Volume 2012, Issue 1 387132
Research Article
Open Access

Lattices Generated by Orbits of Subspaces under Finite Singular Orthogonal Groups II

You Gao

Corresponding Author

You Gao

College of Science, Civil Aviation University of China, Tianjin 300300, China cauc.edu.cn

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XinZhi Fu

XinZhi Fu

College of Science, Civil Aviation University of China, Tianjin 300300, China cauc.edu.cn

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First published: 14 August 2012
Academic Editor: Ch Tsitouras

Abstract

Let be a (2ν + δ + l)-dimensional vector space over the finite field 𝔽q. In this paper we assume that 𝔽q is a finite field of odd characteristic, and O2ν+δ+l,  Δ(𝔽q) the singular orthogonal groups of degree 2ν + δ + l over 𝔽q. Let be any orbit of subspaces under O2ν+δ+l,  Δ(𝔽q). Denote by the set of subspaces which are intersections of subspaces in , where we make the convention that the intersection of an empty set of subspaces of is assumed to be . By ordering by ordinary or reverse inclusion, two lattices are obtained. This paper studies the questions when these lattices are geometric lattices.

1. Introduction

Let 𝔽q be a finite field with q elements, where q is an odd prime power. We choose a fixed nonsquare element z in . Let be a (2ν + δ + l)-dimensional row vector space over the finite field 𝔽q, and let O2ν+δ+l(𝔽q) be one of the singular orthogonal groups of degree 2ν + δ + l over 𝔽q. There is an action of O2ν+δ+l(𝔽q) on defined as follows:
()
Let P be an m-dimensional subspace of , and v1, v2, …, vm be a basis of P. Then, the m × (2ν + δ + l) matrix:
()
is called a matrix representation of P. We usually denote a matrix representation of the m-dimensional subspace P still by P. The above action induces an action on the set of subspaces of , that is, a subspace P is carried by TO2ν+δ+l(𝔽q) into the subspace PT. The set of subspaces of is partitioned into orbits under O2ν+δ+l(𝔽q). Clearly, {0} and are two trivial orbits. Let be any orbit of subspaces under O2ν+δ+l(𝔽q). Denote the set of subspaces which are intersections of subspaces in by () and call () the set of subspaces generated by . We agree that the intersection of an empty set of subspaces is . Then, . Partially ordering () by ordinary or reverse inclusion, we get two posets and denote them by O() and R(), respectively. Clearly, for any two elements P, QO(),
()
where 〈P, Q〉 is a subspace generated by P and Q. Therefore, O() is a finite lattice.
Similarly, for any two elements P, QR(),
()
so R() is also a finite lattice. Both O() and R() are called the lattices generated by .

The results on the geometricity of lattices generated by subspaces in d-bounded distance-regular graphs can be found in Guo et al. [1]; on the geometricity and the characteristic polynomial of lattices generated by orbits of flats under finite affine-classical groups can be found in Wang and Feng [2], Wang and Guo [3]; on inclusion relations, the geometricity and the characteristic polynomial of lattices generated by orbits of subspaces under finite nonsingular classical groups and a characterization of subspaces contained in lattices can be found in Huo [46], Huo and Wan [7, 8]; on inclusion relations, the geometricity and the characteristic polynomial of lattices generated by orbits of subspaces under finite singular symplectic groups, singular unitary groups, and singular pseudosymplectic groups and a characterization of subspaces contained in lattices can be found in Gao and You [912]. In [13], the authors studied the various lattices O() and R() generated by different orbits of subspaces under singular orthogonal group O2ν+δ+l(𝔽q). The study contents include the inclusion relations between different lattices, the characterization of subspaces contained in a given lattice R() (resp., O()), and the characteristic polynomial of R(). The purpose of this paper is to study the questions when R() (resp., O()) are geometric lattices.

2. Preliminaries

In the following, we recall some definitions and facts on ordered sets and lattices (see [8, 14]).

Let A be a partially ordered set, and a, bA. We say that b  covers a and write a < ·  b, if a < b and there exists no cA such that a < c < b. An element mA is called the minimal element if there exists no elements aA such that a < m. If A has a unique minimal element, denote it by 0 and we say that A is a poset with 0.

