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arXiv:1812.05343v1 [math.CA] 13 Dec 2018 tstse h udmna ucinleuto Γ( equation mo an functional the theory, fundamental of number the one t satisfies mechanics, is probability It quantum in it and applications that statistical important known very well natorics, has is and It functions function. special the of tion numbers complex all for (1.1) by given is it of form product eae otegmafnto stedgmao uci,wihi d is which functin, is, or that Γ, impor the of most derivative The is logarithmic function 346]. the by pg. the [9, to see related constant, Euler-Mascheroni the is oe h derivatives the more, ttsis hyaeas once ognrlzdhroi numbe harmonic generalized to ph connected as such also disciplines are a other They functins and special statistics. important in very applications also important are functions polygamma and where aceoiconstant. Mascheroni NQAIISIVLIGTEGMAADDIGAMMA AND GAMMA THE INVOLVING INEQUALITIES si swl nw h am ucini endb h mrprintegr improper the by defined is function gamma the known well is it As 2000 Date e od n phrases. and words Key ac 23,2018. March : ahmtc ujc Classification. Subject Mathematics eeΓi h lsia am ucinand function gamma classical the is Γ Here and n[.AzradN ai,Mntnct rpriso h gam the of properties 778-781]. Monotonicity 20(2007), Batir, Letters, N. Math. and Appl. Alzer [H. in Abstract. γ lim = exp eipoeteuprbud ftefloigieulte pr inequalities following the of bounds upper the improve We n →∞  − ψ 1 2  ′ 1 2 am ucin iam ucin oyam ucin Eul function, , , Gamma ψ , z ψ Γ( ψ + 1  xettennpstv nees n rvdsa exten- an privides and integers, non-positive the except ′ 1 ′′ ( z x x ..., , ) + 1 + 2 1 Γ( = 1. + 3 1 z / r aldplgmafntos h digamma The functions. polygamma called are  FUNCTIONS ze EDTBATIR NECDET 3)) = ) 3 1 Introduction γz + < < Z n Y rmr:3B5 eodr:2A8 26D07. 26A48, Secondary: 33B05; Primary: · · · log ∞ √ 0 =1 ∞ 2 1 πx Γ( x  + t − + 1 z x x − n 1 ) ψ e ψ 1 ψ − ( ( − e x x x n z stedgmafunction. digamma the is − ) Γ = ) log exp <  t < z dt e )= 1) + − 2 1 n ψ z/n   ′ ′ ( ( − x 0 = x , ) ) 1 2 . / z ψ Γ( . Γ( ( 57721 x x ) z  ), afunction, ma .TeWeierstrass’ The ). ula physics. nuclear d , > x ... er,combi- heory, atfunction tant dte have they nd sadmany and rs timportant st oved .Further- 0. sc and ysics al efined er- 2 NECDET BATIR other special functions such as the Riemann , Hurwitz zeta and Clausen func- tions. Over the decades, many mathematicians studied these functions and they obtained remarkable inequalities, interesting properties including monotonicity and convexity, please see [2, 4, 7, 8, 12-22] and references therein. Taking the logarithm of both sides of identity (1.1), we obtain for x> 1 − ∞ x (1.2) log Γ(x +1)= γx + log(x + k) + log k . −  k −  kX=1 Differentiation gives ∞ 1 1 (1.3) ψ(x +1)= γ + . − k − k + x Xk=1 In [3] the authors proved that the function 1 1 G (x) = log Γ(x) x log x + x log(2π)+ ψ(x + c) c − − 2 2 is completely monotonic on (0, ) if and only if c 1/3; while Gb(x) is completely monotonic on (0, ) if and only∞ if b = 0. This≥ result has many− conclusions. For ∞ example, G1/3(x) > 0 and G0(x) < 0 lead to 1 1 Γ(x) 1 (1.4) exp ψ x + < < exp ψ(x) . −2  3 √2πxxe−x −2  ′ ′ Similarly, G1/3(x) < 0 and G0(x) > 0 lead to

