Home Structure of coincidence isometry groups
Article Open Access

Structure of coincidence isometry groups

  • Guixin Deng and Jinxing Zhao EMAIL logo
Published/Copyright: December 31, 2021

Abstract

Let L be a lattice of rank n in an n -dimensional Euclidean space. We show that the coincidence isometry group of L is generated by coincidence reflections if and only if L contains an orthogonal subset of order n .

MSC 2010: 06B05; 20G99

1 Introduction

The theory of coincidence site lattice (CSL) gives partial answers to some questions that appeared in the physics of interfaces and grain boundaries, see [1,2]. The CSL theory mainly studies the coincidence problem between two lattices in a finite-dimensional Euclidean space. Several mathematical approaches were used in the study of this problem, including matrix theory, number theory, and geometric algebra, see [3,4, 5,6,7, 8,9,10, 11,12]. In this paper, we focus on the structure of the coincidence isometry group of a lattice in a finite-dimensional Euclidean space.

Let V be an n -dimensional Euclidean space and let α 1 , , α n be a basis of V . Let L = i = 1 n Z α i be the lattice generated by α 1 , , α n . A linear isometry A of V is called a coincidence isometry of L if L A ( L ) is a sublattice of L with finite index. The coincidence isometry group of L was introduced by Baake [1], which consists of all coincidence isometries of L . It is clear that an isometry A is a coincidence isometry of L if and only if the matrix of A with respect to α 1 , , α n is a rational matrix. It follows that the set of all coincidence isometries of L is a group which we denote by O C ( L ) .

Aragón et al. [3] and Rodríguez et al. [13] used geometric algebra as a tool in the study of the coincidence isometry group. In particular, the coincidence problem was completely solved in the planar case. They also found that coincidence reflections play an important role and conjectured that if L = Z n is the lattice spanned by the canonical basis in R n , then any coincidence isometry is a product of coincidence reflections. Zou in [14] showed that if the reflection defined by an arbitrary nonzero vector of L is a coincidence isometry of L , then any coincidence isometry of L is a product of coincidence reflections defined by the vectors of L . This result includes the conjecture as a special case and an algorithm to decompose a coincidence isometry into coincidence reflections was obtained. Zou also gave example to show that this result is not valid for any lattice. Huck [15] generalized this result to free modules over some subrings of R . In this paper, we show that for any lattice L of rank n in R n , any coincidence isometry of L is a product of coincidence reflections defined by the vectors of L if and only if L contains an orthogonal subset of order n .

In Section 2, we recall some relevant definitions and known results. In Section 3, we obtain many interesting properties of the coincidence reflections of a lattice. The main result is proved in Section 4. We also give a rough classification of coincidence isometry groups in dimension two of three. Section 5 is a concluding section.

2 Preliminaries

The set of integers, rational numbers and real numbers are denoted by Z , Q and R , respectively. For a ring R , the set of all m × n matrices over R is denoted by M m × n ( R ) . Let O ( V ) denote the group of orthogonal transformations of an Euclidean space V .

We recall some notations in linear algebra and the definition of lattice.

Definition 2.1

Let V be an n -dimensional Euclidean space.

  1. Two vectors α , β V are orthogonal, written α β , if ( α , β ) = 0 ;

  2. Two subsets X , Y V are orthogonal, written X Y , if ( α , β ) = 0 for all α X and β Y . We write α Y in place of { α } Y ;

  3. The orthogonal complement of a subset X is the set

    X { β V : β X } .

    We also write α instead of { α } ;

  4. A nonempty subset X of V is called an orthogonal set if 0 V and ( α , β ) = 0 for pairwise distinct vectors in X .

Since any n -dimensional Euclidean space is isomorphic to R n with the standard inner product, we only consider lattices in R n and we write vectors in R n as column vectors.

Definition 2.2

A discrete subset L of R n is a called a lattice of dimension d if it is a free abelian group spanned by a linearly independent set { α 1 , , α d } of R n . We always write it in the form i = 1 d Z α i . A sublattice L of L is also a free abelian group. Let [ L : L ] denote the index of L in L . Two lattices L 1 , L 2 of R n are called commensurate if both the indices [ L 1 : L 1 L 2 ] and [ L 2 : L 1 L 2 ] are finite.

Here we do not require that [ L : L ] is finite for a sublattice L of L . This is because we will study the relationship between the group of coincidence isometries of a lattice L and the group of coincidence isometries of a sublattice L of L having lower rank. Now we introduce the coincidence isometry group of a lattice.

Definition 2.3

Let L be a lattice of R n and let V be the Euclidean subspace of R n spanned by the elements in L . An orthogonal transformation A of V is called a coincidence isometry of L if [ L : L A L ] < . The set of all coincidence isometries of L is a subgroup of O ( V ) and is denoted by O C ( L ) .

Remark 2.1

Each subspace V of R n has a unique orthogonal complement V = { α R n : α V } such that R n = V V . There exists a canonical way to extend an isometry A of V to an isometry of R n :

A ( α + β ) = A ( α ) + β , α V , β V .

Hence, the coincidence isometry group O C ( L ) of a lattice in V can be viewed as a subgroup of O ( R n ) .

Theorem 2.1

[16, Theorem 1] Let L 1 = i = 1 n Z α i and L 2 = i = 1 n Z β i be two lattices in R n . Then the following are equivalent.

  1. L 1 and L 2 are commensurate;

  2. The transition matrix from α 1 , , α n to β 1 , , β n is a rational matrix;

  3. i = 1 n Q α i = i = 1 n Q β i .

Lemma 2.1

Let L 1 = i = 1 n Z α i , L 2 = i = 1 n Z β i be two lattices of R n . If ( β 1 , , β n ) = ( α 1 , , α n ) P and P is a non-singular rational matrix, then O C ( L 1 ) = O C ( L 2 ) .

Proof

It follows immediately from Theorem 2.1 and Lemma 7.2 of [5].□

By Grimmer’s theorem, we see that the coincidence isometry group of lattice with basis α 1 , , α n consists precisely of the isometries whose matrices with respect to the basis α 1 , , α n are rational matrices.