Let A be a poset with 0 and aA. If all maximal ascending chains starting from 0 with endpoint a  have the same finite length, this common length is called the rank r(a) of a. If rank r(a) is defined for every aA, A is said to have the rank function r : A, where is the set consisting of all positive integers and 0.

A poset A is said to satisfy the Jordan-Dedekind (JD) condition if any two maximal chains between the same pair of elements of A have the same finite length.

Proposition 2.1 ([14, Proposition 2.1]). Let A be a poset with 0. If A satisfies the JD condition then A has the rank function r : A which satisfies

  • (i)

    r(0) = 0,

  • (ii)

    a < ·  br(b) = r(a) + 1.

Conversely, if A admits a function r : A satisfying (i) and (ii), then A satisfies the JD condition with r as its rank function.

Let A be a poset with 0. An element aA is called an atom of A if 0 < ·  a. A lattice L with 0 is called an atomic lattice (or a pointlattice) if every element aL∖{0} is a supremum of atoms, that is, a = sup {bL∣0 < ·ba}.

Definition 2.2 ([14, page 46]). A lattice L is called a semimodular lattice if for all a, bL,

()

Proposition 2.3 ([14, Theorem 2.27]). Let L be a lattice with 0. Then, L is a semimodular lattice if and only if L possesses a rank function r such that for all x, yL

()

Definition 2.4 ([14, page 52]). A lattice L is called a geometric lattice if it is

  • an atomic lattice,

  • a semimodular lattice,

  • G3   without infinite chains in L.

According to Definition 2.2, Proposition 2.3, and Definition 2.4, we can obtain the following proposition.

Proposition 2.5. Let L be a lattice with 0. Then, L is a geometric lattice if and only if

  • G1   for every element aL∖{0}, a = sup {bL∣0 < ·ba},

  • G2 L possesses a rank function r and for all x, yL, (2.2) holds,

  • G3   without infinite chains in L.

Let
()
where S = S2ν+δ, δ = 0,1, or 2, and
()
The set of all (2ν + δ + l) × (2ν + δ + l)  nonsingular matrices T over 𝔽q satisfying
()
forms a group which will be called the singular orthogonal group of degree 2ν + δ + l, rank  2ν + δ, and with definite part Δ  over 𝔽q  and denoted by O2ν+δ+l(𝔽q).  Clearly, O2ν+δ+l(𝔽q)  consists of all (2ν + δ + l) × (2ν + δ + l)  nonsingular matrices of the form:
()
where , and T22 is nonsingular.

Two n × n matrices A and B are called to be cogredient if there exists a nonsingular matrix P such that PAPt = B.

An m-dimensional subspace P is said to be a subspace of type (m, 2s + γ, s, Γ), if PSlPt is cogredient to M(m, 2s + γ, s, Γ), where the matrix M(m, 2s + γ, s, Γ), respectively, is as follows
()
or
()
Let e1, e2, …, e2ν+δ, e2ν+δ+1, …, e2ν+δ+l  be a basis of , where
()
1 is in the ith position. Denote by E the l-dimensional subspace of generated by e2ν+δ+1, e2ν+δ+2, …, e2ν+δ+l. An m-dimensional subspace P is called a subspace of type (m, 2s + γ, s, Γ, k)  if
  • (i)

    P is a subspace of type (m, 2s + γ, s, Γ),

  • (ii)

    dim (PE) = k.

Denote the set of all subspaces of type (m, 2s + γ, s, Γ, k)  in by  (m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ). By [15, Theorem 6.28], we know that  (m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ)  is nonempty if and only if
()
or
()

Moreover, if (m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ)  is nonempty, then it forms an orbit of subspaces under O2ν+δ+l(𝔽q). Let (m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ)  denote the set of subspaces which are intersections of subspaces in (m, 2s + γ, s, Γ, k; 2ν + δ + l, Δ), where we make the convention that the intersection of an empty set of subspaces of is assumed to be . Partially ordering (m, 2s + γ, s, Γ, k; 2ν + δ + l, Δ) by ordinary or reverse inclusion, we get two finite lattices and denote them by O(m, 2s + γ, s, Γ, k; 2ν + δ + l, Δ)  and R(m, 2s + γ, s, Γ, k; 2ν + δ + l, Δ), respectively.

