Harmonic functions vanishing on a cone
Dan Mangoubi, Adi Weller-Weiser

TL;DR
This paper investigates the dimensionality of harmonic functions vanishing on a specific quadratic harmonic cone, providing evidence that for the right circular case, this family is finite dimensional, using an innovative arithmetic approach.
Contribution
The paper introduces a novel arithmetic method to analyze harmonic functions on quadratic cones, extending previous ideas and addressing a longstanding open question.
Findings
Harmonic functions vanishing on the right circular harmonic cone are likely finite dimensional.
The new arithmetic method extends Holt and Ille's ideas and resembles Hensel's Lemma.
No known nondegenerate quadratic harmonic cone has a proven infinite-dimensional family of vanishing harmonic functions.
Abstract
Let be a quadratic harmonic cone in . We consider the family of all harmonic functions vanishing on . Is finite or infinite dimensional? Some aspects of this question go back to as early as the 19th century. To the best of our knowledge, no nondegenerate quadratic harmonic cone exists for which the answer to this question is known. In this paper we study the right circular harmonic cone and give evidence that the family of harmonic functions vanishing on it is, maybe surprisingly, finite dimensional. We introduce an arithmetic method to handle this question which extends ideas of Holt and Ille and is reminiscent of Hensel's Lemma.
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Harmonic functions vanishing on a cone
Dan Mangoubi and Adi Weller Weiser
Abstract
Let be a quadratic harmonic cone in . We consider the family of all harmonic functions vanishing on . Is finite or infinite dimensional? Some aspects of this question go back to as early as the 19th century. To the best of our knowledge, no nondegenerate quadratic harmonic cone exists for which the answer to this question is known. In this paper we study the right circular harmonic cone and give evidence that the family of harmonic functions vanishing on it is, maybe surprisingly, finite dimensional. We introduce an arithmetic method to handle this question which extends ideas of Holt and Ille and is reminiscent of Hensel’s Lemma.
1 Introduction
1.1 Background
Consider the family of harmonic functions in the unit ball vanishing on a given set . It was conjectured in [9] and was completely proved by Logunov and Malinnikova in [7] and [8] that possesses compactness properties. More precisely, one can prove a Harnack type inequality for the quotient of two functions in . In the family is locally infinite dimensional (see [9] for examples). In higher dimensions few examples of infinite dimensional are known. In fact, all known examples stem from two dimensional ones (see [7, 4.2]). In particular, in dimension it is not even known whether there exists an infinite dimensional family where is a nondegenerate quadratic harmonic cone (it may be worth mentioning that in dimension there exists such an example, see [7, 4.2]). It turns out that this question and similar ones attracted the attention of several mathematicians.
Maybe the oldest closely related problem is a classical conjecture by Stieltjes (in a letter to Hermite [11, Letter 275]), which concerns arithmetic properties of harmonic functions in which are invariant under rotations around some axis. The present work considers the rotationally equivariant cases (see details in 1.2).
Second, an analogous question was raised and solved in the context of Bessel functions. Siegel [10] proved Bourget’s hypothesis that no two distinct Bessel functions have common zeros (see also [12, pp. 484-485]). To make the resemblance clear we note that the problem we treat here can be formulated as whether an associated Legendre function has a common root with the Legendre polynomial (see 8).
Third, as a possible application to the wave equation, Agranovsky and Krasnov raised in [1] the conjecture that there exists a quadratic harmonic cone such that is finite dimensional.
Last, a spectral theory point of view of the same problem was given recently by Bourgain and Rudnick in [3]. That work shows that given a curve of positive curvature on the standard two dimensional flat torus there exist only a finite number of Laplace eigenfunctions vanishing on that curve. In the case of the sphere, an analogous question would be: Let be a curve of constant latitude which is not the equator. Do there exist only a finite number of eigenfunctions vanishing on ? This question is still open, and the current work can be considered as treating a special case of it.
The aim of the present paper is to study the family where is the right circular harmonic cone in . In some sense, this is the simplest nondegenerate harmonic zero set in . We give evidence that this family is finite dimensional, while introducing a new method for handling this question.
1.2 Results and Methods
1.2.1 Main Result
Let us formulate the following Conjecture.
Conjecture 1**.**
Let where is the unit ball. Consider the family
[TABLE]
Then is finite dimensional.