Lemma 2.2

Suppose that a lattice L of R n is the orthogonal direct sum of sublattices L 1 and L 2 . Then O C ( L 1 ) O C ( L 2 ) is isomorphic to a subgroup of O C ( L ) .

Proof

Without loss of generality, we may assume that L is n -dimensional, L 1 = i = 1 r Z α i and L 2 = i = r + 1 n Z α i . Let V 1 = i = 1 r R α i and V 2 = i = r + 1 n R α i be the respective R -subspaces of R n spanned by the basis vectors of L 1 and L 2 . It is routine to check that the following map

( A 1 , A 2 ) A , A ( α 1 + α 2 ) = A 1 ( α 1 ) + A 2 ( α 2 )

is an injective group homomorphism from O C ( L 1 ) O C ( L 2 ) to O ( R n ) . It remains to show that A O C ( L ) . Let A 1 be the matrix of A 1 (viewed as an element of O ( V 1 ) ) with respect to the basis α 1 , , α r and A 2 be the matrix of A 2 (viewed as an element of O ( V 2 ) ) with respect to the basis α r + 1 , , α n . Then the matrix of A with respect to the basis α 1 , , α n is the quasi-diagonal matrix diag ( A 1 , A 2 ) . Since A i is a coincidence isometry, A i is a rational matrix and is also A . Hence, A is a coincidence isometry of L .□

We need the following result proved by Zou.

Theorem 2.2

[14, Theorem 3.1 and Theorem 3.2] Let L = i = 1 n Z α i be a lattice of R n . Then every non-zero vector of L defines a coincidence reflection of L if and only if ( α i , α j ) ( α k , α k ) are all rational for all 1 i , j , k n . Moreover, in this case any coincidence isometry of L is a product of at most n reflections defined by the vectors in L .

3 Reflections in the coincidence isometry group

The well-known Cartan-Dieudonné theorem states that any isometry in O ( R n ) is the product of at most n reflections. It was found that the coincidence reflections of a lattice L play an important role in the structure of O C ( L ) , see [10] and [14]. In this section, we obtain many interesting properties of a coincidence reflection in the coincidence isometry group. For any nonzero vector v V , let v denote the reflection defined by v , i.e. v ( α ) = α 2 ( v , α ) ( v , v ) v .

Lemma 3.1

Let L = i = 1 n Z α i be a lattice of R n . Suppose that v O C ( L ) . Then there exists a linearly independent subset { β 1 , , β n } of L such that β 1 is parallel to v and ( β 1 , β i ) = 0 for i > 1 .

Proof

We put the proof in the appendix.□

Corollary 3.1

Let L = i = 1 n Z α i be a lattice of R n and let S = { v i = 1 n Q α i : v 0 , v O C ( L ) } . Then S is an invariant set of any A O C ( L ) , that is, A ( v ) S for any A O C ( L ) and v S .

Proof

By Lemma 3.1, there exists a linearly independent subset { β 1 , , β n } of L such that β 1 is parallel to v S and ( β 1 , β i ) = 0 for i > 1 . It suffices to show that A ( β 1 ) S . In fact, let γ i = A ( β i ) , L 1 = i = 1 n Z β i and L 2 = i = 1 n Z γ i . Since A is an isometry, one has ( γ 1 , γ i ) = 0 for i > 1 . It follows that γ 1 ( γ 1 ) = γ 1 and γ 1 ( γ i ) = γ i for i > 1 . Hence, γ 1 is a coincidence reflection of L 2 . Since L and L 2 are commensurate, we have γ 1 O C ( L 2 ) = O C ( L ) by Lemma 2.1. This finishes the proof.□

Lemma 3.2

Let L = i = 1 n Z α i be a lattice of R n . Let V 1 = i = 1 r R α i and V 2 = i = r + 1 n R α i . Suppose that V 1 V 2 . Let v = v 1 + v 2 , 0 v i V i . If v O C ( L ) , then v i O C ( L ) .

Proof

We put the proof in the appendix.□

Lemma 3.3

Let L = i = 1 n Z α i be a lattice of R n and let V = i = 1 n Q α i . Suppose that { v 1 , , v r } is a linearly independent subset of V such that v i O C ( L ) . Applying the Gram-Schmidt orthogonalization process to v 1 , , v r gives that

w 1 = v 1 , w i = v i j = 1 i 1 ( v i , w j ) ( w j , w j ) w j , f o r i = 2 , , r .

Then w i V and w i O C ( L ) for i = 1 , , r .

Proof

We put the proof in the appendix.□

The following theorem is part of the main result.

Theorem 3.1

Let L = i = 1 n Z α i be a lattice of R n and let r be dimension of the Q -space spanned by { v L : v O C ( L ) } . Then

  1. r n 1 .

  2. If 1 r n 2 , then there exist two orthogonal sublattices L 1 of dimension r and L 2 of dimension n r such that O C ( L ) = O C ( L 1 ) O C ( L 2 ) , and O C ( L ) is not generated by the reflections.

Proof

Let V = i = 1 n Q α i and V 1 be the Q -subspace of V spanned by { v L : v O C ( L ) } . Suppose that w 1 , , w r is a basis of V 1 . By Lemmas 3.3 and 3.1, we may assume that { w 1 , , w r } is orthogonal subset of L . By Lemma 3.1 again, W j = { α V : ( α , w j ) = 0 } is an ( n 1 ) -dimensional subspace of V . Let V 2 = j = 1 r W j . Then V 2 is the orthogonal complement of V 1 in the Q -space V and V = V 1 V 2 . Choosing a basis { w r + 1 , , w n } L of V 2 . Then L 1 = i = 1 r Z w i and L 2 = i = r + 1 n Z w i are orthogonal sublattices of L . Since { w 1 , , w n } is a linearly independent subset of V = i = 1 n Q α i , we have V = i = 1 n Q w i and L is commensurate to L = L 1 L 2 by Theorem 2.1. So we have O C ( L ) = O C ( L ) by Lemma 2.1.