The case R(ml, 2s + γ, s, Γ;   2ν + δ, Δ)  has been discussed in [8]. So, we only discuss the case 0 ≤   k   <   l  in this paper.

By [13], we have the following results.

Theorem 2.6. Let 2ν + δ + l > m ≥ 1,  0 ≤ k < l, assume that (m, 2s + γ, s, Γ, k) satisfies conditions (2.10) and (2.11). Then,

()
if and only if
()

Theorem 2.7. Let 2ν + δ + l > m ≥ 1,  0 ≤ k < l. Assume that (m, 2s + γ, s, Γ, k) satisfies condition (2.10), then R(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ) consists of and all the subspaces of type (m1, 2s1 + γ1, s1, Γ1, k1), where (m1, 2s1 + γ1, s1, Γ1, k1)  satisfies condition (2.13).

Theorem 2.8. Let 2ν + δ + l > m ≥ 1,  0 ≤ k < l, and (m, 2s + γ, s, Γ, k) satisfy

()
For any XO(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ), define
()
then r : O(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ) → is a rank function of the lattice O(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ).

Theorem 2.9. Let 2ν + δ + l > m ≥ 1,  0 ≤ k < l, and (m, 2s + γ, s, Γ, k) satisfy (2.14). For any XR(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ), define

()
then r : R(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ) → is a rank function of the lattice R(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ).

3. The Geometricity of Lattices O(m,  2s + γ,  s,  Γ,  k;  2ν + δ + l,  Δ)

Theorem 3.1. Let 2ν + δ + l > m ≥ 1, 0 ≤ k < l, assume that (m, 2s + γ, s, Γ, k)  satisfies conditions (2.10) and (2.11). Then

  • (i)

    each of O(k + 1, 0, 0, ϕ, k;   2ν + δ + l, Δ) and O(k + 1, 1, 0, Γ, k;   2ν + δ + l, Δ)  (Γ = 1  or  z) is a finite geometric lattice, when k = 0, and is a finite atomic lattice, but not a geometric lattice when 0 < k < l;

  • (ii)

    when 2 ≤ mk ≤ 2ν + δ − 1, O(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ) is a finite atomic lattice, but not a geometric lattice.

Proof. By Theorem 2.8, the rank function of O(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ) is defined by formula (2.15), we will show the condition G1 of Proposition 2.5 holds for O(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ). {0} ∈ O(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ) and it is the minimal element, so all 1-dim subspaces in O(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ) are atoms of O(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ).

Let , by Theorem 2.7, U is a subspace of type (m1, 2s1 + γ1, s1, Γ1, k1) and satisfies condition (2.13). If m1 = 1, then U is an atom of O(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ). Assume m1 ≥ 2, then

()
where Γ1 = ϕ, (1), (z), or [1, −z].

Let Ui be an ith (1 ≤ im1) row vector of U, then 〈Ui〉 is a subspace of type (1, 0, 0, ϕ, 0), (1, 1, 0, 1, 0), (1, 1, 0, z, 0), or (1, 0, 0, 0, 1), and 〈Ui〉 ⊂ U. By Theorem 2.7, we know 〈Ui〉 ∈ O(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ), so 〈Ui〉 is an atom of O(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ), and , hence, U is a union of atoms in O(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ). Since |(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ)| ≥ 2, there exist W1, W2(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ), W1W2, such that . W1, W2 are unions of atoms in O(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ), hence, is a union of atoms in O(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ), therefore, G1 holds.

In the following, we prove (i) and (ii).

The Proof of (i). We only prove the formula (2.2) holds for O(k + 1, 1, 0, Γ, k;   2ν + δ + l, Δ). The other can be obtained in the similar way. We consider two cases:

(a) k = 0. O(k + 1, 1, 0, Γ, k;   2ν + δ + l, Δ) consists of and subspaces of type (1, 1, 0, Γ, 0). Let U, WO(1, 1, 0, Γ, 0;   2ν + δ + l, Δ), if U, W are , respectively, then , so r(UW) + r(UW) = r(U) + r(W). If U = W is {0} or , the other is a subspace of type (1, 1, 0, Γ, 0), then UW is {0}  or subspace of type (1, 1, 0, Γ, 0), UW is a subspace of type (1, 1, 0, Γ, 0) or , so r(UW) + r(UW) = r(U) + r(W). If U and W are subspaces of type (1, 1, 0, Γ, 0), then , so r(UW) + r(UW) = r(U) + r(W).

