Effective Bounds for the Andrews spt-function
Madeline Locus Dawsey, Riad Masri

TL;DR
This paper derives an effective asymptotic formula for the Andrews spt-function, proves inequalities involving it and the partition function, and employs trace formulas of singular moduli to establish bounds.
Contribution
It provides the first effective bounds for the spt-function using trace formulas, confirming conjectures and strengthening inequalities related to partition functions.
Findings
Established an asymptotic formula with effective error bounds for spt(n)
Proved inequalities relating spt(n) and p(n) with explicit constants
Demonstrated the use of trace formulas of singular moduli for effective bounds
Abstract
In this paper, we establish an asymptotic formula with an effective bound on the error term for the Andrews smallest parts function . We use this formula to prove recent conjectures of Chen concerning inequalities which involve the partition function and . Further, we strengthen one of the conjectures, and prove that for every there is an effectively computable constant such that for all , we have \begin{equation*} \frac{\sqrt{6}}{\pi}\sqrt{n}\,p(n)<\mathrm{spt}(n)<\left(\frac{\sqrt{6}}{\pi}+\epsilon\right) \sqrt{n}\,p(n). \end{equation*} Due to the conditional convergence of the Rademacher-type formula for , we must employ methods which are completely different from those used by Lehmer to give effective error bounds for . Instead, our approach relies on the fact that…
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Effective bounds for the Andrews spt-function
Madeline Locus Dawsey
Department of Mathematics and Computer Science, Emory University, Atlanta, GA 30322
and
Riad Masri
Department of Mathematics, Mailstop 3368, Texas A&M University, College Station, TX 77843-3368
Abstract.
In this paper, we establish an asymptotic formula with an effective bound on the error term for the Andrews smallest parts function . We use this formula to prove recent conjectures of Chen concerning inequalities which involve the partition function and . Further, we strengthen one of the conjectures, and prove that for every there is an effectively computable constant such that for all , we have
[TABLE]
Due to the conditional convergence of the Rademacher-type formula for , we must employ methods which are completely different from those used by Lehmer to give effective error bounds for . Instead, our approach relies on the fact that and can be expressed as traces of singular moduli.
*This author was previously known as Madeline Locus.
1. Introduction and Statement of Results
The smallest parts function of Andrews is defined for any integer as the number of smallest parts among the integer partitions of size . For example, the partitions of are (with the smallest parts underlined):
[TABLE]
and so . The spt-function has many remarkable properties. For example, Andrews [3] proved the following analogues of the well-known Ramanujan congruences for the partition function :
[TABLE]
One can compute by making use of the generating function
[TABLE]
where
[TABLE]
We use this generating function to compute the values of required for this paper.
In this paper, we will prove the following asymptotic formula for with an effective bound on the error term.
Theorem 1.1**.**
Let . Then for all , we have
[TABLE]
where
[TABLE]
with
[TABLE]
Our interest in proving the effective error bounds of Theorem 1.1 was motivated in part by the following recent conjectures of Chen [10] concerning inequalities which involve and .
Conjecture** (Chen).**
- (1)
For , we have
[TABLE] 2. (2)
For or , we have
[TABLE] 3. (3)
For , we have
[TABLE] 4. (4)
For , we have
[TABLE] 5. (5)
For , we have
[TABLE] 6. (6)
For , we have
[TABLE]
Remark. Conjectures (1) and (2) are slight modifications of Chen’s original claims.
By combining Theorem 1.1 with classical work of Lehmer [20] which gives effective error bounds for , we will prove the following result.
Theorem 1.2**.**
All of Chen’s conjectures are true.
We will also use Theorem 1.1 to prove the following more precise version of Theorem 1.2 regarding Conjecture (1).
Theorem 1.3** (Refined Theorem 1.2 (1)).**
For each , there is an effectively computable constant such that for all , we have
[TABLE]
Remark. The constant of Theorem 1.3 can be computed in practice. For example, by letting in Theorem 1.3, we get Theorem 1.2 (1) for with . We then use a computer to verify Theorem 1.2 (1) in the exceptional range .
Remark. In analogy with the Hardy-Ramanujan asymptotic for , Bringmann [6] used the circle method to establish the asymptotic
[TABLE]
as . Bringmann’s asymptotic for implies that
[TABLE]
as . Theorem 1.3 refines the asymptotic (1.1).
