Home Mathematics On maximal symplectic partial spreads
Article
Licensed
Unlicensed Requires Authentication

On maximal symplectic partial spreads

  • William M. Kantor EMAIL logo
Published/Copyright: October 16, 2017
Become an author with De Gruyter Brill

Abstract

New types of maximal symplectic partial spreads are constructed.

MSC 2010: 51A50; 51E20

Communicated by: G. Korchmáros


Acknowledgement

I am grateful to Markus Grassl for stimulating my interest in maximal symplectic partial spreads by pointing out the scarcity of examples in dimension > 4.

Funding

This research was supported in part by a grant from the Simons Foundation

References

[1] B. Bagchi, N. S. Narasimha Sastry, Even order inversive planes, generalized quadrangles and codes. Geom. Dedicata22 (1987), 137–147. MR877206 Zbl 0609.5101110.1007/BF00181262Search in Google Scholar

[2] B. Bagchi, N. S. Narasimha Sastry, Intersection pattern of the classical ovoids in symplectic 3-space of even order. J. Algebra126 (1989), 147–160. MR1023290 Zbl 0685.5100610.1016/0021-8693(89)90324-4Search in Google Scholar

[3] S. Ball, On ovoids of O(5, q). Adv. Geom. 4 (2004), 1–7. MR2155360 Zbl 1039.5100410.1515/advg.2004.004Search in Google Scholar

[4] A. R. Calderbank, P. J. Cameron, W. M. Kantor, J. J. Seidel, Z4-Kerdock codes, orthogonal spreads, and extremal Euclidean line-sets. Proc. London Math. Soc. (3) 75 (1997), 436–480. MR1455862 Zbl 0916.9401410.1112/S0024611597000403Search in Google Scholar

[5] M. Cimráková, S. De Winter, V. Fack, L. Storme, On the smallest maximal partial ovoids and spreads of the generalized quadrangles W(q) and Q(4,q). European J. Combin. 28 (2007), 1934–1942. MR2344978 Zbl 1126.5100510.1016/j.ejc.2006.11.001Search in Google Scholar

[6] K. Coolsaet, J. De Beule, A. Siciliano, The known maximal partial ovoids of size q2 – 1 of Q(4,q). J. Combin. Des. 21 (2013), 89–100. MR3011983 Zbl 1273.0502410.1002/jcd.21307Search in Google Scholar

[7] B. N. Cooperstein, Hyperplane sections of Kantor’s unitary ovoids. Des. Codes Cryptogr. 23 (2001), 185–195. MR1830940 Zbl 0986.5100410.1023/A:1011264632630Search in Google Scholar

[8] A. Cossidente, On twisted tensor product group embeddings and the spin representation of symplectic groups: The case q odd. International Scholarly Research Notices Geometry (2011), Article 694605.10.5402/2011/694605Search in Google Scholar

[9] W. v. Dam, M. Howard, Bipartite entangled stabilizer mutually unbiased bases as maximum cliques of Cayley graphs. Phys. Rev. A84 (2011) 012117.10.1103/PhysRevA.84.012117Search in Google Scholar

[10] P. Dembowski, Finite geometries. Springer 1968. MR0233275 Zbl 0159.5000110.1007/978-3-642-62012-6Search in Google Scholar

[11] J. F. Dillon, Elementary Hadamard Difference-Sets. PhD thesis, Univ. of Maryland 1974. MR2624542 Zbl 0346.05003Search in Google Scholar

[12] R. H. Dye, Partitions and their stabilizers for line complexes and quadrics. Ann. Mat. Pura Appl. (4) 114 (1977), 173–194. MR0493729 Zbl 0369.5001210.1007/BF02413785Search in Google Scholar

[13] M. Grassl, Unextendible sets of mutually unbiased bases (MUBs). Talk at “Systems of Lines, Applications of Algebraic Combinatorics”, Conference at Worcester Polytechnic Institute, August 10–14, 2015.Search in Google Scholar

[14] B. Huppert, N. Blackburn, Finite groups. III. Springer 1982. MR662826 Zbl 0514.2000210.1007/978-3-642-67997-1Search in Google Scholar