Hence, (2.2) holds and O(k + 1, 1, 0, Γ, k;   2ν + δ + l, Δ) is a finite geometric lattice when k = 0.

(b) 0 < k < l. Let U = 〈e1 + (Γ/2)eν+1〉, W = 〈es+1 + (Γ/2)eν+s+1〉, where sν − 1, then U, WO(k + 1, 1, 0, Γ, k;   2ν + δ + l, Δ). When q = 3(mod   4) or q = 1(mod   4), then −1 is a nonsquare element or a square element, respectively. Thus, [Γ, Γ] is cogredient to either [1, −z] or S2·1, and 〈U, W〉 is a subspace of type (2, 2, 0, Γ, 0), where Γ = [1, −z], or a subspace of type (2, 2, 1, ϕ, 0). So 〈U, W〉 ∉ O(k + 1, 1, 0, Γ, k;   2ν + δ + l, Δ), and we have , UW = {0}. By the definition of rank function, r(UW) = k + 1 + 1 = k + 2, r(UW) = 0, r(U) = r(W) = 1, we have r(UW) + r(UW) = k + 2 > r(U) + r(W) = 2.

Hence, O(k + 1, 1, 0, Γ, k;   2ν + δ + l, Δ) is a finite atomic lattice, but not a geometric lattice when 0 < k < l.

The Proof of (ii). We will show there exist U, WO(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ) such that the formula (2.2) does not hold. As to γ = 0, 1, or 2, we only show the proof of γ = 1, others can be obtained in the similar way. We distinguish the following three cases.

(a) δ = 0, or δ = 1,  Γ ≠ Δ. Then, the formula (2.10) is changed into 2s + 1 ≤ mkν + s. Let σ = ν + sm + k, we distinguish the following two subcases.

(a.1) mk − 2s − 1 ≥ 1. From mk − 2s − 1 ≥ 1 and mkν + s, we have s + 2 ≤ ν. Let

()
where σ1 = mk − 2s − 2, then U is a subspace of type (m − 1, 2s + 1, s, Γ, k), W is a subspace of type (1, 1, 0, Γ, 0). When q = 3(mod   4) or q = 1(mod   4), then −1 is a nonsquare element or a square element, respectively, thus [Γ, Γ] is cogredient to either [1, −z] or S2·1, and 〈U, W〉 is a subspace of type (m, 2s + 2, s, Γ, k) or type (m, 2(s + 1), s + 1, ϕ, k). Consequently, U, WO(m, 2s + 1, s, Γ, k;   2ν + δ + l, Δ), 〈U, W〉 ∉ O(m, 2s + 1, s, Γ, k;   2ν + δ + l, Δ). Thus, we have ,  UW = {0},  r(UW) = m + 1, r(UW) = 0,  r(U) = m − 1,  r(W) = 1.  Then,
()

(a.2) mk − 2s − 1 = 0. From 2 ≤ mk ≤ 2ν + δ − 1, we have s + 1 ≤ ν,  s ≥ 1. Let

()
then U is a subspace of type (m − 1, 2(s − 1) + 1, s − 1, Γ, k), W is a subspace of type (1, 1, 0, −Γ, 0), 〈U, W〉 is a subspace of type (m, 2s, s, ϕ, k). Consequently, U, WO(m, 2s + 1, s, Γ, k;   2ν + δ + l, Δ) , 〈U, W〉 ∉ O(m, 2s + 1, s, Γ, k;   2ν + δ + l, Δ). Thus, we have ,  UW = {0},  r(UW) = m + 1,  r(UW) = 0,  r(U) = m − 1,  r(W) = 1.  Then,
()
Therefore, there exist U, WO(m, 2s + 1, s, Γ, k;   2ν + δ + l, Δ) such that formula (2.2) does not hold.

