A family of entire functions connecting the Bessel function $J_1$ and the Lambert $W$ function
Christian Berg, Eugenio Massa, Ana P. Peron

TL;DR
This paper constructs a family of entire functions linking the Bessel and Lambert W functions to analyze the complete monotonicity of a parameterized exponential function, using Fourier and complex analysis.
Contribution
It introduces a new family of entire functions related to Bessel and Lambert W functions, providing a novel integral representation and properties relevant to complete monotonicity.
Findings
Derived power series expansion for the functions lpha_\u03b1
Identified the relationship between lphand well-known special functions
Estimated the maximum lphaor which _lphare completely monotonic
Abstract
Motivated by the problem of determining the values of for which is a completely monotonic function, we combine Fourier analysis with complex analysis to find a family , , of entire functions such that We show that each function has an expansion in power series, whose coefficients are determined in terms of Bell polynomials. This expansion leads to several properties of the functions , which turn out to be related to the well known Bessel function and the Lambert function. On the other hand, by numerically evaluating the series expansion, we are able to show the behavior of as increases from to and to obtain a very precise approximation of the largest…
Peer Reviews
No public reviews on file for this paper yet. If you reviewed it on a platform where reviews are public (OpenReview, ICLR, NeurIPS, ICML), you can paste yours below so the community can read it here.
Videos
No videos yet. Explain this paper in a talk, walkthrough, or lecture? Add one.
A family of entire functions connecting the Bessel function and the Lambert function
Christian Berg, Eugenio Massa and Ana P. Peron
Abstract
Motivated by the problem of determining the values of for which is a completely monotonic function, we combine Fourier analysis with complex analysis to find a family , , of entire functions such that
We show that each function has an expansion in power series, whose coefficients are determined in terms of Bell polynomials. This expansion leads to several properties of the functions , which turn out to be related to the well known Bessel function and the Lambert function.
On the other hand, by numerically evaluating the series expansion, we are able to show the behavior of as increases from [math] to and to obtain a very precise approximation of the largest such that , or equivalently, such that is completely monotonic.
AMS Subject Classification: 26A48, 30E20, 42A38, 33F05.
Keywords: completely monotonic function, complex analysis, Fourier analysis, Stieltjes moment sequence, Bell polynomials.
1 Introduction and main results
A completely monotonic function is an infinitely differentiable function such that
[TABLE]
and a Bernstein function is an infinitely differentiable function such that for and is completely monotonic. Both classes of functions are treated in [4] and [13]. The only completely monotonic functions, which are also Bernstein functions, are the non-negative constant functions.
Let . In [1, p. 457] it was proved that is completely monotonic if and only if . This was sharpened in [10] to a proof that is logarithmically completely monotonic if and only if . Monotonicity properties of when has been examined in [9] and [8].
For define
[TABLE]
In [1, p. 458] it was left as an open problem to determine the values of for which is completely monotonic or equivalently is completely monotonic. It was proved that is completely monotonic for , and the question was, if is completely monotonic for some . In [2] the problem was given the equivalent formulation of determining the set of values such that is a Bernstein function. It was noticed in [2] that is a Bernstein function, because is completely monotonic, but is not a Bernstein function. Because of the fact that if is a Bernstein function, then so is for , and the fact that the set of Bernstein functions is closed under pointwise convergence, the set in question is of the form , where is an unknown number in the interval . From graphs it looked probable that .
In [14] it was established numerically that This was done looking at monotonicity properties of high order derivatives of . More precisely, defining
[TABLE]
and letting be determined as the ”smallest positive solutions” to
[TABLE]
then decreases to . The estimate for is then obtained from approximate values of for certain up to .
In this paper we shall combine Fourier analysis with complex analysis to find a family of entire functions such that
[TABLE]
By a theorem of Bernstein, cf. [15, p.160], this formula shows that is completely monotonic if and only if for all and therefore is determined as the largest such that for all .
