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already know that 𝑝𝑄.𝑀 = π‘€βˆ’1𝑝𝑄. Let πœŽπ‘π‘„ ∈SL2(R) be a scaling matrix for 𝑝𝑄. Then π‘€βˆ’1πœŽπ‘π‘„ is a scaling matrix for π‘€βˆ’1𝑝𝑄 and thus

(οΈ‚0 0 0 πœ†π‘„.𝑀

)οΈ‚

= (𝑄.𝑀).πœŽπ‘„.𝑀 = (𝑄.𝑀).(π‘€βˆ’1πœŽπ‘π‘„) =

(οΈ‚0 0 0 πœ†π‘„

)οΈ‚

proving the claim.

Given 𝑄 ∈ 𝒬 with 𝑄(π‘₯, 𝑦) = π‘Žπ‘₯2 +𝑏π‘₯𝑦 +𝑐𝑦2 we also define the real-valued rational function 𝑝𝑄(𝜏)by

𝑝𝑄(𝜏) := π‘Ž|𝜏|2+𝑏𝑒+𝑐 (2.3.8) 𝑣

for 𝜏 =𝑒+𝑖𝑣 ∈H. It is easy to check that 𝑝𝑄(𝜏)2 := |𝑄(𝜏,1)|2

𝑣2 βˆ’Ξ”(𝑄).

(2.3.9)

In particular, we note that if Ξ”(𝑄) > 0 the geodesic 𝑐𝑄 is given as the zero set of the rational function 𝑝𝑄(𝜏) inH (without orientation).

all but finitely many 𝑛 < 0, for all𝑛 < 0 or for all 𝑛 ≀ 0, respectively. Moreover, if 𝑓 is meromorphic at 𝑝and 𝑓 ̸≑0 we define theorder of 𝑓 at the cusp𝑝 as

ord𝑝(𝑓) := min{𝑛 ∈Z:π‘Žπ‘“(𝑛;πœŽπ‘)ΜΈ= 0).

(2.4.2)

One can check that these definitions are indeed independent of the choice of representative 𝑝and the corresponding scaling matrixπœŽπ‘. However, the Fourier coefficientsπ‘Žπ‘“(𝑛;πœŽπ‘)∈C do depend on 𝑝and πœŽπ‘. If 𝑝=∞ we always choose πœŽπ‘ = 1 and simply write

π‘Žπ‘“(𝑛) :=π‘Žπ‘“(𝑛; 1) for the corresponding Fourier coefficients.

Letπ‘˜ be an integer. We call a function 𝑓: H β†’C weakly holomorphic modular form, modular form orcusp form of weight π‘˜ and level𝑁 if 𝑓 is holomorphic onH, modular of weightπ‘˜ and level 𝑁, and meromorphic, holomorphic or vanishing at all cusps ofΞ“0(𝑁), respectively. Correspondingly, we call 𝑓: H β†’ C a weakly meromorphic modular form, meromorphic modular form or meromorphic cusp form of weight π‘˜ and level 𝑁 if 𝑓 is modular of weightπ‘˜and level𝑁, and meromorphic, holomorphic or vanishing at all cusps of Ξ“0(𝑁), respectively, but only meromorphic on H.

We denote the complex vector spaces of weakly holomorphic modular form, modular forms or cusp forms of weight π‘˜ and level 𝑁 by π‘€π‘˜!(𝑁), π‘€π‘˜(𝑁) or π‘†π‘˜(𝑁), respectively.

Here the spaces π‘€π‘˜(𝑁) and π‘†π‘˜(𝑁) are finite-dimensional for everyπ‘˜ and 𝑁, and trivial if π‘˜ is negative or odd. Further, the only modular forms of weight 0 are the constant functions.

We will often write a weakly meromorphic modular form 𝑓 in terms of its Fourier expansion at the cusp ∞, i.e., as

𝑓(𝜏) = βˆ‘οΈ

π‘›β‰«βˆ’βˆž

π‘Žπ‘“(𝑛)𝑒(π‘›πœ).

Further, we recall that for π‘˜ β‰₯ 2 even the space of cusp forms π‘†π‘˜(𝑁) can be equipped with an inner product, the so-calledPetersson inner product, given by

(𝑓, 𝑔) :=

∫︁

π‘Œ0(𝑁)

𝑓(𝜏)𝑔(𝜏) Im(𝜏)π‘˜π‘‘πœ‡(𝜏) (2.4.3)

for𝑓, 𝑔 βˆˆπ‘†π‘˜(𝑁). Here the integral is well-defined since the integrand is modular of weight 0, and since 𝑓 and 𝑔 vanish at ∞ the integral converges.

