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Embedding of lattices and K3-covers of an Enriques surface

  • Serkan Sonel EMAIL logo
Published/Copyright: September 11, 2025

Abstract

In this study, we establish necessary conditions for the embeddings of lattices and apply these conditions to the problem of characterizing algebraic K 3 surfaces that cover an Enriques surface. By refining existing criteria and providing a more elementary approach, we offer a new perspective on the structure of such surfaces. Our results apply to any lattices, extending beyond specific cases and offering a comprehensive framework for understanding the embedding conditions in terms of Gram matrices.

MSC 2010: 14J28

1 Introduction

In this work, we give the necessary conditions for the embeddings of lattices and present an application of the provided criterion for the problem of characterizing algebraic K 3 surfaces covering an Enriques surface.

The main result of this article is the following theorem, whose proof is given in Section 3.

Theorem 1.1

Let L and M be even integral lattices of rank ( L ) and rank ( M ) , and let rank 2 ( L ) and rank 2 ( M ) denote their ranks over Z 2 . Let ϕ be an embedding of L into M. Then, one of the following conditions holds:

  1. If rank 2 ( M ) = 0 , then there exists a lattice T such that L T ( 2 ) .

  2. If rank 2 ( M ) > 0 and rank 2 ( L ) = 0 , then

    rank ( L ) rank ( M ) 1 2 rank 2 ( M ) ,

    and there exists a lattice T such that L T ( 2 ) .

  3. If rank 2 ( M ) > 0 and rank 2 ( L ) > 0 , then

    rank ( L ) rank ( M ) 1 2 rank 2 ( M ) + 1 2 rank 2 ( L ) ,

    and there exists an even lattice T such that L T and its associated Gram matrix must have the form

    G T = 2 a 11 a 12 a 1 λ a 12 2 a 22 a 1 λ 2 a λ λ ,

    where a 2 k 1,2 k is odd for each 1 k 1 2 rank 2 ( L ) , and the remaining off-diagonal entries are even.

  4. If rank(L) = rank(M), L M , provided that the embedding is primitive.

Recall that an algebraic K3 surface over C is a smooth projective surface X such that the canonical divisor K X of X is trivial and H 1 X , O X = 0 and an Enriques surface is a smooth projective surface Y such that 2 K Y is trivial and H 1 Y , O Y = H 2 Y , O Y = 0 , where K Y is a canonical divisor of Y . The Néron-Severi lattice N S ( X ) is a sublattice of the cohomology group H 2 ( X , Z ) of X that is a unimodular lattice of rank 22. The rank of N S ( X ) is called the Picard number of X , denoted by ρ ( X ) . The orthogonal complement of N S ( X ) in H 2 ( X , Z ) is called the transcendental lattice T X , which has signature ( 2,20 ρ ( X ) ) .

The following criterion was established by Keum, which was originally proven under an additional assumption that Ohashi subsequently showed to be unnecessary [1].

Theorem 1.2

(Keum’s criterion) [2, Theorem 1] A K3 surface X with transcendental lattice T X covers an Enriques surface if and only if there exists a primitive embedding of T X into Λ U U ( 2 ) E 8 ( 2 ) such that there exists no vector v T X with v 2 = 2 .

Using the criterion mentioned above, Keum proved that every algebraic Kummer surface is a K3 cover of some Enriques surface [2]. Sertöz [3] identified conditions on the entries of the Gram matrix of the transcendental lattice T X under which X covers an Enriques surface when ρ ( X ) = 20 . Subsequently, Lee [4] and Yörük [5] extended these results to cases where ρ ( X ) = 18 and ρ ( X ) = 19 .

In his work [6, Prop. 1.15.1], Nikulin provides a criterion to enumerate all primitive embeddings of a fixed lattice T into lattices of signature ( m + , m ) and discriminant form q for a given pair of nonnegative integers ( m + , m ) and a finite quadratic form q . Brandhorst et al. [7], employed Nikulin’s criterion to enumerate all primitive embeddings of T X into Λ , and applied Keum’s criterion to characterize complex K3 surfaces that cover Enriques surfaces in terms of their Gram matrices.

In this article, we establish necessary conditions for the embeddings of a fixed lattice L into arbitrary lattices by analyzing their Gram matrices over Z 2 , considered up to the action of GL n ( Z 2 ) . By using the necessary conditions above and applying Keum’s criterion, we characterize complex K3 surfaces that cover Enriques surfaces in terms of their Gram matrices.

By Keum’s criterion, there are two reasons why a K3 surface X cannot cover any Enriques surface: firstly, there exists no primitive embedding of T X into Λ , second, for every primitive embedding of T X into Λ , there exists a vector v in the orthogonal complement of T X in Λ with v 2 = 2 . In the latter, the transcendental lattice T X is called a co-idoneal lattice in [7].