It turns out that our calculations leading to (1) are valid for all complex , and for such we define
[TABLE]
[TABLE]
where denotes the cut plane, and is the principal logarithm defined in .
The functions are given as contour integrals in the following theorem:
Theorem 1.1**.**
Let be fixed, and let denote the rectangle with corners considered as a closed contour with positive orientation. Then for
[TABLE]
is an entire function, which is independent of , and (1) holds for all . Moreover is bounded for and tends to 0 for .
Theorem 1.1 is contained in Theorem 2.6 and in Theorem 2.10. In particular, the formula (1) is proved in Theorem 2.10.
The power series of the entire functions are given in the following theorem, depending on a remarkable sequence of polynomials:
Theorem 1.2**.**
Let denote the sequence of polynomials defined by
[TABLE]
and in general
[TABLE]
For
[TABLE]
In particular
[TABLE]
Some properties of the polynomials are given in Proposition 2.8, while Theorem 1.2 is proved in Section 2.
It follows from (6) that is an entire function on , and is not identically zero when , so it has at most countably many zeros which are all isolated. Furthermore when then for .
More results that can be deduced from (6) are contained in the following.
Theorem 1.3**.**
Consider the entire function .
- (i)
[TABLE]
uniformly for in compact subsets of the complex plane.
The limit function has no real zeros but infinitely many complex zeros , where W(k,z) is the ’th branch of the Lambert function, see **[7]**. We have
[TABLE]
- (ii)
Given , has at least non-real zeros, when is sufficiently small.
- (iii)
[TABLE]
uniformly for in compact subsets of the complex plane, where is the Bessel function of order 1.
- (iv)
Given , has at least simple zeros such that for sufficiently large, and they satisfy
[TABLE]
where are the positive zeros of .
If in addition , then .
- (v)
For , the entire functions are of order one and type one.
Remark 1.4**.**
It is worth observing that Property above is an analytical proof of the existence of , in contrast with [2], where this was obtained by computing , which implies that cannot be completely monotonic.**
The proof of Theorem 1.3 is given in Section 6.
If is a Stieltjes moment sequence, i.e., if there exists a positive measure on such that
[TABLE]
then it is easy to see that
[TABLE]
and in particular for and hence .
However, this argument is only useful for , in fact, the following holds.
Theorem 1.5**.**
The following conditions are equivalent:
- (i)
* is a Stieltjes moment sequence.*
- (ii)
* is completely monotonic.*
- (iii)
.
If the equivalent conditions hold, then from (8) is supported by , and is a Hausdorff moment sequence.
The proof is given in Section 3, where we also find the measures for (see the Equations (28) and (35)).
For , on the other hand, we show in Theorem 4.1 that the function can be decomposed as the sum of a completely monotonic function and a suitable contour integral (see Equation (40)).
Even so, we have not been able to find an expression which turns out useful in order to check if is non-negative on . As a consequence, for these values of , we have to rely on numerical calculation. For this purpose one can use the contour integral (3), but we prefer to use the power series (6), because of the following result.
Theorem 1.6**.**
For , , we know that and
[TABLE]
Then the series (6) satisfies the Alternating Series Test for , which allows to obtain an error bound for the truncated series.
The proof of Theorem 1.6 is given in Section 5.
We summarize what can be seen from the numerical calculations in the following.
Theorem 1.7** (Numerical results).**
**
- (i)
.
- (ii)
For we have for .
- (iii)
* for and it has a unique zero of multiplicity two at .*
- (iv)
For , has a finite number of positive zeros which are all simple with the exception that the last can be double.
- (v)
* is a simple zero with , moreover is a decreasing function on .*
Below we present several graphs that support the claims in Theorem 1.7.
In Figure 1 the graph of is sketched for the values : in these cases is strictly positive (see Property ) and, for , also completely monotonic, as stated in Theorem 1.5.