If r = n 1 , then { w 1 , , w n 1 , w n } is an orthogonal basis of L . Thus, w n O C ( L ) = O C ( L ) , which is a contradiction. This proves (1).

Let A O C ( L ) . By Corollary 3.1, the reflection defined by A ( w j ) is also a coincidence isometry of L for j = 1 , , r . It follows that A ( w j ) V 1 and V 1 is an A -invariant subspace of V . Since V 1 V 2 and A is an isometry, V 2 is also an A -invariant subspace of V . It follows that the group homomorphism defined in Lemma 2.2 is an isomorphism in this case.

If v is a coincidence isometry of L defined by a vector v L , then v V 1 by hypothesis. Since V 1 V 2 , it follows that v V 2 = I , and is also for any coincidence isometry which is a product of reflections. Hence, I is not contained in the subgroup of O C ( L ) generated by reflections.□

Corollary 3.2

Let L be an n -dimensional lattice of R n . Suppose that 0 X L and O C ( L ) is generated by the reflections defined by the vectors of X . Then X n .

Proof

Suppose to the contrary that X < n . Let { v 1 , , v r } be a maximal linearly independent subset of X , r X < n . Since O C ( L ) is generated by reflections, by Theorem 3.1 there exist vectors v r + 1 , , v n { v L : v O C ( L ) } such that { v 1 , , v n } is linearly independent. By Lemma 3.3, applying the Gram-Schmidt orthogonalization process to v 1 , , v n , we obtain an orthogonal set { w 1 , , w n } such that w i O C ( L ) . Since X i = 1 r Q v i = i = 1 r Q w i , so w n X . It follows that v ( w n ) = w n for any v X , and is also for any coincidence isometry of L . This contradicts w n O C ( L ) .□

4 Main results

In this section, we present our main result. We first give a criterion so that a reflection is a coincidence isometry.

Lemma 4.1

Let α R n be a nonzero vector. Then α has a basis consisting of vectors in Q n if and only if α is parallel to a nonzero vector of Q n .

Proof

We put the proof in the appendix.□

Theorem 4.1

Let L = i = 1 n Z α i be a lattice in R n and let G = ( ( α i , α j ) ) be the Gram matrix of α 1 , , α n . Let v = i = 1 n k i α i be a non-zero vector of L . Then v O C ( L ) if and only if G ( k 1 , , k n ) T is parallel to a nonzero vector in Q n .

Proof

Let B = ( k 1 , , k n ) T . First assume that v O C ( L ) . By Lemma 3.1, there exists a linearly independent subset { β 1 , , β n } of i = 1 n Q α i such that β 1 = v and ( β 1 , β i ) = 0 for i > 1 . Suppose β i = j = 1 n b i j α j . By the property of Gram matrix, we have for i > 1 ,

B i G B = ( β i , β 1 ) = 0 ,

where B i = ( b i 1 , , b i n ) . By Lemma 4.1, G B is parallel to a nonzero vector in Q n .

Now suppose that G B = r C and C Q n . By Lemma 4.1, there exist n 1 linearly independent row vectors C 1 = ( a 11 , , a 1 n ) , , C n 1 = ( a n 1 , 1 , , a n 1 , n ) such that C i Q n and C i G B = 0 . Set v i = j = 1 n a i j α j i = 1 n Q α i . Then { v 1 , , v n 1 } is also linearly independent and

( v i , v ) = C i G B = 0

by the property of Gram matrix again. We observe that v 1 , , v n 1 , v n = v is a basis of i = 1 n Q α i , and v O C ( i = 1 n Z v i ) = O C ( L ) by Lemma 2.1.□

The following result is an immediate consequence of Theorem 4.1.

Corollary 4.1

Let L = i = 1 n Z α i be a lattice in R n with an orthogonal basis α 1 , , α n . Suppose that v = i = 1 n k i α i L is a nonzero vector and S = { i : k i 0 } . Then v O C ( L ) if and only if ( α i , α i ) ( α j , α j ) Q for any i , j S .

We define a relation Q on the set of nonzero vectors in R n such that α Q β if ( α , α ) ( β , β ) Q . This is clearly an equivalence relation. Now we state and prove our main result.

Theorem 4.2

Let L = i = 1 n Z α i be a lattice in R n and let L be the sublattice of L spanned by a maximal orthogonal subset of { v L : v O C ( L ) } . Then the following are equivalent.

  1. L contains an orthogonal subset of order n ;

  2. dim L = n ;

  3. Any coincidence isometry of L can be decomposed as a product of at most n reflections defined by the vectors in L .

Proof

( 1 ) ( 2 ) Suppose that { w 1 , , w n } is an orthogonal subset of L . Then { w 1 , , w n } is linearly independent and L is commensurate to L = i = 1 n Z w i by Theorem 2.1. Hence, w i O C ( L ) = O C ( L ) by Lemma 2.1 and we have dim L = n .

( 2 ) ( 1 ) is trivial.

( 3 ) ( 1 ) follows from Theorem 3.1 and Lemma 3.3.

( 1 ) ( 3 ) Without loss of generality we may assume that α 1 , , α n is an orthogonal basis of L . Let V = i = 1 n Q α i . Suppose that { α 1 , , α n } = i = 1 r X i be the partition corresponding to the equivalence relation Q restricted on { α 1 , , α n } . Let L i = γ X i Z γ , V i = γ X i Q γ and W i = γ X i R γ be the sublattice of L , the Q -subspace of V and the R -subspace of R n generated by the elements of X i , respectively. Then L = i = 1 r L i . Let α , β V be two nonzero vectors.