We now describe our approach to Theorem 1.1. In particular, we explain some of the difficulties involved in proving effective error bounds for .
In [24], Rademacher established an exact formula for as the absolutely convergent infinite sum
[TABLE]
where is the -Bessel function, is the Kloosterman-type sum
[TABLE]
and is the classical Dedekind sum
[TABLE]
Recently, Ahlgren and Andersen [1] gave a Rademacher-type exact formula for as the conditionally convergent infinite sum
[TABLE]
In order to give an effective bound on the error term for , Lehmer [20] truncated the absolutely convergent sum (1.2) and applied bounds for the Kloosterman-type sum . On the other hand, since the formula (1.3) is only conditionally convergent, bounding is a much more delicate matter. In fact, to resolve the difficult problem of proving that (1.3) converges, Ahlgren and Andersen used advanced methods from the spectral theory of automorphic forms. To give an effective bound on the error term for , we will instead use different types of formulas for and which express these functions as traces of singular moduli.
To state these formulas, consider the weight weakly holomorphic modular form for defined by
[TABLE]
By applying the Maass weight-raising operator to , one gets the following weight zero weak Maass form for ,
[TABLE]
Bruinier and Ono [8] proved the following formula for .
Theorem** (Bruinier–Ono).**
For all , we have
[TABLE]
where the sum is over the equivalence classes of discriminant positive definite, integral binary quadratic forms such that and , and is the Heegner point given by the root in the complex upper half-plane .
Similarly, consider the weight zero weakly holomorphic modular form for defined by
[TABLE]
Ahlgren and Andersen [1] proved the following analogue of (1.4) for .
Theorem** (Ahlgren–Andersen).**
For all , we have
[TABLE]
Identities which express Fourier coefficients of weak Maass forms as traces of singular moduli have been used in many contexts to give strong asymptotic formulas. For example, Bringmann and Ono [7] expressed as a twisted trace of singular moduli by arithmetically reformulating Rademacher’s exact formula (1.2) for . Folsom and the second author [16] then combined the Bringmann-Ono formula with spectral methods and subconvexity bounds for quadratic twists of modular –functions to give an asymptotic formula for with a power-saving error term. In particular, by calculating the main term in this asymptotic formula in terms of the truncated main term in Rademacher’s exact formula for , these authors improved the exponent in Lehmer’s bound [20]. This exponent was further improved by Ahlgren and Andersen [2].
In the works [21, 22, 4], spectral methods and subconvexity bounds were again used to give asymptotic formulas with power-saving error terms for twisted traces of singular moduli. These results were applied to study a variety of arithmetic problems, including the distribution of and , and the distribution of partition ranks. Note that although the constants in the error terms of these results are effective, it would be very difficult to actually give explicit numerical values for these constants because of the techniques involved in the proofs. However, there is an alternative approach which we now describe.
Using (1.4), the formula (1.6) can be written as
[TABLE]
where is the trace of singular moduli for given by
[TABLE]
By applying Lehmer’s effective error bounds for in (1.7), we will reduce the proof of Theorem 1.1 to the following asymptotic formula for the trace with an effective bound on the error term.
Theorem 1.4**.**
Let . Then for all , we have
[TABLE]
where
[TABLE]
with
[TABLE]
Our proof of Theorem 1.4 is inspired by work of Dewar and Murty [14], who used the formula (1.4) to derive the Hardy-Ramanujan asymptotic formula for without using the circle method. In order to give effective bounds, additional care must be taken. For instance, we must give effective bounds for the Fourier coefficients of .
Organization. The paper is organized as follows. In Section 2, we review some facts regarding quadratic forms and Heegner points. In Section 3, we prove Theorem 1.4. In Section 4, we prove Theorem 1.1. In Section 5, we prove Theorem 1.3. Finally, in Section 6, we prove the remaining conjectures.
Acknowledgments. We thank Adrian Barquero-Sanchez, Sheng-Chi Liu, Karl Mahlburg, Ken Ono, Wei-Lun Tsai, and Matt Young for very helpful discussions regarding this work, and Michael Griffin and Lea Beneish for help computing values of . We also thank the referees for many detailed comments and corrections, leading to simplifications of some arguments, sharper estimates, and an improved exposition.
