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Multicomplex Configurations in Algebra

Updated 6 July 2026
  • Multicomplex configurations are specialized projective varieties built from polarizing Artinian monomial ideals, ensuring controlled Gröbner bases and combinatorial invariants.
  • The construction uses finite divisor-closed sets of c-monomials with polarization to transform ideals, followed by substituting homogeneous forms to form configuration ideals.
  • These ideals are Cohen–Macaulay, preserve graded Betti numbers, and lie in the Gorenstein liaison class of a complete intersection, with explicit primary decompositions.

Searching arXiv for the specified paper and closely related work on multicomplex structures and configurations. Multicomplex configurations are a class of projective varieties constructed via specialization of the polarizations of Artinian monomial ideals. In the formulation of "Multicomplex Configurations: a case study in Gorenstein Liaison" (Klein et al., 14 Jul 2025), the basic input is a finite divisor-closed set of bounded monomials, together with ordered families of homogeneous forms used to substitute for the polarization variables. Under suitable xix_i-initial hypotheses and a distinctness condition on the induced complete intersections, the resulting ideals admit Gröbner bases with prescribed initial ideals, have irredundant primary decompositions by linear-space ideals, are Cohen–Macaulay, preserve graded Betti numbers, and lie in the Gorenstein liaison class of a complete intersection.

1. Combinatorial input: cc-multicomplexes and Artinian monomial ideals

The theory is developed over an infinite field KK, with polynomial rings

R=K[x1,,xn]S=K[x1,,xm],mn,R = K[x_1,\ldots,x_n] \subseteq S = K[x_1,\ldots,x_m], \qquad m \ge n,

and with a fixed monomial order << on SS refining x1>x2>>xmx_1>x_2>\cdots>x_m (Klein et al., 14 Jul 2025).

For c=(c1,,cn)Nnc=(c_1,\ldots,c_n)\in\mathbb N^n, a cc-monomial in RR is a monomial cc0 with cc1. A finite set cc2 of cc3-monomials is a cc4-multicomplex if whenever cc5 and cc6, then cc7. The associated monomial ideal is

cc8

Because cc9 is closed under divisors, KK0 is an Artinian, in fact zero-dimensional, KK1-algebra whose standard monomials are exactly those in KK2 (Klein et al., 14 Jul 2025).

Polarization provides the squarefree model behind the construction. One introduces new variables KK3 and replaces each KK4 by the product KK5. This produces a squarefree monomial ideal KK6 in

KK7

The multicomplex configuration is then obtained by specializing these polarization variables to homogeneous forms in a larger polynomial ring.

2. Configuration ideals by specialization of polarization

Fix a KK8-multicomplex KK9. For each R=K[x1,,xn]S=K[x1,,xm],mn,R = K[x_1,\ldots,x_n] \subseteq S = K[x_1,\ldots,x_m], \qquad m \ge n,0, choose an ordered collection of homogeneous forms

R=K[x1,,xn]S=K[x1,,xm],mn,R = K[x_1,\ldots,x_n] \subseteq S = K[x_1,\ldots,x_m], \qquad m \ge n,1

all of the same degree, and set R=K[x1,,xn]S=K[x1,,xm],mn,R = K[x_1,\ldots,x_n] \subseteq S = K[x_1,\ldots,x_m], \qquad m \ge n,2. If R=K[x1,,xn]S=K[x1,,xm],mn,R = K[x_1,\ldots,x_n] \subseteq S = K[x_1,\ldots,x_m], \qquad m \ge n,3 denotes the minimal set of monomial generators of R=K[x1,,xn]S=K[x1,,xm],mn,R = K[x_1,\ldots,x_n] \subseteq S = K[x_1,\ldots,x_m], \qquad m \ge n,4, the multicomplex configuration ideal determined by R=K[x1,,xn]S=K[x1,,xm],mn,R = K[x_1,\ldots,x_n] \subseteq S = K[x_1,\ldots,x_m], \qquad m \ge n,5 is