(b) δ = 1, Γ = Δ. Then, the formula (2.10) is changed into 2s + 1 ≤ mkν + s + 1. Let σ = ν + sm + k + 1, we distinguish the following two subcases.

(b.1) mk − 2s − 1 ≥ 1. From mk − 2s − 1 ≥ 1, and 2 ≤ mk ≤ 2ν, we have s + 1 ≤ ν. Let

()
where σ1 = mk − 2s − 2, then U is a subspace of type (m − 1, 2s + 1, s, Δ, k), W is a subspace of type (1, 1, 0, Δ, 0). When q = 3(mod   4) or q = 1(mod   4), similar to the proof of the case (a.1), 〈U, W〉 is a subspace of type (m, 2s + 2, s, Γ, k) or (m, 2(s + 1), s + 1, ϕ, k). Consequently, U, WO(m, 2s + 1, s, Δ, k;   2ν + 1 + l, Δ), 〈U, W〉 ∉ O(m, 2s + 1, s, Δ, k;   2ν + 1 + l, Δ), and the formula (2.2) does not hold.

(b.2) mk − 2s − 1 = 0. From 2 ≤ mk ≤ 2ν, we have s + 1 ≤ ν. Let

()
then U is a subspace of type (m − 1, 2(s − 1) + 1, s − 1, Δ, k), W is a subspace of type (1, 1, 0, Δ, 0), when q = 3(mod   4) or q = 1(mod   4), 〈U, W〉 is subspace of type (m, 2(s − 1) + 2, s − 1, Γ, k) or (m, 2s, s, ϕ, k). Similar to the proof of the case (a.1), the formula (2.2) does not hold for U and W.

(c) δ = 2. Then, the formula (2.10) is changed into 2s + 1 ≤ mkν + s + 1. Let σ = ν + sm + k + 1, we distinguish the following two subcases.

(c.1) mk − 2s − 1 ≥ 1. From mk − 2s − 1 ≥ 1, and mk ≤ 2ν + 1, we have s + 1 ≤ ν. Let

()
where σ1 = mk − 2s − 2 and x2zy2 = Γ, then U is a subspace of type (m − 1, 2s + 1, s, Γ, k), W is a subspace of type (1, 1, 0, Γ, 0). But when q = 3(mod   4) or q = 1(mod   4), similar to the proof of the case (a.1), 〈U, W〉 is a subspace of type (m, 2s + 2, s, Γ, k) or (m, 2(s + 1), s + 1, ϕ, k). Consequently, U, WO(m, 2s + 1, s, Γ, k;   2ν + δ + l, Δ), 〈U, W〉 ∉ O(m, 2s + 1, s, Γ, k;   2ν + δ + l, Δ), and the formula (2.2) does not hold.

(c.2) mk − 2s − 1 = 0. From 2 ≤ mk ≤ 2ν + 1, we have s ≥ 1 and m ≥ 3. We choose (a, b) and (c, d) being two linearly independent solutions of the equation x2zy2 = Γ. Let

()
then U is a subspace of type (m − 1, 2(s − 1) + 1, s − 1, Γ, k), W is a subspace of type (1, 1, 0, Γ, 0). Let
()
because det   A = −(adbc)2z, hence, A is cogredient to [1, −z]. Then,
()
is cogredient to
()
Therefore, 〈U, W〉 is a subspace of type (m, 2(s − 1) + 2, s − 1, Γ, k). Similar to the proof of the case (a.2), the formula (2.2) does not hold for U and W.

4. The Geometricity of Lattices R(m,  2s + γ,  s,  Γ,  k; 2ν + δ + l,  Δ)

Theorem 4.1. Let 2ν + δ + l > m ≥ 1,  0 ≤ k < l, assume that (m, 2s + γ, s, Γ, k) satisfies conditions (2.10) and (2.11). Then,

  • (i)

    each of R(k + 1, 0, 0, ϕ, k;   2ν + δ + l, Δ), R(k + 1, 1, 0, Γ, k;   2ν + δ + l, Δ) (Γ = 1  or  z) and R(2ν + δ + k − 1, 2s + γ, s, Γ, k;   2ν + δ + l, Δ) is a finite geometric lattice when k = 0, and is a finite atomic lattice, but not a geometric lattice when 0 < k < l;

  • (ii)

    when 2 ≤ mk ≤ 2ν + δ − 2, R(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ) is a finite atomic lattice, but not a geometric lattice.

