## 1 Introduction

Congruences between modular forms have been found and studied for many years. Perhaps, the first interesting example is found in the work of Ramanujan. He studied in great detail the Fourier coefficients $$\tau (n)$$ of the discriminant function $$\Delta (z) = q\prod _{n=1}^{\infty }(1-q^n)^{24}$$ (where $$q = e^{2\pi i z}$$). The significance of $$\Delta$$ is that it is the unique normalized cusp form of weight 12.

Amongst Ramanujan’s mysterious observations was a pretty congruence:

\begin{aligned} \tau (n) \equiv \sigma _{11}(n) \bmod 691. \end{aligned}

Here $$\sigma _{11}(n) = \sum _{d\mid n}d^{11}$$ is a power divisor sum. Naturally, one wishes to explain the appearance of the modulus 691. The true incarnation of this is via the fact that the prime 691 divides the numerator of the “rational part” of $$\zeta (12)$$, i.e., $$\frac{\zeta (12)}{\pi ^{12}}\in \mathbb {Q}$$ (a quantity that appears in the Fourier coefficients of the Eisenstein series $$E_{12}$$).

Since the work of Ramanujan, there have been many generalizations of his congruences. Indeed, by looking for big enough primes dividing numerators of normalized zeta values, one can provide similar congruences at level 1 between cusp forms and Eisenstein series for other weights. In fact, one can even give “local origin” congruences between level p cusp forms and level 1 Eisenstein series by extending the divisibility criterion to include single Euler factors of $$\zeta (s)$$ rather than the global values of $$\zeta (s)$$ (see  for results and examples).

There are also Eisenstein congruences predicted for Hecke eigenvalues of genus 2 Siegel cusp forms. One particular type was conjectured to exist by Harder . There is only a small amount of evidence for this conjecture, and the literature only contains examples at levels 1 and 2 (using methods specific to these levels). The conjecture is also far from being proved. Only one specific level 1 example of the congruence has been proved [5, p. 386].

In this paper, we will see new evidence for a level p version of Harder’s conjecture for various small primes (including $$p=2$$ but not exclusively). The Siegel forms will be of paramodular type and the elliptic forms will be of $$\Gamma _0(p)$$ type. In doing this, we will make use of Jacquet–Langlands style conjectures due to Ibukiyama.

## 2 Harder’s conjecture

Given $$k\ge 0$$ and $$N\ge 1$$, let $$S_{k}(\Gamma _0(N))$$ denote the space of elliptic cusp forms for $$\Gamma _0(N)$$. Also for $$j\ge 0$$ let $$S_{j,k}(K(N))$$ denote the space of genus 2, vector-valued Siegel cusp forms for the paramodular group of level N, taking values in the representation space $$\text {Symm}^j(V) \otimes \text {det}^k(V)$$ of $$\text {GL}_2(\mathbb {C})$$ (where V is the standard representation).

Given $$f\in S_k(\Gamma _0(N))$$, we let $$\Lambda _{\text {alg}}(f,j+k) = \frac{\Lambda (f,j+k)}{\Omega }$$, where $$\Lambda (f,s)$$ is the completed L-function attached to f and $$\Omega$$ is a Deligne period attached to f. The choice of $$\Omega$$ is unique up to scaling by $$\mathbb {Q}_f^{\times }$$ but Harder shows how to construct a more canonical choice of $$\Omega$$ that is determined up to scaling by $$\mathcal {O}_{\mathbb {Q}_f}^{\times }$$ .

In this paper, we consider the following paramodular version of Harder’s conjecture (when $$N=1$$ this is the original conjecture found in ).

### Conjecture 2.1

Let $$j>0$$, $$k\ge 3$$ and let $$f\in S_{j+2k-2}^{\text {new}}(\Gamma _0(N))$$ be a normalized Hecke eigenform with eigenvalues $$a_n$$. Suppose that $$\text {ord}_\lambda (\Lambda _{alg}(f,j+k)) > 0$$ for some prime $$\lambda$$ of $$\mathbb {Q}_f$$ lying above a rational prime $$l > j+2k-2$$ (with $$l\not \mid N$$).

Then there exists a Hecke eigenform $$F\in S_{j,k}^{\text {new}}(K(N))$$ with eigenvalues $$b_n\in \mathbb {Q}_F$$ such that

\begin{aligned} b_q \equiv q^{k-2} + a_q + q^{j+k-1} \bmod \Lambda \end{aligned}

for all primes $$q\not \mid N$$ (where $$\Lambda$$ is some prime lying above $$\lambda$$ in the compositum $$\mathbb {Q}_f\mathbb {Q}_F$$).

It should be noted that Harder’s conjecture has still not been proved for level 1 forms. However, the specific example with $$j=4, k=10$$, and $$l=41$$ mentioned in Harder’s paper has recently been proved in a paper by Chenevier and Lannes . The proof uses the Niemeier classification of 24-dimensional lattices and is specific to this particular case.

Following the release of the level 1 conjecture, Faber and Van der Geer were able to do computations when $$\text {dim}(S_{j,k}(\text {Sp}_4(\mathbb {Z})))=1$$. They have now exhausted such spaces and in each case have verified the congruence for a significant number of Hecke eigenvalues. Ghitza, Ryan, and Sulon give extra evidence for the case $$j=2$$ . More recently, Cléry, Faber, and Van der Geer gave more examples for the cases $$j=4,6,8,10,12$$, and 14 .

For the level p conjecture, a substantial amount of evidence has been provided by Bergström et al for level 2 forms . Their methods are specific to this level. A small amount of evidence is known beyond level 2. In particular, a congruence has been found with $$(j,k,p,l) = (0,3,61,43)$$ by Mellit [16, p. 99].

In this paper, we use the theory of algebraic modular forms to provide evidence for the conjecture at levels $$p=2,3,5,7$$. The methods discussed can be extended to work for other levels.

## 3 Algebraic modular forms

In general, it is quite tough to compute Hecke eigensystems for paramodular forms. Fortunately, for a restricted set of levels, there is a (conjectural) Jacquet–Langlands style correspondence for $$\text {GSp}_4$$ due to Ihara and Ibukiyama .

Explicitly, it is expected that there is a Hecke equivariant isomorphism between the spaces $$S_{j,k}^{\text {new}}(K(p))$$ and certain spaces of algebraic modular forms. Bearing this in mind, we give the reader a brief overview of the general theory of such forms. For more details, see the introductory article of Loeffler in .

### 3.1 The spaces $$\mathcal {A}(G,K_f,V)$$ of algebraic forms

Let $$G/\mathbb {Q}$$ be a connected reductive group with the added condition that the Lie group $$G(\mathbb {R})$$ is connected and compact modulo center. Fix an open compact subgroup $$K_f \subset G(\mathbb {A}_f)$$. Also let V be (the space of) a finite dimensional algebraic representation of G, defined over a number field F.

### Definition 3.1

The F-vector space of algebraic modular forms of level $$K_f$$ and weight V for G is

\begin{aligned}&\mathcal {A}(G,K_f,V) \\&\quad \cong \{f: G(\mathbb {A}_f) \rightarrow V\,|\,f(\gamma g k) = \gamma f(g), \forall (\gamma ,g,k)\in G(\mathbb {Q})\times G(\mathbb {A})\times K_f\}. \end{aligned}

Fix a set of representatives $$T = \{z_1,z_2,\ldots ,z_h\}\in G(\mathbb {A}_f)$$ for $$G(\mathbb {Q})\backslash G(\mathbb {A}_f)/ K_f$$. There is a natural embedding:

\begin{aligned}&\phi : \mathcal {A}(G,K_f,V) \longrightarrow V^h\\&f \longmapsto (f(z_1),\ldots ,f(z_h)). \end{aligned}

### Theorem 3.2

The map $$\phi$$ induces an isomorphism:

\begin{aligned} \mathcal {A}(G,K_f,V) \cong \bigoplus _{m=1}^h V^{\Gamma _m}, \end{aligned}

where $$\Gamma _m = G(\mathbb {Q})\cap z_m K_f z_m^{-1}$$ for each m.

### Corollary 3.3

The spaces $$\mathcal {A}(G,K_f, V)$$ are finite dimensional.

A pleasing feature of the theory is that the groups $$\Gamma _m$$ are often finite. Gross gives many equivalent conditions for when this happens . One such condition is the following.

### Proposition 3.4

The groups $$\Gamma _m$$ are finite if and only if $$G(\mathbb {Z})$$ is finite.

### 3.2 Hecke operators

Let $$u\in G(\mathbb {A}_f)$$ and fix a decomposition $$K_f u K_f = \coprod _{i=1}^r u_i K_f$$. It is well known that finitely many representatives occur. Then $$T_u$$ acts on $$f\in \mathcal {A}(G,K_f,V)$$ via

\begin{aligned} T_u(f)(g):= \sum _{i=1}^r f(gu_i), \qquad \forall g\in G(\mathbb {A}_f). \end{aligned}

It is easy to see that this is independent of the choice of representatives $$u_i$$ since they are determined up to right multiplication by $$K_f$$.

We wish to find the Hecke representatives $$u_i$$ explicitly and efficiently. To this end, a useful observation can be made when the class number is one.

### Proposition 3.5

If $$h=1$$, then we may choose Hecke representatives that lie in $$G(\mathbb {Q})$$.

Finally, we note that for G satisfying Proposition 3.4 there is a natural inner product on the space $$\mathcal {A}(G,K,V)$$. This is given in Gross’ paper  but we shall give the rough details here.

### Lemma 3.6

Let G satisfy the property of Proposition 3.4 and V be a finite dimensional algebraic representation of G, defined over $$\mathbb {Q}$$. Then there exists a character $$\mu : G \rightarrow \mathbb {G}_m$$ and a positive definite symmetric bilinear form $$\langle ,\rangle : V\times V\rightarrow \mathbb {Q}$$ such that

\begin{aligned} \langle \gamma u, \gamma v\rangle = \mu (\gamma )\langle u,v\rangle \end{aligned}

for all $$\gamma \in G(\mathbb {Q})$$.