R=K[x1,,xn]S=K[x1,,xm],mn,R = K[x_1,\ldots,x_n] \subseteq S = K[x_1,\ldots,x_m], \qquad m \ge n,6

Equivalently, one first forms the polarization R=K[x1,,xn]S=K[x1,,xm],mn,R = K[x_1,\ldots,x_n] \subseteq S = K[x_1,\ldots,x_m], \qquad m \ge n,7, then applies the R=K[x1,,xn]S=K[x1,,xm],mn,R = K[x_1,\ldots,x_n] \subseteq S = K[x_1,\ldots,x_m], \qquad m \ge n,8-algebra map R=K[x1,,xn]S=K[x1,,xm],mn,R = K[x_1,\ldots,x_n] \subseteq S = K[x_1,\ldots,x_m], \qquad m \ge n,9 to obtain <<0 as the image of <<1 (Klein et al., 14 Jul 2025).

A basic example takes

<<2

so that

<<3

In <<4, choose

<<5

Then

<<6

For this choice, <<7 is four points in <<8, each cut out by one of the pairwise-distinct ideals

<<9

(Klein et al., 14 Jul 2025).

3. Gröbner bases, initial ideals, and primary decomposition

The central Gröbner-theoretic hypotheses are that each SS0 is SS1-initial, meaning that for every SS2,

SS3

and that the complete intersection ideals

SS4

for SS5 with SS6 are all distinct. Under these assumptions, Theorem 3.1 gives three structural conclusions (Klein et al., 14 Jul 2025).

First,

SS7

Second, the collection

SS8

is a Gröbner basis of SS9. Third,

x1>x2>>xmx_1>x_2>\cdots>x_m0

is the irredundant primary decomposition.

The proof proceeds through a chain of inclusions and numerical equalities. For each minimal generator x1>x2>>xmx_1>x_2>\cdots>x_m1,

x1>x2>>xmx_1>x_2>\cdots>x_m2

so x1>x2>>xmx_1>x_2>\cdots>x_m3. If x1>x2>>xmx_1>x_2>\cdots>x_m4, then for each x1>x2>>xmx_1>x_2>\cdots>x_m5 at least one coordinate satisfies x1>x2>>xmx_1>x_2>\cdots>x_m6, so x1>x2>>xmx_1>x_2>\cdots>x_m7 divides x1>x2>>xmx_1>x_2>\cdots>x_m8; consequently every x1>x2>>xmx_1>x_2>\cdots>x_m9 lies in

c=(c1,,cn)Nnc=(c_1,\ldots,c_n)\in\mathbb N^n0

and hence c=(c1,,cn)Nnc=(c_1,\ldots,c_n)\in\mathbb N^n1. The argument then uses the fact that both chains of inclusions

c=(c1,,cn)Nnc=(c_1,\ldots,c_n)\in\mathbb N^n2

preserve codimension c=(c1,,cn)Nnc=(c_1,\ldots,c_n)\in\mathbb N^n3 and degree c=(c1,,cn)Nnc=(c_1,\ldots,c_n)\in\mathbb N^n4, which forces equality throughout (Klein et al., 14 Jul 2025).

These equalities have immediate geometric consequences. Since c=(c1,,cn)Nnc=(c_1,\ldots,c_n)\in\mathbb N^n5 is Cohen–Macaulay of codimension c=(c1,,cn)Nnc=(c_1,\ldots,c_n)\in\mathbb N^n6, the ideal c=(c1,,cn)Nnc=(c_1,\ldots,c_n)\in\mathbb N^n7 is also Cohen–Macaulay. Moreover, each primary component has degree c=(c1,,cn)Nnc=(c_1,\ldots,c_n)\in\mathbb N^n8, so

c=(c1,,cn)Nnc=(c_1,\ldots,c_n)\in\mathbb N^n9

Thus the specialization preserves both a combinatorial counting invariant and a rigid linear-space decomposition.

