already know that ππ.π = πβ1ππ. Let πππ βSL2(R) be a scaling matrix for ππ. Then πβ1πππ is a scaling matrix for πβ1ππ and thus
(οΈ0 0 0 ππ.π
)οΈ
= (π.π).ππ.π = (π.π).(πβ1πππ) =
(οΈ0 0 0 ππ
)οΈ
proving the claim.
Given π β π¬ with π(π₯, π¦) = ππ₯2 +ππ₯π¦ +ππ¦2 we also define the real-valued rational function ππ(π)by
ππ(π) := π|π|2+ππ’+π (2.3.8) π£
for π =π’+ππ£ βH. It is easy to check that ππ(π)2 := |π(π,1)|2
π£2 βΞ(π).
(2.3.9)
In particular, we note that if Ξ(π) > 0 the geodesic ππ is given as the zero set of the rational function ππ(π) inH (without orientation).
all but finitely many π < 0, for allπ < 0 or for all π β€ 0, respectively. Moreover, if π is meromorphic at πand π ΜΈβ‘0 we define theorder of π at the cuspπ as
ordπ(π) := min{π βZ:ππ(π;ππ)ΜΈ= 0).
(2.4.2)
One can check that these definitions are indeed independent of the choice of representative πand the corresponding scaling matrixππ. However, the Fourier coefficientsππ(π;ππ)βC do depend on πand ππ. If π=β we always choose ππ = 1 and simply write
ππ(π) :=ππ(π; 1) for the corresponding Fourier coefficients.
Letπ be an integer. We call a function π: H βC weakly holomorphic modular form, modular form orcusp form of weight π and levelπ if π is holomorphic onH, modular of weightπ and level π, and meromorphic, holomorphic or vanishing at all cusps ofΞ0(π), respectively. Correspondingly, we call π: H β C a weakly meromorphic modular form, meromorphic modular form or meromorphic cusp form of weight π and level π if π is modular of weightπand levelπ, and meromorphic, holomorphic or vanishing at all cusps of Ξ0(π), 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 π by ππ!(π), ππ(π) or ππ(π), respectively.
Here the spaces ππ(π) and ππ(π) are finite-dimensional for everyπ and π, 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 π in terms of its Fourier expansion at the cusp β, i.e., as
π(π) = βοΈ
πβ«ββ
ππ(π)π(ππ).
Further, we recall that for π β₯ 2 even the space of cusp forms ππ(π) can be equipped with an inner product, the so-calledPetersson inner product, given by
(π, π) :=
β«οΈ
π0(π)
π(π)π(π) Im(π)πππ(π) (2.4.3)
forπ, π βππ(π). Here the integral is well-defined since the integrand is modular of weight 0, and since π and π vanish at β 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 Ξ0(π) modulo the corresponding stabilizer, namely (Ξ0(π))β, containing all elements of the form (οΈΒ±1 π
0 Β±1
)οΈ with πβZ. The following definition general-izes this idea to arbitrary cusps of Ξ0(π).
Definition 2.4.1. Let π β Z be even with π β₯ 4 and let π be a cusp of Ξ0(π). The Eisenstein series of weightπ and level π associated to the cusp π is defined by
πΈπ,π(π) = βοΈ
πβ(Ξ0(π))πβΞ0(π)
1
β
β
βπ
ππβ1π
for π βH. Here ππ βSL2(π )is a parabolic scaling matrix associated to the cusp π.
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 forππ, ππβ² βSL2(R) both satisfying (2.2.1) we have πβ1π ππβ² =(οΈΒ±1 π
0 Β±1
)οΈ for some πβR and thus 1β
βππβ1π = (οΈ
1
β
β
βπ
(οΈΒ±1 π 0 Β±1
)οΈ)οΈ β
β
βπππβ²β1 = (Β±1)βπβ
βπππβ²β1 = 1β
βππβ²β1π ,
as π is even. Hence, the Eisenstein seriesπΈπ,π is a well-defined holomorphic function on H, which is by construction modular of weight π and level π.
Proposition 2.4.2. Let π β Z be even with π β₯ 4 and let π be a cusp of Ξ0(π). The Eisenstein series πΈπ,π is a modular form of weight π and level π, vanishing at all cusps but π.
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 sinceπ, πβ² βΞ0(π) have the same bottom row if and only ifπ πβ²β1 is of the form (οΈ1 π
0 1
)οΈwith π βZ, the holomorphic Eisenstein seriesπΈπ,β can also be written as πΈπ,β(π) = 1 +βοΈ
π>0 π|π
βοΈ
πβZ (π,π)=1
(ππ +π)βπ = 1 2π(π)
βοΈ
(π,π)βZ2β{0}
(π ππ +π)βπ. (2.4.4)
Here π(π ) = βοΈβ
π=1πβπ is the usual Riemann zeta function. Thus, up to the constant factor 2π(π)1 we can understandπΈπ,β as the sum of allβπβth powers of linear polynomials of the formπ ππ+π. Therefore, it is natural to try to replace the sum of linear polynomials by quadratic ones.