We claim that:

  1. If α , β V i for some i { 1 , , r } , then ( α , α ) ( β , β ) Q ;

  2. If α V i , β V j and i j , then ( α , α ) ( β , β ) Q .

Suppose α = α k X i l k α k V i and β = α k X j m k α k V j , where l k , m k Q . Fix α X i and β X j . If i = j , then

( α , α ) ( β , β ) = α k X i l k 2 ( α k , α k ) α k X i m k 2 ( α k , α k ) = l k 2 s k m k 2 s k Q ,

where s k = ( α k , α k ) ( α , α ) Q . This proves claim ( 1 ) . If i j , then α Q β by the construction of the partition of { α 1 , , α n } = i = 1 r X i . By claim ( 1 ) , we have α Q α and β Q β . Since Q is an equivalence relation, one has α Q β . This proves claim ( 2 )

By Corollary 4.1, for any nonzero vector w L , w O C ( L ) if and only if w L i for some i . Now choose a nonzero vector v L i and A O C ( L ) . By Corollary 3.1, there exists an index j such that A ( v ) V j . Since A is an isometry, one has ( v , v ) = ( A ( v ) , A ( v ) ) . By claim ( 2 ) , we have i = j . This shows that A ( V i ) = V i , A ( W i ) = W i and A W i is a coincidence isometry of the lattice L i considered in the subspace W i . It follows that

O C ( L ) O C ( L 1 ) O C ( L 2 ) O C ( L r ) ,

and A = A 1 A 2 A r , where A i W i = A W i and A i W j = I for i j .

By Theorem 2.2, each A i is a product of at most X i reflections defined by the vectors in L i , and hence A is a product of at most i = 1 r X i = n reflections defined by the vectors in L . The proof is complete.□

Corollary 4.2

With the same notations in the above theorem. The subgroup of O C ( L ) generated by coincidence reflections is isomorphic to O C ( L ) .

Proof

It follows immediately from Theorems 4.2 and 2.2.□

Remark 4.1

Now we compare our main result and Theorem 2.2 by Zou. Let L be a lattice of rank n in R n . Set

  1. ( α , α ) ( β , β ) Q for any nonzero vectors α , β L ;

  2. Every nonzero vector of L defines a coincidence reflection of L ;

  3. Any coincidence isometry of L is a product of at most n reflections defined by the vectors in L ;

  4. L contains an orthogonal subset of order n .

Then Theorem 2.2 states that

( 1 ) ( 2 ) ( 3 ) ,

and Theorem 4.2 states that

( 3 ) ( 4 ) ( 2 ) .

Let L = Z α 1 Z α 2 be the lattice, where α 1 = ( a , 0 ) T , α 2 = ( 1 , b ) T . Zou [14] showed that one of the following is satisfied:

  1. If a , b 2 Q , then every non-zero vector of L defines a coincidence reflection of L and O C ( L ) is generated by these reflections;

  2. If a Q but b 2 Q , then O C ( L ) = { ± I , ± α 1 } Z 2 2 ;

  3. If a Q but a 1 + b 2 Q , then O C ( L ) = { ± I , ± α 2 } Z 2 2 ;

  4. If a , a 1 + b 2 Q , then O C ( L ) = { ± I } Z 2 .

This example also shows that ( 3 ) ( 2 ) in Remark 4.1. It should be mentioned that the coincidence problem was completely solved in the planar case by using Clifford Algebra, see [13]. We give a rough classification of the coincidence isometry groups in two and three dimensional based on our main result. We also put the proof of the following two examples in the appendix.

Example 4.1

Let L = Z α 1 Z α 2 be a lattice in R 2 . Then one of the following is satisfied.

  1. There are no reflections in O C ( L ) and O C ( L ) = { ± I } Z 2 ;

  2. There are exactly two reflections v 1 , v 2 in O C ( L ) and O C ( L ) = { ± I , v 1 , v 2 } Z 2 2 ;

  3. Each vector in L defines a coincidence reflection of L and O C ( L ) is generated by coincidence reflections.

Example 4.2

Let L = i = 1 3 Z α i be a lattice in R 3 . Suppose that X is a maximal orthogonal subset of { v L : v O C ( L ) } . Then exactly one of the following is satisfied.

  1. X = and O C ( L ) = { ± I } Z 2 ;

  2. X = { v } and O C ( L ) = { ± I , ± v } Z 2 2 ;

  3. X = { v 1 , v 2 , v 3 } and one of the following holds:

    1. Neither ( v 1 , v 1 ) ( v 2 , v 2 ) nor ( v 2 , v 2 ) ( v 3 , v 3 ) is rational, O C ( L ) = { ± I , ± v 1 , ± v 2 , ± v 3 } Z 2 3 ;

    2. ( v 1 , v 1 ) ( v 2 , v 2 ) Q and ( v 2 , v 2 ) ( v 3 , v 3 ) Q , O C ( L ) O C ( Z v 1 Z v 2 ) Z 2 , where every nonzero vector of L = Z v 1 Z v 2 defines a coincidence reflection of L ;

    3. Both ( v 1 , v 1 ) ( v 2 , v 2 ) and ( v 2 , v 2 ) ( v 3 , v 3 ) are rational, and every nonzero vector of L defines a coincidence reflection of L .

5 Concluding remark

In this work, we focus on the structure of coincidence isometry groups of lattices in R n . We obtain a necessary and sufficient condition for an arbitrary coincidence isometry of certain lattices L to be a product of at most n coincidence reflections defined by the vectors of L . In particular, we show that if L has an orthogonal basis, then there exists an orthogonal decomposition of L = i = 1 r L i into its sublattices such that O C ( L ) i = 1 r O C ( L i ) , where v O C ( L ) if and only if v L i for some i .

Acknowledgements

The authors thank the referee(s) for reading the manuscript very carefully and making a number of valuable and kind comments which improved the presentation.

  1. Funding information: This research was supported by the National Natural Science Foundation of China (11801104, 11961050, 12161062) and Inner Mongolia Natural Science Foundation (2018MS01017, 2021MS01005).

  2. Conflict of interest: Authors state no conflict of interest.

  3. Data availability statement: No data were used to support this study.

Appendix A.1 Proof of Lemma 3.1

Let v = i = 1 n x i α i , x i R . Since v ( α j ) = α j 2 ( α j , v ) ( v , v ) i = 1 n x i α i , it follows that x i ( α j , v ) ( v , v ) Q for any i , j { 1 , , n } . Without loss of generality, we may assume that x i ( α 1 , v ) 0 . It follows that for j i

x j x i = x j ( α 1 , v ) ( v , v ) ( v , v ) x i ( α 1 , v ) Q .

