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# Ramanujan’s mock theta functions

Edited* by George E. Andrews, Pennsylvania State University, University Park, PA, and approved February 28, 2013 (received for review January 8, 2013)

## Abstract

In his famous deathbed letter, Ramanujan introduced the notion of a *mock theta function*, and he offered some alleged examples. Recent work by Zwegers [Zwegers S (2001) *Contemp Math* 291:268–277 and Zwegers S (2002) PhD thesis (Univ of Utrecht, Utrecht, The Netherlands)] has elucidated the theory encompassing these examples. They are *holomorphic parts* of special harmonic weak Maass forms. Despite this understanding, little attention has been given to Ramanujan’s original definition. Here, we prove that Ramanujan’s examples do indeed satisfy his original definition.

## 1. Introduction and Statement of Results

Ramanujan’s deathbed letter (1) gave tantalizing hints of his theory of *mock theta functions*. Thanks to Zwegers (2, 3), it is now known that these functions are essentially the holomorphic parts of weight 1/2 *harmonic weak Maass forms*^{†} whose nonholomorphic parts are period integrals of weight 3/2 unary theta functions. This realization has many applications (e.g., refs. 5, 6).

Here, we revisit Ramanujan’s original definition from his deathbed letter (1, p 221). After a discussion of the asymptotics of certain modular forms, which are given as *Eulerian series*, he writes:…Suppose there is a function in the Eulerian form, and suppose that all or an infinity of points are exponential singularities[,] and also suppose that at these points the asymptotic form of the function closes as neatly as in the cases of (A) and (B). The question is: [Is] the function taken the sum of two functions[,] one of which is an ordinary theta function and the other a (trivial) function which is O(1) at all the points ? The answer is it is not necessarily so. When it is not so, I call the function Mock ϑ-function. I have not proved rigorously that it is not necessarily so. But I have constructed a number of examples in which it is inconceivable to construct a ϑ-function to cut out the singularities of the original function.

##### Remark:

By *ordinary theta function*, Ramanujan meant a *weakly holomorphic modular form* with weight on some Γ_{1}(*N*) (background is provided in ref. 7). Recall that a weakly holomorphic modular form is a meromorphic modular form whose poles (if any) are supported at cusps.

Little attention has been given to Ramanujan’s original definition, prompting Berndt^{‡} to remark that “it has not been proved that any of Ramanujan’s mock theta functions are really mock theta functions according to his definition.” The following fact fills in this gap.

### Theorem 1.1.

*Suppose that f(z) = f*^{−}(*z*) *+ f*^{+}(*z*) *is a harmonic weak Maass form of weight* *on* Γ_{1}(*N*)*, where f*^{−}(*z*) [*resp. f*^{+}(*z*)] *is the nonholomorphic* (*resp. holomorphic*) *part of f*(*z*). *If f*^{−}(*z*) *is nonzero and g*(*z*) *is a weight k weakly holomorphic modular form on any* Γ_{1}(*N*′), *then f*^{+}(*z*) − *g*(*z*) *has exponential singularities as q approaches infinitely many roots of unity ζ.*

##### Remark:

Harmonic weak Maass forms in this paper have principal parts at all cusps.

As a corollary, we obtain the following fitting conclusion to Ramanujan’s enigmatic question by proving that his alleged examples indeed satisfy his original definition (throughout, we let *q*: = *e*^{2πiz}). More precisely, we prove the following.

### Corollary 1.2.

*Suppose that M*(*z*) *is one of Ramanujan’s mock theta functions, and let γ and δ be integers for which q*^{γ} *M*(*δz*) *is the holomorphic part of a weight* 1/2 *harmonic weak Maass form. Then, there does not exist a weakly holomorphic modular form g*(*z*) *of any weight* *on any congruence subgroup* Γ_{1}(*N*′), *such that for every root of unity ζ, we have*