[15] W. M. Kantor, Ovoids and translation planes. Canad. J. Math. 34 (1982), 1195–1207. MR675685 Zbl 0467.5100410.4153/CJM-1982-082-0Search in Google Scholar

[16] W. M. Kantor, Codes, quadratic forms and finite geometries. In: Different aspects of coding theory (San Francisco, CA, 1995), volume 50 of Proc. Sympos. Appl. Math., 153–177, Amer. Math. Soc. 1995. MR1368640 Zbl 0867.9403610.1090/psapm/050/1368640Search in Google Scholar

[17] W. M. Kantor, MUBs inequivalence and affine planes. J. Math. Phys. 53 (2012), 032204. MR2798212 Zbl 1274.4605910.1063/1.3690050Search in Google Scholar

[18] W. M. Kantor, M. E. Williams, Symplectic semifield planes and ℤ4-linear codes. Trans. Amer. Math. Soc. 356 (2004), 895–938. MR1984461 Zbl 1038.5100310.1090/S0002-9947-03-03401-9Search in Google Scholar

[19] G. Lunardon, Partial ovoids and generalized hexagons. In: Finite geometry and combinatorics (Deinze, 1992), volume 191 of London Math. Soc. Lecture Note Ser., 233–248, Cambridge Univ. Press 1993. MR1256280 Zbl 0792.5100510.1017/CBO9780511526336.024Search in Google Scholar

[20] P. Mandayam, S. Bandyopadhyay, M. Grassl, W. K. Wootters, Unextendible mutually unbiased bases from Pauli classes. Quantum Inf. Comput. 14 (2014), 823–844. MR324227010.26421/QIC14.9-10-8Search in Google Scholar

[21] T. Penttila (unpublished).Search in Google Scholar

[22] T. Penttila, B. Williams, Ovoids of parabolic spaces. Geom. Dedicata82 (2000), 1–19. MR1789057 Zbl 0969.5100810.1023/A:1005244202633Search in Google Scholar

[23] V. Pepe, C. Rössing, L. Storme, A spectrum result on maximal partial ovoids of the generalized quadrangle 𝒬(4, q), q odd. In: Finite fields: theory and applications, volume 518 of Contemp. Math., 349–362, Amer. Math. Soc. 2010. MR2648559 Zbl 1235.5101410.1090/conm/518/10217Search in Google Scholar

[24] C. Rössing, L. Storme, A spectrum result on maximal partial ovoids of the generalized quadrangle Q(4,q), q even. European J. Combin. 31 (2010), 349–361. MR2552614 Zbl 1190.5100510.1016/j.ejc.2009.01.003Search in Google Scholar

[25] M. Suzuki, On a class of doubly transitive groups. Ann. of Math. (2) 75 (1962), 105–145. MR0136646 Zbl 0106.2470210.2307/1970423Search in Google Scholar

[26] D. E. Taylor, The geometry of the classical groups. Heldermann 1992. MR1189139 Zbl 0767.20001Search in Google Scholar

[27] J. A. Thas, Old and new results on spreads and ovoids of finite classical polar spaces. In: Combinatorics 90 (Gaeta, 1990), volume 52 of Ann. Discrete Math., 529–544, North-Holland 1992. MR1195834 Zbl 0767.5100410.1016/S0167-5060(08)70936-1Search in Google Scholar

[28] K. Thas, Unextendible mutually unbiased bases (after Mandayam, Bandyopadhyay, Grassl and Wootters). Entropy18 (2016), 395. arXiv:1402.2778v1 [quant-ph]10.3390/e18110395Search in Google Scholar

[29] J. Tits, Sur la trialité et certains groupes qui s’en déduisent. Inst. Hautes Études Sci. Publ. Math. no. 2 (1959), 13–60. MR1557095 Zbl 0088.3720410.1007/BF02684706Search in Google Scholar

[30] J. Tits, Ovoϊ des à translations. Rend. Mat. e Appl. (5) 21 (1962), 37–59. MR0143086 Zbl 0107.38103Search in Google Scholar

[31] J. Tits, Ovoϊ des et groupes de Suzuki. Arch. Math. 13 (1962), 187–198. MR0140572 Zbl 0109.3940210.1007/BF01650065Search in Google Scholar

Appendices

A Mutually unbiased bases

Equip ℂN with its usual hermitian inner product (,). Orthonormal bases 𝓑1 and 𝓑2 are called mutually unbiased if |(u1, u2)| = 1/N whenever ui ∈ 𝓑i for i = 1, 2. Any set of MUBs (mutually unbiased bases) has size at most N + 1.