Taking adelic points, we have a character $$\mu ':G(\mathbb {A}) \rightarrow \mathbb {A}^{\times }$$. Let $$\mu _{\mathbb {A}} = f\circ \mu '$$, where $$f: \mathbb {A}^{\times } \rightarrow \mathbb {Q}^{\times }$$ is the natural projection map coming from the decomposition $$\mathbb {A}^{\times } = \mathbb {Q}^{\times }\mathbb {R}^+\hat{\mathbb {Z}}^{\times }$$.

### Proposition 3.7

Let G satisfy the property of Proposition 3.4. Then $$\mathcal {A}(G,K,V)$$ has a natural inner product given by

\begin{aligned} \langle f,g\rangle = \sum _{m=1}^h \frac{1}{|\Gamma _m|\mu _{\mathbb {A}}(z_m)}\langle f(z_m), g(z_m) \rangle . \end{aligned}

### 3.3 Trace of Hecke operators

The underlying representation V of G is typically big in dimension and so the action of Hecke operators is, although explicit, quite tough to compute. Fortunately, there is a simple trace formula for Hecke operators on spaces of algebraic modular forms. The details of the formula can be found in  but we give brief details here.

Note that $$G(\mathbb {A}_f)$$ acts on the set Z on the left by setting $$w\cdot z_i = z_j$$ if and only if $$G(\mathbb {Q})(wz_i)K_f = G(\mathbb {Q})z_jK_f$$. For each $$m=1,2,\ldots ,h$$, we consider the set $$S_m = \{i\,|\, u_i\cdot z_m = z_m\}$$. Next for each $$i\in S_m$$ choose elements $$k_{m,i}\in K_f$$ and $$\gamma _{m,i}\in G(\mathbb {Q})$$ such that $$\gamma _{m,i}^{-1} u_i z_m k_{m,i} = z_m$$.

Let $$\chi _V$$ denote the character of the representation of $$G(\mathbb {Q})$$ on V. Then the trace formula is as follows.

### Theorem 3.8

(Dummigan)

\begin{aligned} \text {tr}(T_u) = \sum _{m=1}^{h}\frac{1}{|\Gamma _m|}\sum _{\gamma \in \Gamma _m , i \in S_m} \chi _V(\gamma _{m,i}\gamma ). \end{aligned}

More generally,

\begin{aligned} \text {tr}(T_u^d) = \sum _{m=1}^{h}\frac{1}{|\Gamma _m|}\sum _{\gamma \in \Gamma _m, (i_n)\in S_m^d} \chi _V\left( \left( \prod _{n=1}^d \gamma _{m,i_n}\right) \gamma \right) . \end{aligned}

Letting $$u=\text {id}$$, we recover the following:

### Corollary 3.9

\begin{aligned} \text {dim}(\mathcal {A}(G,K_f,V)) = \sum _{m=1}^{h}\frac{1}{|\Gamma _m|}\sum _{\gamma \in \Gamma _m} \chi _V(\gamma ). \end{aligned}

When $$h=1$$, the situation becomes much simpler. In this case, we may choose $$z_1 = \text {id}$$ and $$\gamma _{1,i} = u_i\in G(\mathbb {Q})$$ for each i (this is possible by Corollary 3.5).

### Corollary 3.10

If $$h=1$$, then we have

\begin{aligned} \text {tr}(T_u) = \frac{1}{|\Gamma |}\sum _{\gamma \in \Gamma , 1\le i\le r}\chi _V(u_i \gamma ), \end{aligned}

where $$\Gamma = G(\mathbb {Q}) \cap K_f$$.

The trace formula was introduced to test a U(2, 2) analogue of Harder’s conjecture. In this paper, we will use it to test the level p paramodular version of Harder’s conjecture given by Conjecture 2.1.

## 4 Eichler and Ibukiyama correspondences

### 4.1 Eichler’s correspondence

From now on, D will denote a quaternion algebra over $$\mathbb {Q}$$ ramified at $$\{p,\infty \}$$ (for a fixed prime p) and $$\mathcal {O}$$ will be a fixed maximal order. Since D is definite, we have that $$D_{\infty }^{\times } = D^{\times }\otimes \mathbb {R} \cong \mathbb {H}^{\times }$$ is compact modulo center (and is also connected). Thus, we may consider algebraic modular forms for the group $$G = D^{\times }$$.

Also note that in this case each $$\Gamma _m$$ will be finite since $$D^{\times }(\mathbb {Z}) = \mathcal {O}^{\times }$$ is finite.

Let $$D_q:= D \otimes \mathbb {Q}_q$$ be the local component at prime q (no restriction on q) and let $$D_{\mathbb {A}_f}$$ be the restricted direct product of $$D_q$$’s with respect to the local maximal orders $$\mathcal {O}_q:= \mathcal {O} \otimes \mathbb {Z}_q$$.

Note that if $$q\ne p$$ then $$D_q^{\times } \cong (\text {M}_2(\mathbb {Q}_q))^{\times } = \text {GL}_2(\mathbb {Q}_q)$$. Thus, locally away from the ramified prime, $$D^{\times }$$ behaves like $$\text {GL}_2$$.

In fact more is true. It is the case that the reductive groups $$D^{\times }$$ and GL$$_2$$ are inner forms of each other. So by the principle of Langlands functoriality we expect a transfer of automorphic forms between $$D^{\times }$$ and GL$$_2$$. Eichler gives an explicit description of this transfer.

Let $$V_n = \text {Symm}^n(\mathbb {C}^2)$$ (for $$n\ge 0$$). Then $$V_n$$ gives a well-defined representation of $$\text {SU}(2)/\{\pm I\}$$ if and only if n is even. Thus, we get a well-defined action on $$V_n$$ by $$D^{\times }$$ through

\begin{aligned} D^{\times } \hookrightarrow \mathbb {H}^{\times } \longrightarrow \mathbb {H}^{\times }/\mathbb {R}^{\times } \cong \text {SU}(2)/\{\pm I\}. \end{aligned}

Take $$U = \prod _{q}\mathcal {O}_q^{\times }$$. This is an open compact subgroup of $$D_{\mathbb {A}_f}^{\times }$$.

### Theorem 4.1

(Eichler) Let $$k>2$$. Then there is a Hecke equivariant isomorphism:

\begin{aligned} S_{k}^{\text {new}}(\Gamma _0(p)) \cong \mathcal {A}(D^{\times },U, V_{k-2}). \end{aligned}

For $$k=2$$, the above holds if on the right we quotient out by the space of constant functions.

It remains to describe how the Hecke operators transfer over the isomorphism. Fix a prime $$q\ne p$$ and an isomorphism $$\psi : D_q^{\times } \cong \text {GL}_2(\mathbb {Q}_q)$$. Choose $$u \in D_{\mathbb {A}_f}^{\times }$$ such that $$\psi (u_q) = \text {diag}(1,q)$$ and is the identity at all other places. The corresponding Hecke operator corresponds to the classical $$T_q$$ operator under Eichler’s correspondence.

### 4.2 Ibukiyama’s correspondence

Ibukiyama’s correspondence is a (conjectural) generalization of Eichler’s correspondence to Siegel modular forms. The details can be found in  but we explain the main ideas.

Given the setup in the previous subsection, consider the unitary similitude group:

\begin{aligned} \mathrm {GU}_{n}(D) = \{g \in \text {M}_n(D)\,|\,g\bar{g}^{T} = \mu (g) I, \, \mu (g)\in \mathbb {Q}^{\times }\}. \end{aligned}

Here $$\bar{g}$$ means componentwise application of the standard involution of D. This group is the similitude group of the standard Hermitian form on $$D^n$$.

### Lemma 4.2

For any field K, there exists a similitude-preserving isomorphism $$\mathrm {GU}_2(\mathrm {M}_2(K)) \cong \mathrm {GSp}_4(K)$$.

### Proof

Conjugation by the matrix $$M = \text {diag}(1,A,1)\in \text {M}_4(K)$$, where $$A = \left( \begin{array}{cc} 0 &{} 1\\ 1 &{} 0\end{array}\right)$$ gives such an isomorphism. $$\square$$

One consequence of this is that the group GU$$_2(D)$$ behaves like GSp$$_4$$ locally away from the ramified prime. It is indeed true that these groups are also inner forms of each other.

A simple argument also shows that $$\text {GU}_2(\mathbb {H})/Z(\text {GU}_2(\mathbb {H})) \cong \text {USp}(4)/\{\pm I\}$$. Thus GU$$_2(D_{\infty })$$ is compact modulo center and connected. Thus, we may consider algebraic modular forms for this group. Once again, we are guaranteed that the $$\Gamma _m$$ groups are finite by the following.

### Lemma 4.3

$$\mathrm {GU}_2(\mathcal {O})= \{\gamma \in \mathrm {GU}_2(D)\cap \mathrm {M}_2(\mathcal {O})\,|\,\mu (\gamma )\in \mathbb {Z}^{\times }\}$$ is finite.

### Proof

Solving the equations gives

\begin{aligned} \text {GU}_2(\mathcal {O}) = \left\{ \left( \begin{array}{cc} \alpha &{} 0\\ 0 &{} \beta \end{array}\right) , \left( \begin{array}{cc} 0 &{} \alpha \\ \beta &{} 0\end{array}\right) \,\Bigg |\,\alpha ,\beta \in \mathcal {O}^{\times }\right\} . \end{aligned}

$$\square$$

One consequence of Lemma 4.2 is that GU$$_2(D_q) \cong \text {GSp}_4(\mathbb {Q}_q)$$for all $$q\ne p$$.