2. Quadratic forms and Heegner points
Let be a positive integer and be a negative discriminant coprime to . Let be the set of positive definite, integral binary quadratic forms
[TABLE]
of discriminant with . There is a (right) action of on defined by
[TABLE]
where for we have
[TABLE]
Given a solution of , we define the subset of forms
[TABLE]
Then the group also acts on . The number of equivalence classes in is given by the Hurwitz-Kronecker class number .
The preceding facts remain true if we restrict to the subset of primitive forms in ; i.e., those forms with
[TABLE]
In this case, the number of equivalence classes in is given by the class number .
To each form , we associate a Heegner point which is the root of given by
[TABLE]
The Heegner points are compatible with the action of in the sense that if , then
[TABLE]
3. Proof of Theorem 1.4
In this section, we prove Theorem 1.4, which gives an asymptotic formula with an effective bound on the error term for the trace of the weight zero weakly holomorphic modular form for defined by (1.5). This will be used crucially in the proof of Theorem 1.1.
Let for and define the trace of by
[TABLE]
First, we decompose as a linear combination of traces involving primitive forms. Let be any discriminant with and define the class polynomials
[TABLE]
and
[TABLE]
Let be the group of Atkin-Lehner involutions for . Since
[TABLE]
with for and for , then arguing exactly as in the proof of [9, Lemma 3.7], we get the identity
[TABLE]
where if and otherwise. Comparing terms on both sides of (3.2) yields the class number relation
[TABLE]
and the decomposition
[TABLE]
where
[TABLE]
Next, following [14] we express as a trace involving primitive forms of level 1. The group has index 12 in . We choose the following 12 right coset representatives:
[TABLE]
We denote this set of coset representatives by . Each matrix maps the cusp to one of the four cusps of the modular curve , which have widths 1, 2, 3, and 6, respectively. In particular, we have , , , and .
Recall that a form is reduced if
[TABLE]
and if either or , then . Let denote a set of primitive, reduced forms representing the equivalence classes in . For each , there is a unique choice of coset representative such that
[TABLE]
This induces a bijection
[TABLE]
see the Proposition on page 505 in [17], or more concretely, [14, Lemma 3], where an explicit list of the matrices is given.
Using the bijection (3.4) and the compatibility relation (2.1) for Heegner points, the trace can be expressed as
[TABLE]
Therefore, to study the asymptotic distribution of , we need the Fourier expansion of with respect to the matrices , and .
In [1, Section 4], Ahlgren and Andersen compute the Fourier expansion of at the cusp . The basic idea is as follows. The weakly holomorphic modular form has a Fourier expansion of the form
[TABLE]
for some integers for . One can construct a weight zero weak Maass form for with eigenvalue whose analytic continuation at is a harmonic function on with the Fourier expansion
[TABLE]
where
[TABLE]
Here is the Möbius function, is the Kloosterman sum
[TABLE]
and are the Bessel functions of order 1 (note that is the multiplicative inverse of ). From these Fourier expansions, one can see that the functions and have the same principal parts in the cusps , hence the function is bounded on the compact Riemann surface . Since a bounded harmonic function on a compact Riemann surface is constant, the function is constant.
Now, using the Fourier expansions of and , we use SageMath to compute
[TABLE]
In particular, . On the other hand, in Lemma 3.1 we show by a direct calculation that . Since is constant, we have
[TABLE]
Finally, since , then by uniqueness of Fourier expansions we have for , , and for .
We next use the Fourier expansion
[TABLE]
to compute the Fourier expansion of with respect to the matrices , and .
The Atkin-Lehner involutions for are given by
[TABLE]
For each and , let and
[TABLE]
We have
Note that and
[TABLE]
Let be any matrix such that . Then
[TABLE]
so that
[TABLE]
where is the stabilizer of the cusp . In particular, there is an integer such that
[TABLE]
By solving for for each cusp, we have
[TABLE]
Now, by (3.1) we have for and for . Hence
[TABLE]
The Fourier expansion of with respect to the matrices can now be determined from the Fourier expansion at using these identities. In particular, if is a primitive sixth root of unity, we have
[TABLE]
Given a form and corresponding coset representative , let be the width of the cusp , and let and be the sixth roots of unity defined as follows:
Then we can write
[TABLE]
In the following lemma we evaluate and give effective bounds for the Fourier coefficients for .
Lemma 3.1**.**
We have and
[TABLE]
where
[TABLE]
Proof.