For a prime p set V = Zpn (row vectors) with its usual dot product xy. Consider ℂN, N = pn, with the standard basis labeled 𝓑 := {ev|vV} and the usual hermitian inner product (,). Let ζ ∈ ℂ be a primitive pth root of unity (so that ζ = −1 if p = 2).

The MUBs mentioned in Section 1 can be described using sets 𝓢 of symmetric n × n matrices M such that the difference of any two is nonsingular; explicit sets 𝓢 are in [4; 17; 13]. Each partial symplectic spread Σ can be written (after a choice of bases) as the subspaces of VV of the form O ≥ V or (V ≥ O) (IMOI) for M varying through a set 𝓢 as above. (The alternating bilinear form is ((x, y), (x′, y′)) = xy′ − x′ ⋅ y.)

Let QM : V → ℤp be a quadratic form associated with the symmetric bilinear form uMv on V, so that QM(u + v) = QM(u) + QM(v) + uMv for all u, vV. If p > 2 then QM(v) = vMv/2. If p = 2 use QM(v) = vUMv, where UM is obtained from M by replacing all entries below the diagonal by 0. If

F(Σ):={B,BMS|MS},BMS:={1NvVζav+QM(v)ev|aV},(A.1)

then 𝓕(Σ) is a set of MUBs when p > 2. If p = 2 then 𝓕 (Σ) is a set of real MUBs (i.e., in ℝN) provided that Σ is an orthogonal partial spread. Using the quadratic form Q((x, y)) = xy this means that 𝓢 consists of skew-symmetric matrices M (i.e., symmetric with zero diagonal, so that Q((x, xM)) = 0).

Complex MUBs also arise when p = 2. Let

B^MS:={1NvVi2a^v^+v^M^v^ev|aV},(A.2)

where “hats” denote that the vector or matrix has entries 0, 1 viewed inside4 (so that a^,v^Z4n). Then {B,B^MS|MS} is again a set of MUBs.

See [4; 17] for proofs and the related finite group framework. Our maximal symplectic partial spreads produce sets of MUBs that are maximal within that framework. It is not at all clear that these are also maximal as sets of MUBs in ℂN, though this may be the case if Σ is sufficiently large.

B Desarguesian ovoids in O+(8, q)-space

In order to prove Theorem 7.3 we will consider a specific orthogonal ovoid in an O+(8, q)-space with q > 2 even. Let F = 𝔽q3K = 𝔽q, with trace map T: FK and norm N: FK. Then Q(a, β, γ, d):= ad + T(βγ) turns V := KFFK into an O+(8, q)-space.

The q3 + 1 points 〈(0,0,0,1)〉 and 〈(1, t, tq + q2, N(t))〉, tF, form an ovoid Ω on which G := SL(2, q3) acting 3-transitively. In [15, p. 1204] this is called a desarguesian ovoid (since it arises from a desarguesian spread of an Sp(6, q)-space using Lemma 6.1(ii) and triality), and it is observed that G has exactly two orbits of singular points of V, one of which is Ω. If q > 2 and p is any singular point not in Ω, then 〈pΩ〉 = p [15, p. 1204], as required in Lemma 7.1.

Notation B.1

Let πF with T(π) = 0 ≠ T(π1+q). Use the nondegenerate symmetric K-bilinear form T(xy) on F to see that πq ∉ {tFT(πt) = 0} = K + Kπ.

Lemma B.2

Ifp1andp2are distinct singular points not inΩ, then|p1p2Ω|5q5.