Proof . By Theorem 2.9, the rank function of R(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ) is defined by formula (2.16), is the minimal element of R(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ), all subspaces of type (m, 2s + γ, s, Γ, k) in R(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ) are atoms of R(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ).

The Proof of (i). By [8], R(k + 1, 0, 0, ϕ, k;   2ν + δ + l, Δ), R(k + 1, 1, 0, Γ, k;   2ν + δ + l, Δ), and R(2ν + δ + k − 1, 2s + γ, s, Γ, k;   2ν + δ + l, Δ) are finite geometric lattices when k = 0; in the following, we will show that they are finite atomic lattices, but not geometric lattices when 0 < k < l.

(a) Let

()
Then, both U and W are subspaces of type (k + 1, 0, 0, ϕ, k), and UW = 〈e2ν+δ+2, e2ν+δ+3, …, e2ν+δ+k〉, 〈U, W〉 is a subspace of type (k + 3, 2, 1, ϕ, k + 1). Consequently, 〈U, W〉 ∉ R(k + 1, 0, 0, ϕ, k;   2ν + δ + l, Δ), ,  r(UW) = r(UW) = k + 2 − (k − 1) = 3,  r(U) = r(W) = k + 2 − (k + 1) = 1. Thus,
()
That is, (2.2) does not hold for U and W. Hence, R(k + 1, 0, 0, ϕ, k;   2ν + δ + l, Δ) are not geometric lattices when 0 < k < l.

(b) Let

()
Then, both U and W are subspaces of type (k + 1, 1, 0, Γ, k), and UW = 〈e2ν+δ+2, e2ν+δ+3, …, e2ν+δ+k〉, 〈U, W〉 is a subspace of type (k + 3, 2, 0, Γ, k + 1) or (k + 3, 2, 1, ϕ, k + 1) when q = 3(mod   4) or q = 1(mod   4). Consequently, 〈U, W〉 ∉ R(k + 1, 1, 0, Γ, k;   2ν + δ + l, Δ),  ,  r(UW) = r(UW) = k + 2 − (k − 1) = 3,  r(U) = r(W) = k + 2 − (k + 1) = 1. Thus,
()
That is, (2.2) does not hold for U and W. Hence, R(k + 1, 1, 0, Γ, k;   2ν + δ + l, Δ) are not geometric lattices when 0 < k < l.

(c) From the condition (2.10), the following hold.

  • (i)

    If γ = δ = 1, Γ ≠ Δ, then 2ν + δ − 1 ≤ ν + s, that is, νs, ν = s, hence 2ν + 1 ≤ 2ν, and it is a contradiction.

  • (ii)

    If γ = δ, Γ = Δ, then 2ν + δ − 1 ≤ ν + s + δ, that is, ν − 1 ≤ s, hence s = ν, or s = ν − 1. When s = ν, from 2s + γ ≤ 2ν + δ − 1, we obtain 2ν + δ ≤ 2ν + δ − 1, and it is a contradiction. When s = ν − 1, we have 2ν + δ − 2 ≤ 2ν + δ − 1. That is, in this situation, ν − 1 = s  holds.

  • (iii)

    If γδ, then 2ν + δ − 1 ≤ ν + s + min {δ, γ} ≤ ν + s + δ, that is, ν − 1 ≤ s, hence s = ν, or s = ν − 1. When s = ν, we have 2ν + γ ≤ 2ν + δ − 1, then γδ − 1. When s = ν − 1, we have 2ν + γ − 2 ≤ 2ν + δ − 1, then γ − 1 ≤ δ.