#### Remark:

The limits in *Corollary 1.2* are radial limits taken from within the unit disk. As his letter indicates (1), Ramanujan was inspired by the intimate relationship between the exponential singularities of modular forms at roots of unity and the asymptotics of their corresponding Fourier coefficients. As a toy model of his question, we begin by considering the following question, whose solution would have been clear to him: If *f*(*z*) is a weight *k*_{1} weakly holomorphic modular form that has some exponential singularities at cusps, then can there be another weakly holomorphic modular form of different weight *k*_{2}, say *g*(*z*), that exactly cuts out its singularities at roots of unity? The answer is *no*. If such a *g*(*z*) existed, then both *f*(*z*) and *g*(*z*) must have the same principal parts at all cusps, and at least one of these must be nonconstant. Without loss of generality, suppose that the principal part at the cusp infinity is nonconstant, and then consider the function *h*(*z*): = *f*(*z*) −*g*(*z*). By hypothesis, *h*(*z*) has bounded radial limits as *q* approaches every root of unity. Now, because *f*(*z*) and *g*(*z*) are modular on some common subgroup Γ_{1}(*N*′), if we take with , then we have

Letting , we find that and *g*(*z*) cannot cut out the same exponential singularities at roots of unity because of the difference between the weights.

In the case of Ramanujan’s examples, the situation is much more subtle, and this is the point of his last letter and this paper.

#### Example:

Although a weakly holomorphic modular form and a mock theta function cannot cut out each other’s singularities, Ramanujan discusses a *near miss*. He considers his mock theta function

and he compares it with a *q*-series , which is essentially a weight 1/2 weakly holomorphic modular form. He then conjectures, as *q* approaches an even order primitive root of unity *ζ*, that

Watson (8) confirmed this, and Folsom et al. (9) went further by deriving formulas for the numbers as explicit numbers in .

*Theorem 1.1* follows from recent developments in the theory of harmonic Maass forms; in particular, we make use of the extended Petersson scalar product of Bruinier and Funke (4). Their work implies that a harmonic weak Maass form that is not a weakly holomorphic modular form must have a nonconstant principal part at some cusp. To obtain the corollary, we use the theory of the Poincaré series and the method of quadratic twists to show first that a putative modular form must have weight 1/2. *Corollary 1.2* then follows by applying *Theorem 1.1*.

The paper is organized as follows. In section 2, we recall the basic facts about harmonic weak Maass forms and the pairing of Bruinier and Funke (4). In section 3, we describe the construction of the Poincaré series. In section 4, we conclude with the proof of *Theorem 1.1* and *Corollary 1.2*.

## 2. Harmonic Weak Maass Forms

Here, we recall some of the work of Bruinier and Funke (4) on harmonic weak Maass forms.

### 2.1. Definitions.

Throughout, we suppose that . The usual weight *k* hyperbolic Laplacian operator is given by

where For weights , we note that the level *N* of must be a multiple of 4. In this case, we define for odd *d* by

##### Definition 2.1:

A *harmonic weak Maass form* of weight *k* on a congruence subgroup is any smooth function satisfying:

For all ,

We have that .

There is a polynomial such that for some as . We require the analogous condition at all the cusps of .

We denote the space of weight *k* harmonic weak Maass forms on by .

##### Three Remarks:

The polynomials in

*Definition 2.1*(*3*) are the*principal parts*of at cusps.This space corresponds to in the notation of Bruinier and Funke (4).

Weakly holomorphic modular forms are harmonic weak Maass forms; however, in this paper, we will primarily be interested in Maass forms that are nonholomorphic.

### 2.2. Fourier Expansions.

Harmonic weak Maass forms have two components (4), a holomorphic piece and a nonholomorphic piece. If we let and we let , then every decomposes as , where

We refer to as the *holomorphic part* and as the *nonholomorphic part*.

### Fact 2.2.

*Suppose that* *is one of Ramanujan’s alleged examples of a mock theta function. Thanks to Zwegers* (2, 3), *there are integers γ and δ for which* *is the holomorphic part of a weight* 1/2 *harmonic weak Maass form* *on a congruence subgroup* . *Moreover, the nonholomorphic part of this form is the period integral of a weight* 3/2 *unary theta function. In particular, there are finitely many positive integers* *for which* *unless* *for some* *and some integer m*.