By providing the necessary conditions for the embeddings of lattices, we obtain the following theorem, whose proof is given in Section 4.

Theorem 1.3

Let X be a K3 surface with 10 ρ ( X ) 20 whose transcendental lattice T X is of rank λ and signature ( 2 , λ 2 ) . Then, X covers an Enriques surface if and only if one of the following conditions holds:

  1. 11 ρ ( X ) 20 , and there exists an even lattice T such that T X T ( 2 ) .

  2. 11 ρ ( X ) 20 , and there exists an odd lattice T such that T X T ( 2 ) except when T X is co-idoneal.

  3. 11 ρ ( X ) 20 , and there exists an even lattice T such that T X T and its associated Gram matrix must be in the following form:

    G T = 2 a 11 a 12 a 1 λ a 12 2 a 22 a 1 λ 2 a λ λ ,

    such that a i j is even for each 1 i , j λ except a 11 , a 12 .

  4. ρ ( X ) = 10 , and T X Λ .

Furthermore, we will derive refined characterizations of the forms of exceptional lattices, referred to as co-idoneal lattices in Section 5.

2 Preliminaries

An integral lattice ( L , β ) is a finitely generated, free Z -module equipped with an integral symmetric bilinear form β , L Z n , β . The lattice L is even if β ( x , x ) 0 mod 2 for all x L , and is odd otherwise.

Let B = e 1 , , e n be a basis of Z -module L . The symmetric matrix G = ( a i j ) , given by a i j = β ( e i , e j ) , is the Gram matrix of L with respect to this basis B , written as L G L . The discriminant of a lattice L is the determinant of G L .

Let L and M be two Z -modules, β and β be bilinear forms on L and M , respectively. A module homomorphism ϕ : L M is called a lattice morphism if it satisfies the isometry relation, i.e., β ( x , y ) = β ( ϕ ( x ) , ϕ ( y ) ) for all x , y L . Furthermore, a lattice morphism ϕ : L M is called a lattice embedding if ϕ is a monomorphism. The embedding is called primitive if M ϕ ( L ) is a free module, i.e., it has a basis. L M if ϕ is also an epimorphism.

Two matrices T 1 and T 2 are said to be Z -equivalent if there exists an element g G L ( n , Z ) together with its transpose g τ such that

T 2 = g τ T 1 g .

The negative definite exceptional lattice is denoted E n , and the hyperbolic lattice is denoted U .

For any integer n , we denote by [ n ] , the lattice Z e of rank 1 with β ( e , e ) = n . For any integer n , and L G = ( a i j ) , the lattice L ( n ) has G L ( n ) = ( n a i j ) . By abuse of language, a symmetric bilinear form β will be denoted by dot product.

The following theorem in [3] characterizes the primitive embeddings of lattices.

Theorem 2.1

[3] A lattice embedding is primitive if and only if the greatest common divisor of the maximal minors of the embedding matrix with respect to any choice of basis is 1.

Under certain assumptions on the discriminant of a lattice, an odd indefinite lattice can be decomposed into one of the following forms:

Theorem 2.2

[8, Theorem 1] Let L be an odd indefinite Z -lattice of rank l 3 with square free discriminant d. Then,

(2.1) L m [ 1 ] n [ 1 ] B ,

where B is a lattice of rank 2, and m , n 0 . Moreover, if d is even, then B can be chosen to be definite or indefinite.

Theorem 2.3

[9, Theorem 6] Let L be an odd indefinite Z -lattice of rank l 3 and cube-free discriminant d 0 ( mod 4 ) . Then, L has an orthogonal splitting

(2.2) L m [ 1 ] n [ 1 ] B ,

where B is an indefinite odd lattice of rank 3, and m , n 0 .

Lemma 2.4

The map G L n ( Z ) G L n ( Z 2 Z ) is surjective.

Proof

Indeed, GL n ( Z 2 Z ) SL n ( Z 2 Z ) is generated by transvections (elementary), and these obviously lift to GL n ( Z ) .□

3 Necessary conditions of embeddings of lattices

In this section, we will provide the necessary conditions for the embedding of lattices.

Theorem 3.1

Let F be a finite field of characteristic 2. Then, every symmetric matrix M n over F with zero diagonal is congruent to i = 1 q H i = 1 n 2 q [ 0 ] or i = 1 n [ 0 ] , where q N + and

H 0 1 1 0 .

Furthermore, two symmetric matrices with zero diagonal over the field F are congruent if and only if they have the same rank.

Proof

Suppose that M = 0 , the result is trivial.