### Lemma 4.4

For any $$q\ne p$$, there exists a similitude-preserving isomorphism $$\psi : \mathrm {GU}_{2}(D_q) \rightarrow \mathrm {GSp}_4(\mathbb {Q}_q)$$ that preserves integrality:

\begin{aligned} \psi (\mathrm {GU}_2(D_q)\cap \mathrm {M}_2(\mathcal {O}_q)) = \mathrm {GSp}_4(\mathbb {Q}_q)\cap \mathrm {M}_4(\mathbb {Z}_q). \end{aligned}

### Proof

Choose an isomorphism of quaternion algebras $$D_q \cong \mathrm {M}_2(\mathbb {Q}_q)$$ that preserves the norm, trace, and integrality. This induces an isomorphism with the required properties since

\begin{aligned} \text {GU}_2(D_q) \cong \text {GU}_2(\mathrm {M}_2(\mathbb {Q}_q)) \cong \text {GSp}_4(\mathbb {Q}_q). \end{aligned}

$$\square$$

Let $$V_{j,k-3}$$ be the irreducible representation of USp(4) with Young diagram parameters $$(j+k-3,k-3)$$. This gives a well-defined representation of USp$$(4)/\{\pm I\}$$ if and only if j is even. Thus, GU$$_2(D)$$ acts on this through

\begin{aligned} \text {GU}_2(D) \hookrightarrow \text {GU}_2(\mathbb {H}) \longrightarrow \text {GU}_2(\mathbb {H})/Z(\text {GU}_2(\mathbb {H})) \cong \text {USp}(4)/\{\pm I\}. \end{aligned}

The groups $$\text {GU}(D)$$ and $$\text {GSp}_4$$ are inner forms. Thus (as with Eichler), one expects a transfer of automorphic forms. The following is found in Ibukiyama’s paper .

### Conjecture 4.5

(Ibukiyama) Let $$j\ge 0$$ be an even integer and $$k\ge 3$$. Suppose $$(j,k) \ne (0,3)$$. Then there is a Hecke equivariant isomorphism:

\begin{aligned}&S_{j,k}^{\text {new}}(\Gamma _0(p)) \longrightarrow \mathcal {A}^{\text {new}}(GU_2(D),U_1,V_{j,k-3})\\&S_{j,k}^{\text {new}}(K(p)) \longrightarrow \mathcal {A}^{\text {new}}(\text {GU}_2(D),U_2, V_{j,k-3}), \end{aligned}

where $$U_1, U_2, V_{j,k-3}$$ are to be defined.

If $$(j,k) = (0,3)$$, then we also get an isomorphism after taking the quotient by the constant functions on the right.

Since our eventual goal is to study Harder’s conjecture for paramodular forms, we will neglect the first of these isomorphisms. However, it will turn out that the open compact subgroup $$U_1$$ will prove useful in later calculations.

#### 4.2.1 The levels $$U_1$$ and $$U_2$$.

In Eichler’s correspondence, the “level 1” open compact subgroup $$U = \prod _q \mathcal {O}_q^{\times } \subset D_{\mathbb {A}_f}^{\times }$$ can be viewed as Stab$$_{D_{\mathbb {A}_f}^{\times }}(\mathcal {O})$$ under an action defined by right multiplication. Similarly, one can produce open compact subgroups Stab$$_{\text {GU}_2(D_{\mathbb {A}_f})}(L)\subseteq \text {GU}_2(D_{\mathbb {A}_f})$$, where L is a left $$\mathcal {O}$$-lattice of rank 2 in $$D^2$$ (a free left $$\mathcal {O}$$-module of rank 2).

A left $$\mathcal {O}$$-lattice $$L\subseteq D^2$$ gives rise to a left $$\mathcal {O}_q$$-lattice $$L_q = L\otimes \mathbb {Z}_q \subseteq D_q^2$$ for each prime q. A result of Shimura tells us the possibilities for $$L_q$$ (see ).

### Theorem 4.6

Let D be a quaternion algebra over $$\mathbb {Q}$$. If D is split at q, then $$L_q$$ is right $$\mathrm {GU}_2(D_q)$$ equivalent to $$\mathcal {O}_q^2$$. If D is ramified at q, then there are exactly two possibilities for $$L_q$$, up to right $$\mathrm {GU}_2(D_q)$$ equivalence (one being $$\mathcal {O}_q^2$$).

When D is ramified at $$\{p,\infty \}$$, it is clear from this result that there are only two possibilities for L, up to local equivalence.

### Definition 4.7

Let D be ramified at $$p,\infty$$ for some prime p:

• If $$L_p$$ is locally right equivalent to $$\mathcal {O}_p^2$$ for all q, then we say that L lies in the principal genus.

• If $$L_p$$ is locally right inequivalent to $$\mathcal {O}_p^2$$, then we say that L lies in the non-principal genus.

$$\square$$

Given L, results of Ibukiyama  allow us to write $$L = \mathcal {O}^2 g$$ for some $$g\in \mathrm {GL}_2(D)$$ and determine the genus of L based on g.

### Theorem 4.8

1. (1)

L lies in the principal genus if and only if $$g\overline{g}^T = mx$$ for some positive $$m\in \mathbb {Q}$$ and some $$x\in \mathrm {GL}_n(\mathcal {O})$$ such that $$x = \overline{x}^T$$ and such that x is positive definite, i.e., $$yx\overline{y}^T > 0$$ for all $$y\in D^n$$ with $$y\ne 0$$.

2. (2)

L lies in the non-principal genus if and only if $$g\overline{g}^T = m\left( \begin{array}{cc} ps &{} r\\ \overline{r} &{} pt\end{array}\right)$$, where $$m\in \mathbb {Q}$$ is positive, $$s,t\in \mathbb {N}, r\in \mathcal {O}$$ lies in the two-sided ideal of $$\mathcal {O}$$ above p and is such that $$p^2st - N(r) = p$$ (so that the matrix on the right has determinant p).

The lattice $$\mathcal {O}^2$$ is clearly in the principal genus and corresponds to the choice $$g=I$$. Alternatively, fix a choice of g such that $$\mathcal {O}^2 g$$ is in the non-principal genus. Let $$U_1,U_2$$ denote, respectively, the corresponding open compact subgroups of $$\text {GU}_2(D_{\mathbb {A}_f})$$ (as described above).

#### 4.2.2 Hecke operators

The transfer of Hecke operators in Ibukiyama’s correspondence is similar to the Eichler correspondence but there are subtle differences. Fix a prime $$q\ne p$$ and an isomorphism $$\psi$$ as in Lemma 4.4. Then we may find $$v_q\in \text {GU}_2(D_q)$$ such that $$\psi (v_q) = \text {diag}(1,1,q,q)$$.

Recall that D is split at q. By Theorem 4.6, there exists $$h_q\in \text {GU}_2(D_q)$$ such that $$\mathcal {O}^2g_q = \mathcal {O}^2h_q$$ (where $$g_q$$ is the image of g under the standard embedding $$\text {GU}_2(D)\hookrightarrow \text {GU}_2(D_q)$$). Fix such a choice.

Let $$u\in \text {GU}_2(D_{\mathbb {A}_f})$$ have $$u_q = h_q v_q h_q^{-1}$$ as the component at q and have identity component elsewhere.

### Definition 4.9

Given u as above, the corresponding Hecke operator on $$\mathcal {A}^{\text {new}}(\text {GU}_2(D),U_2, V_{j,k-3})$$ will be called $$T_{u,q}$$. $$\square$$

Under Ibukiyama’s correspondence, it is predicted that $$T_{u,q}$$ corresponds to the classical $$T_q$$ operator acting on $$S_{j,k}^{\text {new}}(K(p))$$).

#### 4.2.3 The new subspace

Our final task in defining Ibukiyama’s correspondence is to explain what is meant by the new subspace $$\mathcal {A}^{\text {new}}(\text {GU}_2(D),U_2,V_{j,k-3})$$. We will not go into too much detail but will refer the reader to Ibukiyama’s papers [21, 22].

Let $$G = D^{\times }\times \text {GU}_2(D)$$. Then we have an open compact subgroup $$U' = U\times U_2$$ and finite dimensional representations $$W_{j,k-3}:= V_{j}\otimes V_{j,k-3}$$ of $$G(\mathbb {A}_f)$$.

\begin{aligned} \mathcal {A}(G,U',W_{j,k-3}) \cong \mathcal {A}(D^{\times },U,V_j)\otimes \mathcal {A}(\text {GU}_2(D),U_2,V_{j,k-3}). \end{aligned}

Ibukiyama takes $$F\in \mathcal {A}(G,U',W_{j,k-3})$$. If F is an eigenform, then $$F = F_1\otimes F_2$$ for eigenforms $$F_1,F_2$$. He then associates an explicit theta series $$\theta _F$$ to F. This is an elliptic modular form for $$\mathrm {SL}_2(\mathbb {Z})$$ of weight $$j+2k-2$$ (if $$j+2k-6\ne 0$$, then it is a cusp form). It is known that $$\theta _F$$ is an eigenform for all Hecke operators if and only if $$\theta _F \ne 0$$.

### Definition 4.10

The subspace of old forms $$A_{j,k-3}^{\text {old}}(D) \subseteq A_{j,k-3}(D)$$ is generated by the eigenforms $$F_2$$ such that there exists an eigenform $$F_1$$ satisfying $$\theta _{F_1 \otimes F_2} \ne 0$$.

The subspace of new forms $$A_{j,k-3}^{\text {new}}(D)$$ is the orthogonal complement of the old space with respect to the inner product in Proposition 3.7. $$\square$$

It should be noted that by Eichler’s correspondence $$F_1$$ can be viewed as an elliptic modular form for $$\Gamma _0(p)$$ of weight $$j+2$$. Further it will be a new cusp form precisely when $$j>0$$. Thus, computationally it is not difficult to find the new and old subspaces.

## 5 Finding evidence for Harder’s conjecture

Now that we have linked spaces of Siegel modular forms $$S_{j,k}^{\text {new}}(K(p))$$ with spaces of algebraic modular forms $$A_{j,k-3}^{\text {new}}(D) = \mathcal {A}^{\text {new}}(\text {GU}_2(D),U_2, V_{j,k-3})$$, we can begin to generate evidence for Harder’s conjecture.