In Figure 2 one can see the graph of for the value given in , where it presents a unique zero , which is also a global minimum, as described in . On the other hand, is still strictly positive for and has a region of negative values between two simple zeros for .
As increases, the first zero decreases as described in (Figure 3). For (Figure 4) a new double zero appears on the right of and , and then more and more oscillations appear by the same mechanism (Figure 5). In Figure 6, for instance, is represented with 3 different scales, and one can see at least 10 zeros.
The graphs are obtained in Maple by truncating the series (6), taking into consideration Theorem 1.6. The approximated values of given in Theorem 1.7- are also obtained from the truncated series by seeking the minimal value for which is zero at some . The approximation for is then improved using the fact that .
2 The family and the polynomials
From (2) it is easy to see that
[TABLE]
Moreover, for all , so is both completely monotonic and a Bernstein function, while is completely monotonic for all because of [4, Proposition 9.2], where we use that
[TABLE]
is a Bernstein function. In particular is not a Bernstein function when . This means that the set of such that is a Bernstein function is the closed interval .
For an open set we denote by the set of holomorphic functions defined in .
Clearly , but we shall see that extends to a holomorphic function in . In fact, for we have
[TABLE]
so defining , we see that , where
[TABLE]
Now for yields a holomorphic extension of to .
In the next two results we obtain suitable power series expansions for , and .
Proposition 2.1**.**
The power series of given by (12) can be written
[TABLE]
where is the sequence of polynomials defined in (4) and (5).
Proof.
We use the formula
[TABLE]
where are the exponential Bell partition polynomials, cf. [6, Section 11.2]. It is known that
[TABLE]
and in general we have the recursion formula
[TABLE]
Defining , this gives for
[TABLE]
where we have defined
[TABLE]
We see by induction that is a polynomial in of degree such that (4) holds, and the recursion (5) follows like this
[TABLE]
∎
Corollary 2.2**.**
For we have the Laurent expansions
[TABLE]
and in particular
[TABLE]
In the following lemma we study the restriction of the function to the imaginary axis.
Lemma 2.3**.**
Let . As a function of
[TABLE]
is continuous and tends to 0 for . It belongs to .
Proof.
We have for
[TABLE]
where is the inverse of . The continuity of for follows, and the behavior at including the integrability properties follows from Corollary 2.2. ∎
By Plancherel’s Theorem is the Fourier-Plancherel transform of another -function :
[TABLE]
where the limit is in , and by the inversion theorem is given as
[TABLE]
where again the limit is in . For certain sequences we also know that
[TABLE]
for almost all . Furthermore,
[TABLE]
Remark 2.4**.**
The above formulas (16)-(19) hold trivially for with .**
Lemma 2.5**.**
We have for .
Proof.
Let denote the half-circle with radius
[TABLE]
considered as a positively oriented closed contour.
Since is holomorphic in with a continuous extension to the closed right half-plane bounded by the vertical line , we have by Cauchy’s integral theorem
[TABLE]
The absolute value of the integrand to the right is by (15) bounded by
[TABLE]
for a suitable depending on . If we assume , then for when , so the integral to the right tends to 0 by dominated convergence. Using (18) we now see that for almost all . Since is an equivalence class of square integrable functions, we can assume that for . ∎
Exploiting the holomorphy of in we can prove part of Theorem 1.1, which is contained in the following.
Theorem 2.6**.**
For , the function defined in (3) is an entire function, which is independent of .
Moreover, the function
[TABLE]
is equal to for almost all .
Remark 2.7**.**
In the following we denote the function given by (20) as . **
Proof.
It is clear that the function from (3) is entire, and also that it is independent of by Cauchy’s integral theorem.