Suppose that M 0 , so that there exists some non-zero element a i j of M . Since GL n ( Z 2 Z ) SL n ( Z 2 Z ) is generated by the elementary matrices E i j ( α ) , where α Z 2 , performing the elementary congruent transformations, we may write

M H B t B A , where H 0 1 1 0 .

Performing successive elementary congruent transformations of E i j ( α ) , i varying from 3 to n , we obtain a symmetric matrix such that

M H 0 0 A 1 , where H 0 1 1 0 .

A 1 is an ( n 2 ) -rowed symmetric matrix with zero diagonal. Therefore, we may proceed recursively and obtain a symmetric matrix of the form i = 1 q H i = 1 n 2 q [ 0 ] congruent to the given matrix M .

Because of the fact that the congruence of matrices is an equivalence relation possessing symmetry and transitivity, and by the above reasoning, two symmetric matrices of M n with zero diagonal over the field F are congruent if and only if they have the same rank. This completes the proof.□

As a direct consequence, we obtain the following.

Corollary 3.2

The number o ( n ) of orbits of the even symmetric matrix M n of size n × n over Z 2 Z with a zero diagonal under the action of G L n ( Z 2 Z ) by the transposition is given by

o ( n ) = 1 2 ( n + 1 ) , if n i s o d d , 1 2 ( n + 2 ) , if n i s e v e n .

The map G L n ( Z ) G L n ( Z 2 Z ) is surjective by Lemma 2.4; therefore, we can consider the action of G L n ( Z 2 Z ) by the transposition on the set of the even symmetric matrices M n of size n × n over Z 2 Z .

We will characterize associated Gram matrices of lattices with respect to their ranks over Z 2 by the following.

Definition 3.3

Let L be an integral even lattice of rank λ and G L be its associated Gram matrix. Let L be an induced Z 2 -module of L by restriction of ring of integers Z to Z 2 and their associated Gram matrices G L = ( a i j ) of L and G L = ( a i j ( mod 2 ) ) of L . The rank of G L of L over the field of characteristic 2, will be the rank of G L of L , denoted by rank 2 ( L ) .

Lemma 3.4

Let L be an integral even lattice of rank λ and G L be its associated Gram matrix, with rank 2 ( L ) = 2 q . Then,

G L 2 a 11 a 12 a 1 λ a 12 2 a 22 a 1 λ 2 a λ λ ,

such that a 2 k 1,2 k is odd for each 1 k q , and the remaining off-diagonal entries are even.

Proof

Let L be an even lattice. The Gram matrix G L of L is symmetric, and its diagonal entries are even.

Reduction of G L modulo 2 yields a symmetric matrix over Z 2 Z . The diagonal entries, being even, reduce to zero, so the reduced matrix has zero diagonal entries, and the off-diagonal entries are either 0 or 1.

By Lemma 2.4, the map G L n ( Z ) G L n ( Z 2 Z ) is surjective. Therefore, we can use the action of G L n ( Z 2 Z ) to bring G L mod 2 into a canonical form.

Over Z 2 Z , by Theorem 3.1, every symmetric matrix with zero diagonal can be reduced, via congruence, to a block diagonal form consisting of 2x2 blocks of the type:

H = 0 1 1 0

and possibly zero blocks.

The number of such blocks corresponds to the rank of the matrix modulo 2. Let rank 2 ( L ) = 2 q , which means G L mod 2 can be transformed into a block diagonal matrix with q blocks of the form H , while the remaining part of the matrix consists of zero blocks.

Once we have the canonical form of G L mod 2 , we lift this back to an integral matrix over Z . For each block H in the reduced matrix, the corresponding entries in the lifted matrix G L will be odd. That is, the off-diagonal terms a 2 k 1,2 k are odd for each k = 1,2 , , q . The remaining off-diagonal terms, which were zero modulo 2, will be even in G L . This completes the proof.□

Proof of Theorem 1.1

Let L have a Gram matrix G L and let M have a Gram matrix G M . The induced Z 2 -modules are given by

L i = 1 l ( Z 2 ) x i and M i = 1 m ( Z 2 ) u i ,

where { x i } i and { u i } i are basis for L and M of ranks l and m , respectively.

By Theorem 3.1 and Corollary 3.2, we know that:

G L i = 1 p H i = 1 l 2 p [ 0 ] or i = 1 l [ 0 ] ,

where rank 2 ( L ) = 2 p . Similarly,

G M i = 1 q H i = 1 m 2 q [ 0 ] or i = 1 m [ 0 ] ,

where rank 2 ( M ) = 2 q . They are uniquely determined by their ranks over Z and Z 2 by Theorem 3.1 and Corollary 3.2.

Consider the embedding ϕ : L M and the induced embedding ϕ : L M . Since ϕ and ϕ are embeddings, the necessary conditions for the embedding of L into M are that

rank ( L ) rank ( M ) , rank 2 ( L ) rank 2 ( M ) .