### 5.1 Brief plan of the strategy

In this paper, we deal with cases where $$h=1$$ and dim$$(A_{j,k-3}^{\text {new}}(D)) = 1$$.

Strategy

1. (1)

Find all primes p such that $$h=1$$.

2. (2)

For each such p calculate $$\Gamma ^{(2)} = \text {GU}_2(D)\cap U_2$$.

3. (3)

Using Corollary 3.9 find all jk such that $$\text {dim}(A_{j,k}^{\text {new}}(D))=1$$.

4. (4)

For each pair (jk) look in the space of elliptic forms $$S_{j+2k-2}^{\text {new}}(\Gamma _0(p))$$ for normalized eigenforms f which have a “large prime” dividing $$\Lambda _{\text {alg}}(f,j+k)\in \mathbb {Q}_f$$.

5. (5)

Find the Hecke representatives for the $$T_{u,q}$$ operator at a chosen prime q.

6. (6)

Use the trace formula to find tr$$(T_{u,q})$$ for $$T_q$$ acting on $$A_{j,k-3}(D)$$.

7. (7)

Subtract off the trace contribution of $$T_{u,q}$$ acting on $$A_{j,k-3}^{\text {old}}(D)$$ in order to get the trace of the action on $$A_{j,k-3}^{\text {new}}(D)$$. Since dim$$(A_{j,k-3}^{\text {new}}(D))=1$$, this trace should be exactly the Hecke eigenvalue of a new paramodular eigenform by Ibukiyama’s conjecture.

8. (8)

Check that Harder’s congruence holds.

The above strategy can be modified to work for the case $$\text {dim}(A_{j,k-3}^{\text {new}}(D)) = d > 1$$ but one must compute $$\text {tr}(T_{u,q}^t)$$ for $$1\le t \le d$$.

### 5.2 Finding $$\Gamma ^{(2)}$$

For $$\theta \in \mathbb {Q}^{\times }$$, consider the subset:

\begin{aligned} \text {GU}_{n}(D)_{\theta } = \{\gamma \in \text {GU}_2(D)\,|\,\mu (\gamma ) = \theta \}. \end{aligned}

In particular let SU$$_2(D):= \text {GU}_2(D)_1$$.

### Lemma 5.1

The group $$\Gamma ^{(2)}$$ consists of the following set of matrices:

\begin{aligned} \Gamma ^{(2)} =\mathrm {SU}_{2}(D)\cap g^{-1}\mathrm {GL}_2(\mathcal {O})g, \end{aligned}

where $$g\in \mathrm {GL}_2(D)$$ satisfies the condition in Theorem 4.8.

### Proof

We know that

\begin{aligned} \Gamma ^{(2)}&= \text {Stab}_{\text {GU}_2(D)}(\mathcal {O}^2 g) = \text {GU}_2(D) \cap \text {Stab}_{\text {GL}_2(D)}(\mathcal {O}^2 g)\\&= \text {GU}_2(D) \cap g^{-1}Sg = \text {GU}_{2}(D)\cap g^{-1}\text {GL}_2(\mathcal {O})g. \end{aligned}

A simple calculation shows that any such matrix has similitude 1. $$\square$$

Recall also the open compact subgroup $$U_1 = \text {Stab}_{\text {GU}_2(\mathbb {A}_f)}(\mathcal {O}^2) \subset \text {GU}_2(D_{\mathbb {A}_f})$$. This is the stabilizer of a left $$\mathcal {O}$$-lattice lying in the principal genus.

In this case, the analogue of the group $$\Gamma ^{(2)}$$ is the group $$\Gamma ^{(1)} = \text {GU}_2(D) \cap U_1$$. We can employ identical arguments to the above to show the following:

### Lemma 5.2

\begin{aligned} \Gamma ^{(1)} = \mathrm {SU}_2(D) \cap \mathrm {GL}_2(\mathcal {O}) = \mathrm {GU}_2(\mathcal {O}). \end{aligned}

We already have an explicit description of $$\Gamma ^{(1)}$$ (see Lemma 4.3). Computationally, it is not straightforward to find the elements of $$\Gamma ^{(2)}$$ due to the non-integrality of the entries of such matrices.

For $$\theta \in \mathbb {Q}^{\times }$$, consider the sets

\begin{aligned} Y_{\theta } = \text {GU}_{2}(D)_{\theta }\cap g^{-1} \mathrm {M}_2(\mathcal {O})^{\times }g \end{aligned}

and

\begin{aligned} W_{\theta } = \{\nu \in \mathrm {M}_2(\mathcal {O})^{\times }\,|\,\nu A \overline{\nu }^{T} = \theta A\}, \end{aligned}

where $$\mathrm {M}_2(\mathcal {O})^{\times } = \mathrm {GL}_2(D)\cap \mathrm {M}_2(\mathcal {O})$$ and $$A = g\bar{g}^T$$.

Then in particular $$Y_1 = \Gamma ^{(2)}$$. Later, the sets $$Y_q$$ for prime $$q\ne p$$ will appear when finding Hecke representatives.

### Proposition 5.3

For each $$\theta \in \mathbb {Q}^{\times }$$, conjugation by g gives a bijection

\begin{aligned} \Phi _{\theta }: Y_{\theta } \longrightarrow W_{\theta }. \end{aligned}

To calculate the sets $$W_{\theta }$$ we diagonalize A. Choose a matrix $$P\in \text {GL}_2(D)$$ such that $$PA\overline{P}^{T} = B$$, where $$B\in \mathrm {M}_2(D)$$ is a diagonal matrix.

### Proposition 5.4

For each $$\theta \in \mathbb {Q}^{\times }$$, conjugation by P gives a bijection:

\begin{aligned} W_{\theta } \longrightarrow Z_{\theta }:=\{\eta \in P\,\mathrm {M}_2(\mathcal {O})^{\times }\, P^{-1}\,|\,\eta B\overline{\eta }^{T} = \theta B\}. \end{aligned}

If we make an appropriate choice of g and P, then we can diagonalize A in such a way as to preserve one integral entry in $$P\nu P^{-1}$$.

### Lemma 5.5

Suppose we can choose $$\lambda ,\mu \in \mathcal {O}$$ such that $$N(\lambda )= p-1$$, $$N(\mu ) = p$$ and $$\text {tr}(r) = 0$$ (where $$r = \lambda \overline{\mu }$$). Then

\begin{aligned} g_{\lambda ,\mu }:= \left( \begin{array}{cc} 1 &{} \lambda \\ 0 &{} \mu \end{array}\right) \quad \text {and}\quad P_{\lambda ,\mu } = \left( \begin{array}{cc} 1 &{} \frac{\overline{r}}{p}\\ 0 &{} 1\end{array}\right) \end{aligned}

are valid choices for g and P.

Further $$P_{\lambda ,\mu }^{-1} = \overline{P_{\lambda ,\mu }}$$.

### Proof

A simple calculation shows that

\begin{aligned} A_{\lambda ,\mu } = \left( \begin{array}{cc} 1 &{} \lambda \\ 0 &{} \mu \end{array}\right) \left( \begin{array}{cc} 1 &{} 0\\ \overline{\lambda } &{} \overline{\mu }\end{array}\right) = \left( \begin{array}{cc} 1 + N(\lambda ) &{} \lambda \overline{\mu }\\ \mu \overline{\lambda } &{} N(\mu )\end{array}\right) = \left( \begin{array}{cc} p &{} r\\ \overline{r} &{} p\end{array}\right) , \end{aligned}

and also that det$$(A_{\lambda ,\mu }) = p^2 - N(r) = p^2 - p(p-1) = p$$ as required.

To prove the second claim, we note that $$r^2 = -p(p-1)$$ by the Cayley–Hamilton theorem (since $$\text {tr}(r) = 0$$ and $$N(r) = p(p-1)$$). Then

\begin{aligned} P_{\lambda ,\mu }A\overline{P_{\lambda ,\mu }}^T = \left( \begin{array}{cc} 1 &{} \frac{\overline{r}}{p}\\ 0 &{} 1\end{array}\right) \left( \begin{array}{cc} p &{} r\\ \overline{r} &{} p\end{array}\right) \left( \begin{array}{cc} 1 &{} 0\\ \frac{r}{p} &{} 1\end{array}\right) = \left( \begin{array}{cc} p + \frac{r^2}{p} + \frac{\overline{r}}{p}(\text {tr}(r)) &{} \text {tr}(r)\\ \text {tr}(r) &{} p\end{array}\right) \end{aligned}

and so $$P_{\lambda ,\mu }A\overline{P_{\lambda ,\mu }}^T =\text {diag}(1,p)$$.

The final claim follows from the fact that $$P_{\lambda ,\mu }\overline{P_{\lambda ,\mu }} = I$$ (which again uses the fact that $$\text {tr}(r) = 0$$). $$\square$$

It is in fact always possible to find some maximal order $$\mathcal {O}$$ of D where such $$\lambda ,\mu$$ exist. For proof of this I refer to an online discussion with John Voight , of which the author is grateful. We fix such a choice from now on.

### Corollary 5.6

Let $$\nu \in \mathrm {M}_2(\mathcal {O})$$. Then the bottom left entries of $$\nu$$ and $$P_{\lambda ,\mu }\nu \overline{P_{\lambda ,\mu }}$$ are equal (in particular this entry remains in $$\mathcal {O}$$).