2.4.2 Zagierβs cusp forms associated to discriminants
In his famous work [Zag75b] Zagier introduced modular forms defined as the sum of all
βπ-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 β Z with π β₯ 2. Given π β π¬ with π ΜΈβ‘ 0 we define the associated modular form as
ππ,π(π) = βοΈ
πβ²β[π]
πβ²(π,1)βπ for π βHβπ»π, whereπ»π is given as in (2.3.4).
One can check that for π β₯ 2 the sum defining ππ,π(π) is absolutely and locally uni-formly convergent for π β Hβπ»π. Thus, ππ,π is a well-defined meromorphic function on H, which is holomorphic if Ξ(π) β₯ 0, and which is holomorphic up to poles at the Ξ0(π)-translates of the Heegner point ππ if Ξ(π)<0. Moreover, since
(πβ².π)(π,1) =π(π, π)2πβ²(π π,1) (2.4.5)
for πβ² β π¬, π β Ξ0(π) and π β H the function ππ,π is modular of weight 2π and level π. Furthermore, if π β₯ 2 is odd and π βΌ βπ then all terms in the sum defining ππ,π
cancel, giving ππ,π β‘0. We noted earlier that this can only happen if Ξ(π)>0.
Proposition 2.4.4. Let π β₯2 and let π β π¬ with π ΜΈβ‘0. The function ππ,π is a cusp form, modular form or meromorphic cusp form of weight 2π and level π if Ξ(π) > 0, Ξ(π) = 0 or Ξ(π)<0, respectively.
As for the holomorphic Eisenstein series we omit the proof of this proposition. Instead, we refer to the Appendix 2 in [Zag75b] forπβ π¬withΞ(π)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 π = 1, the general case stated here follows analogously.
As mentioned earlier, for π β π¬ with π ΜΈβ‘ 0 and Ξ(π) = 0 the function ππ,π is essentially the Eisenstein series of weight 2π associated to the corresponding cusp ππ. More precisely, we have the following proposition:
Proposition 2.4.5. Let π β₯ 2 and let π β π¬ with Ξ(π) = 0 and π ΜΈβ‘ 0. Then up to a constant factor ππ,π equals the Eisenstein series of weight 2π and level π associated to the cusp ππ, i.e.,
ππ,π(π) = πβππ πΈ2π,ππ(π)
for π βH. Here ππ 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 π = 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 ππ,π defined above.
Definition 2.4.6. Let π β Z with π β₯ 2. Given π½ β Z/2πZ and Ξ β Z with Ξ β‘ π½2 mod4π we define the associated modular forms as
ππ,π½,Ξ(π) = βοΈ
πβπ¬π½,Ξ πΜΈβ‘0
π(π,1)βπ
for π βHβπ»π½,Ξ, where π»π½,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 π½ and discriminant Ξ if Ξ < 0.
Clearly, we can write
ππ,π½,Ξ(π) = βοΈ
πβπ¬π½,Ξ/Ξ0(π) πΜΈβ‘0
ππ,π(π), (2.4.6)
where the sum on the right-hand side is finite if ΞΜΈ= 0. Thus, Proposition 2.4.4 implies:
Corollary 2.4.7. Letπ β₯2,π½ βZ/2πZandΞβZwithΞβ‘π½2 mod 4π. The function ππ,π½,Ξ(π) is a cusp form, modular form or meromorphic cusp form of weight 2π and level π if Ξ>0, Ξ = 0 or Ξ<0, respectively.
We further note that, ifπβ₯2 is odd and π½ β‘ βπ½ inZ/2πZthen π¬π½,Ξ=βπ¬π½,Ξ, and thus the modular formππ,π½,Ξvanishes completely in this case. In contrast to the functions ππ,π defined before, whose defining sum could only cancel if Ξ(π) >0, the vanishing of the functions ππ,π½,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 π is squarefree, there is only one modular form ππ,π½,0 of weight 2π and discriminant 0, namely ππ,0,0, and this function takes the following nice form:
Corollary 2.4.8. Let π be squarefree and let πβ₯2. If π is even then ππ,0,0(π) = 2π(π) βοΈ
πβπΆ(Ξ0(π))
πΈ2π,π(π)
for π βH, and if π is odd the function ππ,0,0 vanishes identically, i.e, ππ,0,0 β‘0.
Proof. By Proposition 2.4.5 we have
ππ,0,0(π) = βοΈ
πβπ¬0,0/Ξ0(π) πΜΈβ‘0
πβππ πΈ2π,ππ(π).
Further, Lemma 2.3.4 states that the map [π]β¦β([ππ], ππ) is a bijection between classes of quadratic forms in(π¬0,0β {0})/Ξ0(π) and tuples inπΆ(Ξ0(π))Γ(Zβ {0}), giving
ππ,0,0(π) = (οΈ
βοΈ
πβZβ{0}
πβπ )οΈ(οΈ
βοΈ
πβπΆ(Ξ0(π))
πΈ2π,π(π) )οΈ
.
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.