Choose m Z such that m x j x i Z for all j { 1 , , n } , then β 1 = m x i v L .

We also have

( α j , v ) ( α 1 , v ) = x i ( α j , v ) ( v , v ) ( v , v ) x i ( α 1 , v ) = q j Q ,

and thus β 1 α j q j α 1 for j = 2 , , n . There exists a nonzero integer m 1 such that m 1 q j Z for all j { 2 , , n } . Let β j = m 1 ( α j q j α 1 ) . Then { β 1 , , β n } is a linearly independent subset of L and β 1 β i for i > 1 . The proof is complete.

A.2 Proof of Lemma 3.2

By Lemma 3.1, after a scalar multiplication we may assume that v = i = 1 n k i α i L . It suffices to show that v 2 O C ( L ) . Since v O C ( L ) , one has ( α i , v ) ( v , v ) Q for all i { 1 , , n } . Since V 1 V 2 , we have

( v 2 , v 2 ) ( v , v ) = ( v 2 , v ) ( v , v ) = i = r + 1 n k i ( α i , v ) ( v , v ) Q .

Note that v 2 ( α j ) = α j for 1 j r and for j r + 1 ,

( α j , v 2 ) ( v 2 , v 2 ) = ( α j , v ) ( v 2 , v 2 ) = ( α j , v ) ( v , v ) ( v , v ) ( v 2 , v 2 ) Q .

It follows that v 2 O C ( L ) .

A.3 Proof of Lemma 3.3

We induct on i . Suppose that w j V and w j O C ( L ) for any j i 1 . Then ( v i , w j ) ( w j , w j ) Q and w i = v i u V , where u = j = 1 i 1 ( v i , w j ) ( w j , w j ) w j . Since w j O C ( L ) , by Lemma 3.1, W j = { α V : ( α , w j ) = 0 } is an ( n 1 ) -dimensional Q -subspace of V . Set V 1 = j = 1 i 1 Q w j and V 2 = j = 1 i 1 W j . Then V = V 1 V 2 is an orthogonal direct sum. We have v i = w i + u , where u V 1 and w i V 2 . By Lemma 3.2, we obtain that w i O C ( L ) .

B.1 Proof of Lemma 4.1

If α = r β , β Q n , r R { 0 } , then by the standard result of solution of system of linear equations there exists a Q -linearly independent subset { β 1 , , β n 1 } of Q n with that ( α , β i ) = 0 , and it is also linearly independent over R and consists of a basis of α .

Conversely, suppose β 1 , , β n 1 is a basis of α such that β i Q n . Without loss of generality we may assume that α = ( p 1 , , p n ) with p n 0 . It suffices to show that p i p n Q . Since

γ 1 = 1 0 0 p 1 p n , γ 2 = 0 1 0 p 2 p n , , γ n 1 = 0 0 1 p n 1 p n

is also a basis of α , there exists an invertible matrix A = ( a i j ) M n 1 ( R ) such that

( β 1 , , β n 1 ) = ( γ 1 , , γ n 1 ) A = I n 1 P A = A P A ,

where P = ( p 1 p n , , p n 1 p n ) . Hence, A M n 1 ( Q ) , P A M 1 × ( n 1 ) ( Q ) , and we obtain P = ( P A ) A 1 M 1 × ( n 1 ) ( Q ) . This finishes the proof.

B.2 Proof of Example 4.1

Let ( α 1 , α 2 ) = a b c d = A . It is well known that each linear isometry of R 2 is either a reflection or a rotation, see [17]. Let T θ denote the rotation through the angle θ . If T θ O C ( L ) for some θ 0 , π , then

B = A 1 cos θ sin θ sin θ cos θ A = 1 det A det A cos θ ( a b + c d ) sin θ ( b 2 + d 2 ) sin θ ( a 2 + c 2 ) sin θ det A cos θ + ( a b + c d ) sin θ

is a rational matrix. It follows that cos θ Q and

a b + c d a 2 + c 2 = ( α 1 , α 2 ) ( α 1 , α 1 ) Q , a 2 + c 2 b 2 + d 2 = ( α 1 , α 1 ) ( α 2 , α 2 ) Q .

By Theorem 2.2, any reflection defined by the vectors in L is a coincidence isometry, in this case Statement (3) holds.

Let us now assume that T θ O C ( L ) for any θ 0 , π . If in addition O C ( L ) contains no reflection, then O C ( L ) = { T 0 , T π } = { ± I } . If O C ( L ) contains a reflection v 1 , v 1 L , then by Theorem 4.2 there exists v 1 , v 2 L with ( v 1 , v 2 ) = 0 and ( v 1 , v 1 ) ( v 2 , v 2 ) Q . Hence, Statement ( 2 ) is satisfied.

B.3 Proof of Example 4.2

We have X = 0 , 1 , or 3 by Theorem 3.1. Statement ( 3 ) follows immediately from Theorem 2.2 and Theorem 4.2.

We claim that: if A is a coincidence isometry of L and A ± I , then there exists an eigenvector v of A such that v O C ( L ) .

Let f ( x ) Q [ x ] be the characteristic polynomial of A . Since deg f ( x ) = 3 and A is an orthogonal transformation, f ( x ) has a real root t { 1 , 1 } . If A is diagonalizable, then f ( x ) = ( x + 1 ) ( x 1 ) 2 or ( x 1 ) 2 ( x + 1 ) , if A is not diagonalizable, then f ( x ) = ( x t ) g ( x ) , where g ( x ) is irreducible over R . In both cases, there is a factorization of f ( x ) = ( x t ) h ( x ) such that gcd ( x t , h ( x ) ) = 1 . Let V = i = 1 3 Q α i . By the primary decomposition of A V , see [18], we have V = V 1 V 2 , where V 1 = ker ( A t I ) V and V 2 = ker h ( A ) V , and both V 1 and V 2 are A -invariant spaces. We will show that V 1 V 2 . Since A is an isometry, we have ( v 1 , v 2 ) = ( A ( v 1 ) , A ( v 2 ) ) = ( t v 1 , A ( v 2 ) ) = ( v 1 , t A ( v 2 ) ) for any v 1 V 1 and v 2 V 2 . Since t = ± 1 , we have ( v 1 , ( t A I ) ( v 2 ) ) = 0 = ( v 1 , ( A t I ) ( v 2 ) ) . Note that ( A t I ) V 2 is an invertible linear transformation, we obtain v 1 V 2 . Since dim V 1 = 1 , v 1 is a coincidence reflection. This proves the claim.