1 ′ 1 ′ (1.5) ψ (x +1/3) < log x ψ(x) < ψ (x). 2 − 2 In 2011 C. Mortici [11] improved the upper and lower bounds given in (1.4) and proved the following inequalities for x 2: ≥ 1 1 1 Γ(x) exp ψ x + + < −2  3 72x2  √2πxxe−x 1 1 1 11 (1.6) < exp ψ x + + + . −2  3 72x2 3240x3  The lower bounds in (1.4) and (1.5) are very accurate but the same thing is not valid for the upper bounds. In the new paper [5] the author improved the upper bound given in (1.4) and proved for x> 0 that

1 Γ(x) 1 ∗ (1.7) exp ψ(δ∗(x)) < < exp ψ(δ (x)) , −2  √2πxxe−x −2  where 1 ∗ 1 1 δ∗(x)= x + and δ (x)= . 3 2 (x + 1) log(1 + 1/x) 1 − In the same paper the author established the following inequalities x x (1.8) exp xψ < Γ(x + 1) < exp xψ +1 .  log(x + 1)   2  The function x log(x) ψ(x) in (1.5) has attracted the attentions of many mathematicians and→ they have− offered bounds of different forms for it. For example, GAMMAANDPOLYGAMMAFUNCTIONS 3 in [10] the authors developed the following inequality for x> 1: 1 1 (1.9) < log x ψ(x) < . 2x − x In [1] the author extended it to x> 0. Refinements of (1.9) were given in [6, Thm. 5] as following: 1 1 1 1 + < log x ψ(x) < + 2x 12(x +1/4)2 − 2x 12x2 and 1 1 1 1 1 1 + < log x ψ(x) < + . 2x 12x2 − 12x4 − 2x 12x2 − 120(x +1/8)4 Our aim in this work is to improve the upper bounds given in (1.4) and (1.5). We also offer simplier lower bound in (1.8). In the proofs we need the following identities. Taking logarithm of both sides of identity (1.1), we obtain for x> 1 − ∞ x (1.10) log Γ(x +1)= γx + log(x + k) + log k . − k − Xk=1 h i Differentiation gives ∞ 1 1 (1.11) ψ(x +1)= γ + x> 1. − k − k + x − Xk=1 Differentiation successively gives for n N and z C , which is not a negative integer, ∈ ∈ ∞ − 1 ψ(n)(z) = ( 1)n 1n! . − (z + k)n+1 kX=0

2. Main results Theorem 2.1. For x> 0 the following inequalties hold:

1 ′ 1 ′ (2.1) ψ (α(x)) < log x ψ(x) < ψ (β(x)), 2 − 2 where 1 1 α(x)= x + and β(x)= . 3 2/x 2 log(1 + 1/x) − p Proof. If we use the functional equation Γ(x +1)= xΓ(x), we get log x = log Γ(x + 1) log Γ(x). − Hence, if we employ (1.2), we obtain ∞ 1 (2.2) log x = γ + log(x + k) + log(x + k 1) . − k − −  kX=1 From Taylor’s theorem it follows that 1 1 (2.3) log(x + k) log(x + k 1) = , − − x + k 1 − 2(k + τ(k))2 − 4 NECDET BATIR where x 1 < τ(k) < x . Thus by the help of (2.3), (2.2) can be written as following: − ∞ 1 1 1 (2.4) log x = γ + + . − k − x + k 1 2(k + τ(k))2  kX=1 − Taking into account (1.11), (2.4) becomes ∞ 1 1 (2.5) log x ψ(x)= . − 2 (k + τ(k))2 Xk=1 From (2.3) we get − 1 2 1 2 (2.6) τ(k)= 2 log 1+ k. x + k 1 −  x + k 1 − − − We shall show that τ is strictly increasing on (1, ). For this purpose we define ∞ − 1 1 1 2 f(u)= 2 log 1+ u.  u −  u − Differentiating f, after replacing u by 1/t, we get