We first evaluate . Recall that
[TABLE]
Since , we can evaluate the Ramanujan sum as
[TABLE]
where the last equality follows from [19, Equation (3.4)]. Hence
[TABLE]
Now, if we have
[TABLE]
A similar calculation yields
[TABLE]
Then using we get
[TABLE]
We next estimate for . From the series (see dlmf.nist.gov/10.25.2)
[TABLE]
we get
[TABLE]
Also, using the asymptotic expansion (see dlmf.nist.gov/10.40.1) and the error bounds (see dlmf.nist.gov/10.40.(ii)), we get
[TABLE]
Let . Then using the Weil bound
[TABLE]
where is the number of divisors of , and the estimates (3.7) and (3.8), we get
[TABLE]
where
[TABLE]
and
[TABLE]
Using the bound (see [23])
[TABLE]
which implies that for , we get
[TABLE]
Also,
[TABLE]
Then combining estimates yields
[TABLE]
where
[TABLE]
∎
We are now in position to prove Theorem 1.4, which we restate for the convenience of the reader.
Theorem 3.2**.**
For all , we have
[TABLE]
where
[TABLE]
with
[TABLE]
Proof.
By (3.3), (3.5) and (3.6) we have
[TABLE]
where
[TABLE]
We have
[TABLE]
Next, observe that
[TABLE]
where is the primitive -th root of unity
[TABLE]
Since is reduced, the corresponding Heegner point lies in the standard fundamental domain for . In particular, we have
[TABLE]
which implies that
[TABLE]
Since , we have
[TABLE]
Then using (3.9) and Lemma 3.1, we get
[TABLE]
Combining the preceding estimates yields
[TABLE]
To estimate the infinite sum, we write
[TABLE]
and observe that
[TABLE]
in which case we have
[TABLE]
We then split the infinite sum into appropriate ranges and use the preceding bound to get
[TABLE]
A calculation shows that
[TABLE]
and
[TABLE]
We have now shown that
[TABLE]
where
[TABLE]
It remains to analyze the main term. Write the main term as
[TABLE]
where
[TABLE]
Observe that for any form , we have
[TABLE]
and
[TABLE]
Now, by [14, (4.2)] there are exactly 4 forms with , and these are given by
[TABLE]
Moreover, the corresponding coset representatives such that
[TABLE]
are given by
[TABLE]
Write
[TABLE]
where
[TABLE]
By (3.10) we have for all , hence using (3.11) we get
[TABLE]
Similarly, by (3.10) we have for all , hence for we have
[TABLE]
Then by (3.11) we have
[TABLE]
Since and for , using (3.11) we get
[TABLE]
Also, from the Fourier expansion of with respect to , and given previously, we have
[TABLE]
Hence
[TABLE]
By combining the preceding results, we get
[TABLE]
where with
[TABLE]
To complete the proof, we require only a crude effective upper bound for the Hurwitz-Kronecker class number .
Write with a fundamental discriminant and . Then we have the class number relation
[TABLE]
Inserting the formula (see e.g. [12, p. 233])
[TABLE]
into (3.12) yields
[TABLE]
where
[TABLE]
Now, a simple estimate yields
[TABLE]
where is the number of prime divisors of . We have
[TABLE]
and by [25, Théorème 13] we have
[TABLE]
Hence
[TABLE]
Using the class number formula
[TABLE]
and the evaluation
[TABLE]
another simple estimate yields
[TABLE]
Then combining the preceding estimates gives
[TABLE]
Finally, using the class number bound we get
[TABLE]
This completes the proof.
∎
4. Proof of Theorem 1.1
In this section, we prove Theorem 1.1. We will require an asymptotic formula for with an effective bound on the error term due to Lehmer [20]. For convenience, define
[TABLE]
Inspired by the Hardy-Ramanujan asymptotic for , Rademacher [24] obtained the exact formula
[TABLE]
where is the Kloosterman-type sum
[TABLE]
and is the Dedekind sum
[TABLE]
Using Rademacher’s formula, Lehmer [20] proved the following result.
Theorem 4.1** (Lehmer).**
For all , we have
[TABLE]
where
[TABLE]
We first use Theorem 4.1 to deduce the following effective bound.
Lemma 4.2**.**
For all , we have
[TABLE]
where
[TABLE]
Proof.
