n

= lnx− 1

2x − 1

12x2 + 1

120x4 − 1

252x6 +· · · and

ψ0(x)∼ 1 x + 1

2x2 +

X

n=1

B2n x2n+1

= 1 x + 1

2x2 + 1

6x3 − 1

30x5 + 1

42x7 − 1

30x9 +· · · , whereB2nis the Bernoulli number of index2n.

Theorem 3.2. Leta ∈ (0,+∞). We consider the sequence (yn)n∈N from the state- ment of Theorem2.1, the limit of which we denoted byγ(a).

(10)

Generalization of Euler’s Constant Alina Sînt ˘am ˘arian vol. 9, iss. 2, art. 46, 2008

Title Page Contents

JJ II

J I

Page10of 15 Go Back Full Screen

Close

Then 1

2(a+n−1) +α ≤yn−γ(a)< 1

2(a+n−1) +β, for eachn ∈N\ {1,2}, withα = y 1

3−γ(a) −2(a+ 2)andβ = 13.

Moreover, the constantsαandβare the best possible with this property.

Proof. The inequalities from the statement of the theorem can be rewritten in the form

β < 1

yn−γ(a) −2(a+n−1)≤α, for eachn∈N\ {1,2}.

Taking into account that ψ(x+ 1) = ψ(x) + 1x, for eachx ∈ (0,+∞), we can write that

ψ(a+n)−ψ(a) = 1 a + 1

a+ 1 +· · ·+ 1 a+n−1, for eachn∈N(see, for example, [1, p. 258]).

It is known that we have the series expansion (see, for example, [9, p. 336])

ψ(x) = lnx−

X

k=0

1

x+k −ln

1 + 1 x+k

,

for eachx∈ (0,+∞). So, we are able to write the following relation betweenγ(a) and the logarithmic derivative of the gamma function:

γ(a) = lna−ψ(a) (see [6, Theorem 7], [11, Theorem 4.1, Remark 4.2]).

(11)

Generalization of Euler’s Constant Alina Sînt ˘am ˘arian vol. 9, iss. 2, art. 46, 2008

Title Page Contents

JJ II

J I

Page11of 15 Go Back Full Screen

Close

Then

yn−γ(a) = ψ(a+n)−ψ(a)−lna+n−1

a −[lna−ψ(a)]

=ψ(a+n)−ln(a+n−1),

for eachn∈N. It means that, in fact, we have to prove that

β < 1

ψ(a+n)−ln(a+n−1) −2(a+n−1)≤α,

for eachn∈N\ {1,2}, and that the constantsαandβare the best possible with this property.

We consider the functionf : (0,+∞)→R, defined by f(x) = 1

ψ(x+ 1)−lnx −2x, for eachx∈(0,+∞). Differentiating, we get that

f0(x) =

1

x−ψ0(x+ 1)−2[ψ(x+ 1)−lnx]2 [ψ(x+ 1)−lnx]2 ,

for eachx∈(0,+∞). Using the inequalities from Lemma3.1, we are able to write that

1

x −ψ0(x+ 1)−2[ψ(x+ 1)−lnx]2

< 1

2x2 − 1

6x3 + 1

30x5 − 1

42x7 + 1 30x9 −2

1

2x − 1

12x2 + 1

120x4 − 1 252x6

2

=− 1

72x4 + 1

60x5 + 1

360x6 − 1

63x7 − 221

151200x8 + 1

30x9 + 1

7560x10 − 1 31752x12

=:g(x),

(12)

Generalization of Euler’s Constant Alina Sînt ˘am ˘arian vol. 9, iss. 2, art. 46, 2008

Title Page Contents

JJ II

J I

Page12of 15 Go Back Full Screen

Close

for each x ∈ (0,+∞). It is not difficult to verify that g(x) < 0, for each x ∈ 3

2,+∞

(32 not being the best lower value possible with this property). It follows thatf0(x) < 0, for eachx ∈ 3

2,+∞

. So, the function f is strictly decreasing on 3

2,+∞

. This means that the sequence (f(a +n −1))n≥3 is strictly decreasing.

Therefore

k→∞lim f(a+k−1)< f(a+n−1)

≤f(a+ 2)

= 1

y3−γ(a) −2(a+ 2), for eachn∈N\ {1,2}.

The asymptotic formula for the function ψ, mentioned in Remark4, permits us to write that

x→∞lim f(x) = lim

x→∞

1

6 +O x12

1

2 +O 1x = 1 3.

Theorem 3.3. Leta ∈ 1

2,+∞

. We consider the sequence(yn)n∈Nfrom the state- ment of Theorem2.1, the limit of which we denoted byγ(a).

Then 1

2(a+n−1) +α ≤yn−γ(a)< 1

2(a+n−1) +β, for eachn ∈N\ {1}, withα= y 1

2−γ(a)−2(a+ 1)andβ = 13.

Moreover, the constantsαandβare the best possible with this property.

Proof. Sincea∈1

2,+∞

, it follows that the sequence(f(a+n−1))n≥2 is strictly decreasing, wheref is the function defined in the proof of Theorem3.2.

(13)

Generalization of Euler’s Constant Alina Sînt ˘am ˘arian vol. 9, iss. 2, art. 46, 2008

Title Page Contents

JJ II

J I

Page13of 15 Go Back Full Screen

Close

Theorem 3.4. Leta ∈ 3

2,+∞

. We consider the sequence(yn)n∈Nfrom the state- ment of Theorem2.1, the limit of which we denoted byγ(a).