Therefore, each embedding ϕ of L into M must satisfy

rank ( L ) rank ( M ) , rank 2 ( L ) rank 2 ( M ) .

Now we can analyze each case.

Case I: rank 2 ( M ) = 0 .

Since rank 2 ( M ) = 0 , G M i = 1 m [ 0 ] . It implies that

G L i = 1 l [ 0 ] ,

where l m .

By Lemma 3.4, there exists a lattice T such that L T ( 2 ) . Thus, we have:

L T ( 2 )

for some lattice T . This completes the proof for Case I.

Case II: rank 2 ( M ) > 0 and rank 2 ( L ) = 0 .

Since rank 2 ( L ) = 0 , we conclude that G L i = 1 l [ 0 ] . Suppose that

rank ( L ) > rank ( M ) 1 2 rank 2 ( M ) .

By Theorem 3.1, Corollary 3.2, we have

(3.1) G L i = 1 t H i = 1 l 2 t [ 0 ]

for some t N + . This contradicts the condition that rank 2 ( L ) = 0 . Therefore,

rank ( L ) rank ( M ) 1 2 rank 2 ( M ) .

The existence of a lattice T such that L T ( 2 ) follows from Lemma 3.4. This completes the proof for Case II.

Case III: rank 2 ( M ) > 0 and rank 2 ( L ) > 0 .

Suppose that

rank ( L ) > 1 2 rank 2 ( L ) + rank ( M ) 1 2 rank 2 ( M ) .

By Theorem 3.1 and Corollary 3.2, we have

(3.2) G L i = 1 t H i = 1 l 2 t [ 0 ]

for some t N + such that t > rank 2 ( L ) . This leads to a contradiction with the uniqueness of its canonical form. Hence, we obtain the following rank condition:

rank ( L ) rank ( M ) 1 2 rank 2 ( M ) + 1 2 rank 2 ( L ) .

By Lemma 3.4, we can express the Gram matrix G L of L in the specified form:

G L 2 a 11 a 12 a 1 λ a 12 2 a 22 a 1 λ 2 a λ λ ,

where a 2 k 1,2 k is odd for each 1 k 1 2 rank 2 ( L ) , and the remaining off-diagonal entries are even.

This completes the proof for Case III.

Case IV: rank ( L ) = rank ( M ) .

If rank(L) = rank(M), then L M . The claim trivially follows by the definition of a primitive embedding.

By addressing each case, we have proved that for any embedding ϕ of L into M , one of the conditions stated in the theorem must hold. Therefore, the proof is complete.□

4 Proof of Theorem 1.3

As a consequence of the foregoing theorem, we derive the following:

Theorem 4.1

Let T X be transcendental lattice of signature ( 2 , λ 2 ) . If there exists an embedding of T X into Λ , then rank 2 ( T X ) = 0 or 2. Particularly, the associated Gram matrix of each embedding of T X into Λ must be one of the following types:

  1. T X T ( 2 ) , where T is an even lattice,

  2. T X T ( 2 ) , where T is an odd lattice,

  3. rank 2 ( T X ) = 2 ,

    G T X 2 a 11 a 12 a 1 λ a 12 2 a 22 a 1 λ 2 a λ λ ,

    such that a i j is even for each 1 i , j λ except a 11 , a 12 .

Proof

Let { x i } i be a basis of the transcendental lattice T X and let { u 1 , u 2 } and { v 1 , v 2 } be the standard basis of U and U ( 2 ) , respectively.

If ϕ : T X Λ is an embedding defined generically by

(4.1) ϕ ( x i ) = a i 1 u 1 + a i 2 u 2 + a i 3 v 1 + a i 4 v 2 + w i ,

where a i j are integers and w i E 8 ( 2 ) for 1 i λ and 1 j 4 then, we have that,

(4.2) ϕ ( x i ) ϕ ( x i ) = 2 a i 1 a i 2 + 4 a i 3 a i 4 + w 1 2 = 2 a i i ,

for 1 i λ and

(4.3) ϕ ( x i ) ϕ ( x k ) = a i 1 a k 2 + a i 2 a k 1 + 2 a i 3 a k 4 + 2 a i 4 a k 4 + w i w k = a i k

for 1 i < k λ .

By Theorem 1.1, equations (4.2) and (4.3) are solvable over Z 2 if and only if rank 2 ( T X ) rank 2 ( Λ ) . Since rank 2 ( Λ ) = 2 , rank 2 ( T X ) is either 0 or 2.

Case I: rank 2 ( T X ) = 0 .