Let and consider the following three positively oriented closed contours: two quarter circles with radius
[TABLE]
and a rectangle with corners . By Cauchy’s integral theorem we have
[TABLE]
Adding these three integrals to the contour integral in (3) yields
[TABLE]
where is the following contour
[TABLE]
For we have
[TABLE]
In fact, for we have , hence for suitable by (15). This gives
[TABLE]
which tends to 0 for because for . The function
[TABLE]
converges to in for by (17), so for a suitable sequence we know that converges to for almost all . It follows that for almost all . Since apriori we only know that is an equivalence class of square integrable functions, we can use formula (20) as a representative of . ∎
At this point we are able to prove Theorem 1.2, that is, to obtain the power series expansion of .
Proof of Theorem 1.2.
From (3) and the compactness of the contour we get
[TABLE]
Using that is holomorphic outside , we can replace the contour by the circle , where . We next use the Laurent expansion (14) and get
[TABLE]
which shows (6). ∎
In the following proposition we list several properties of the polynomials that appear in the series (6). We prove below the Properties through , in particular, Properties through will be needed in Theorem 2.10, in order to conclude the proof of Theorem 1.1. The remaining properties rely partially on the results of Section 3 and will be proved in Section 5. See also Remark 7.1 and Equation (55) in the Appendix, for an alternative expression for the polynomials , based on Stirling numbers.
Proposition 2.8**.**
The polynomials from Theorem 1.2 satisfy Theorem 1.6 and
- (i)
*, where and *
* *
- (ii)
.
- (iii)
0\leq p_{n}(\alpha)\leq\left\{\begin{array}[]{lll}1,&\mbox{when }\,0\leq\alpha\leq 1,\\ \alpha^{n},&\mbox{when }\,1\leq\alpha,\\ n,&\mbox{when }\,0\leq\alpha\leq 2,n\geq 1.\end{array}\right.**
- (iv)
For and we have the addition formula
[TABLE]
- (v)
The sequence is \left\{\begin{array}[]{lll}\text{strictly decreasing, }&\text{ for 0<\alpha\leq 1, }\\ \text{increasing, }&\text{ for 2\leq\alpha. }\end{array}\right.
- (vi)
\displaystyle\lim_{n\to\infty}p_{n}(\alpha)=\left\{\begin{array}[]{ll}0,&\mbox{when }\,0<\alpha<1,\\ e^{-1},&\mbox{when }\,\alpha=1,\\ \infty,&\mbox{when }\,\alpha>1.\end{array}\right.**
- (vii)
.
Proof of Proposition 2.8: (i) through (iv).
Property follows easily by induction using the recursion (5), while Property follows because the coefficients of are non-negative.
Property follows by induction, as described below. The two first inequalities hold for , and assuming the assertion for we get by (5), for
[TABLE]
and for
[TABLE]
The last inequality holds for , and by induction using and for we find, for ,
[TABLE]
To see we notice that by (2) we get
[TABLE]
and by (14)
[TABLE]
This implies that
[TABLE]
which clearly holds for . Multiplying the absolutely convergent power series for in (21), we get the addition formula. ∎
By Theorem 1.2 and Proposition 2.8- we obtain the following.
Corollary 2.9**.**
The entire functions satisfy for
[TABLE]
The order and type of when are given in Theorem 1.3-.
We can finally conclude the proof of Theorem 1.1, as a consequence of the following.
Theorem 2.10**.**
For any , is bounded for and tends to 0 for . The following formula holds
[TABLE]
Proof.
Let us write (3) in another way. Introducing
[TABLE]
and
[TABLE]
we have for
[TABLE]
We see by Riemann-Lebesgue’s lemma that . Furthermore,
[TABLE]
and
[TABLE]
show that
[TABLE]
By (23) it follows that . This property together with the continuity of imply that is bounded on .
To prove the formula (22) we note that the right-hand side is holomorphic for , and so is the left-hand side.
For we have by Proposition 2.8-
[TABLE]
For we have
[TABLE]
Assume now . For the last expression converges to by Corollary 2.2. The integrand in the first expression converges for each to with an integrable majorant because of (24), so by Lebesgue’s Theorem on dominated convergence, we get
[TABLE]
This is enough to conclude (22). ∎
As discussed in the Introduction, we can now state the following important result.