### Proof

Let $$\nu = \left( \begin{array}{cc} \alpha &{} \beta \\ \gamma &{} \delta \end{array}\right)$$ with $$\alpha ,\beta ,\gamma ,\delta \in \mathcal {O}$$. Then a simple calculation shows that

\begin{aligned} P_{\lambda ,\mu }\nu \overline{P_{\lambda ,\mu }} = \left( \begin{array}{cc} \alpha + \frac{\overline{r}\gamma }{p} &{} (\frac{\alpha r}{p}+\beta ) + \frac{\overline{r}}{p}(\frac{\gamma r}{p} + \delta )\\ \gamma &{} \frac{\gamma r}{p} + \delta \end{array}\right) . \end{aligned}

$$\square$$

The matrix $$\eta = \left( \begin{array}{cc}x &{} y\\ z &{} w\end{array}\right) \in \mathrm {M}_2(D)$$ belongs to $$Z_{\theta }$$ if and only if

\begin{aligned} \eta \left( \begin{array}{cc} 1 &{} 0\\ 0 &{} p\end{array}\right) \overline{\eta }^T = \theta \left( \begin{array}{cc} 1 &{} 0\\ 0 &{} p\end{array}\right) . \end{aligned}

Equivalently,

\begin{aligned}&N(x) + pN(y) = \theta \\&N(z) + pN(w) = \theta p \\&x\overline{z} + py\overline{w} = 0. \end{aligned}

Clearly, these equations can have no solutions for $$\theta < 0$$ and so we only consider $$\theta \ge 0$$.

A quick calculation shows that $$N(x) = N(w)$$ and $$N(z) = p^2N(y)$$ (a fact we will use soon).

### Corollary 5.7

Let $$\theta \ge 0$$. Then $$W_{\theta }$$ consists of all matrices $$\nu = \left( \begin{array}{cc} \alpha &{} \beta \\ \gamma &{} \delta \end{array}\right) \in \mathrm {M}_2(\mathcal {O})^{\times }$$ such that

\begin{aligned}&pN(p\alpha + \overline{r}\gamma ) + N(p(\alpha r + p\beta ) + \overline{r}(\gamma r + p\delta )) = \theta p^3\\&pN(\gamma ) + N(\gamma r +p\delta ) = \theta p^2\\&p\alpha \overline{\gamma } + (\alpha r+p\beta )(\overline{\gamma r + p\delta }) = -\theta p \overline{r}. \end{aligned}

The following algorithm allows us to compute $$W_{\theta }$$ for $$\theta \in \mathbb {N}$$. Denote by $$X_i$$ the subset of $$\mathcal {O}$$ consisting of norm i elements.

Algorithm 1

Step 0: Set $$j:=0$$. For each integer $$0\le i\le \theta p$$, generate the norm lists $$X_i, X_{p(\theta p - i)}, X_{p^2 i}$$.

Step 1: Loop through all $$(\gamma ,\gamma ')\in X_j\times X_{p(\theta p-j)}$$ and test whether $$\delta := \frac{\gamma '-\gamma r}{p}\in \mathcal {O}$$. Whenever successful store the pair $$(\gamma ,\delta )$$.

Step 2: Loop through each pair from Step 1 and each $$\gamma ''\in X_{p(\theta p - j)}$$, testing whether $$\alpha := \frac{\gamma '' - \overline{r}\gamma }{p}\in \mathcal {O}$$. Whenever successful store the tuple $$(\alpha ,\gamma ,\delta )$$.

Step 3: Loop through each triple from Step 2 and each $$\gamma '''\in X_{p^2 j}$$, testing whether $$\beta := \frac{\gamma ''' - (\overline{r}(\gamma r + p\delta ) + p\alpha r)}{p^2}\in \mathcal {O}$$. Whenever successful store the tuple $$(\alpha ,\beta ,\gamma ,\delta )$$.

Step 4: For each tuple from Step 3, check whether the entries satisfy the third equation of Corollary 5.7.

Step 5: Set $$j:=j+1$$ and repeat steps 1–4 until $$j>\theta p$$.

Of course, once the elements of $$W_{\theta }$$ have been found, it is straightforward to generate the elements of $$Y_{\theta }$$ by inverting the bijection $$\Phi _{\theta }$$ in Proposition 5.3.

It should be noted that if we run this algorithm for $$p=2$$ with the following choices:

\begin{aligned} D&= \left( \frac{-1,-1}{\mathbb {Q}}\right) \\ \mathcal {O}&= \mathbb {Z}\oplus \mathbb {Z}i\oplus \mathbb {Z}j\oplus \mathbb {Z}\frac{1+i+j+k}{2}\\ \lambda&= -1\\ \mu&= i-k\\ \theta&= 1, \end{aligned}

then we get exactly the same elements for $$Y_1 = \Gamma ^{(2)}$$ as Ibukiyama does on [19, p. 592].

### 5.3 Finding h

We can use mass formulae to get information on class numbers $$h_1$$ and $$h_2$$ for $$U_1$$ and $$U_2$$.

Define the mass of open compact $$U\subset \text {GU}_2(D_{\mathbb {A}_f})$$ as follows:

\begin{aligned} M(U):= \sum _{m=1}^{h}\frac{1}{|\Gamma _m|}, \end{aligned}

where $$\Gamma _m = \text {GU}_2(D) \cap z_m U z_m^{-1}$$ for representatives $$z_1, z_2, \ldots , z_m\in \text {GU}_2(D_{\mathbb {A}_f})$$ of $$\text {GU}_2(D)\backslash \text {GU}_2(D_{\mathbb {A}_f})/ U$$.

Ibukiyama provides the following formulae for $$M(U_1)$$ and $$M(U_2)$$ in .

### Theorem 5.8

If D is ramified at p and $$\infty$$, then

\begin{aligned}&M(U_1) = \frac{(p-1)(p^2+1)}{5760},\\&M(U_2) = \frac{p^2 - 1}{5760}. \end{aligned}

This formula is analogous to the Eichler mass formula and is also a special case of the mass formula of Gan et al. .

### Proposition 5.9

$$h_1=1$$ if and only if $$|\Gamma ^{(1)}| = \frac{5760}{(p-1)(p^2+1)}$$. Similarly $$h_2=1$$ if and only if $$|\Gamma ^{(2)}| = \frac{5760}{p^2-1}$$.

### Corollary 5.10

$$h_1 = 1$$ if and only if $$p=2,3$$. Similarly $$h_2=1$$ if and only if $$p=2,3,5,7,11$$.

### Proof

A quick calculation shows that the only primes to satisfy $$\frac{5760}{(p-1)(p^2+1)}\in \mathbb {N}$$ are $$p=2,3$$. Recall $$|\Gamma ^{(1)}| = 2|\mathcal {O}^{\times }|^2$$. For $$p=2,3$$, we have $$|\mathcal {O}^{\times }| = 24, 12$$, respectively, and one checks that both values satisfy the equation.

The primes satisfying $$\frac{5760}{p^2-1}\in \mathbb {N}$$ are $$p=2,3,5,7,11,17,19,31$$. Using Algorithm 1, one finds that $$|\Gamma ^{(2)}| = \frac{5760}{p^2-1}$$ for the cases $$p=2,3,5,7,11$$. $$\square$$

Ibukiyama and Hashimoto have produced formulae in  and  that give the values of $$h_1$$ and $$h_2$$ for any ramified prime. Their formulae agree with this result.

### 5.4 Finding the Hecke representatives

Now that we have found an algorithm to generate the elements of $$\Gamma ^{(2)}$$, we consider the same question for the Hecke representatives for the $$T_{u,q}$$ operator on $$A_{j,k-3}(D)$$ (where $$q\ne p$$ is a fixed prime).

### Theorem 5.11

Let D be a quaternion algebra over $$\mathbb {Q}$$ ramified at $$p,\infty$$ for some $$p\in \{2,3,5,7,11\}$$. Suppose $$u\in \mathrm {GU}_2(D_{\mathbb {A}_f})$$ is chosen as in Definition 4.9. Then

\begin{aligned} U_2 u U_2 = \coprod _{[x_i]\in Y_q / \Gamma ^{(2)}} x_i U_2. \end{aligned}

### Proof

Consider an arbitrary decomposition:

\begin{aligned} U_2 u U_2 = \coprod x_i U_2. \end{aligned}

By Proposition 3.5, we may take $$x_i\in \text {GU}_2(D)$$ for each i. For the rest of the proof, we embed $$\text {GU}_2(D) \hookrightarrow \text {GU}_2(D_{\mathbb {A}_f})$$ diagonally.

Note that for any prime $$l\ne q$$ we have

\begin{aligned} U_{2,l} u_l U_{2,l} = U_{2,l} = \text {Stab}_{\text {GU}_2(D_l)}(\mathcal {O}_l^2 g_l) =\text {GU}_2(D_l) \cap g_l^{-1}\text {GL}_2(\mathcal {O}_l) g_l. \end{aligned}

Thus, $$x_i\in \text {GU}_2(D_l) \cap g_l^{-1} \mathrm {M}_2(\mathcal {O}_l)^{\times } g_l$$ and $$\mu (x_i) \in \mathbb {Z}_l^{\times }$$ for all i.

It remains to study the double coset locally at q. Note that $$h_q g_q^{-1}\in \text {GL}_2(\mathcal {O}_q)$$ so that $$h_q = k_q g_q$$ for some $$k_q\in \text {GL}_2(\mathcal {O}_q)\subseteq \mathrm {M}_2(\mathcal {O}_q)^{\times }$$.

Conjugation by $$h_q$$ gives a bijection between $$U_{2,q} u_q U_{2,q}$$ and $$G v_q G$$, where $$G = \text {GU}_2(D_q)\cap \text {GL}_2(\mathcal {O}_q)$$. If we fix an isomorphism as in Lemma 4.4, then this is in bijection with $$\text {GSp}_4(\mathbb {Z}_q) M_q \text {GSp}_4(\mathbb {Z}_q)$$ (where $$M_q = \text {diag}(1,1,q,q)$$).

Since by definition $$v_q \mapsto M_q\in \text {GSp}_4(\mathbb {Q}_q)\cap \mathrm {M}_4(\mathbb {Z}_q)$$, we see that $$v_q \in M_2(\mathcal {O}_q)^{\times }$$ and so $$u_q \in \text {GU}_2(D_q)\cap h_q^{-1} \mathrm {M}_2(\mathcal {O}_q)^{\times } h_q$$.