Since rank 2 ( T X ) = 0 , T X i = 1 λ [ 0 ] , λ 11 using Theorem 1.1. By Lemma 3.4, there are two types of associated Gram matrices of T X rising after lifting up to Z :

  • T X T ( 2 ) , where T is an even lattice,

  • T X T ( 2 ) , where T is an odd lattice.

Case II: rank 2 ( T X ) = 2

If rank 2 ( T X ) = 2 , by Theorem 1.1 and Lemma 3.4,

G T X 2 a 11 a 12 a 1 λ a 12 2 a 22 a 1 λ 2 a λ λ ,

such that a 12 is odd and the remaining off-diagonal entries are even.

To determine the parities of diagonal entries of T X , we need to consider the equations (4.2) and (4.3). If both a 11 and a 22 are odd, it contradicts with equations (4.2) and (4.3). Suppose both a 11 and a 22 are even. Then, under the action of element g GL ( λ , Z ) where all diagonal entries are 1, the ( 2,1 ) -entry is 1, and all other off-diagonal entries are 0, both a 11 and a 12 will be odd, the parities of remaining entries of T X will be invariant. Hence, without loss of generality, assume that a 11 is odd and a 22 is even. Since a 11 is odd, it enforces that a 11 and a 12 are odd by equation (4.2). a 12 is odd, it also enforces that a 21 and a 22 have a different parity by equation (4.3). Thus, by equations (4.2) and (4.3), both a i 1 and a i 2 are even for 3 i λ , it implies that a i i 2 Z for 3 i λ . This completes the proof.□

We will now present and prove the subsequent theorems that broaden the criteria for K3-covers an Enriques surface, showing that for each embedding of T X into Λ or an induced embedding T X into Λ , there exists no v T X with v 2 = 2 , as opposed to relying solely on primitive embeddings. By Lemma 3.4 and Theorem 1.1, the following result can be generalized to any embedding of a lattice L into another lattice M , provided that rank 2 ( L ) = rank 2 ( M ) . However, we will limit our focus to the specific case of embedding T X into Λ .

Lemma 4.2

Let T X be an even lattice of signature ( 2 , λ 2 ) , rank 2 ( T X ) = 2 . Then, for each embedding of T X into Λ , there exists no v T X with v 2 = 2 .

Proof

Let { x i } i be a basis of the transcendental lattice T X , and let { u 1 , u 2 } and { v 1 , v 2 } be the standard basis of U and U ( 2 ) , respectively. Consider the embedding ϕ : T X Λ defined generically by

(4.4) ϕ ( x i ) = a i 1 u 1 + a i 2 u 2 + a i 3 v 1 + a i 4 v 2 + w i ,

where a i j are integers and w i E 8 ( 2 ) for 1 i λ and 1 j 4 .

By Theorem 4.1, a 11 is odd, it enforces that a 11 and a 12 are odd. Similarly, a 12 is odd, it also enforces that a 21 and a 22 have a different parity.

To prove the orthogonal complement of the image of ϕ in Λ contains no self-intersection 2 vector, let f = X u 1 + x u 2 + Y v 1 + y v 2 + e Λ , where e E 8 ( 2 ) with e e = 4 k , k 0 . From the equation,

f ϕ ( x 2 ) = ( X u 1 + x u 2 + Y v 1 + y v 2 + e ) ( a 21 u 1 + a 22 u 2 + a 23 v 1 + a 24 v 2 + w i ) = 0 ,

we obtain that

(4.5) x a 21 + X a 22 x 0 mod 2 .

Since a 21 and a 22 have a different parity, x or X must be even. We obtain

(4.6) f f = 2 X x + 4 Y y + e e 0 mod 4 .

Therefore, the orthogonal complement of the image of ϕ in Λ contains no self-intersection 2 vector.□

Lemma 4.3

Let T X be an even lattice of signature ( 2 , λ 2 ) and T X T ( 2 ) , where T is an even lattice. Then, for each embedding of T X into Λ , there exists an induced embedding such that there exists no v T X with v 2 = 2 .

Proof

Let { x i } i be a basis of the transcendental lattice T X , and let { u 1 , u 2 } and { v 1 , v 2 } be the standard basis of U and U ( 2 ) , respectively. Consider the embedding ϕ : T X Λ defined generically by

(4.7) ϕ ( x i ) = a i 1 u 1 + a i 2 u 2 + a i 3 v 1 + a i 4 v 2 + w i ,

where a i j are integers and w i E 8 ( 2 ) for 1 i λ and 1 j 4 .

Suppose T X T ( 2 ) , where T is an even lattice, a i j is even for 1 i , j λ 11 by Theorem 4.1.

Since T X is an even lattice of signature ( 2 , λ 2 ) , there exists a i j such that a i j 0 for 1 i λ and 1 j 2 .