Theorem 2.11**.**
For , is completely monotonic if and only if for . In the affirmative case is integrable on and
[TABLE]
Moreover, in this case (22) holds for and
[TABLE]
Proof.
The first assertion follows from Bernstein’s characterization of completely monotonic functions as Laplace transforms of positive measures. Equation (25) follows from (11), (22) and the monotonicity theorem of Lebesgue.
When is integrable over , the right-hand side of (22) is continuous in the half-plane , and since is also continuous there, we see that (22) holds for . The Equation (26) follows easily from (25). ∎
3 The cases
As mentioned in Section 1, it was proved in [1] that is completely monotonic for and equivalently is non-negative on for these values of . We shall use the previous results to give a new proof of this. We recall that a function is called a Stieltjes function, if it has the form
[TABLE]
where and is a positive measure on . A Stieltjes function is completely monotonic but the converse is not true. For more information about Stieltjes functions see [4] and [3].
We have the following result.
Theorem 3.1**.**
The function is a Stieltjes function for , but not for .
The cases , and are treated separately in Theorem 3.2, Corollary 3.4 and Proposition 3.5.
Theorem 3.2**.**
For we have
[TABLE]
and
[TABLE]
Proof.
Assume and let in the contour from Theorem 2.6 be chosen such that and .
Let now in (23). The first two terms tend to 0. Using that is real we can write
[TABLE]
and replacing by in this expression, we get
[TABLE]
We have
[TABLE]
where
[TABLE]
and .
We therefore have (leaving out the arguments in to simplify notation)
[TABLE]
and hence
[TABLE]
We have the following inequalities for , using that ,
[TABLE]
and since , the last expression is an integrable majorant over . By Lebesgue’s Theorem we therefore get
[TABLE]
so for and .
[TABLE]
By the identity theorem for holomorphic functions (31) holds for . ∎
Equation (30) shows that is completely monotonic for . For we get that is completely monotonic and in particular non-negative, and by [4, Section 14.12] we get that is a Stieltjes function.
To find the representations of and in analogy with (30) and (31), it turns out not to be correct to replace by 1 in these formulas.
Let us introduce the notation
[TABLE]
Clearly , and is seen to be bounded by , while
[TABLE]
Proposition 3.3**.**
For define
[TABLE]
Then for any we have
[TABLE]
Proof.
We need the following partial results:
Step 1: for , uniformly for for any .
This is clear.
Step 2:
[TABLE]
To see this, note that by (28) and (7)
[TABLE]
and
[TABLE]
see [1, Lemma 2, p. 4]. Therefore
[TABLE]
which has limit 1 for , proving Step 2.
Let now . Let be given and by continuity choose such that for . We can then write
[TABLE]
and hence
[TABLE]
By Step 1 we know that for . Furthermore, by (33) and (34) we find
[TABLE]
Finally, tends to 0 for because
[TABLE]
and we then use Step 1 and Step 2.
In total we get
[TABLE]
and (32) follows. ∎
Applying the above result to the continuous functions and for we get
Corollary 3.4**.**
[TABLE]
[TABLE]
Proposition 3.5**.**
The function is not a Stieltjes function when
Proof.
By (27) a non-constant Stieltjes function has an extension to a holomorphic function in satisfying
[TABLE]
because for we have
[TABLE]
For let be chosen such that . For we have
[TABLE]
and proceeding as in the proof of Theorem 3.2 we get
[TABLE]
This shows that for sufficiently small. By (36) this shows that is not a Stieltjes function when . ∎
Using the formulas for in Theorem 3.2 and Corollary 3.4 we can prove that the sequence is a Hausdorff moment sequence, i.e., the moment sequence of a positive measure on .
Theorem 3.6**.**
For we have
[TABLE]
while for
[TABLE]
Proof.