2.4.1 Holomorphic Eisenstein series of weight π‘˜

The simplest example of a modular form is obtained by averaging the constant one-function over the group Ξ“0(𝑁) modulo the corresponding stabilizer, namely (Ξ“0(𝑁))∞, containing all elements of the form (οΈ€Β±1 𝑏

0 Β±1

)οΈ€ with π‘βˆˆZ. The following definition general-izes this idea to arbitrary cusps of Ξ“0(𝑁).

Definition 2.4.1. Let π‘˜ ∈ Z be even with π‘˜ β‰₯ 4 and let 𝑝 be a cusp of Ξ“0(𝑁). The Eisenstein series of weightπ‘˜ and level 𝑁 associated to the cusp 𝑝 is defined by

πΈπ‘˜,𝑝(𝜏) = βˆ‘οΈ

π‘€βˆˆ(Ξ“0(𝑁))π‘βˆ–Ξ“0(𝑁)

1

βƒ’

βƒ’

βƒ’π‘˜

πœŽπ‘βˆ’1𝑀

for 𝜏 ∈H. Here πœŽπ‘ ∈SL2(𝑅)is a parabolic scaling matrix associated to the cusp 𝑝.

The sum defining the series is absolutely and locally uniformly convergent for π‘˜ β‰₯ 4 even. Moreover, it is independent of the choice of scaling matrix since forπœŽπ‘, πœŽπ‘β€² ∈SL2(R) both satisfying (2.2.1) we have πœŽβˆ’1𝑝 πœŽπ‘β€² =(οΈ€Β±1 𝑏

0 Β±1

)οΈ€ for some π‘βˆˆR and thus 1βƒ’

βƒ’π‘˜πœŽβˆ’1𝑝 = (οΈ‚

1

βƒ’

βƒ’

βƒ’π‘˜

(οΈ‚Β±1 𝑏 0 Β±1

)οΈ‚)οΈ‚ βƒ’

βƒ’

βƒ’π‘˜πœŽπ‘β€²βˆ’1 = (Β±1)βˆ’π‘˜βƒ’

βƒ’π‘˜πœŽπ‘β€²βˆ’1 = 1βƒ’

βƒ’π‘˜πœŽβ€²βˆ’1𝑝 ,

as π‘˜ is even. Hence, the Eisenstein seriesπΈπ‘˜,𝑝 is a well-defined holomorphic function on H, which is by construction modular of weight π‘˜ and level 𝑁.

Proposition 2.4.2. Let π‘˜ ∈ Z be even with π‘˜ β‰₯ 4 and let 𝑝 be a cusp of Ξ“0(𝑁). The Eisenstein series πΈπ‘˜,𝑝 is a modular form of weight π‘˜ and level 𝑁, vanishing at all cusps but 𝑝.

We omit the corresponding proof and instead refer to Section 2.6 of [Miy06], where the above Proposition is given (in a more general setting) as Theorem 2.6.9.

Note that since𝑀, 𝑀′ βˆˆΞ“0(𝑁) have the same bottom row if and only if𝑀 π‘€β€²βˆ’1 is of the form (οΈ€1 𝑏

0 1

)οΈ€with 𝑏 ∈Z, the holomorphic Eisenstein seriesπΈπ‘˜,∞ can also be written as πΈπ‘˜,∞(𝜏) = 1 +βˆ‘οΈ

𝑐>0 𝑁|𝑐

βˆ‘οΈ

π‘‘βˆˆZ (𝑐,𝑑)=1

(π‘πœ +𝑑)βˆ’π‘˜ = 1 2𝜁(π‘˜)

βˆ‘οΈ

(𝑐,𝑑)∈Z2βˆ–{0}

(𝑁 π‘πœ +𝑑)βˆ’π‘˜. (2.4.4)

Here 𝜁(𝑠) = βˆ‘οΈ€βˆž

𝑛=1π‘›βˆ’π‘  is the usual Riemann zeta function. Thus, up to the constant factor 2𝜁(π‘˜)1 we can understandπΈπ‘˜,∞ as the sum of allβˆ’π‘˜β€™th powers of linear polynomials of the form𝑁 π‘πœ+𝑑. Therefore, it is natural to try to replace the sum of linear polynomials by quadratic ones.