### 2.3. Bruinier–Funke Pairing.

Here, we recall the Bruinier and Funke pairing (4), defined using the operator , which induces a surjective map onto the space of weight *k* cusp forms on . The image is nonzero if and only if *f* has a nonzero nonholomorphic part. Bruinier and Funke (4) used to define a bilinear pairing by

where is the usual Petersson scalar product. Here, denotes the space of weight *k* holomorphic modular forms on . Proposition 3.5 of Bruinier and Funke (4) gives this pairing in terms of the coefficients of and . In particular, suppose that at a cusp *ρ*, has the expansion and has the expansion . They prove that

The first sum is over the components of a vector-valued form. In the work of Bruinier and Funke (4), all forms have level 1, and higher level forms may be viewed as level 1 vector-valued forms organized by cusps.

This pairing has the important property that when . However, because is a cusp form, [**2.4**] immediately gives the following.

### Theorem 2.3 (Bruinier–Funke Pairing).

*If* *has a nonzero nonholomorphic part*, *then* *must have a nonconstant principal part at some cusp*.

## 3. Poincaré Series

We require Maass–Poincaré series, which were considered previously in work of Niebur (10, 11). Their principal parts will serve as a basis for the principal parts of the mock theta functions. For and , we let , where is the usual *M*-Whittaker function, which satisfies

Because spaces of forms on are a direct sum over the spaces of Maass forms on with Nebentypus, it suffices to construct Poincaré series on with arbitrary Nebentypus *χ*. For a positive integer *m*, we define , and we define the Poincaré series on with Nebentypus *χ* and weight by

It turns out that is an eigenfunction of with eigenvalue . Therefore, is a weak Maass form of weight *k* on Γ with character *χ* whenever the series is absolutely convergent. This is clear if because because . To obtain a *harmonic* Maass form, we choose (or if ). Convergence for this choice of *s* for weight Poincaré series is only questionable if or . We are primarily interested in the case where .

The Fourier expansion of such series is well known (e.g., refs. 10, 12⇓⇓–15). We recall the *Kloosterman sum* of weight for with Nebentypus *χ*:

where *d* runs through primitive residue classes mod *c* and is the multiplicative inverse of *d* mod *c*. We then have the following.

### Proposition 3.1.

*If m is a positive integer, then the Poincaré series* *for* *with Nebentypus χ has the Fourier expansion*

*where the coefficients* *are given by*

In the proposition above, is the usual modified Bessel function and is the Bessel function of the first kind. If and equals or , then these Poincaré series converge and are harmonic weak Maass forms. For , it is known that the formulas still hold. For completeness, we shall give brief remarks below concerning the convergence.

Before we discuss the weight case, we stress that this proposition allows us to determine easily the asymptotics of the coefficients of holomorphic parts of harmonic weak Maass forms. This follows from the well known asymptotic

The Poincaré series constructed above have nonconstant principal parts only at the cusp infinity. We may similarly construct Poincaré series at any cusp *h*. We let denote the Poincaré series, which is defined by modifying [**3.1**] as

where is the stabilizer of *h*. As in the case of the cusp at infinity, we obtain a weak Maass form with order principal part at the cusp *h* and constant principal parts at all other cusps.

These facts allow us to conclude with the following crucial fact.

### Fact 3.2.

*Suppose that* *is a weight* 1/2 *harmonic weak Maass form with a nonconstant principal part at some cusp. Let* *be the weight* 1/2 *harmonic weak Maass form that is a linear combination of Maass–Poincaré series and that matches, up to constants, the principal parts of* *at all cusps. By Theorem 1.1, it follows that* *is a weight* 1/2 *holomorphic modular form, which, by the Serre–Stark Basis Theorem (e.g., ref*. 7), *implies that* *is a linear combination of weight 1/2 unary theta functions. Therefore, the subexponential growth of the I-Bessel function, combined with the periodicity of the Kloosterman sums in n, when m and c are fixed, then implies that a positive proportion of the coefficients of the holomorphic part of* *are nonzero. Indeed, this gives arithmetic progressions of coefficients with smooth asymptotic subexponential growth.*