Suppose that a i 1 and a i 2 have different parity for 1 i λ , then by the same reasoning as in Lemma 4.2, the orthogonal complement of the image of ϕ in Λ contains no self-intersection 2 vector.

Suppose that a i 1 and a i 2 are of the form a i j = 2 k i j . m i j , where k i j Z + , m i j 2 Z for all a i j 0 , 1 i λ , 1 j 2 . Let k be a minimum among the all υ 2 ( a i 1 ) the exponent of the largest power of 2 of a i 1 0 . Without loss of generality, let k = k 11 . If we insert a i 1 = 2 k i 1 k . m i 1 and a i 2 = 2 k i 2 + k . m i 2 in the place of a i 1 0 , a i 2 0 , respectively; equations (4.2) and (4.3) are satisfied for the new embedding ϕ induced by the embedding ϕ for i , j , 1 i λ , 1 j 2 . Particularly, if ϕ is primitive, then the induced embedding ϕ is also primitive by Theorem 2.1.

Since a 11 and a 12 have different parity, then, again by the same reasoning as in Theorem 4.2, the orthogonal complement of the image of ϕ in Λ contains no self-intersection 2 vector.□

Proof of Theorem 1.3

Let X be a K3 surface of 11 ρ ( X ) 20 with its transcendental lattice T X of rank λ and signature ( 2 , λ 2 ) . Each primitive embedding of T X into Λ is also an embedding, by Theorem 4.1, the associated Gram matrix of T X of each embedding of T X into Λ must be one of the following types:

  • T X T ( 2 ) , where T is an even lattice,

  • T X T ( 2 ) , where T is an odd lattice,

  • rank 2 ( T X ) = 2 ,

    G T X 2 a 11 a 12 a 1 λ a 12 2 a 22 a 1 λ 2 a λ λ ,

    such that a i j is even for each 1 i , j λ except a 11 , a 12 .

If T X T ( 2 ) , where T is an even lattice, by Lemma 4.3, for each embedding of T X into Λ , there exists an induced embedding such that there exists no v T X with v 2 = 2 . By Theorem 1.2, the claim follows.

If T X T ( 2 ) , where T is an odd lattice, and T X is not a co-idoneal lattice, by the definition of the co-idoneal lattice and Theorem 1.2, the claim follows.

If rank 2 ( T X ) = 2 , by Lemma 4.2, for each embedding of T X into Λ , there exists no v T X with v 2 = 2 . Hence, by Theorem 1.2, the claim follows.

Finally, if ρ ( X ) = 10 , then rank ( T X ) = rank ( Λ ) , T X Λ , so the claim is trivial.□

5 Exceptional lattices

Recall that a transcendental lattice T X is called a co-idoneal lattice if, for every primitive embedding of T X into Λ , there exists a vector v in the orthogonal complement of T X in Λ with v 2 = 2 .

The following theorem, obtained as Corollary 3.13 in [7], will be proven using elementary techniques.

Theorem 5.1

If T X is a co-idoneal lattice, T X T ( 2 ) , where T is an odd lattice.

Proof

The proof of this theorem is a direct consequence of Theorem 4.1 and Lemmas 4.2 and 4.3.□

For the transcendental lattices T X of rank λ 3 , we prove the following theorems:

Theorem 5.2

If T X is a co-idoneal lattice such that T X T ( 2 ) , where T has a square free discriminant d, then T X must be the following forms: m [ 2 ] n [ 2 ] B ( 2 ) for some m , n N , where B is a lattice of rank 2, 0 m 2 . Moreover, if d is even, T X must be the one of the following forms: 2 [ 2 ] n [ 2 ] B ( 2 ) for some n, where B is a negative definite lattice of rank 2, or n [ 2 ] B ( 2 ) , where B is a positive definite lattice of rank 2 .

Proof

By Theorem 5.1, since T X is a co-idoneal lattice, T X T ( 2 ) , where T is an odd lattice. By Theorem 2.2, all odd lattices with a square-free discriminant d can be diagonalized in that form. Hence, the result follows.□

Theorem 5.3

If T X is a co-idoneal lattice such that T X T ( 2 ) , where T has a cube free discriminant d, then T X must be the following forms: m [ 2 ] n [ 2 ] B ( 2 ) for some m , n N , where B is a lattice of rank 3, and 0 m 2 .

Proof

By Theorem 5.1, since T X is a co-idoneal lattice, T X T ( 2 ) , where T is an odd lattice. By Theorem 2.3, all odd lattices with a cube-free discriminant d can be diagonalized in that form. Hence, the result follows.□

Acknowledgements

I am grateful to Mesut Şahin, M. Anıl Tokmak, A. Sinan Sertöz, Alex Degtyarev, Davide C. Veniani, and the referees for their valuable insights, comments, and contributions through many conversations.