However,

\begin{aligned} h_q^{-1} \mathrm {M}_2(\mathcal {O}_q)^{\times } h_q = g_q^{-1} (k_q^{-1} \mathrm {M}_2(\mathcal {O}_q)^{\times } k_q) g_q = g_q^{-1} \mathrm {M}_2(\mathcal {O}_q)^{\times } g_q. \end{aligned}

Thus, $$u_q\in \text {GU}_2(D_q)\cap g_q^{-1} \mathrm {M}_2(\mathcal {O}_q)^{\times } g_q$$ and the same can be said about $$x_i$$.

Also since both the conjugation and our chosen isomorphism respect similitude, we find that $$\mu (u_q) = \mu (M_q) = q$$ and so $$\mu (U_{2,q} u_q U_{2,q})\subseteq q\mathbb {Z}_q^{\times }$$. In particular $$\mu (x_i) \in q\mathbb {Z}_q^{\times }$$.

Globally, we now see that

\begin{aligned} x_i \in \text {GU}_2(D)\cap \prod _l\left( \text {GU}_2(D_l)\cap g_l^{-1}\mathrm {M}_2(\mathcal {O}_l)^{\times }g_l\right) = \text {GU}_2(D) \cap g^{-1}\mathrm {M}_2(\mathcal {O})^{\times }g \end{aligned}

for each i. We also observe that $$\mu (x_i)\in \mathbb {Z}\cap \left( q\mathbb {Z}_q^{\times }\prod _{l\ne q}\mathbb {Z}_l^{\times }\right) = \{\pm q\}$$. However, in our case, the similitude is positive definite so that $$\mu (x_i) = q$$.

Thus, $$x_i$$ can be taken to lie in $$Y_q$$. It is clear that each such element lies in the double coset.

It remains to see which elements of $$Y_q$$ generate the same left coset. We have $$x_i U_2 = x_j U_2$$ if and only if $$x_j^{-1} x_i \in U_2$$. But also $$x_i, x_j\in \text {GU}_2(D)$$, hence $$x_j^{-1} x_i\in \text {GU}_2(D) \cap U_2 = \Gamma ^{(2)}$$. So equivalence of left cosets is up to right multiplication by $$\Gamma ^{(2)}$$. $$\square$$

We have a nice formula for the degree of $$T_{u,q}$$, found in the work of Ihara .

### Proposition 5.12

For $$q\ne p$$, we have that deg$$(T_{u,q}) = (q+1)(q^2+1)$$.

Employing similar arguments to Theorem 5.11, we get the following:

### Theorem 5.13

Let D be a quaternion algebra over $$\mathbb {Q}$$ ramified at $$p,\infty$$ for some $$p\in \{2,3\}$$. Suppose $$u\in \mathrm {GU}_2(D_{\mathbb {A}_f})$$ is chosen as in Definition 4.9. Then

\begin{aligned} U_1 u U_1 = \coprod _{[x_i]\in (\text {GU}_2(D)_q\cap \mathrm {M}_2(\mathcal {O})^{\times })/ \Gamma ^{(1)}} x_i U_1. \end{aligned}

Since $$\Gamma ^{(1)}$$ is given explicitly, it is possible to write down explicit representatives in this case.

### Corollary 5.14

Let $$n\in \mathbb {N}$$. For each $$k\in \mathbb {N}$$, let $$X_k = \{\alpha \in \mathcal {O}\,|\,N(\alpha ) = k\}$$, $$t_k = |X_k/\mathcal {O}^{\times }|$$, and $$x_{1,k}, x_{2,k}, \ldots , x_{t_k,k}$$ be a set of representatives for $$X_k/\mathcal {O}^{\times }$$. For such a choice of k, define

\begin{aligned} R_{k}:= \left\{ \left( \begin{array}{cc} x_{i,k} &{} v\\ w &{} x_{j,k}\end{array}\right) \,\Bigg |\,\begin{array}{c} 1\le i,j\le t_k,\quad v,w\in X_{n-k}\\ x_{i,k}\overline{w} + v\overline{x_{j,k}} = 0\end{array}\right\} . \end{aligned}

The following matrices are representatives for $$(\mathrm {GU}_2(D)_n\cap \mathrm {M}_2(\mathcal {O})^{\times })/ \Gamma ^{(1)}$$:

\begin{aligned}&\bigcup _{k=m+1}^n R_k, \quad {\mathrm{if}\quad n=2m+1 \quad \mathrm{is}\,\,\mathrm{odd}},\\&\left( \bigcup _{k=m+1}^n R_k\right) \cup R_{m}',\quad {\mathrm{if}\quad n=2m \quad \mathrm{is}\quad \mathrm{even}}. \end{aligned}

The finite subset $$R_{m}'\subset R_m$$ is to be constructed in the proof.

### Proof

Let $$\nu = \left( \begin{array}{cc} \alpha &{} \beta \\ \gamma &{} \delta \end{array}\right) \in \mathrm {M}_2(\mathcal {O})^{\times }$$. In order for $$\nu \in \text {GU}_2(D)_n$$ to hold, we must satisfy the equations:

\begin{aligned}&N(\alpha ) + N(\beta ) = n\\&N(\gamma ) + N(\delta ) = n\\&\alpha \overline{\gamma } + \beta \overline{\delta } = 0. \end{aligned}

In a similar vein to previous discussion, these equations imply that $$N(\alpha ) = N(\delta )$$ and $$N(\beta ) = N(\gamma )$$. Note that the first equation implies that $$0\le N(\alpha ) \le n$$.

We wish to study equivalence of these matrices under right multiplication by $$\Gamma ^{(1)}$$.

Case 1: $$N(\alpha ) \ne N(\beta )$$.

We may assume that $$N(\alpha ) > \frac{n}{2}$$ since for $$x,y\in \mathcal {O}^{\times }$$

\begin{aligned} \left( \begin{array}{cc} \alpha &{} \beta \\ \gamma &{} \delta \end{array}\right) \left( \begin{array}{cc} 0 &{} x\\ y &{} 0\end{array}\right) = \left( \begin{array}{cc} \beta y &{} \alpha x\\ \delta y &{} \gamma x\end{array}\right) \end{aligned}

and $$N(\beta y) = N(\beta ) = n - N(\alpha ) > n - \frac{n}{2} = \frac{n}{2}$$.

Under this assumption, there are no anti-diagonal equivalences so it remains to check for diagonal equivalences.

Now

\begin{aligned} \left( \begin{array}{cc} \alpha &{} \beta \\ \gamma &{} \delta \end{array}\right) \left( \begin{array}{cc} x &{} 0\\ 0 &{} y \end{array}\right) = \left( \begin{array}{cc} \alpha x &{} \beta y\\ \gamma x &{} \delta y \end{array}\right) . \end{aligned}

Letting $$k = N(\alpha )$$, choose $$x,y\in \mathcal {O}^{\times }$$ so that $$\alpha x = x_{i,k}$$ and $$\delta y = x_{j,k}$$ for some $$1\le i,j\le t_{k}$$. Then $$\nu$$ is equivalent to $$\left( \begin{array}{cc} x_{i,k} &{} v\\ w &{} x_{j,k}\end{array}\right)$$. Clearly the matrices of this form are inequivalent.

It is now clear that $$R_k$$ gives representatives for the particular subcase $$N(\alpha )=k > \frac{n}{2}$$.

Case 2: $$N(\alpha ) = N(\beta )=\frac{n}{2} = m$$.

The matrices $$\left( \begin{array}{cc} x_{i,m} &{} v\\ w &{} x_{j,m}\end{array}\right)$$ may now have extra anti-diagonal equivalences.

Suppose

\begin{aligned} \left( \begin{array}{cc} x_{i,m} &{} v\\ w &{} x_{j,m}\end{array}\right) \left( \begin{array}{cc} 0 &{} x\\ y &{} 0 \end{array}\right) = \left( \begin{array}{cc} x_{s,m} &{} v'\\ w' &{} x_{t,m}\end{array}\right) . \end{aligned}

Then xy are uniquely determined as follows:

\begin{aligned}&x = \frac{\overline{w}x_{t,m}}{m}\\&y =\frac{\overline{v}x_{s,m}}{m}. \end{aligned}

Thus, each such matrix $$\left( \begin{array}{cc} x_{i,m} &{} v\\ w &{} x_{j,m}\end{array}\right)$$ with $$v,w\in X_m$$ can only be equivalent to at most one other matrix:

\begin{aligned} \left( \begin{array}{cc} x_{s,m} &{} \frac{x_{i,m}\overline{w}x_{t,m}}{m}\\ \frac{x_{j,m}\overline{v}x_{s,m}}{m} &{} x_{t,m} \end{array}\right) , \end{aligned}

where $$v\sim x_{s,m}$$ and $$w\sim x_{t,m}$$ under the action of right unit multiplication.