Using standard tools of harmonic analysis (see [2] and 8) it is not difficult to show that Conjecture 1 is equivalent to the following one, which concerns the associated Legendre functions . The Legendre polynomials () will simply be denoted by .
Conjecture 1*′*.
The number of pairs such that is finite.
Here, for odd , means that divides the polynomial . The case of the preceding conjecture would follow from a conjecture of Stieltjes [11, Letter 275] concerning the irreducibility of the Legendre polynomials over . As such, it arose the interest of several authors and, in fact, was proved by Holt [5] and Ille [6]. The main new contribution of the current work comes in the cases where . We prove the following theorem (where we include the case for completeness).
Theorem 2**.**
For , if and only if .
For , if and only if .
If is even, then there exists at most one such that .
If is odd, then for all .
In fact, we prove a stronger statement in the case where is even. We show that in some sense there exists a unique dyadic integer such that . For the precise meaning of this please see 1.2.2 and Theorems 13 and 21.
1.2.2 Method
The method we use in this paper consists of two steps. In the first step, following an idea of Holt for the case , we transform to a polynomial whose coefficients are dyadic integers. As such, this polynomial can be studied using modular arithmetic. The question is whether this polynomial vanishes at the point . In the second step we consider as a (non-polynomial) function of . We ask whether . Our analysis shows that, if is even, is well defined on and that a solution modulus can be lifted uniquely to a solution modulus . In this way we get a unique dyadic integer such that (Propositions 12 and 20; Theorems 13 and 21). This idea is reminiscent of Hensel’s Lemma. However, we cannot apply Hensel’s Lemma in our case since the nature of the coefficients in Taylor’s expansion of is unclear.
1.2.3 Secondary Results
We describe a second approach to Conjecture 1, under significant additional assumptions. We prove
Theorem 3**.**
Let be a harmonic function. Then the product is harmonic if and only if for some .
Under the same assumption we can also break the rotational symmetry of the quadratic cone and get
Theorem 4**.**
Let be a harmonic function and . Then the product is harmonic if and only if for some .
The additional assumption on the harmonicity of lets us give a proof of Theorems 3 and 4 without arithmetic considerations. Perhaps our assumptions on can be weakened.
Acknowledgments
We are grateful to Charles Fefferman from whose discussions with the first author the work on this topic originated. We thank Zeev Rudnick for his interest in the present work and for helpful comments. We thank Eran Asaf, Nir Avni, Alexander Logunov, Eugenia Malinnikova and Amit Ophir for interesting discussions. This paper is part of the second author’s research towards a Ph.D. dissertation, conducted at the Hebrew University of Jerusalem. The cases of and odd in Theorem 2 together with Theorems 3 and 4 were proved in [13]. We gratefully acknowledge the support of ISF grant no. 753/14.
2 Step 1: Holt-Ille Transformation
In this section we transform the associated Legendre function to a polynomial of degree . The main property of is that its coefficients are dyadic integers, making it useful in analyzing whether and share a common root. This idea was developed by Holt [5] and Ille [6] for the case and we extend it here to the cases where .
We recall the following integral representation of the associated Legendre functions:
[TABLE]
for , where [4, Ch.VII, p. 505]. By Lemma 25 the integral on the right hand side is of the form where with and is a real homogeneous polynomial of degree . If we define
[TABLE]
then we can express and by
[TABLE]
Substituting the preceding expressions in gives
[TABLE]
where is a polynomial of degree normalized so that and the constant depends on and (for details see proof of Lemma 7 in 9). We note
Proposition 5**.**
* if and only if .*
Proof.
. Hence if and only if . The proposition now follows from (2) and (3). ∎
Notation 6**.**
We denote by coefficients such that the following holds
[TABLE]
The formulas for are recorded in the following lemma.
Lemma 7**.**
If is even, then
[TABLE]
and if is odd, then
[TABLE]
In both cases
[TABLE]
A proof for these formulas is included in 9.
3 Proof of Theorem 2: The case of odd
It will be convenient to use the following
Notation.
We denote
[TABLE]
We first assume that is odd. We rewrite formula (4) as follows,
[TABLE]
The term is even, since either or is even.
For we have that is even, since there are at least two consecutive numbers at the nominator of the second factor, and no even numbers in the denominator.
Combined with (6), it follows that . From Proposition 5 we get that .
If is even, essentially the same argument holds replacing formula (4) by formula (5). We leave the details to the reader.
4 Proof of Theorem 2: The case of
4.1 Recovering the lowest three bits of
Proposition 8**.**
If and then .