Proof

By the transitivity of G we may assume that p1 = 〈(0, 0, π, 0)〉 and p2 = 〈(a, β, γ, d)〉 for some a, β, g, d. We need to estimate the number of solutions t to the equations

T(tπ)=0=aN(t)+d+T(βtq+q2+γt)

corresponding to points 〈(1, t, tq + q2, t1+q+q2)〉. By (B.1) we can write t = u + vπ with u, vK. Then the second equation is

aN(u+vπ)+d+T(β[u+vπ]q+q2+γ[u+vπ])=0,

which expands to

a{u3+uv2T(πq+q2)+v3N(π)}+d+u2T(β)+uvT(βπ)+v2T(βπq+q2)+uT(γ)+vT(γπ)=0.(B.3)

For each u this is a K-polynomial in v of degree at most three, and hence has at most three roots vK if it is not the zero polynomial. Let B be the number of “bad” u for which this polynomial in v is the zero polynomial. Then |p1p2Ω|(qB)3+Bq+1 (the last term occurs since 〈(0, 0, 0, 1)〉 may be in the intersection). We will show that B ≤ 2, which produces the bound in the lemma.

The coefficients of our polynomial show that, for a “bad” u, we must have aN(π) = 0, T(βπq + q2) = 0, uT(βπ) + T(γπ) = 0 and u2T(β) + uT(γ) + d = 0. If T(βπ) ≠ 0 then there is one “bad” u, while if T(βπ ) = T(γπ) = 0 then there are at most two “bad” u unless T(β) = T(γ) = d = 0.

Thus, we must show that T(βπq + q2) = T(βπ) = T(γπ) = T(β) = T(γ) = 0} cannot all occur. Since T(β) =T(βπ) = 0, by (B.1) we have β = xπ with xK. Then 0 = T(βπq + q2)= xT(N(π)), so that x = 0. Similarly, since T(γ) = T(γπ) = 0 we have γ = yπ with yK. Now p2=〈(0, 0, yπ, 0)〉 = p1, which is not the case.□

Notation B.4

Let Ω0Ω consist of 〈(0, 0, 0, 1) 〉 and 〈(1, t, tq + q2, t1+q+q2)〉, tK. There are (q + 1)2 singular points in Ω0, all having the form 〈(0, β, γ, 0)〉 with T(β) = T(γ) = T(βγ) = 0. The sets Ω0 and Ω0 are acted on by a naturally embedded subgroup G0 = SL(2, q) of G containing the transformations

us:(a,β,γ,d)(a,β+sa,γ+as2+βqs+βq2s,d+as3+T(β)s2+T(γ)s)j:(a,β,γ,d)(d,γ,β,a)

with sK. These act on each of the q + 1 lines 〈(0, β, 0, 0), (0, 0,β, 0) 〉 with T(β) = 0 ≠ β that partition the (q + 1)2 singular points in Ω0, sending

us:(0,β,γ,0)(0,β,γ+βs,0)j:(0,β,γ,0)(0,γ,β,0).(B.5)

Definition B.6

An ordinary point is a singular point in Ω0 of the form 〈(0, β, γ, 0)〉 such that either β = 0 and T(γ1+q) ≠ 0, or T(β1+q) ≠ 0 (recall that T(β) = T(γ) = T(βγ) = 0 ). Since any βF* has characteristic polynomial x3 + T(β) x2 + T(β1+q)x + N(β), the ordinary requirement can fail for some β, γ if and only if q ≡ 1 (mod 3). Moreover, if βF-K then {βqβK} ⇔ {βq − 1K} ⇔ β(q − 1, q2 + q + 1)Kβ3KT(β1+q) = 0.

For π in (B.1), since T((aπ + πq)(aπ + πq) q) = (a2 + a + 1) T (π1+q) all points of the line 〈(0, aπ + πq, 0, 0), (0, 0, aπ + πq, 0) 〉, aK, are ordinary if and only if a2 + a + 1 ≠ 0, so that all points are ordinary if q ≡ 2 (mod 3), but there are two lines of this form all of whose points are not ordinary when q ≡ 1 (mod 3).

The significance of ordinary points is the following

Lemma B.7

Ifpis an ordinary point then

  1. p has the form 〈(0, 0, γ, 0)〉 withT(γ) = 0 or 〈(0, β, aβ, 0)〉 withT(β) = 0 andaK, and

  2. pg = 〈(0, 0, π′, 0)〉 for some gG0, whereπbehaves asπdoes in (B.1): T(π′) = 0 ≠ T(π′1+q).

Proof

We may assume that p = 〈(0, β, γ, 0)〉 with β ≠ 0.