Using the identity
[TABLE]
we may write Theorem 4.1 (with the choice ) as
[TABLE]
where
[TABLE]
Now, using (4.1) and (4.2) we get
[TABLE]
where
[TABLE]
Using (4.1) we have the bound
[TABLE]
Then an estimate using the trivial bound
[TABLE]
and (4.3) yields
[TABLE]
Similarly, two straightforward estimates yield
[TABLE]
and
[TABLE]
Hence
[TABLE]
∎
4.1. Proof of Theorem 1.1
Using (1.4), the formula (1.6) can be written as
[TABLE]
Then using (4.4), Theorem 1.4, and Lemma 4.2, a straightforward calculation yields
[TABLE]
where the error term
[TABLE]
satisfies the bound
[TABLE]
∎
As pointed out by Bessenrodt and Ono [5], it is straightforward to obtain from Theorem 4.1 that
[TABLE]
for all .
We will use Theorem 1.1 to prove the following analogous statement for , where is replaced by any positive integral power of .
Theorem 4.3**.**
For each and , there is an effectively computable positive integer such that for all , we have
[TABLE]
Proof.
By Theorem 1.1 we have the bounds
[TABLE]
where
[TABLE]
Clearly, there is an effectively computable positive integer such that the inequality
[TABLE]
holds for all . For instance, if then . This completes the proof. ∎
5. Proof of Theorem 1.3
By Theorem 1.1 and Lemma 4.2, we may write
[TABLE]
and
[TABLE]
where
[TABLE]
Also, for we define
[TABLE]
We must prove that there exists an effectively computable positive constant such that for all , we have
[TABLE]
First, using (5.1) and (5.2) we find that the lower bound in (5.3) is equivalent to
[TABLE]
where . Now, the error bounds in Theorem 1.1 and Lemma 4.2 imply that
[TABLE]
where
[TABLE]
Then noting that for all , we find that (5.4) is implied by the bound
[TABLE]
or equivalently, the bound
[TABLE]
A calculation shows that (5.5) holds for all .
Similarly, using (5.1) and (5.2) we find that the upper bound in (5.3) is equivalent to
[TABLE]
where . The error bounds in Theorem 1.1 and Lemma 4.2 imply that
[TABLE]
where
[TABLE]
Moreover, there exists an effectively computable positive constant such that for all . Then arguing as above, we find that if , the bound (5.6) is implied by the bound
[TABLE]
where . Clearly, there exists an effectively computable positive constant such that (5.7) holds for all .
Let . Then the inequalities (5.3) hold for all . ∎
6. Proof of Theorem 1.2
6.1. Proof of Conjecture (1)
Let in Theorem 1.3. We need to determine the constant . A calculation shows that the inequality holds if where . Next, we need to find the smallest positive integer such that the bound
[TABLE]
holds for all . A calculation shows that this constant is given by . We now have
[TABLE]
Therefore, the inequalities
[TABLE]
hold for all . Finally, one can verify with a computer that these inequalities also hold for . ∎
6.2. Proof of Conjecture (2)
We follow closely the proof of [5, Theorem 2.1]. By taking in Theorem 4.3 (recall that ), we find that
[TABLE]
holds for all . One can verify with a computer that (6.1) also holds for .
Now, assume that , and let where . From (6.1) we get the inequalities
[TABLE]
and
[TABLE]
Hence, for all but finitely many cases, it suffices to find conditions on and such that
[TABLE]
For convenience, define
[TABLE]
Then by taking logarithms, we find that (6.2) is equivalent to
[TABLE]
As functions of , it can be shown that is increasing and is decreasing for , and thus
[TABLE]
and
[TABLE]
Hence it suffices to show that
[TABLE]
Moreover, since
[TABLE]
for all and all , it suffices to show that
[TABLE]
By computing the values and , we find that (6.4) holds for all .
To complete the proof, assume that . For each such integer , we calculate the real number for which
[TABLE]
The values are listed in the table below.
[TABLE]
By the discussion above, if is an integer for which , then (6.3) holds, which in turn gives the theorem in these cases. Only finitely many cases remain, namely the pairs of integers where and . We compute , and in these cases to complete the proof. ∎
6.3. Proof of Conjecture (3)
We require some lemmas and a proposition analogous to those of Desalvo and Pak [13] in order to prove the remaining conjectures.