  1. Funding information: The author acknowledges the support of Bilkent University and the following research projects: TÜBİTAK 123F111.

  2. Author contributions: The author confirms sole responsibility for the conception and design of the study, the analysis and interpretation of the presented results, as well as the preparation and writing of the manuscript.

  3. Conflict of interest: The author states no conflicts of interest.

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Received: 2024-10-14
Revised: 2025-05-29
Accepted: 2025-07-04
Published Online: 2025-09-11

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Articles in the same Issue

  1. On I-convergence of nets of functions in fuzzy metric spaces
  2. Special Issue on Contemporary Developments in Graphs Defined on Algebraic Structures
  3. Forbidden subgraphs of TI-power graphs of finite groups
  4. Finite group with some c#-normal and S-quasinormally embedded subgroups
  5. Classifying cubic symmetric graphs of order 88p and 88p 2
  6. Two-sided zero-divisor graphs of orientation-preserving and order-decreasing transformation semigroups
  7. Simplicial complexes defined on groups
  8. Further results on permanents of Laplacian matrices of trees
  9. Algebra
  10. Classes of modules closed under projective covers
  11. On the dimension of the algebraic sum of subspaces
  12. Green's graphs of a semigroup
  13. On an uncertainty principle for small index subgroups of finite fields
  14. On a generalization of I-regularity
  15. Algorithm and linear convergence of the H-spectral radius of weakly irreducible quasi-positive tensors
  16. The hyperbolic CS decomposition of tensors based on the C-product
  17. On weakly classical 1-absorbing prime submodules
  18. Equational characterizations for some subclasses of domains
  19. Algebraic Geometry
  20. Spin(8, ℂ)-Higgs bundles fixed points through spectral data
  21. Embedding of lattices and K3-covers of an Enriques surface
  22. Kodaira-Spencer maps for elliptic orbispheres as isomorphisms of Frobenius algebras
  23. Applications in Computer and Information Sciences
  24. Dynamics of particulate emissions in the presence of autonomous vehicles
  25. Exploring homotopy with hyperspherical tracking to find complex roots with application to electrical circuits
  26. Category Theory
  27. The higher mapping cone axiom
  28. Combinatorics and Graph Theory
  29. 𝕮-inverse of graphs and mixed graphs
  30. On the spectral radius and energy of the degree distance matrix of a connected graph
  31. Some new bounds on resolvent energy of a graph
  32. Coloring the vertices of a graph with mutual-visibility property
  33. Ring graph induced by a ring endomorphism
  34. A note on the edge general position number of cactus graphs
  35. Complex Analysis
  36. Some results on value distribution concerning Hayman's alternative
  37. Freely quasiconformal and locally weakly quasisymmetric mappings in metric spaces
  38. A new result for entire functions and their shifts with two shared values
  39. On a subclass of multivalent functions defined by generalized multiplier transformation
  40. Singular direction of meromorphic functions with finite logarithmic order
  41. Growth theorems and coefficient bounds for g-starlike mappings of complex order λ
  42. Refinements of inequalities on extremal problems of polynomials
  43. Control Theory and Optimization
  44. Averaging method in optimal control problems for integro-differential equations
  45. On superstability of derivations in Banach algebras
  46. The robust isolated calmness of spectral norm regularized convex matrix optimization problems
  47. Observability on the classes of non-nilpotent solvable three-dimensional Lie groups
  48. Differential Equations
  49. The ill-posedness of the (non-)periodic traveling wave solution for the deformed continuous Heisenberg spin equation
  50. A note on the global existence and boundedness of an N-dimensional parabolic-elliptic predator-prey system with indirect pursuit-evasion interaction
  51. Blow-up of solutions for Euler-Bernoulli equation with nonlinear time delay
  52. Periodic or homoclinic orbit bifurcated from a heteroclinic loop for high-dimensional systems
  53. Regularity of weak solutions to the 3D stationary tropical climate model
  54. Local minimizers for the NLS equation with localized nonlinearity on noncompact metric graphs
  55. Global existence and blow-up of solutions to pseudo-parabolic equation for Baouendi-Grushin operator
  56. Bubbles clustered inside for almost-critical problems
  57. Existence and multiplicity of positive solutions for multiparameter periodic systems
  58. Existence of positive periodic solutions for evolution equations with delay in ordered Banach spaces
  59. On a nonlinear boundary value problems with impulse action
  60. Normalized ground-states for the Sobolev critical Kirchhoff equation with at least mass critical growth
  61. Multiple positive solutions to a p-Kirchhoff equation with logarithmic terms and concave terms