2.4.2 Zagier’s cusp forms associated to discriminants

In his famous work [Zag75b] Zagier introduced modular forms defined as the sum of all

βˆ’π‘˜-th powers of quadratic forms of a given non-negative discriminantΞ”. For Ξ” = 0 this is essentially the holomorphic Eisenstein series of weight 2π‘˜ and level 1, and for positive discriminant theses forms appear as the Fourier coefficients of the holomorphic kernel function of the Shimura and Shintani lift between half-integral and integral weight cusp forms (see [KZ81] and [Koh85]).

Later on analogous functions have been defined and studied in the case of negative discriminants by Bengoechea (see [Ben13] and [Ben15]). These functions turn out to be meromorphic on the upper half-plane with poles at all Heegner points of the given (negative) discriminant.

28

Definition 2.4.3. Let π‘˜ ∈ Z with π‘˜ β‰₯ 2. Given 𝑄 ∈ 𝒬 with 𝑄 ̸≑ 0 we define the associated modular form as

π‘“π‘˜,𝑄(𝜏) = βˆ‘οΈ

π‘„β€²βˆˆ[𝑄]

𝑄′(𝜏,1)βˆ’π‘˜ for 𝜏 ∈Hβˆ–π»π‘„, where𝐻𝑄 is given as in (2.3.4).

One can check that for π‘˜ β‰₯ 2 the sum defining π‘“π‘˜,𝑄(𝜏) is absolutely and locally uni-formly convergent for 𝜏 ∈ Hβˆ–π»π‘„. Thus, π‘“π‘˜,𝑄 is a well-defined meromorphic function on H, which is holomorphic if Ξ”(𝑄) β‰₯ 0, and which is holomorphic up to poles at the Ξ“0(𝑁)-translates of the Heegner point πœπ‘„ if Ξ”(𝑄)<0. Moreover, since

(𝑄′.𝑀)(𝜏,1) =𝑗(𝑀, 𝜏)2𝑄′(𝑀 𝜏,1) (2.4.5)

for 𝑄′ ∈ 𝒬, 𝑀 ∈ Ξ“0(𝑁) and 𝜏 ∈ H the function π‘“π‘˜,𝑄 is modular of weight 2π‘˜ and level 𝑁. Furthermore, if π‘˜ β‰₯ 2 is odd and 𝑄 ∼ βˆ’π‘„ then all terms in the sum defining π‘“π‘˜,𝑄

cancel, giving π‘“π‘˜,𝑄 ≑0. We noted earlier that this can only happen if Ξ”(𝑄)>0.

Proposition 2.4.4. Let π‘˜ β‰₯2 and let 𝑄 ∈ 𝒬 with 𝑄 ̸≑0. The function π‘“π‘˜,𝑄 is a cusp form, modular form or meromorphic cusp form of weight 2π‘˜ and level 𝑁 if Ξ”(𝑄) > 0, Ξ”(𝑄) = 0 or Ξ”(𝑄)<0, respectively.

As for the holomorphic Eisenstein series we omit the proof of this proposition. Instead, we refer to the Appendix 2 in [Zag75b] forπ‘„βˆˆ 𝒬withΞ”(𝑄)β‰₯0, and to Proposition 2.1 and 2.2 in [Ben15] for the case of a negative discriminant. Though Zagier and Bengoechea only deal with the case 𝑁 = 1, the general case stated here follows analogously.

As mentioned earlier, for 𝑄 ∈ 𝒬 with 𝑄 ̸≑ 0 and Ξ”(𝑄) = 0 the function π‘“π‘˜,𝑄 is essentially the Eisenstein series of weight 2π‘˜ associated to the corresponding cusp 𝑝𝑄. More precisely, we have the following proposition:

Proposition 2.4.5. Let π‘˜ β‰₯ 2 and let 𝑄 ∈ 𝒬 with Ξ”(𝑄) = 0 and 𝑄 ̸≑ 0. Then up to a constant factor π‘“π‘˜,𝑄 equals the Eisenstein series of weight 2π‘˜ and level 𝑁 associated to the cusp 𝑝𝑄, i.e.,

π‘“π‘˜,𝑄(𝜏) = πœ†βˆ’π‘˜π‘„ 𝐸2π‘˜,𝑝𝑄(𝜏)

for 𝜏 ∈H. Here πœ†π‘„ is the factor given in part (b) of Lemma 2.3.3.

We omit the corresponding proof since this will be a special case of Proposition 2.5.6 evaluated at 𝑠= 0 for π‘˜ β‰₯2.

Instead of just summing over a single equivalence class of a given quadratic form we may also sum over all quadratic forms of a given class and discriminant, which is what Zagier originally did in [Zag75b]. These functions can be regarded as averaged versions of the meromorphic modular forms π‘“π‘˜,𝑄 defined above.