Inserting the power series for in Equation (28) and interchanging summation and integration, we get the power series expansion for . Compared with (6) this yields (37).
To get the case we can proceed similarly with the formula for in Corollary 3.4, or we can apply Proposition 3.3 to . ∎
See Remark 7.2 in the Appendix, for a proof that the sequence is also a Hausdorff moment sequence.
We can now prove the equivalence of the three conditions in Theorem 1.5.
Proof of Theorem 1.5.
”” If is a Stieltjes moment sequence, i.e., (8) holds for a positive measure on , then . Without loss of generality we can assume . By Proposition 2.8- we know that , where , which implies that is supported by the interval . By (6) we then get
[TABLE]
which shows that is completely monotonic.
”” If is completely monotonic, hence of the form
[TABLE]
for a positive measure , we get, using (6),
[TABLE]
but this is only possible if . Furthermore,
[TABLE]
so is a Stieltjes function and hence by Theorem 3.1.
”” follows from Theorem 3.6. ∎
4 The case
In the previous section we were able to express the functions with as in Equation (9), proving that they are nonnegative on The purpose of this section is to show that, for , we can still find a component in analogous to (9), but a correcting term needs to be added, which is given by a contour integral on a suitable circle that goes around the singularity : see Equations (40) and (41).
For and we denote by the positively oriented circle with center and radius .
Let be fixed, and let . We consider the closed positively oriented contour starting at , then moving left along the horizontal line till it cuts the circle at a point denoted . We then move along the circle till we reach the complex conjugate point (passing on the way), and then we move along the horizontal line till we reach , which is connected to via the vertical segment .
The contour can replace the contour of Theorem 2.6 so we have
[TABLE]
We shall now obtain a new expression for by letting tend to 0. Note that .
This leads to the following result.
Theorem 4.1**.**
For we have
[TABLE]
where
[TABLE]
and is given in (2). The first term on the right-hand side of (40) is a completely monotonic function.
Proof.
Letting in (39), we note that the contribution from tends to [math], and we get
[TABLE]
where
[TABLE]
and
[TABLE]
In (42) we used that the term has integral 0 over the circle, because it is an entire function of . We further get
[TABLE]
where we have used the same technique as in the proof of Theorem 3.2. This gives formula (40). ∎
5 Properties of the sequences .
This section is devoted to the proof of the remaining properties of the polynomials , which were stated in Proposition 2.8 and Theorem 1.6.
Proof of Proposition 2.8-(v, vi).
In the case Properties and follow directly from the formulas (37) and (38).
From (5) we estimate, for ,
[TABLE]
and for this proves .
Property for will be proved in Proposition 5.1. ∎
In order to study further the sequence it is useful to introduce the sequence of the mean-values
[TABLE]
which satisfies the recursion
[TABLE]
Note that by (5)
[TABLE]
Observe that for any we can estimate, for ,
[TABLE]
where the last sum in (46) is positive.
Proposition 5.1**.**
For we have
[TABLE]
Proof.
The case .
In this case by (45), and then (44) implies that , so increases to . We claim that and the proposition is proved because of (45). We shall see that the assumption leads to a contradiction. We choose a sufficiently small so that
[TABLE]
and next so that for . We then get
[TABLE]
which leads to a contradiction, since it implies that will eventually exceed .
The case .
We proceed in steps:
Step 1: The sequence is unbounded.
Assume for contradiction that for all . Then also , and since by Proposition 2.8-, we also get .
For a given we choose the smallest so that
[TABLE]
and such that
[TABLE]
From (46) we then get
[TABLE]
and since the last term tends to 0 for , we get
[TABLE]
where is sufficiently large. Therefore for and finally exists and .
Let now be so small that by (47)
[TABLE]
and let be so large that for . By (46) we get for
[TABLE]
hence
[TABLE]
where is sufficiently large. Therefore will eventually be larger than , which is a contradiction, and we have proved Step 1.