Then 1

2(a+n−1) +α ≤yn−γ(a)< 1

2(a+n−1) +β, for eachn ∈N, withα= y 1

1−γ(a) −2a = a[2aγ(a)−1]

1−aγ(a) andβ = 13.

Moreover, the constantsαandβare the best possible with this property.

Proof. Sincea∈3

2,+∞

, it follows that the sequence(f(a+n−1))n∈Nis strictly decreasing, wheref is the function defined in the proof of Theorem3.2.

(14)

Generalization of Euler’s Constant Alina Sînt ˘am ˘arian vol. 9, iss. 2, art. 46, 2008

Title Page Contents

JJ II

J I

Page14of 15 Go Back Full Screen

Close

References

[1] M. ABRAMOWITZ AND I.A. STEGUN, Handbook of Mathematical Func- tions with Formulas, Graphs, and Mathematical Tables, National Bureau of Standards Applied Mathematics Series 55, Washington, 1964.

[2] H. ALZER, Inequalities for the gamma and polygamma functions, Abh. Math.

Sem. Univ. Hamburg, 68 (1998), 363–372.

[3] C.-P. CHEN AND F. QI, The best lower and upper bounds of harmonic se- quence, RGMIA 6(2) (2003), 303–308.

[4] D.W. DeTEMPLE, A quicker convergence to Euler’s constant, Amer. Math.

Monthly, 100(5) (1993), 468–470.

[5] K. KNOPP, Theory and Application of Infinite Series, Blackie & Son Limited, London and Glasgow, 1951.

[6] D.H. LEHMER, Euler constants for arithmetical progressions, Acta Arith., 27 (1975), 125–142.

[7] I. NEDELCU, Problem 21753, Gazeta Matematic˘a, Seria B, 94(4) (1989), 136.

[8] P.J. RIPPON, Convergence with pictures, Amer. Math. Monthly, 93(6) (1986), 476–478.

[9] I.M. RÎJICANDI.S. GRAD ¸STEIN, Tabele de integrale. Sume, serii ¸si produse (Tables of Integrals. Sums, Series and Products), Editura Tehnic˘a, Bucure¸sti, 1955.

[10] A. SÎNT ˘AM ˘ARIAN, Approximations for a generalization of Euler’s constant (submitted).

(15)

Generalization of Euler’s Constant Alina Sînt ˘am ˘arian vol. 9, iss. 2, art. 46, 2008

Title Page Contents

JJ II

J I

Page15of 15 Go Back Full Screen

Close

[11] A. SÎNT ˘AM ˘ARIAN, About a generalization of Euler’s constant, Aut. Comp.

Appl. Math., 16(1) (2007), 153–163.

[12] A. SÎNT ˘AM ˘ARIAN, A generalization of Euler’s constant, Numer. Algorithms, 46(2) (2007), 141–151.

[13] T. TASAKA, Note on the generalized Euler constants, Math. J. Okayama Univ., 36 (1994), 29–34.

[14] S.R. TIMSANDJ.A. TYRRELL, Approximate evaluation of Euler’s constant, Math. Gaz., 55(391) (1971), 65–67.

[15] L. TÓTH, Problem E3432, Amer. Math. Monthly, 98(3) (1991), 264.

[16] L. TÓTH, Problem E3432 (Solution), Amer. Math. Monthly, 99(7) (1992), 684–

685.

[17] A. VERNESCU, Ordinul de convergen¸t˘a al ¸sirului de defini¸tie al constantei lui Euler (The convergence order of the definition sequence of Euler’s constant), Gazeta Matematic˘a, Seria B, 88(10-11) (1983), 380–381.

[18] E.T. WHITTAKERANDG.N. WATSON, A Course of Modern Analysis, Cam- bridge University Press, Cambridge, 1996.

[19] R.M. YOUNG, Euler’s constant, Math. Gaz., 75(472) (1991), 187–190.

Hivatkozások

KAPCSOLÓDÓ DOKUMENTUMOK

STEGUN, Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables, National Bureau of Standards Applied Mathematics Series 55, Washington, 1964..

DRAGOMIR, Trapezoidal type rules from an inequalities point of view, Handbook of Analytic-Computational Methods in Applied Mathematics, CRC Press N.Y.(2000),

STEGUN (Eds.), Handbook of Mathematical Functions with Formu- las, Graphs, and Mathematical Tables, National Bureau of Standards, Applied Mathematics Series 55, 9th printing, Dover,

STEGUN, Handbook of Mathematical Func- tions with Formulas, Graphs, and Mathematical Tables, 9th printing. GRADSHTEYN

By introducing some parameters and the β function and improving the weight func- tion, we obtain a generalization of Hilbert’s integral inequality with the best constant factor.. As

VYAS, Fourier series with small gaps and func- tions of generalized variations, J. SHIBA, On the absolute convergence of Fourier series of functions of

Some classical and new inequalities of an approximate integration are obtained with use of Hadamard type inequalities and delta–convex functions of higher orders.. 2000

IGARI, Some integrability theorems of trigonometric series and monotone decreasing functions, Tohoku Math.. LEINDLER, Generalization of inequalities of Hardy and Littlewood,