From the discussion above, we know that

(c.1) If s = ν, then γδ − 1, and we have δ = 1,  γ = 0;  δ = 2,  γ = 0, and δ = 2,  γ = 1 three possible cases. For R(2ν + δ + k − 1, 2ν + γ, ν, Γ, k;   2ν + δ + l, Δ), here we just give the proof of the case δ = 2,  γ = 1, others can be obtained in the similar way. We choose (a, b) and (c, d) being two linearly independent solutions of the equation x2zy2 = Γ. Let

()
then U is a subspace of type (2ν + k + 1, 2ν + 1, ν, Γ, k), W is a subspace of type (2, 1, 0, Γ, 1), and 〈U, W〉 is a subspace of type (2ν + k + 3, 2ν + 2, ν, Γ, k + 1). Consequently, U, WR(2ν + k + 1, 2ν + 1, ν, Γ, k;   2ν + δ + l, Δ), 〈U, W〉 ∉ R(2ν + k + 1, 2ν + 1, ν, Γ, k;   2ν + δ + l, Δ). Thus, we have UW = {0},  ,  r(UW) = r(UW) = 2ν + k + 2,  r(UW) = 0,  r(U) = 2ν + k + 2 − 2νk − 1 = 1,  r(W) = 2ν + k + 2 − 2 = 2ν + k. Then,
()
That is, (2.2) does not hold for U and W. Hence, R(2ν + k + 1, 2ν + 1, ν, 1, k;   2ν + δ + l, Δ) are not geometric lattices when 0 < k < l.

(c.2) If s = ν − 1, then we have γδ,   γ − 1 ≤ δ; or γ = δ, Γ = Δ. As to R(2ν + δ + k − 1, 2(ν − 1) + γ, ν − 1, Γ, k;   2ν + δ + l, Δ), we consider δ = 0,  δ = 1, and δ = 2 three cases. Here we just give the proof of the case δ = 1, and we also discuss the following three subcases:

(c.2.1) δ = 1, γ = 0. For R(2ν + k, 2(ν − 1), ν − 1, ϕ, k;   2ν + δ + l, Δ), let

()
then U is a subspace of type (2ν + k, 2(ν − 1), ν − 1, ϕ, k + 1), W is a subspace of type (2, 1, 0, Δ, 0), and 〈U, W〉 is a subspace of type (2ν + k + 2, 2ν + 1, ν, Δ, k + 1). If ν = 1, then s = 0, and as to W, from the condition (2.10), we obtain 2 ≤ 1, that is, it is a contradiction. Consequently, ν ≥ 2, and U, WR(2ν + k, 2(ν − 1), ν − 1, ϕ, k;   2ν + δ + l, Δ),〈U, W〉 ∉ R(2ν + k, 2(ν − 1), ν − 1, ϕ, k;   2ν + δ + l, Δ). Thus, we have , r(UW) = r(UW) = 2ν + k + 1, r(UW) = 0, r(U) = 2ν + k + 1 − 2νk = 1, r(W) = 2ν + k + 1 − 2 = 2ν + k − 1. Then,
()
That is, (2.2) does not hold for U and W. Hence, R(2ν + k, 2(ν − 1), ν − 1, ϕ, k;   2ν + δ + l, Δ)  are not geometric lattices when 0 < k < l.

(c.2.2) δ = 1, γ = 1, Γ = Δ. For R(2ν + k, 2(ν − 1) + 1, ν − 1, Δ, k;   2ν + δ + l, Δ), let

()
then U is a subspace of type (2ν + k, 2(ν − 1) + 1, ν − 1, Δ, k), W is a subspace of type (2, 1, 0, Δ, 0), and 〈U, W〉 is a subspace of type (2ν + k + 2, 2ν + 1, ν, Δ, k + 1). Consequently, U, WR(2ν + k, 2(ν − 1) + 1, ν − 1, Δ, k;   2ν + δ + l, Δ),〈U, W〉 ∉ R(2ν + k, 2(ν − 1) + 1, ν − 1, Δ, k;   2ν + δ + l, Δ). Thus, we have UW = {0}, , r(UW) = r(UW) = 2ν + k + 1, r(UW) = 0, r(U) = 2ν + k + 1 − 2νk = 1, r(W) = 2ν + k + 1 − 2 = 2ν + k − 1. Then,
()
That is, (2.2) does not hold for U and W. Hence, R(2ν + k, 2(ν − 1) + 1, ν − 1, Δ, k;   2ν + δ + l, Δ)  are not geometric lattices when 0 < k < l.