The following is [13, Lemma 2.1].
Lemma 6.1**.**
Suppose is a positive, increasing function with two continuous derivatives for all , and that is decreasing, and is increasing for all . Then for all , we have
[TABLE]
By Theorem 1.1, we may write
[TABLE]
where
[TABLE]
and
[TABLE]
Lemma 6.2**.**
Let
[TABLE]
Then for all , we have
[TABLE]
Proof.
We can write from (6.5) as
[TABLE]
so that
[TABLE]
Then we have
[TABLE]
Since the functions and satisfy the hypotheses of Lemma 6.1, we get
[TABLE]
Computing derivatives gives
[TABLE]
for all , from which we deduce that
[TABLE]
for all . ∎
Lemma 6.3**.**
Define the functions ,
[TABLE]
and
[TABLE]
Then for all , we have
[TABLE]
and
[TABLE]
Proof.
First observe that for all , we have
[TABLE]
The bound is equivalent to
[TABLE]
Clearly, there is an effectively computable positive integer such that the inequality (6.7) holds for all . A calculation shows that (6.7) holds for all with . On the other hand, one can verify with a computer that
[TABLE]
Hence for all . Then using (6.6) and the inequalities
[TABLE]
and
[TABLE]
we get
[TABLE]
for all . Similarly, we get
[TABLE]
for all . ∎
Proposition 6.4**.**
Let
[TABLE]
Then we have
[TABLE]
for all and
[TABLE]
for all .
Proof.
We first bound by
[TABLE]
Then recalling that
[TABLE]
and , we take logarithms in the preceding inequalities to get
[TABLE]
It follows immediately from Lemmas 6.2 and 6.3 that for all , we have
[TABLE]
and
[TABLE]
Then a calculation shows that
[TABLE]
for all and
[TABLE]
for all . This completes the proof. ∎
To prove Conjecture (3), we must show that
[TABLE]
for . Taking logarithms, we see that this is equivalent to By the lower bound in Proposition 6.4, we have for all . Finally, one can verify with a computer that for all . This completes the proof. ∎
6.4. Proof of Conjecture (4)
We follow closely the proof of [13, Theorem 5.1]. Recall that a sequence of non-negative integers is log-concave if
[TABLE]
for all . Moreover, it is known that log-concavity implies strong log-concavity
[TABLE]
for all and (see e.g. [26]).
Now, we have proved that
[TABLE]
for all . Therefore, if we take , , and , then
[TABLE]
for all with .
We next consider the case with . We will prove that
[TABLE]
for all with . On the other hand, one can verify with a computer that
[TABLE]
for all with . This completes the proof of Conjecture (4), subject to verifying the inequalities (6.9).
Since , we have
[TABLE]
Moreover, since we have
[TABLE]
and thus
[TABLE]
This verifies the first and third inequalities in (6.9).
It remains to prove that
[TABLE]
for all . Taking logarithms in (6.10), we see that it suffices to prove
[TABLE]
for all . By [18, Section 2] and [15, (4)], respectively, we have the lower and upper bounds
[TABLE]
for all . Then by the inequality stated in Conjecture (1) (which is true by Theorem 1.2), we have
[TABLE]
for all . Using the inequalities (6.12) and , we see that the left hand side of (6.11) is bounded below by the function
[TABLE]
for all . A calculation shows that this function is positive for all . ∎
6.5. Proof of Conjecture (5)
Taking logarithms, we find that Conjecture (5) is equivalent to
[TABLE]
for all . By the upper bound in Proposition 6.4 and some straightforward estimates, we have
[TABLE]
for all . Finally, one can verify with a computer that the conjectured inequality holds for all . This completes the proof. ∎
6.6. Proof of Conjecture (6)
We follow closely the proof of [11, Conjecture 1.3]. Taking logarithms, we find that Conjecture (6) is equivalent to
[TABLE]
for all . By (6.8) we have
[TABLE]
for all . On the other hand, by [11, (2.3)] we have
[TABLE]
for all , and by [11, (2.23)] we have
[TABLE]
for all . Therefore, for all we have
[TABLE]
Now, a calculation shows that
[TABLE]
for all . Hence
[TABLE]
for all . Then using the inequality
[TABLE]
we get
[TABLE]
for all . Finally, one can verify with a computer that this inequality also holds for all . This completes the proof. ∎
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