Statement ( 1 ) is an immediate consequence of the claim. It remains to prove Statement ( 2 ) . If X = { v } , then O C ( L ) contains a unique reflection v . By Lemma 3.1 and Theorem 2.1, there exists a linearly independent subset { w 1 , w 2 } of L such that ( v , w 1 ) = ( v , w 2 ) = 0 and L is commensurate to L = Z v Z w 1 Z w 2 . Let W = R w 1 R w 2 . By the claim, v is a common eigenvector of all coincidence isometries of L . Thus, A ( v ) = ± v and A W is a coincidence isometry of the lattice Z w 1 Z w 2 . Since v W , we see that if α W is a coincidence reflection of Z w 1 Z w 2 for some nonzero vector α W , then α is also a coincidence reflection of L . Therefore, O C ( Z w 1 Z w 2 ) has no reflection by the hypothesis X = { v } is a maximal orthogonal subset of { v L : v O C ( L ) = O C ( L ) } . From Example 4.1, we have shown that A W = ± I for any A O C ( L ) . That is, O C ( L ) = { I , I , v , v } and the matrices of these isometries with respect to the ordered basis v , w 1 , w 2 are

1 0 0 0 1 0 0 0 1 , 1 0 0 0 1 0 0 0 1 , 1 0 0 0 1 0 0 0 1 , 1 0 0 0 1 0 0 0 1 ,

respectively.

References

[1] M. Baake, M. Birkner, and U. Grimm, Non-Periodic Systems with Continuous Diffraction Measures, in: The Mathematics of Aperiodic Order, R. V. Moody, (ed.), 9–44, Kluwer Academic Publishers, Dordrecht, 1997. 10.1007/978-3-0348-0903-0_1Search in Google Scholar

[2] W. Bollmann, Crystal Defects and Crystalline Interfaces, Berlin: Springer, 1970. 10.1007/978-3-642-49173-3Search in Google Scholar

[3] G. Aragón, J. L. Aragón, F. Dávila, Z. Gómez, and M. A. Rodríguez, Modern geometric calculations in crystallography, in: E. Bayro Corrochano, G. Sobczyk (eds.), Geometric Algebra with Applications in Science and Engineering, Birkhaüser, Boston, 2001, pp. 371–386. 10.1007/978-1-4612-0159-5_18Search in Google Scholar

[4] M. Baake, U. Grimm, M. Heuer, and P. Zeiner, Coincidence rotations of the root lattice A4, European J. Combin. 29 (2008), no. 8, 1808–1819, https://doi.org/10.1016/j.ejc.2008.01.012. Search in Google Scholar

[5] M. Baake and P. Zeiner, Geometric enumeration problems for lattices and embedded Z-modules, in: M. Baake and U. Grimm (eds.), Aperiodic Order (Encyclopedia of Mathematics and its Applications), Cambridge University Press, Cambridge, 2017, pp. 73–172, https://doi.org/10.1017/9781139033862.005. Search in Google Scholar

[6] M. A. Fortes, Crystallographic applications of the elementary divisor theorem, Acta Cryst. 39 (1983), 348–350, https://doi.org/10.1107/S0108767383000781. Search in Google Scholar

[7] H. Grimmer, The generating function for coincidence site lattices in the cubic system, Acta Cryst. A40 (1984), 108–112, https://doi.org/10.1107/S0108767384000246. Search in Google Scholar

[8] P. A. B. Pleasants, M. Baake, and J. Roth, Planar coincidence for N-fold symmetry, J. Math. Phys. 37 (1996), 1029–1058. 10.1063/1.531424Search in Google Scholar

[9] S. Ranganathan, On the geometry of coincidence-site lattices, Acta Cryst. 21 (1966), 197–199, https://doi.org/10.1107/S0365110X66002615. 10.1107/S0365110X66002615Search in Google Scholar

[10] M. A. Rodríguez-Andrade, G. Aragón-González, J. L. Aragón, A. Goméz-Rodríguez, and D. Romeu, The coincidence site Lattices in 2D hexagonal lattices using Clifford algebra, Adv. Appl. Clifford Algebr. 25 (2015), 425–440, https://doi.org/10.1007/s00006-014-0508-7. Search in Google Scholar

[11] P. Zeiner, Multiplicativity in the theory of coincidence site lattices, J. Phys.: Conf. Ser. 226 (2010), 012025, https://doi.org/10.1088/1742-6596/226/1/012025. Search in Google Scholar

[12] P. Zeiner, Similar submodules and coincidence site modules, Acta Phys. Polon. A 126 (2014), no. 2, 641–644, http://dx.doi.org/10.12693/APhysPolA.126.641. Search in Google Scholar

[13] M. A. Rodríguez, J. L. Aragón, and L. Verde-Star, Clifford algebra approach to the coincidence problem for planar lattices, Acta Cryst. A61 (2005), 173–184, https://doi.org/10.1107/S0108767304025358. Search in Google Scholar PubMed

[14] Y. Zou, Structure of coincidence symmetry groups, Acta Cryst. A62 (2006), 109–114, https://doi.org/10.1107/S0108767305033489. 10.1107/S0108767305033489Search in Google Scholar PubMed

[15] C. Huck, A note on coincidence isometries of modules in Euclidean space, Zeitschrift für Kristallographie 224 (2009), no. 7, 341–344, https://doi.org/10.1524/zkri.2009.1148. Search in Google Scholar