Let $$R_{m}'$$ be a set consisting of a choice of matrix from each of these equivalence pairs (as $$x_{i,m}$$ and $$x_{j,m}$$ run through representatives for $$X_m/\mathcal {O}^{\times }$$ and vw run through elements of $$X_m$$ satisfying $$x_{i,m}\overline{w} + v\overline{x}_{j,m}=0$$). Then it is now clear that $$R_{m}'$$ is a set of representatives for this subcase. $$\square$$

In the subcase $$k=n-1$$, it is often easier to use anti-diagonal equivalence (since $$X_1/\mathcal {O}^{\times } = \{1\}$$). In this case, we can identify

\begin{aligned} R_{n-1} \longleftrightarrow \left\{ \left( \begin{array}{cc} 1 &{} z\\ -\overline{z} &{} 1\end{array}\right) \, | \,z\in X_{n-1}\right\} . \end{aligned}

When $$n=2$$ exactly half of these will form a set of representatives. In fact, it is simple to see that the equivalent pairs would be

\begin{aligned} \left( \begin{array}{cc} 1 &{} z\\ -\overline{z}&{} 1\end{array}\right) \sim \left( \begin{array}{cc} 1 &{} -z\\ \overline{z} &{} 1 \end{array}\right) . \end{aligned}

Thus

\begin{aligned} R_{1}' = \left\{ \left( \begin{array}{cc} 1 &{} z_i\\ -\overline{z_i} &{} 1 \end{array}\right) \, | \,[z_i]\in \mathcal {O}^{\times }/\{\pm 1\}\right\} . \end{aligned}

### Example 5.15

If we apply Corollary 5.14 to the choices

\begin{aligned}&D = \left( \frac{-1,-1}{\mathbb {Q}}\right) ,\\&\mathcal {O} = \mathbb {Z}\oplus \mathbb {Z}i\oplus \mathbb {Z}j\oplus \mathbb {Z}\frac{1+i+j+k}{2},\\&n=3,\\&X_3/\mathcal {O}^{\times } = \{[1\pm i\pm j],\}, \end{aligned}

we find that Hecke representatives for $$U_1$$ with ramified prime $$p=2$$ and $$q=3$$ are given by

\begin{aligned}&\left( \begin{array}{cc} x &{} 0\\ 0 &{} y\end{array}\right) , \qquad x,y\in \{1\pm i \pm j\},\\&\left( \begin{array}{cc} 1 &{} z \\ -\overline{z} &{} 1 \end{array}\right) , \qquad z\in \mathcal {O}, N(z)=2. \end{aligned}

There are 40 representatives here as expected and they agree with the explicit representatives given by Ibukiyama on [19, p. 594]. $$\square$$

So far we have not needed the open compact subgroup $$U_1$$, but it is actually of use to us in studying $$U_2$$.

### Lemma 5.16

Let $$u\in \mathrm {GU}_2(D_{\mathbb {A}_f})$$ be chosen to form the $$T_{u,q}$$ operator with respect to both $$U_1$$ and $$U_2$$ (for prime $$q\ne p$$). Then the Hecke representatives for $$T_{u,q}$$ with respect to $$U_1$$ and $$U_2$$ can be taken to be the same.

### Proof

Recall that u has identity component away from q and $$u_q\notin U_{2,q}$$ so we need only to check the local condition that $$U_{2,q} = U_{1,q}$$.

This is clear since

\begin{aligned} U_{2,q} = \text {Stab}_{\text {GU}_2(D_q)}(\mathcal {O}_q^2 g_q) = \text {Stab}_{\text {GU}_2(D_q)}(\mathcal {O}_q^2 h_q) = \text {Stab}_{\text {GU}_2(D_q)}(\mathcal {O}_q^2) = U_{1,q}. \end{aligned}

$$\square$$

This result is useful since we have seen that it is generally easier to generate Hecke representatives for $$T_{u,q}$$ with respect to $$U_1$$.

### Corollary 5.17

Let the ramified prime of D be $$p\in \{2,3\}$$. Then we may use the representatives from Corollary 5.14 as Hecke representatives for $$T_{u,q}$$ with respect to $$U_2$$ (for $$q \ne p$$).

### Proof

Since $$p\in \{2,3\}$$, we know that both the class numbers of $$U_1,U_2$$ are 1. Hence both admit rational Hecke representatives.

We also know that given Hecke representatives for $$T_{u,q}$$ with respect to $$U_1$$ we may use them for $$U_2$$. Thus, the rational representatives from Corollary 5.14 can be used for $$U_2$$. $$\square$$

### 5.5 Implementing the trace formula

Now that we have algorithms that generate the data needed to use the trace formula, we discuss some of the finer details in its implementation, namely how to find character values. Denote by $$\chi _{j,k-3}$$ the character of the representation $$V_{j,k-3}$$.

Given $$g = \left( \begin{array}{cc} \alpha &{} \beta \\ \gamma &{} \delta \end{array}\right) \in \text {GU}_2(D)$$, we may produce a matrix $$A\in \text {GSp}_4(\mathbb {C})$$ via the embedding

\begin{aligned} g \longmapsto \left( \begin{array}{cccc} \alpha _1 + \alpha _2 \sqrt{a} &{} \beta _1 + \beta _2\sqrt{a} &{} \alpha _3 + \alpha _4\sqrt{a} &{} \beta _3 + \beta _4\sqrt{a}\\ \gamma _1 + \gamma _2\sqrt{a} &{} \delta _1 + \delta _2\sqrt{a} &{} \gamma _3 + \gamma _4\sqrt{a} &{} \delta _3 + \delta _4\sqrt{a}\\ b(\alpha _3 - \alpha _4\sqrt{a}) &{} b(\beta _3 - \beta _4\sqrt{a}) &{} \alpha _1 - \alpha _2\sqrt{a} &{} \beta _1 - \beta _2\sqrt{a}\\ b(\gamma _3 - \gamma _4\sqrt{a}) &{} b(\delta _3 - \delta _4\sqrt{a}) &{} \gamma _1 - \gamma _2\sqrt{a} &{} \delta _1 - \delta _2\sqrt{a}\end{array}\right) , \end{aligned}

where $$a = i^2$$ and $$b=j^2$$ in D.

This embedding is the composition of the standard embedding $$D^{\times }\hookrightarrow \mathrm {M}_2(K(\sqrt{a}))$$ and the isomorphism $$\text {GU}_2(\mathrm {M}_2(K(\sqrt{a}))) \cong \text {GSp}_4(K(\sqrt{a})) \subseteq \text {GSp}_4(\mathbb {C})$$ given in Lemma 4.2.

We know that the image of $$\text {GU}_2(\mathbb {H})_1\cap \text {GU}_2(D)$$ under this embedding is a subgroup of $$\text {USp}(4)$$, so that the matrix $$B = \frac{A}{\sqrt{\mu (A)}}\in \text {USp}(4)$$. By writing $$A = (\sqrt{\mu (A)}I)B$$, it follows that

\begin{aligned} \chi _{j,k-3}(g) = \chi _{j,k-3}(A) = \mu (A)^{\frac{j+2k-6}{2}}\chi _{j,k-3}(B). \end{aligned}

In order to find $$\chi _{j,k-3}(B)$$, we first find the eigenvalues of B. This is equivalent to conjugating into the maximal torus of diagonal matrices. Since $$B\in \text {USp}(4)$$, these eigenvalues will come in two complex conjugate pairs $$z,\overline{z}, w, \overline{w}$$ for zw on the unit circle.

The Weyl character formula gives

\begin{aligned} \chi _{j,k-3}(B) = \frac{w^{j+1}(w^{2(k-2)}-1)(z^{2(j+k-1)}-1) - z^{j+1}(z^{2(k-2)}-1)(w^{2(j+k-1)}-1)}{(z^2-1)(w^2-1)(zw-1)(z-w)(zw)^{j+k-3}}. \end{aligned}

For any of the cases $$z^2=1, w^2=1, zw=1, z=w$$, one must formally expand this concise formula into a polynomial expression (not an infinite sum since each factor on the denominator except zw divides the numerator). It is easy for a computer package to compute this expansion for a given jk.

### 5.6 Finding the trace contribution for the new subspace

Let $$\text {tr}(T_{u,q})^{\text {new}}$$ and $$\text {tr}(T_{u,q})^{\text {old}}$$ be the traces of the action of $$T_{u,q}$$ on $$A_{j,k-3}^{\text {new}}(D)$$ and $$A_{j,k-3}^{\text {old}}(D)$$, respectively. Then $$\text {tr}(T_{u,q})^{\text {new}} = \text {tr}(T_{u,q}) - \text {tr}(T_{u,q})^{\text {old}}$$.

Recall that each eigenform in $$\mathcal {A}_{j,k-3}^{\text {old}}(D)$$ is given by a special pair of eigenforms $$F_1\in \mathcal {A}(D^{\times },U,V_j)$$ and $$F_2\in \mathcal {A}(\text {GU}_2(D),U_2,V_{j,k-3})$$. If $$j>0$$, then $$F_1$$ corresponds to a unique eigenform in $$S_{j+2}^{\text {new}}(\Gamma _0(p))$$ by Eichler’s correspondence. Attached to the pair $$(F_1,F_2)$$ is an eigenform $$\theta _{F_1\otimes F_2} \ne 0$$ in $$M_{j+2k-2}(\text {SL}_2(\mathbb {Z}))$$ (it is a cusp form if $$j+2k-6 \ne 0$$).

Let $$\alpha _n, \beta _n, \gamma _n$$ be the Hecke eigenvalues of $$F_1,F_2, \theta _{F_1\otimes F_2}$$, respectively. Ibukiyama links the eigensystems as follows.

### Theorem 5.18

For $$q\ne p$$, we have the following identity in $$\mathbb {C}(t)$$:

\begin{aligned} \sum _{k=0}^{\infty } \beta _{q^k}t^k = \frac{1 - q^{j+2k-4}t^2}{(1 - \alpha _q q^{k-2} t + q^{j+2k-3}t^2)(1 - \gamma _q t + q^{j+2k-3}t^2)}. \end{aligned}

### Corollary 5.19

For $$q\ne p$$, we have $$\beta _q = \gamma _q + q^{k-2}\alpha _q$$.

Ibukiyama conjectures that there is a bijection between pairs of eigenforms $$(F_1, \theta _F)$$ and eigenforms $$F_2$$. With this in mind, it is now possible to calculate the oldform trace contribution.

### Corollary 5.20

Suppose $$j+2k-6 \ne 0$$. Let $$g_1, g_2, \ldots , g_m\in S_{j+2k-2}(\mathrm {SL}_2(\mathbb {Z}))$$ and $$h_1, h_2, \ldots , h_n\in S_{j+2}^{\text {new}}(\Gamma _0(p))$$ be the bases of normalized eigenforms with Hecke eigenvalues $$a_{q,g_i}$$ and $$a_{q,h_i}$$, respectively.