Step 2: The sequence is eventually strictly increasing.
Once this is proved, we know that for otherwise is a bounded sequence, and so is by (45), and this contradicts Step 1.
To see Step 2 we note that by Step 1 there exist indices such that is strictly increasing to infinity. By (45) we get that
[TABLE]
We now use that and hence for by Proposition 2.8-. From (46) we then get for
[TABLE]
Since , there exists so that for
[TABLE]
This gives and hence .
We prove now by induction that is strictly increasing for . We have just established the start of the induction proof.
Assume that for some
[TABLE]
By (48) we have
[TABLE]
where the last inequality follows from (49). ∎
Proof of Proposition 2.8-(vii).
We will only prove , then follows from [12, Theorem 3.37].
For every , by (43),
[TABLE]
For , we already know from Proposition 2.8- that and then
[TABLE]
[TABLE]
For , by (45) and Property in Proposition 2.8 we have
[TABLE]
[TABLE]
For a given the sum in the denominator is bounded because of (52). Then we obtain, using (51),
[TABLE]
Since is any integer, along with (50), this proves that
[TABLE]
For we use (48) instead of (46), to obtain
[TABLE]
Again, for a fixed the sum in the denominator is bounded and since we conclude as above. ∎
Proof of Theorem 1.6.
In the case , Equation (10) follows immediately from Proposition 2.8-.
For , using that is increasing by Proposition 2.8- we get
[TABLE]
Finally, in the case , Equation (10) can be obtained combining (51) with (45):
[TABLE]
while .
Now, for and we have
[TABLE]
if and only if
[TABLE]
Since the left-hand side is by Equation (10), we see that the power series (6) satisfies the Alternating Series Test for . ∎
Remark 5.2**.**
Property in Proposition 2.8 does not consider the case . From numerical calculations it seems true that is increasing whenever , which is when . For , is decreasing for and increasing for , where is decreasing in . However, we have not been able to prove this.**
6 Proof of Theorem 1.3
In this section we prove several properties of the family of functions , that were listed in Theorem 1.3
In the proof of Theorem 1.3- we need the following lemma. The proof is left as an exercise.
Lemma 6.1**.**
Let
[TABLE]
be power series of entire functions and . Assume that for all
[TABLE]
where for all .
Then uniformly for in compact subsets of the complex plane.
Proof of Theorem 1.3-(i, ii).
We use that
[TABLE]
The first assertion follows from Proposition 2.8-, and the second assertion follows from Proposition 2.8- together with (5).
Lemma 6.1 now shows that
[TABLE]
uniformly for in compact subsets of . It is easy to see that the sum of this power series is equal to the function
[TABLE]
The zeros of are given by , which has no real solutions different from 0. The equation has countably many non-real solutions, which can be given using the branches of the Lambert function, available in Maple. For each the ’th branch is denoted and satisfies . It follows that the solutions to are , but and the other values given are calculated in Maple.
Assertion now follows from Hurwitz’ Theorem. ∎
Proof of Theorem 1.3-.
For simplicity we introduce
[TABLE]
Note that
[TABLE]
by Proposition 2.8-. Lemma 6.1 therefore shows that
[TABLE]
uniformly for in compact subsets of the complex plane.
The Bessel function of order 1 is defined by the series
[TABLE]
and hence
[TABLE]
The zeros of are all real and simple and equal to , where is a well-known sequence of positive numbers tending to infinity.
The zeros of the right-hand side of (54) are . In a sufficiently small disc centered at , has a unique zero , when is sufficiently large. It is simple and we have
[TABLE]
This is according to a theorem of Hurwitz. If the complex zeros of must appear in conjugate pairs, and therefore must be real and hence positive for otherwise would contain two zeros, when is sufficiently large. ∎
Proof of Theorem 1.3-(v).