1 ′ t − − 1 f (t)= 2 3/2(h(t)) 3/2 + , −t2 −t +1 t2 where h(t)= t log(t + 1). Therefore in order to show that τ is strictly increasing, we only need to− see t2 θ(t) := h(t) < 0. − 2(t + 1)2/3 Differentiation gives 2/3 2 −1/3 ′ t t(t + 1) t (t + 1) /3 θ (t)= − t +1 − (t + 1)4/3 t 2t = (t + 1)2/3 1 < 0 (t + 1)5/3  − − 3  by the well known Bernoulli inequality (1 + x)δ < 1+ δx, 0 <δ< 1 and t > 0. Thus, we have θ(t) >θ(0) = 0, that is, f is strictly increasing on (0, ). Hence we conclude from (2.6) that ∞ ∞ ∞ 1 1 1 1 (2.7) < log x ψ(x) < . 2 (k + τ( ))2 − 2 (k + τ(1))2 Xk=1 ∞ Xk=1 From (2.3) we have − 1 2 2 (2.8) τ(1) = 2 log(1 + 1/x) 1. x −  − Applying L’Hospital rule it is not difficult to see that 1 (2.9) τ( ) = lim τ(k) = lim f(1/t)+ x 1= x + 1. ∞ k→∞ t→0 − 3 − Using (2.8) and (2.9) the proof follows from (2.7).  The upper bound in (1.7) is very accurate but it is not very useful in practise be- cause of it structure. The following theorem gives much simpler upper bound, which clearly improves the upper bound of (2.1), and has the advantages of simplicity. GAMMAANDPOLYGAMMAFUNCTIONS 5

Theorem 2.2. For x 0 we have ≥ 1 ′ 1 1 ′ 1 1 (2.10) ψ x + < log x ψ(x) < ψ x + . 2  3 − 2  3 − 12x +3 Proof. Since ψ′ is strictly decreasing on (0, ), in the light of Theorem 2.1, it suffices to show for x> 0 that ∞ 1 1 1 (2.11) > x + 2 3 − 12x +3 x 2 log(1 + 1/x) q − or simplifying 1 1 H(x) := log(1 + 1/x) + 2 > 0. − x 1 1 2 x + 3 12x+3  −  Differentiation gives ′ 63 + 188x H (x)= , −x3(x + 1)(12x + 7)3 so that H is strictly decreasing on (0, ). This concludes with H(x) > limx→∞ H(x)= 0. ∞  Our next theorem improves the upper bound given in (1.4). Theorem 2.3. For x> 0 we have 1 1 Γ(x) 1 1 1 exp ψ x + < < exp ψ x + . −2  3 √2πxxe−x −2  3 − 18x +3 Proof. Since the function e−ψ(x) is strictly decreasing on (0, ), in the light of (1.7), the only thing we need to show for x> 0 is the following∞ inequality: 1 1 1 1 > x + 2 (x + 1) log(1 + 1/x) 1 3 − 18x +3 − or equivalently 1+12x + 12x2 P (x) := log(1 + 1/x) < 0. − 6x(x + 1)(2x + 1) Differentiation gives

′ 1 P (x)= > 0. 6x2(1 + x)2(1+2x)2

Thus, P is strictly increasing on (0, ), which implies that P (x) < limx→∞ P (x)= 0. ∞  Theorem 2.4. For all x> 0, we have x x2 x (2.12) exp xψ +1 < Γ(x + 1) < exp xψ +1 .   2 − 12+2x   2  Proof. Since the function ψ is an increasing function, taking into account (1.8), it suffices to see

x x2 x (2.13) +1 < 2 − 12+2x log(x + 1) 6 NECDET BATIR or after a little simplification, x2 +6x (2.14) p(x) := log(x + 1) > 0. − 4x +6 Differentiating, we get 2 ′ x p (x)= , −(x +1)(3+2x)2 so that p is strictly decreasing on (0, ). Thus we have p(x) > limx→∞ p(x) = 0. ∞ 

Remark 2.5. The upper bounds in (1.6) and (1.9) are slightly better than those of (2.3) and (2.5), but the upper bounds in (2.3) and (2.5) have the advantage of simplicity.

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department of mathematics, nevs¸ehir hbv university, nevs¸ehir, 50300 turkey E-mail address: [email protected]