The proof is by ruling out the other possibilities one by one.
Lemma 9**.**
If and either or then .
Proof.
In these cases both and (see (7)) are even. Rewriting formulas (4) and (5) modulus 2, we get
[TABLE]
For every we have that is even, since it has the even factor . Summing over we get . ∎
Lemma 10**.**
If and then .
Proof.
Here is odd and is even. We calculate using formula (5).
[TABLE]
and
[TABLE]
From basic divisibility properties (Lemma 27) we also have
[TABLE]
Summing over we get . ∎
Lemma 11**.**
If and then .
Proof.
We let . By formula (4)
[TABLE]
[TABLE]
and
[TABLE]
where in the last calculation we used the fact that (Lemma 27). From basic divisibility properties (Lemma 27) we have for all . Summing over we get .
∎
To be complete we verify the remaining case .
Proposition 12**.**
If and then .
Proof.
We let . By formula (4)
[TABLE]
[TABLE]
and
[TABLE]
From basic divisibility properties (Lemma 27) we have for all . Summing over we get . ∎
4.2 Recovering the high bits of
In this section we introduce an idea in the spirit of Hensel’s lemma to recover the high bits of .
Theorem 13**.**
Let and suppose that . Then there exists a unique such that . Moreover, .
Using Proposition 8, Theorem 13 is an immediate corollary of
Proposition 14**.**
Let and . Fix and write with . Then .
Remark*.*
In particular, it follows that if then .
To prove Proposition 14 we first observe
Lemma 15**.**
Let , and . If then .
We postpone the proof of this Lemma to the end of the section.
Proof of Proposition 14.
By Lemma 15, for all we have that . For we calculate explicitly.
From (6) we have .
Let . From the assumptions we have . Using this and the assumptions that and is even we get the following expressions for the next terms.
[TABLE]
[TABLE]
Elementary manipulations of this expression, noticing that , , is even and that is odd, give
[TABLE]
Moving on to the next term, using again that and noticing that is even we get
[TABLE]
[TABLE]
At this point we observe that (since ). A similar circumstance occurs in the next two terms.
[TABLE]
[TABLE]
[TABLE]
and
[TABLE]
[TABLE]
Summing over we get that . ∎
It remains to prove Lemma 15.
Proof of Lemma 15.
For any let be the dyadic valuation of (see Notation 26). For such that we have that for all (see Lemma 27). Hence we may assume that
[TABLE]
In particular, since it follows that
[TABLE]
Let with . Collecting terms in (4) according to the powers of we see that
[TABLE]
where is the elementary symmetric polynomial of degree in the variables .
We now show that all the coefficients with vanish modulus . This is enough since is determined by modulus .
Case (i): . We use (8) and (9) to get .
Case (ii): . We may assume . Here (see proof of Lemma 27). Since we also have . So .
Case (iii): . Here a direct examination of the few possibilities, taking into account that , shows that . We use (8) and get . ∎
5 Proof of Theorem 2: The case of
The arguments in this section are similar to the ones in 4.
5.1 Recovering the lowest three bits of
Proposition 16**.**
If and then .
The proof is by ruling out the other possibilities one by one.
Lemma 17**.**
If and either or then .
Proof.
In these cases both and are odd. Repeating the proof of Lemma 9, rewriting formulas (4) and (5) modulus 2, we get
[TABLE]
For every we have that is even, since it has the even factor . So . ∎
Lemma 18**.**
If and then .
Proof.
Here is even and is odd. We calculate using formula (4).
[TABLE]
and
[TABLE]
From basic divisibility properties (Lemma 27) we also have
[TABLE]
Summing over we get . ∎
Lemma 19**.**
If and then .
Proof.
We denote and look at the terms of individually using formula (5). Using the assumption that is odd we get
[TABLE]
and by Lemma 28
[TABLE]
From basic divisibility properties (Lemma 27) we have for all . Summing over we get . ∎
To be complete we verify the remaining case for .
Proposition 20**.**
If and then .
Proof.
We let . By formula (5)
[TABLE]
and by Lemma 28
[TABLE]
From basic divisibility properties (Lemma 27) we have for all . Summing over we get . ∎
5.2 Recovering the high bits of
Theorem 21**.**
Let and suppose that . Then there exists a unique such that . Moreover .
Using Proposition 16, Theorem 21 is an immediate corollary of
Proposition 22**.**
Let and . Fix and write with . Then .