  1. Since p is ordinary, we have seen that βqKβ, so that β and βq span kerT. Write γ = kβ + bβq with k, bK. Then 0 = T(βγ) = bT(β1+q) implies that b = 0.

  2. By (B.5), pukj = 〈(0, 0, β, 0)〉 behaves as stated.□

Lemma B.8

Ifp1, p2andp3are pairwise non-perpendicular ordinary points, then

  1. |Qp1p2Ω|=2qand

  2. |p1p2p3Ω|=q+2.

Proof

By Lemma B.7(ii) we may assume that p1 has the form 〈(0, 0, π, 0)〉 and p2 = 〈(0, β, γ, 0)〉, where T(β) = T(γ) = T(βγ) = 0. Also T(βπ) ≠ 0 since p1 and p2 are not perpendicular. All (0, 0, 0, 1) and (1, t, tq + q2, N(t)), tK, are in each of the stated intersections, so we will focus on vectors (1, t, tq + q2, N(t)) with t = u + vπK that lie in an intersection.

  1. Here (B.3) states that

    uvT(βπ)+v2T(βπq+q2)+vT(γπ)=0.(B.9)

    Since T(βπ) ≠ 0, each v ≠ 0 determines a unique u. This argument reverses: the intersection size is (q + 1) + (q − 1).

    Before continuing we massage (B.9). By Lemma B.7(i), γ = kβ for some kK. Since dim ker T = 2 we can write β = xπ + yπq with x, yK. Since 0 ≠ T(βπ) = yT(π1+q) we have y ≠ 0 and β ∈ ((x/y)π + πq)K. We may assume that β = aπ + πq with aK. Then

    p2=(0,aπ+πq,k(aπ+πq),0).(B.10)

    Also T(βπ) = T(π1+q), so that (B.9) becomes

    uT(π1+q)+v[aN(π)+T(π2q+q2)]+kT(π1+q)=0.(B.11)
  2. We may assume that p3 = 〈(0, β′, γ′, 0〉) with γ′ = kβ′ and β′ = aπ + πq for some k′, a′ ∈ K. Then (a + a′)(k + k′) T (ππq) = T(βγ′ + γβ′) ≠ 0 since p2 and p3 are not perpendicular. Then aa′, and the two versions of (B.11) imply that

    v=k+ka+aT(π1+q)N(π),u=k+k+ka+a(a+T(π2q+q2)N(π)),(B.12)

    which proves (ii). □

Example B.13

  1. If 𝓢 ⊆ {〈(0, 0, π, 0)〉, 〈(0, aπ + πq, a2π + aπq, 0)〉 ∣ {aK, a2 + a + 1 ≠ 0}, then

    |pSpΩ|=q2+1if|S|=12qif|S|=2q+2if|S|3.
  2. If 𝓢 ⊆ {〈(0, 0, π, 0)〉, 〈(0, πq, 0, 0)〉, 〈(0, π + πq, π + πq, 0)〉, 〈(0, aπ + πq, a3π + a2πq, 0)〉} for an arbitrary aK − {0, 1} such that a2 + a + 1 ≠ 0, then

    |pSpΩ|=q2+1if|S|=12qif|S|=2q+2if|S|=3q+1if|S|=4.

Proof

All of the stated points are ordinary. Since |pΩ| = q2 + 1 [15, p. 1204], we will assume that |𝓢| ≥ 2.

  1. In (B.10), k = a for all listed points other than 〈(0, 0, π, 0)〉. By (B.12), t=T(π2q+q2)N(π)+T(π1+q)N(π)π is in every intersection (which is easily checked directly); so is Ω0, so that every intersection has size ≥ q + 2. Since any intersection of three sets pΩ has size q + 2 (by Lemma B.8(ii)), so does any intersection of at least four such sets.

  2. The last three of these four ordinary points correspond to the pairs (a, k) = (0, 0), (1, 1), (a, a2) in (B.10). Then (B.12) and different 3-sets in 𝓢 produce different values of v, so that {|⋂p∈ 𝓢pΩ|} = q + 1 if |𝓢| = 4. The remaining sizes are given in Lemma B.8.