The order and type does not change when we multiply an entire function by a constant, then we may work with as in (53). Defining
[TABLE]
it is known, cf. e.g. [5], that the order of is
[TABLE]
but since
[TABLE]
by Proposition 2.8- and Stirling’s formula, we get
[TABLE]
which converges to 1, hence .
The type is given by
[TABLE]
but since , we get . ∎
7 Appendix
In this appendix we add a few remarks that came up after the submission of this work.
Remark 7.1**.**
A referee has kindly pointed out that the coefficients of the polynomials can be expressed by the following formula
[TABLE]
where the are the Stirling numbers of the first kind defined by
[TABLE]
, see [6, p.278]. Note that for , so in (55) one may sum from as well. To see (55) we use the formula
[TABLE]
where the partial Bell partition polynomials are defined as
[TABLE]
cf. [6, Section 11.2]. The sum is over the set of all integers satisfying
[TABLE]
In the special case we then get
[TABLE]
In [11, Theorem 1] one finds the evaluation
[TABLE]
and hence by (13)
[TABLE]
and finally one obtains (55).
We observe that, from (55), it is possible to deduce the explicit formula for given in Proposition 2.8-, using that , and also, since with being the harmonic number, to obtain the following formula for :
[TABLE]
Further formulas can be obtained in terms of generalized harmonic numbers but they become increasingly more complicated.
Also the explicit formula for given in Proposition 2.8- can be obtained, by using (56) and the definition of :
[TABLE]
Remark 7.2**.**
Alan Sokal asked the first author if Theorem 3.6 can be replaced by the stronger statement that is a Hausdorff moment sequence when . The answer is yes, but the reader is warned that Equations (37) and (38) do not hold for .
In fact, if we get for
[TABLE]
where we have used (29) and (11), and there is a similar calculation in case . Using the Hausdorff moment sequence we find for
[TABLE]
showing that is a Hausdorff moment sequence when . We similarly get and
[TABLE]
Acknowledgments
This work was initiated during a visit of the first author to the Department of Mathematics at the University of São Paulo in São Carlos, Brazil, in March 2018. He wants to thank the Department for generous support and hospitality during his stay.
The second author was supported by: grant 303447/2017-6, CNPq/Brazil.
The third author was supported by: grant 2016/09906-0, São Paulo Research Foundation (FAPESP).
The authors thank a referee for useful references leading in particular to Remark 7.1.
The reference list from the paper itself. Each links out to its DOI / PubMed record.
- 1[1] H. Alzer and C. Berg, Some classes of completely monotonic functions , Ann. Acad. Sci. Fenn. Math. 27 (2002), 445-460.
- 2[2] C. Berg, Problem 1. Bernstein functions , J. Comput. Appl. Math. 178 (2005), 525-526.
- 3[3] C. Berg, Stieltjes-Pick-Bernstein-Schoenberg and their connection to complete monotonicity. Pages 15–45 in Positive Definite Functions: From Schoenberg to Space-Time challenges . J. Mateu and E. Porcu eds. Castellón de la Plana 2008.
- 4[4] C. Berg and G. Forst, Potential Theory on Locally Compact Abelian Groups, Ergebnisse der Mathematik und ihrer Grenzgebiete Band 87, Springer-Verlag, Berlin-Heidelberg-New York, 1975.
- 5[5] R. P. Boas, Entire functions, Academic Press, New York, 1954.
- 6[6] C. A. Charalambides, Enumerative Combinatorics, Chapman & Hall / CRC, 2002.
- 7[7] R. M. Corless, G. H. Gonnet, D. E. G. Hare, D. J. Jeffrey and D. E. Knuth, On the Lambert W 𝑊 W Function . Advances in Computational Mathematics. 5 (1996), 329–359.
- 8[8] B. -N. Guo and F. Qi, A property of logarithmically absolutely monotonic functions and the logarithmically complete monotonicity of a power-exponential function , U.P.B. Sci. Bull., Series A, 72 no. 2 (2010), 21–30.