Definition 2.4.6. Let π‘˜ ∈ Z with π‘˜ β‰₯ 2. Given 𝛽 ∈ Z/2𝑁Z and Ξ” ∈ Z with Ξ” ≑ 𝛽2 mod4𝑁 we define the associated modular forms as

π‘“π‘˜,𝛽,Ξ”(𝜏) = βˆ‘οΈ

π‘„βˆˆπ’¬π›½,Ξ” 𝑄̸≑0

𝑄(𝜏,1)βˆ’π‘˜

for 𝜏 ∈Hβˆ–π»π›½,Ξ”, where 𝐻𝛽,Ξ” is given as in (2.3.2).

Again, the above sum converges absolutely and locally uniformly for π‘˜ β‰₯2, and thus defines a meromorphic function on H, which is holomorphic if Ξ” β‰₯ 0, and which is holomorphic up to poles at all Heegner points of class 𝛽 and discriminant Ξ” if Ξ” < 0.

Clearly, we can write

π‘“π‘˜,𝛽,Ξ”(𝜏) = βˆ‘οΈ

π‘„βˆˆπ’¬π›½,Ξ”/Ξ“0(𝑁) 𝑄̸≑0

π‘“π‘˜,𝑄(𝜏), (2.4.6)

where the sum on the right-hand side is finite if Ξ”ΜΈ= 0. Thus, Proposition 2.4.4 implies:

Corollary 2.4.7. Letπ‘˜ β‰₯2,𝛽 ∈Z/2𝑁ZandΞ”βˆˆZwithΔ≑𝛽2 mod 4𝑁. The function π‘“π‘˜,𝛽,Ξ”(𝜏) is a cusp form, modular form or meromorphic cusp form of weight 2π‘˜ and level 𝑁 if Ξ”>0, Ξ” = 0 or Ξ”<0, respectively.

We further note that, ifπ‘˜β‰₯2 is odd and 𝛽 ≑ βˆ’π›½ inZ/2𝑁Zthen 𝒬𝛽,Ξ”=βˆ’π’¬π›½,Ξ”, and thus the modular formπ‘“π‘˜,𝛽,Ξ”vanishes completely in this case. In contrast to the functions π‘“π‘˜,𝑄 defined before, whose defining sum could only cancel if Ξ”(𝑄) >0, the vanishing of the functions π‘“π‘˜,𝛽,Ξ” does not depend on sign of the discriminant Ξ”.

Moreover, ifΞ” = 0we can rewrite the sum in (2.4.6) as an (infinite) sum of holomorphic Eisenstein series using Proposition 2.4.5. Further assuming that 𝑁 is squarefree, there is only one modular form π‘“π‘˜,𝛽,0 of weight 2π‘˜ and discriminant 0, namely π‘“π‘˜,0,0, and this function takes the following nice form:

Corollary 2.4.8. Let 𝑁 be squarefree and let π‘˜β‰₯2. If π‘˜ is even then π‘“π‘˜,0,0(𝜏) = 2𝜁(π‘˜) βˆ‘οΈ

π‘βˆˆπΆ(Ξ“0(𝑁))

𝐸2π‘˜,𝑝(𝜏)

for 𝜏 ∈H, and if π‘˜ is odd the function π‘“π‘˜,0,0 vanishes identically, i.e, π‘“π‘˜,0,0 ≑0.

Proof. By Proposition 2.4.5 we have

π‘“π‘˜,0,0(𝜏) = βˆ‘οΈ

π‘„βˆˆπ’¬0,0/Ξ“0(𝑁) 𝑄̸≑0

πœ†βˆ’π‘˜π‘„ 𝐸2π‘˜,𝑝𝑄(𝜏).

Further, Lemma 2.3.4 states that the map [𝑄]↦→([𝑝𝑄], πœ†π‘„) is a bijection between classes of quadratic forms in(𝒬0,0βˆ– {0})/Ξ“0(𝑁) and tuples in𝐢(Ξ“0(𝑁))Γ—(Zβˆ– {0}), giving

π‘“π‘˜,0,0(𝜏) = (οΈƒ

βˆ‘οΈ

π‘›βˆˆZβˆ–{0}

π‘›βˆ’π‘˜ )οΈƒ(οΈƒ

βˆ‘οΈ

π‘βˆˆπΆ(Ξ“0(𝑁))

𝐸2π‘˜,𝑝(𝜏) )οΈƒ

.

Now if π‘˜ is even the first sum is simply twice the Riemann zeta function, and if π‘˜ is odd the sum cancels completely. This proves the claimed statement.