##### Remark:

We briefly discuss the convergence in *Proposition 3.1* for weight 1/2 harmonic weak Maass forms. To show this, we need similar estimates for sums of the Kloosterman sums as in theorem 4.1 of the paper by Bringmann and Ono (14). In that work, the Kloosterman sums were rewritten as Salie-type sums, which were then estimated using the equidistibution of CM points [similar results may also be found in the paper by Duke (16)]. It is clear that the shape of the Salie-type sums do not depend on the multiplier system in a crucial way. Alternatively, the more general case, the results of Goldfeld and Sarnak (17), and the spectral theory of automorphic forms apply. By the asymptotics for Bessel functions, it suffices to consider the continuation of the Selberg–Kloosterman zeta function

Namely, for , we need to show convergence at . The convergence we require was shown for a special case in theorem 2.1 of the paper by Folsom and Ono (18). The general case follows *mutatis mutandis*.

### Theorem 3.3.

*If m is a positive integer, then* *is convergent at* .

## 4. Proof of Theorem 1.1 and Corollary 1.2

Here, we prove *Theorem 1.1* and *Corollary 1.2*.

### 4.1. Proof of Theorem 1.1.

Suppose that is a weakly holomorphic modular form on , for some , which cuts out the exponential singularities of as *q* approaches roots of unity. Then, is a harmonic weak Maass form of weight *k* on with a nonconstant nonholomorphic part. By *Theorem 2.3*, has a nonconstant principal part at some cusp. Because the nonholomorphic part exhibits exponential decay at cusps, it follows that is also as cusps. Suppose that has a nonconstant principal part at infinity (a similar argument applies at other cusps). By choosing matrices , combined with the fact that

we find that infinitely many roots of unity are exponential singularities for .

### 4.2. Proof of Corollary 1.2.

Suppose that is one of Ramanujan’s alleged examples of a mock theta function. Then, there are integers *γ* and *δ* for which is the holomorphic part of the weight 1/2 harmonic weak Maass form. Now suppose that is a weakly holomorphic modular form of some weight *k* that cuts out the exponential singularities of . Following the proof of theorem 1.4 of Bringmann and Ono (19), we can use *Fact 2.2*, *Fact 3.2*, and the theory of quadratic (and trivial) twists to obtain a weight 1/2 weakly holomorphic modular form . By *Fact 3.2*, this can be done so that is nontrivial and has nonconstant principal parts at some cusp. Applying the same procedure to gives a weakly holomorphic modular form . We then have that and cut out exactly the same exponential singularities at all roots of unity. By the discussion after *Corollary 1.2*, it then follows that . Therefore, if there is such a , then is a weight 1/2 harmonic weak Maass form that has a nonvanishing nonholomorphic part, which also has the property that has no exponential singularities at any roots of unity. This contradicts *Theorem 1.1*.

## Footnotes

- ↵
^{1}To whom correspondence may be addressed. E-mail: mjgrif3{at}emory.edu, ono{at}mathcs.emory.edu, or lrolen{at}emory.edu.

Author contributions: M.G., K.O., and L.R. designed research; M.G., K.O., and L.R. performed research; and M.G., K.O., and L.R. wrote the paper.

The authors declare no conflict of interest.

↵*This Direct Submission article had a prearranged editor.

↵

^{†}These forms were defined recently by Bruinier and Funke (4).↵

^{‡}Berndt BC. Ramanujan, his lost notebook, its importance.*Navigating Across Mathematical Cultures and Times*, eds Vandoulakis IM, Dun L.

## References

- ↵
- Berndt BC,
- Rankin RA

- ↵
- Zwegers S

*q*-series with applications to combinatorics, number theory, and physics. Contemp Math 291:268–277. - ↵
- Zwegers S

- ↵
- ↵
- Ono K

- ↵
- Zagier D

- ↵
- Ono K

- ↵
- Watson GN

- ↵Folsom A, Ono K, Rhoades RC (2013) Ramanujan's radial limits.
*Proceedings of the Ramanujan 125 Conference*, eds Alladi K, Garvan F, Yee AJ (Springer-Verlag, New York), in press. - ↵
- Niebur D

- ↵
- ↵
- Fay J

- ↵
- Bruinier J

- ↵
- ↵
- Bringmann K,
- Ono K

- ↵
- ↵
- ↵
- Folsom A,
- Ono K

- ↵
- Bringmann K,
- Ono K

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