To prove Proposition 22 we first observe
Lemma 23**.**
Let , and . If then .
Proof.
The only difference from the proof of Lemma 15 is a division by an odd number which does not influence the calculations. ∎
Now we move on to the proof of the main proposition of this section.
Proof of Proposition 22.
By Lemma 23, for all we have that . For we calculate explicitly.
From (6) we have .
Denote , from the assumptions we get that . Using this and the assumption we get
[TABLE]
The next term is
[TABLE]
Elementary manipulations of this expression, noticing that , and that (since is odd), give
[TABLE]
Moving on to the next term, using again and we get
[TABLE]
[TABLE]
At this point we observe that (since ). A similar circumstance occurs in the next two terms.
By Lemma 28 so also . Hence,
[TABLE]
[TABLE]
[TABLE]
and
[TABLE]
[TABLE]
Summing over we get that . ∎
6 Proof of Theorem 2: The special cases
and
In these cases we trivially see that and we can easily check that . The general statement for even shows that these are the only solutions. Note that corresponds to the harmonic polynomials and .
7 Harmonic products of two harmonic polynomials
We prove Theorem 3, giving evidence to the validity of Conjecture 1.
Proof of Theorem 3.
We let and let . We assume that both and are harmonic. Harmonic functions are analytic, so they can be represented as infinite sums of homogeneous polynomials. If is harmonic and then every homogeneous component of , denoted , is also harmonic and has to give . So we can assume is a homogeneous harmonic polynomial of degree .
Let . The Laplacian of is
[TABLE]
Since the product is harmonic every coefficient of every monomial of the above expression has to vanish. If then . Combining this with we get . Hence can only be of the form . Since is harmonic,
[TABLE]
where is a polynomial in .
We assume so and we have .
A straightforward calculation gives that the only harmonic homogeneous polynomials of degree 3 such that the product is harmonic are linear combinations of and , so the harmonic functions such that is harmonic are of the form with . ∎
Proof of Theorem 4.
The proof is in the same spirit of the proof of Theorem 3, for details see [13]. ∎
8 The equivalence of Conjectures 1
and 1*′*
In this section we explain why Conjectures 1 and 1*′* are equivalent. We note that this equivalence was already observed by Armitage [2].
Let and . It is known from [7] that if and only if there exists an analytic function such that . In view of this, the equivalence of Conjectures 1 and 1*′* follows from the following theorem.
Theorem 24**.**
Let . The following statements are equivalent:
Let . There exists a harmonic polynomial of degree such that . 2. 2.
* such that .*
Proof.
Assume statement 2. Notice that . If let .
Conversely, assume is a harmonic polynomial of degree such that . Since is harmonic it can be written in spherical coordinates in the form with some . The polynomial vanishes on , where . Since and are each a linearly independent set of functions, we get that for some . ∎
9 Auxiliary Lemmas and Special Notation
Lemma 25**.**
For non-negative integers :
[TABLE]
Proof.
This becomes easy to check by writing and noting that . ∎
Proof of Lemma 7.
We use formula (1) and set such that .
[TABLE]
[TABLE]
[TABLE]
[TABLE]
[TABLE]
[TABLE]
[TABLE]
[TABLE]
Recalling relation (3), the normalization and Notation 6, we obtain the desired formulas. ∎
Notation 26**.**
The dyadic valuation.
For an integer , denote
[TABLE]
For a rational number denote
[TABLE]
Lemma 27**.**
**
Proof.
can also be written in the form
[TABLE]
so there are consecutive numbers in the nominator and no even numbers in the denominator. ∎
Lemma 28**.**
For and , .
Proof.
Here is even and is odd. The only factors with powers of two in this term are the following
[TABLE]
∎
The reference list from the paper itself. Each links out to its DOI / PubMed record.
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- 3[3] J. Bourgain and Z. Rudnick. On the nodal sets of toral eigenfunctions. Invent. Math. , 185(1):199–237, 2011.
- 4[4] R. Courant and D. Hilbert. Methods of mathematical physics. Vol. I . Interscience Publishers, Inc., New York, N.Y., 1953.
- 5[5] J. B. Holt. On the irreducibility of legendre’s polynomials. Proceedings of the London Mathematical Society , 2(1):126–132, 1913.
- 6[6] H. Ille. Zur Irreduzibilität der Kugelfunktionen . Ph D thesis, Universität Berlin, 1924.
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