[16] H. Grimmer, Coincidence-site lattices, Acta Cryst. A32 (1976), 783–785, https://doi.org/10.1107/S056773947601231X. 10.1107/S056773947601231XSearch in Google Scholar

[17] M. Artin, Algebra, Prentice Hall, New Jersey, 1991. Search in Google Scholar

[18] S. Roman, Advanced Linear Algebra, Third Edition, Springer-Verlag, New York, 2008. 10.1007/978-0-387-72831-5Search in Google Scholar

Received: 2020-09-25
Revised: 2021-08-14
Accepted: 2021-08-19
Published Online: 2021-12-31

© 2021 Guixin Deng and Jinxing Zhao, published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

Articles in the same Issue

  1. Regular Articles
  2. Sharp conditions for the convergence of greedy expansions with prescribed coefficients
  3. Range-kernel weak orthogonality of some elementary operators
  4. Stability analysis for Selkov-Schnakenberg reaction-diffusion system
  5. On non-normal cyclic subgroups of prime order or order 4 of finite groups
  6. Some results on semigroups of transformations with restricted range
  7. Quasi-ideal Ehresmann transversals: The spined product structure
  8. On the regulator problem for linear systems over rings and algebras
  9. Solvability of the abstract evolution equations in Ls-spaces with critical temporal weights
  10. Resolving resolution dimensions in triangulated categories
  11. Entire functions that share two pairs of small functions
  12. On stochastic inverse problem of construction of stable program motion
  13. Pentagonal quasigroups, their translatability and parastrophes
  14. Counting certain quadratic partitions of zero modulo a prime number
  15. Global attractors for a class of semilinear degenerate parabolic equations
  16. A new implicit symmetric method of sixth algebraic order with vanished phase-lag and its first derivative for solving Schrödinger's equation
  17. On sub-class sizes of mutually permutable products
  18. Asymptotic solution of the Cauchy problem for the singularly perturbed partial integro-differential equation with rapidly oscillating coefficients and with rapidly oscillating heterogeneity
  19. Existence and asymptotical behavior of solutions for a quasilinear Choquard equation with singularity
  20. On kernels by rainbow paths in arc-coloured digraphs
  21. Fully degenerate Bell polynomials associated with degenerate Poisson random variables
  22. Multiple solutions and ground state solutions for a class of generalized Kadomtsev-Petviashvili equation
  23. A note on maximal operators related to Laplace-Bessel differential operators on variable exponent Lebesgue spaces
  24. Weak and strong estimates for linear and multilinear fractional Hausdorff operators on the Heisenberg group
  25. Partial sums and inclusion relations for analytic functions involving (p, q)-differential operator
  26. Hodge-Deligne polynomials of character varieties of free abelian groups
  27. Diophantine approximation with one prime, two squares of primes and one kth power of a prime
  28. The equivalent parameter conditions for constructing multiple integral half-discrete Hilbert-type inequalities with a class of nonhomogeneous kernels and their applications
  29. Boundedness of vector-valued sublinear operators on weighted Herz-Morrey spaces with variable exponents
  30. On some new quantum midpoint-type inequalities for twice quantum differentiable convex functions
  31. Quantum Ostrowski-type inequalities for twice quantum differentiable functions in quantum calculus
  32. Asymptotic measure-expansiveness for generic diffeomorphisms
  33. Infinitesimals via Cauchy sequences: Refining the classical equivalence
  34. The (1, 2)-step competition graph of a hypertournament
  35. Properties of multiplication operators on the space of functions of bounded φ-variation
  36. Disproving a conjecture of Thornton on Bohemian matrices
  37. Some estimates for the commutators of multilinear maximal function on Morrey-type space
  38. Inviscid, zero Froude number limit of the viscous shallow water system
  39. Inequalities between height and deviation of polynomials
  40. New criteria-based ℋ-tensors for identifying the positive definiteness of multivariate homogeneous forms
  41. Determinantal inequalities of Hua-Marcus-Zhang type for quaternion matrices
  42. On a new generalization of some Hilbert-type inequalities
  43. On split quaternion equivalents for Quaternaccis, shortly Split Quaternaccis
  44. On split regular BiHom-Poisson color algebras
  45. Asymptotic stability of the time-changed stochastic delay differential equations with Markovian switching
  46. The mixed metric dimension of flower snarks and wheels
  47. Oscillatory bifurcation problems for ODEs with logarithmic nonlinearity
  48. The B-topology on S-doubly quasicontinuous posets
  49. Hyers-Ulam stability of isometries on bounded domains
  50. Inhomogeneous conformable abstract Cauchy problem
  51. Path homology theory of edge-colored graphs
  52. Refinements of quantum Hermite-Hadamard-type inequalities
  53. Symmetric graphs of valency seven and their basic normal quotient graphs
  54. Mean oscillation and boundedness of multilinear operator related to multiplier operator
  55. Numerical methods for time-fractional convection-diffusion problems with high-order accuracy
  56. Several explicit formulas for (degenerate) Narumi and Cauchy polynomials and numbers
  57. Finite groups whose intersection power graphs are toroidal and projective-planar
  58. On primitive solutions of the Diophantine equation x2 + y2 = M
  59. A note on polyexponential and unipoly Bernoulli polynomials of the second kind
  60. On the type 2 poly-Bernoulli polynomials associated with umbral calculus
  61. Some estimates for commutators of Littlewood-Paley g-functions
  62. Construction of a family of non-stationary combined ternary subdivision schemes reproducing exponential polynomials
  63. On the evolutionary bifurcation curves for the one-dimensional prescribed mean curvature equation with logistic type
  64. On intersections of two non-incident subgroups of finite p-groups
  65. Global existence and boundedness in a two-species chemotaxis system with nonlinear diffusion
  66. Finite groups with 4p2q elements of maximal order
  67. Positive solutions of a discrete nonlinear third-order three-point eigenvalue problem with sign-changing Green's function
  68. Power moments of automorphic L-functions related to Maass forms for SL3(ℤ)
  69. Entire solutions for several general quadratic trinomial differential difference equations
  70. Strong consistency of regression function estimator with martingale difference errors
