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(V1(v(¯x11),...,v(¯x1k),y1),...,V t(v(¯xt1),...,v(¯xtk),yt)) = ¯µ,
(H1(h(¯x11),...,h(¯xt1),z1),...,H k(h(¯x1k),...,h(¯xtk),zk))∈C#/bracerightBig
is a¯µ-component that satisfies the generalized parity-check law with
σi(·,...,·,·) =Vi(v(·),...,v(·),·).
5(The elements of F(q−1)kt+k+t
q in this construction may be thought of as three-dimensional
arrays where the elements of ¯xijare z-lined, every underlined block is y-lined, and the
tuple of blocks is x-lined. Naturally, the multary quasigroups Vimay be named “vertical”
andHi, “horizontal”.)
The proof of the code distance is similar to that in [9], and the other pr operties of a
¯µ-component are straightforward. The existence of admissible ( q−1)-ary quasigroups v
andhis the only restriction on the q(this concerns the next subsection as well). If Fqis
a finite field, there are linear examples: v(y1,...,y q−1) =y1+...+yq−1,v(y1,...,y q−1) =
α1y1+...+αq−1yq−1whereα1, ...,αq−1are all the non-zero elements of Fq. Ifqis not
a prime power, the existence of a q-ary perfect code of length q+1 is an open problem
(with the only exception q= 6, when the nonexistence follows from the nonexistence of
two orthogonal 6 ×6 Latin squares [1, Th.6]).
3.2. Generalized Phelps construction
Here we describe another way to construct ¯ µ-components, which generalizes the construc-
tion of binary perfect codes from [8].
Lemma 2. Let¯µ∈Ft
q. Let for every ifrom1tot+1the codesCi,j,j= 0,1,...,qk−k
form a partition of Fk
qinto perfect codes and γi:Fk
q→ {0,1,...,qk−k}be the corre-
sponding partition function:
γi(¯y) =j⇐⇒¯y∈Ci,j.
Letvandhbe(q−1)-ary quasigroups of order qsuch that the code {(¯y|v(¯y)|h(¯y)) :
¯y∈Fq−1
q}is perfect. Let V1, ...,Vtbe(k+ 1)-ary quasigroups of order qandQbe a
t-ary quasigroup of order qk−k+1.
K¯µ=/braceleftBig
(¯x11|...|¯x1k|y1|¯x21|...|¯x2k|y2|...|¯xt1|...|¯xtk|yt|z1|z2|...|zk) :
¯xij∈Fq−1
q,
(V1(v(¯x11),...,v(¯x1k),y1),...,V t(v(¯xt1),...,v(¯xtk),yt)) = ¯µ,
Q(γ1(h(¯x11),...,h(¯x1k)),...,γ t(h(¯xt1),...,h(¯xtk))) =γt+1(z1,...,zk)/bracerightBig
is a¯µ-component that satisfies the generalized parity-check law with
σi(·,...,·,·) =Vi(v(·),...,v(·),·).
The proof consists of trivial verifications.
4. On the number of perfect codes
In this section we discuss some observations, which result in the bes t known lower bound
on the number of q-ary perfect codes, q≥3. The basic facts are already contained in
other known results: lower bounds on the number of multary quasig roups of order q, the
6construction [9] of perfect codes from multary quasigroups of or derq, and the possibility
to choose the quasigroup independently for every vector of the o uter code (this possibility
was not explicitly mentioned in [9], but used in the previous paper [8]).
A general lower bound, in terms of the number of multary quasigrou ps, is given by
Lemma 3. In combination with Lemma 4, it gives explicit numbers.
Lemma 3. The number of q-ary perfect codes of length nis not less than
Q/parenleftBiggn−1
q,q/parenrightBiggRn−1
q
whereQ(m,q)is the number of m-ary quasigroups of order qand whereRn′=qn′/(n′q−
q+1)is the cardinality of a perfect code of length n′.
Proof. Constructing a perfect code like in Theorem 2 with t=n−1
q, we combine
Rn−1
qdifferent ¯µ-components.
Constructing every such a component as in Lemma 2, k= 1,t=n−1
q, we are free
to choose the t-ary quasigroup Qof orderqinQ(t,q) ways. Clearly, different t-ary
quasigroups give different components. (Equivalently, we can use L emma 1 and choose
the (t+1)-ary quasigroup H1, but should note that the value of H1in the construction is
always fixed when k= 1, because C#consists of only one vertex; so we again have Q(t,q)
different choices, not Q(t+1,q)). △
Lemma 4. The number Q(m,q)ofm-ary quasigroups of order qsatisfies:
(a) [5]Q(m,3) = 3·2m;
(b) [11]Q(m,4) = 3m+1·22m+1(1+o(1));
(c) [4]Q(m,5)≥23n/3−0.072;
(d) [10]Q(m,q)≥2((q2−4q+3)/4)n/2for oddq(the previous bound [4]wasQ(m,q)≥
2⌊q/3⌋n);
(e) [4]Q(m,q1q2)≥Q(m,q1)·Q(m,q2)qm
1.
For oddq≥5, the number of codes given by Lemmas 3 and 4(c,d) improves the
constantcin the lower estimation of form eecn(1+o(1))for the number of perfect codes, in
comparison with the last known lower bound [6]. Informally, this can be explained in the
following way: the construction in [6] can be described in terms of mu tually independent
small modifications of the linear multary quasigroup of order q, while the lower bounds
in Lemma 4(c,d) are based on a specially-constructed nonlinear multa ry quasigroup that
allows a lager number of independent modifications. For q= 3 andq= 2s, the number
of codes given by Lemmas 3 and 4(a,b,e) also slightly improves the boun d in [6], but do
not affect on the constant c.
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