  62. Infinitely many solutions for a class of Kirchhoff-type equations
  63. Real and non-real eigenvalues of regular indefinite Sturm–Liouville problems
  64. Existence of global solutions to a semilinear thermoelastic system in three dimensions
  65. Limiting profile of positive solutions to heterogeneous elliptic BVPs with nonlinear flux decaying to negative infinity on a portion of the boundary
  66. Morse index of circular solutions for repulsive central force problems on surfaces
  67. Differential Geometry
  68. On tangent bundles of Walker four-manifolds
  69. Pedal and negative pedal surfaces of framed curves in the Euclidean 3-space
  70. Discrete Mathematics
  71. Eventually monotonic solutions of the generalized Fibonacci equations
  72. Dynamical Systems Ergodic Theory
  73. Dynamical properties of two-diffusion SIR epidemic model with Markovian switching
  74. A note on weighted measure-theoretic pressure
  75. Pullback attractors for a class of second-order delay evolution equations with dispersive and dissipative terms on unbounded domain
  76. Pullback attractor of the 2D non-autonomous magneto-micropolar fluid equations
  77. Functional Analysis
  78. Spectrum boundary domination of semiregularities in Banach algebras
  79. Approximate multi-Cauchy mappings on certain groupoids
  80. Investigating the modified UO-iteration process in Banach spaces by a digraph
  81. Tilings, sub-tilings, and spectral sets on p-adic space
  82. Continuity and essential norm of operators defined by infinite tridiagonal matrices in weighted Orlicz and l spaces
  83. A family of commuting contraction semigroups on l 1 ( N ) and l ( N )
  84. q-Stirling sequence spaces associated with q-Bell numbers
  85. Chlodowsky variant of Bernstein-type operators on the domain
  86. Hyponormality on a weighted Bergman space of an annulus with a general harmonic symbol
  87. Characterization of derivations on strongly double triangle subspace lattice algebras by local actions
  88. Fixed point approaches to the stability of Jensen’s functional equation
  89. Geometry
  90. The regularity of solutions to the Lp Gauss image problem
  91. Solving the quartic by conics
  92. Group Theory
  93. On a question of permutation groups acting on the power set
  94. A characterization of the translational hull of a weakly type B semigroup with E-properties
  95. Harmonic Analysis
  96. Eigenfunctions on an infinite Schrödinger network
  97. Maximal function and generalized fractional integral operators on the weighted Orlicz-Lorentz-Morrey spaces
  98. Subharmonic functions and associated measures in ℝn
  99. Mathematical Logic, Model Theory and Foundation
  100. A topology related to implication and upsets on a bounded BCK-algebra
  101. Boundedness of fractional sublinear operators on weighted grand Herz-Morrey spaces with variable exponents
  102. Number Theory
  103. Fibonacci vector and matrix p-norms
  104. Recurrence for probabilistic extension of Dowling polynomials
  105. Carmichael numbers composed of Piatetski-Shapiro primes in Beatty sequences
  106. The number of rational points of some classes of algebraic varieties over finite fields
  107. Classification and irreducibility of a class of integer polynomials
  108. Decompositions of the extended Selberg class functions
  109. Joint approximation of analytic functions by the shifts of Hurwitz zeta-functions in short intervals
  110. Fibonacci Cartan and Lucas Cartan numbers
  111. Recurrence relations satisfied by some arithmetic groups
  112. The hybrid power mean involving the Kloosterman sums and Dedekind sums
  113. Numerical Methods
  114. A modified predictor–corrector scheme with graded mesh for numerical solutions of nonlinear Ψ-caputo fractional-order systems
  115. A kind of univariate improved Shepard-Euler operators
  116. Probability and Statistics
  117. Statistical inference and data analysis of the record-based transmuted Burr X model
  118. Multiple G-Stratonovich integral in G-expectation space
  119. p-variation and Chung's LIL of sub-bifractional Brownian motion and applications
  120. Real Analysis
  121. Chebyshev polynomials of the first kind and the univariate Lommel function: Integral representations
  122. Multiple solutions for a class of fourth-order elliptic equations with critical growth
  123. Majorization-type inequalities for (m, M, ψ)-convex functions with applications
  124. The evaluation of a definite integral by the method of brackets illustrating its flexibility
  125. Some new Fejér type inequalities for (h, g; α - m)-convex functions
  126. Some new Hermite-Hadamard type inequalities for product of strongly h-convex functions on ellipsoids and balls
  127. Topology
  128. Unraveling chaos: A topological analysis of simplicial homology groups and their foldings
  129. A generalized fixed-point theorem for set-valued mappings in b-metric spaces
  130. On SI2-convergence in T0-spaces
  131. Generalized quandle polynomials and their applications to stuquandles, stuck links, and RNA folding
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