C Suzuki–Tits ovoids: background

We will need information concerning a Suzuki–Tits ovoid Ω in an O(5, q)-space U with radical r, where q = 22e+1. The standard view of these ovoids is in symplectic space. For our purposes, the view from an O(5, q)-space has advantages, such as lying in an O+(8, q)-space.

Let Ω denote a standard Suzuki–Tits ovoid in the symplectic 4-space U/r [31]. If 〈x, r〉/rΩ then the line 〈x, r〉 has a unique singular point. Thus, there is a set Ω of q2 + 1 singular points of U that projects onto Ω. The group Sz(q) lifts from a subgroup of Sp(4, q) to a group G < O(5, q) preserving Ω.

See [10, Section 6.4] for information concerning the inversive plane 𝓙(Ω) produced by Ω.

We will assume that q > 2. Then U = 〈Ω〉 since G does not act on an O±(4, q)-space. (If q = 2 then Ω spans an O(4,2)-space.)

Lemma C.1

Every hyperplane meetsΩ. More precisely, there are exactly five G-orbits of hyperplanesHof U:

  1. Tangent hyperplanes H = pfor pΩ, withrHand HΩ = {p};

  2. Secant hyperplanes H = xcontainingr, where xis a singular point not inΩ, xΩis a circle of 𝓙(Ω) andxΩ〉 = x;

  3. O(4, q)-hyperplanes H for which HΩis an orbit of a cyclic subgroup ofGof order |HΩ| = q ± 2q + 1 acting irreducibly on U/ r; and

  4. O+(4, q)-hyperplanes Hfor whichHΩcontains an orbit of a cyclic subgroup of G of order |HΩ| − 2 = q − 1 that fixes two points of HΩ. Moreover, HΩis not one of the circles in (ii).

Proof

  1. Projecting mod r shows that each point of Ω behaves as stated.

  2. If x is a singular point not in Ω then each of the q + 1 t.s. lines on x meets Ω since Ω is an ovoid, so that |xΩ| = q + 1. Also, dim〈xΩ〉 = 4, as otherwise xΩ would project into a plane of U/r, and hence be contained in a conic, which is not the case since q > 2 [30, pp. 51–52]. Since 〈xΩ〉 lies in the 4-space x, these subspaces coincide.

  3. This is [2, Theorem 1(a)].

  4. The set of singular points of H is partitioned by q + 1 t.s. lines, and each t.s. line of U meets Ω since Ω is an ovoid. Thus, |HΩ| = q + 1.

We use the orbits of G to find GH. There are exactly two point-orbits on U/r: Ω and the remaining q(q2 + 1) points. There is a subgroup of G of order q − 1 that fixes four points of U/r and induces all scalars on each of these 1-spaces [14, P. 183]. Since each line containing r has a unique singular point, the two point-orbits on U/r produce four point-orbits on U − {r}.

Since G has five point-orbits it also has five hyperplane-orbits, so that all q2(q2 + 1)/2 hyperplanes H in (iv) lie in an orbit. Then |GH| = |G|/[q2(q2 + 1)/2] = 2(q − 1), so that GH is dihedral of order 2(q − 1), with orbits of size 2 and q − 1 on Ω [25, Theorem 9].

For the final assertion, if HΩ lies in two hyperplanes then it is in a plane, and hence is a conic, whereas in (ii) we already saw that 〈xΩ〉 = x.□

Remarks C.2

Finally, we collect elementary properties of the group T appearing in Lemma C.1(iv). Consider the action of G = Sz(q) on Ω.

  1. The stabilizer of a circle has order q(q − 1) [25, Theorem 9] and fixes a unique point c. Here Gc is a Frobenius group of order q2(q − 1).

  2. A subgroup T of order q − 1 fixes two points c, dΩ and has q + 1 other orbits on Ω of size q − 1.

If 1 ≠ tT then t fixes exactly two circles: it lies in a unique subgroup of order q(q − 1) of the Frobenius group Gc (or Gd). If C is either of these circles then T is transitive on C − {c, d}.

Received: 2016-1-13
Published Online: 2017-10-16
Published in Print: 2017-10-26

© 2017 by Walter de Gruyter Berlin/Boston

Downloaded on 13.12.2025 from https://www.degruyterbrill.com/document/doi/10.1515/advgeom-2017-0033/html
Scroll to top button