Then, for $$q\ne p$$ and $$j>0$$,

\begin{aligned} \text {tr}(T_{u,q})^{\text {old}} = n\left( \sum _{i=1}^m a_{q,g_i}\right) + mq^{k-2}\left( \sum _{i=1}^n a_{q,h_i}\right) . \end{aligned}

## 6 Examples and summary

The following table highlights the choices for $$D, \mathcal {O}, \lambda , \mu$$ that were used.

 p D $$\mathcal {O}$$ $$\lambda$$ $$\mu$$ 2 $$\left( \frac{-1,-1}{\mathbb {Q}}\right)$$ $$\mathbb {Z}\oplus \mathbb {Z} i\oplus \mathbb {Z} j\oplus \mathbb {Z}\left( \frac{1+i+j+k}{2}\right)$$ 1 $$i-k$$ 3 $$\left( \frac{-1,-3}{\mathbb {Q}}\right)$$ $$\mathbb {Z}\oplus \mathbb {Z} i\oplus \mathbb {Z} \left( \frac{1+j}{2}\right) \oplus \mathbb {Z}\left( \frac{i+k}{2}\right)$$ $$1+i$$ j 5 $$\left( \frac{-2,-5}{\mathbb {Q}}\right)$$ $$\mathbb {Z}\oplus \mathbb {Z}\left( \frac{2-i+k}{4}\right) \oplus \mathbb {Z}\left( \frac{2+3i+k}{4}\right) \oplus \mathbb {Z}\left( \frac{-1+i+j}{2}\right)$$ 2 j 7 $$\left( \frac{-1,-7}{\mathbb {Q}}\right)$$ $$\mathbb {Z}\oplus \mathbb {Z} i\oplus \mathbb {Z} \left( \frac{1+j}{2}\right) \oplus \mathbb {Z}\left( \frac{i+k}{2}\right)$$ $$2+\frac{1}{2}i - \frac{1}{2}k$$ j 11 $$\left( \frac{-1,-11}{\mathbb {Q}}\right)$$ $$\mathbb {Z}\oplus \mathbb {Z} i\oplus \mathbb {Z} \left( \frac{1+j}{2}\right) \oplus \mathbb {Z}\left( \frac{i+k}{2}\right)$$ $$1+3i$$ j

Using these choices along with the algorithms and results mentioned previously, one can calculate the groups $$\Gamma ^{(1)},\Gamma ^{(2)}$$ for each such p, hence generating tables of dimensions of the spaces $$A_{j,k-3}^{\text {new}}(D)$$. These tables are given in Appendix 1.

From these tables, one isolates 1-dimensional spaces. For each possibility, the MAGMA command LRatio allows us to test for large primes dividing $$\Lambda _{\text {alg}}$$ on the elliptic side. The cases that remained were ones where we expect to find examples of Harder’s congruence.

Tables of the congruences observed can be found in Appendix 2. In particular, for $$p=2$$ one observes congruences provided in Bergström . We finish with some new examples for $$p=3$$.

### Example 6.1

By Appendix 1, we see that

\begin{aligned} \text {dim}(A_{2,5}(D)) = \text {dim}(A_{2,5}^{\text {new}}(D)) = \text {dim}(S_{2,8}^{\text {new}}(K(3)))= 1. \end{aligned}

Then $$j=2$$ and $$k=8$$ so that $$j+2k-2 = 16$$. Let $$F\in S_{2,8}^{\text {new}}(K(3))$$ be the unique normalized eigenform.

One easily checks that dim$$(S_{16}^{\text {new}}(\Gamma _0(3))) = 2$$. This space is spanned by the two normalized eigenforms with q-expansions:

\begin{aligned} f_1(\tau )&= q - 234q^2 - 2187q^3 + 21988q^4 + 280710q^5 + \cdots \\ f_2(\tau )&= q - 72q^2 + 2187q^3 - 27584q^4 -221490q^5 + \cdots \end{aligned}

Indeed, MAGMA informs us that $$\text {ord}_{109}(\Lambda _{\text {alg}}(f_1, 10)) = 1$$ and so we expect a congruence of the form:

\begin{aligned} b_q \equiv a_q + q^9 + q^6 \bmod 109 \end{aligned}

for all $$q\ne 3$$, where $$b_q$$ are the Hecke eigenvalues of F and $$a_q$$ the Hecke eigenvalues of $$f_1$$. As discussed earlier, we will only work with the case $$q=2$$ for simplicity.

The algorithms mentioned earlier then calculate the necessary $$\frac{5760}{3^2-1} = 720$$ matrices belonging to $$\Gamma ^{(2)}$$ and the $$(2+1)(2^2+1) = 15$$ Hecke representatives for the operator $$T_{u,2}$$. Applying the trace formula, we find that $$\text {tr}(T_{u,2}) = -312$$.

Now since $$A_{2,5}(D) = A_{2,5}^{\text {new}}(D)$$, we have that $$\text {tr}(T_{u,2}) = \text {tr}(T_{u,2})^{\text {new}}$$. Also the spaces are 1-dimensional and so in fact $$b_2 = \text {tr}(T_{u,2})^{\text {new}} = -312$$.

The congruence is then simple to check:

\begin{aligned} -312 \equiv -234 + 2^9 + 2^6 \bmod 109. \end{aligned}

$$\square$$

### Example 6.2

We see an example where we must subtract off the oldform contribution from the trace. By Appendix 1, we see that

\begin{aligned} \text {dim}(A_{8,2}(D)) = 3, \end{aligned}

whereas

\begin{aligned} \text {dim}(A_{8,2}^{\text {new}}(D)) = \text {dim}(S_{8,5}^{\text {new}}(K(3))) = 1. \end{aligned}

Then $$j=8$$ and $$k=5$$ so that $$j+2k-2 = 16$$ again. Let $$F\in S_{8,5}^{\text {new}}(K(3))$$ be the unique normalized eigenform.

MAGMA informs us that $$\text {ord}_{67}(\Lambda _{\text {alg}}(f_2, 13)) = 1$$ and so we expect a congruence of the form

\begin{aligned} b_q \equiv a_q + q^{12} + q^3 \bmod 67, \end{aligned}

for all $$q\ne 3$$.

Applying the trace formula this time gives $$\text {tr}(T_{u,2}) = 300$$. However, since $$\text {dim}(A_{8,2}(D)) > \text {dim}(A_{8,2}^{\text {new}}(D))$$, there is an oldform contribution to this trace. In order to find it, we need Hecke eigenvalues of normalized eigenforms for the spaces $$S_{16}(\mathrm {SL}_2(\mathbb {Z}))$$ and $$S_{10}^{\text {new}}(\Gamma _0(3))$$.

It is known that dim$$(S_{16}(\mathrm {SL}_2(\mathbb {Z}))) = 1$$ and that the unique normalized eigenform has q-expansion:

\begin{aligned} g(\tau ) = q + 216q^2 -3348q^3 + 13888q^4 + 52110+ \cdots \end{aligned}

Also dim$$(S_{10}^{\text {new}}(\Gamma _0(3))) = 2$$ and the normalized eigenforms have the following q-expansions:

\begin{aligned} h_1(\tau )&= q - 36q^2 - 81q^3 + 784q^4 - 1314q^5 + \cdots \\ h_2(\tau )&= q + 18q^2 + 81q^3 - 188q^4 - 1540q^5 + \cdots \end{aligned}

Thus, using Corollary 5.20 the oldform contribution is

\begin{aligned} \text {tr}(T_{u,2})^{\text {old}} = 2a_{2,g} + 2^3(a_{2,h_1} + a_{2,h_2})&= 512 +8(-36+18)\\&= 288. \end{aligned}

Hence $$\text {tr}(T_{u,2})^{\text {new}} = \text {tr}(T_{u,2}) - \text {tr}(T_{u,2})^{\text {old}} = 300 - 288 = 12$$. Since our space of algebraic forms is 1-dimensional, we must have $$b_2 = \text {tr}(T_{u,2})^{\text {new}} = 12$$.

The congruence is then simple to check:

\begin{aligned} 12 \equiv -72 + 2^{12} + 2^3 \bmod 67. \end{aligned}

$$\square$$

### Example 6.3

Our final example is a case where the Hecke eigenvalues of the elliptic modular form lie in a quadratic extension of $$\mathbb {Q}$$.

By Appendix 1, we see that

\begin{aligned} \text {dim}(A_{6,2}(D)) = \text {dim}(A_{6,2}^{\text {new}}(D)) = \text {dim}(S_{6,5}^{\text {new}}(K(3))) = 1. \end{aligned}

Then $$j=6$$ and $$k=5$$ so that $$j+2k-2 = 14$$. Let $$F\in S_{6,5}^{\text {new}}(K(3))$$ be the unique normalized eigenform.

One easily checks that dim$$(S_{14}^{\text {new}}(\Gamma _0(3))) = 3$$. This space is spanned by the three normalized newforms with q-expansions:

\begin{aligned} f_1(\tau )&= q - 12q^2 - 729q^3 + \cdots \\ f_2(\tau )&= q - (27 + 3\sqrt{1969})q^2 + 729q^3 + \cdots \\ f_3(\tau )&= q - (27 - 3\sqrt{1969})q^2 + 729q^3+ \cdots \end{aligned}

MAGMA informs us that $$\text {ord}_{47}(N_{\mathbb {Q}(\sqrt{1969})/\mathbb {Q}}(\Lambda _\text {alg}(f_2, 11))) = 1$$ and so we expect a congruence of the form

\begin{aligned} b_q \equiv a_q + q^{10} + q^3 \bmod \lambda \end{aligned}

for some prime ideal $$\lambda$$ of $$\mathbb {Z}\left[ \frac{1+\sqrt{1969}}{2}\right]$$ satisfying $$\lambda \mid 47$$ (note that 47 splits in this extension).

The trace formula gives $$\text {tr}(T_{u,2}) = 72$$ and the usual arguments show that $$b_2 = 72$$. It is then observed that

\begin{aligned} N_{\mathbb {Q}(\sqrt{1969})/\mathbb {Q}}(b_2 - a_2 - 2^{10} - 2^3) = N_{\mathbb {Q}(\sqrt{1969})/\mathbb {Q}}(-933 + 3\sqrt{1969}) = 852768. \end{aligned}

This is divisible by 47 and so the congruence holds for $$q=2$$. $$\square$$