(c.2.3) δ = 1, γ = 2. See the proof of the Theorem 7 in [12].

The Proof of (ii). Let U(m, 2s + γ, s, Γ, k;   2ν + δ + l, Δ), then

()
where Λ1 = S2s+γ. Hence, there exists a (2ν + δ + lm) × (2ν + δ + l) matrix Z such that
()
where Λ* takes values in Table 1 as follows.

In Table 1 as follows .

As to δ = 0;   δ = 1, Δ = 1;   δ = 1, Δ = z, and δ = 2 four cases, we only show the proof of the case δ = 0, others can be obtained in the similar way. We also distinguish the following three subcases.

(a) If γ = 0, then Λ1 = S2s, Λ* = S2(νm+k+s). Let u1, u2, …, us, v1, v2, …, vs, us+1, …, umks, w1, …, wk and vs+1, …, vmks, umks+1, …, uν, vmks+1, …, vν, wk+1, …, wl be row vectors of U and Z, respectively,

()
then W(m, 2s, s, ϕ, k;   2ν + l).

From mk ≤ 2ν − 2, we know s < ν. If mk = 2s, then mks = s < ν, so uν, vνU. If mk > 2s, then s < ν − 1, so vν−1, vνU. In a word, dim 〈U, W〉 ≥ m + 2, dim (UW) ≤ m − 2. That is, , r(UW) = 0, r(UW) ≥ m + 1 − (m − 2) = 3, r(U) = r(W) = m + 1 − m = 1. Consequently, r(UW) + r(UW) > r(U) + r(W).

(b) If γ = 1, then Λ1 = S2s+1,Γ, Λ* = S2(νm+k+s)+1,−Γ, and Γ = (1)  or  (z). Let u1, u2, …, us, v1, v2, …, vs, ω, us+1, …, umks−1, w1, …, wk and vs+1, …, vmks−1, umks, …, uν−1, vmks, …, vν−1, ω*, wk+1, …, wl be row vectors of U and Z, respectively

()
because ((1/2)Γuν−1 + vν−1)S2ν((1/2)Γuν−1 + vν−1) t = Γ, and
()
then W(m, 2s + 1, s, Γ, k;   2ν + l). From the conditions 2s + 1 ≤ mk ≤ 2ν − 2 and mkν + s, we can obtain mks − 1 ≤ ν − 1 and sν − 1, hence (1/2)Γuν−1 + vν−1U. Obviously, ω*U. Similar to the proof of the case (a), r(UW) + r(UW) > r(U) + r(W).

(c) If γ = 2, then Λ1 = S2s+2,Γ, Λ* = S2(νm+k+s)+2,Γ, and Γ = [1, −z]. Let u1, u2, …, us, v1, v2, …, vs, ω1, ω2, us+1, …, umks−2, w1, …, wk and be row vectors of U and Z, respectively,

()
then W(m, 2s + 2, s, Γ, k;   2ν + l). Obviously, . Similar to the proof of the case (a), r(UW) + r(UW) > r(U) + r(W).

From the discussion above, we know that when 2 ≤ mk ≤ 2ν − 2, R(m, 2s + γ, s, Γ, k;   2ν + l) is a finite atomic lattice, but not a geometric lattice.

δ = 0 δ = 1,  Δ = 1 δ = 1,  Δ = z δ = 2
γ = 0 Σ0 [Σ0,  1] [Σ0,  z ] [Σ0,  1,   − z ]
γ = 1,  Γ = 1 [Σ0,   − 1 ] Σ1 [Σ0,   − 1,  z ] [Σ1,   − z ]
γ = 1,  Γ = z [Σ0,   − z] [Σ0,  1,   − z] Σ1 [Σ1,   − 1 ]
γ = 2 [Σ0,  1,   − z] [Σ1,  z] [Σ1,  1 ] Σ2

Acknowledgments

This work is supported by the National Natural Science Foundation of China under Grant no. 61179026 and the Fundamental Research Funds for the Central Universities under Grant no. ZXH2012K003. The authors would like to thank the referee for his suggestions on simplifying the earlier version of the paper.

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