  71. Fractional Hermite-Hadamard-type inequalities for interval-valued co-ordinated convex functions
  72. Montgomery identity and Ostrowski-type inequalities via quantum calculus
  73. Universal inequalities of the poly-drifting Laplacian on smooth metric measure spaces
  74. On reducible non-Weierstrass semigroups
  75. so-metrizable spaces and images of metric spaces
  76. Some new parameterized inequalities for co-ordinated convex functions involving generalized fractional integrals
  77. The concept of cone b-Banach space and fixed point theorems
  78. Complete consistency for the estimator of nonparametric regression model based on m-END errors
  79. A posteriori error estimates based on superconvergence of FEM for fractional evolution equations
  80. Solution of integral equations via coupled fixed point theorems in 𝔉-complete metric spaces
  81. Symmetric pairs and pseudosymmetry of Θ-Yetter-Drinfeld categories for Hom-Hopf algebras
  82. A new characterization of the automorphism groups of Mathieu groups
  83. The role of w-tilting modules in relative Gorenstein (co)homology
  84. Primitive and decomposable elements in homology of ΩΣℂP
  85. The G-sequence shadowing property and G-equicontinuity of the inverse limit spaces under group action
  86. Classification of f-biharmonic submanifolds in Lorentz space forms
  87. Some new results on the weaving of K-g-frames in Hilbert spaces
  88. Matrix representation of a cross product and related curl-based differential operators in all space dimensions
  89. Global optimization and applications to a variational inequality problem
  90. Functional equations related to higher derivations in semiprime rings
  91. A partial order on transformation semigroups with restricted range that preserve double direction equivalence
  92. On multi-step methods for singular fractional q-integro-differential equations
  93. Compact perturbations of operators with property (t)
  94. Entire solutions for several complex partial differential-difference equations of Fermat type in ℂ2
  95. Random attractors for stochastic plate equations with memory in unbounded domains
  96. On the convergence of two-step modulus-based matrix splitting iteration method
  97. On the separation method in stochastic reconstruction problem
  98. Robust estimation for partial functional linear regression models based on FPCA and weighted composite quantile regression
  99. Structure of coincidence isometry groups
  100. Sharp function estimates and boundedness for Toeplitz-type operators associated with general fractional integral operators
  101. Oscillatory hyper-Hilbert transform on Wiener amalgam spaces
  102. Euler-type sums involving multiple harmonic sums and binomial coefficients
  103. Poly-falling factorial sequences and poly-rising factorial sequences
  104. Geometric approximations to transition densities of Jump-type Markov processes
  105. Multiple solutions for a quasilinear Choquard equation with critical nonlinearity
  106. Bifurcations and exact traveling wave solutions for the regularized Schamel equation
  107. Almost factorizable weakly type B semigroups
  108. The finite spectrum of Sturm-Liouville problems with n transmission conditions and quadratic eigenparameter-dependent boundary conditions
  109. Ground state sign-changing solutions for a class of quasilinear Schrödinger equations
  110. Epi-quasi normality
  111. Derivative and higher-order Cauchy integral formula of matrix functions
  112. Commutators of multilinear strongly singular integrals on nonhomogeneous metric measure spaces
  113. Solutions to a multi-phase model of sea ice growth
  114. Existence and simulation of positive solutions for m-point fractional differential equations with derivative terms
  115. Bernstein-Walsh type inequalities for derivatives of algebraic polynomials in quasidisks
  116. Review Article
  117. Semiprimeness of semigroup algebras
  118. Special Issue on Problems, Methods and Applications of Nonlinear Analysis (Part II)
  119. Third-order differential equations with three-point boundary conditions
  120. Fractional calculus, zeta functions and Shannon entropy
  121. Uniqueness of positive solutions for boundary value problems associated with indefinite ϕ-Laplacian-type equations
  122. Synchronization of Caputo fractional neural networks with bounded time variable delays
  123. On quasilinear elliptic problems with finite or infinite potential wells
  124. Deterministic and random approximation by the combination of algebraic polynomials and trigonometric polynomials
  125. On a fractional Schrödinger-Poisson system with strong singularity
  126. Parabolic inequalities in Orlicz spaces with data in L1
  127. Special Issue on Evolution Equations, Theory and Applications (Part II)
  128. Impulsive Caputo-Fabrizio fractional differential equations in b-metric spaces
  129. Existence of a solution of Hilfer fractional hybrid problems via new Krasnoselskii-type fixed point theorems
  130. On a nonlinear system of Riemann-Liouville fractional differential equations with semi-coupled integro-multipoint boundary conditions
  131. Blow-up results of the positive solution for a class of degenerate parabolic equations
  132. Long time decay for 3D Navier-Stokes equations in Fourier-Lei-Lin spaces
  133. On the extinction problem for a p-Laplacian equation with a nonlinear gradient source
  134. General decay rate for a viscoelastic wave equation with distributed delay and Balakrishnan-Taylor damping
  135. On hyponormality on a weighted annulus
  136. Exponential stability of Timoshenko system in thermoelasticity of second sound with a memory and distributed delay term
  137. Convergence results on Picard-Krasnoselskii hybrid iterative process in CAT(0) spaces
  138. Special Issue on Boundary Value Problems and their Applications on Biosciences and Engineering (Part I)
  139. Marangoni convection in layers of water-based nanofluids under the effect of rotation
  140. A transient analysis to the M(τ)/M(τ)/k queue with time-dependent parameters
  141. Existence of random attractors and the upper semicontinuity for small random perturbations of 2D Navier-Stokes equations with linear damping
  142. Degenerate binomial and Poisson random variables associated with degenerate Lah-Bell polynomials
  143. Special Issue on Fractional Problems with Variable-Order or Variable Exponents (Part I)
  144. On the mixed fractional quantum and Hadamard derivatives for impulsive boundary value problems
  145. The Lp dual Minkowski problem about 0 < p < 1 and q > 0
Downloaded on 7.9.2025 from https://www.degruyterbrill.com/document/doi/10.1515/math-2021-0096/html
Scroll to top button