4. Gorenstein liaison and the inductive mechanism

A principal result is that cc0 is in the Gorenstein liaison class of a complete intersection, or glicci. The proof is by double induction on cc1 and on cc2, and it uses geometric polarization, geometric vertex decomposition, and elementary G-biliaison (Klein et al., 14 Jul 2025).

For one-step geometric polarization, fix a variable cc3 and a polynomial

cc4

with cc5 and no cc6 divisible by cc7. Introducing a new variable cc8, define

cc9

If RR0 is a Gröbner basis of an ideal RR1 all of whose leading terms come from the RR2-part, then RR3 is a Gröbner basis of the polarized ideal in RR4, provided RR5 remains a nonzerodivisor.

For geometric vertex decomposition, with RR6 fixed and the term order RR7-compatible, suppose RR8 admits a Gröbner basis of the form

RR9

with no lead term divisible by cc00 except the cc01. Then

cc02

where

cc03

is the geometric link and

cc04

is the geometric deletion.

Elementary G-biliaison is formulated for unmixed Cohen–Macaulay ideals cc05 of the same height, with cc06 a Cohen–Macaulay cc07 ideal such that

cc08

and such that there is a graded isomorphism

cc09

over cc10. Such a step sits inside two direct G-links, hence preserves glicci.

The inductive proof for multicomplex configurations splits into two cases. If cc11 divides every minimal generator of cc12, one peels off the linear form cc13 and reduces to the case cc14. Otherwise, one applies one-step polarization in the cc15-direction to the Gröbner basis cc16. In this situation, cc17 is regular, the geometric link is the configuration ideal for the smaller multicomplex

cc18

in the ring with variable cc19, and the geometric deletion is the configuration for

cc20

Both cc21 and cc22 have strictly smaller size or support, so by induction their configuration ideals are glicci. The resulting elementary G-biliaison links cc23 to these smaller ideals, and this yields the glicci property for cc24 (Klein et al., 14 Jul 2025).

5. Invariants, Betti numbers, and the model example

The summary theorem packages the principal invariants of the construction. If cc25 is a cc26-multicomplex, cc27 is a monomial order on cc28 refining cc29, and for each cc30 one chooses an cc31-initial set of linear forms

cc32

such that the complete-intersection ideals

cc33

are pairwise distinct, then cc34 satisfies the following properties (Klein et al., 14 Jul 2025):

  1. cc35 is an irredundant intersection of linear-space ideals of codimension cc36.
  2. cc37 is a Gröbner basis and cc38.
  3. cc39, cc40, and cc41 is Cohen–Macaulay.
  4. cc42 is in the Gorenstein liaison class of a complete intersection.
  5. The graded Betti numbers are preserved: cc43

The Betti-number statement is attributed to the usual distraction arguments: because each cc44 is cc45-initial, the graded Betti numbers of cc46 in cc47 coincide with those of cc48 in cc49. This makes the construction a specialization that is geometrically nontrivial but homologically controlled.

The running example illustrates all of these statements concretely. For

cc50

one has

cc51

cc52

and

cc53

The ideal is Cohen–Macaulay, and one-step polarization in cc54 introduces cc55 and leads to a G-biliaison linking cc56 to two smaller configurations, each of which is a complete intersection or known to be glicci; hence cc57 is glicci (Klein et al., 14 Jul 2025).

In this subject, “multicomplex configuration” refers specifically to the algebraic-geometric construction obtained by specializing polarizations of Artinian monomial ideals (Klein et al., 14 Jul 2025). The term “multicomplex,” however, has broader usage across several research areas.

In commutative algebra and algebraic structures, the purely complex-signature family cc58 is exactly the classical multicomplex algebra cc59 of Segre–Price, and more generally commutative analogues of Clifford algebras are either isomorphic to a multicomplex space or to a multi split-complex space (Sharma et al., 28 Apr 2025). In complex dynamics, multicomplex numbers support Multibrot and Julia theories: every multicomplex tridimensional principal slice of the Multibrot sets is equivalent to a tricomplex slice up to an affine transformation (Brouillette et al., 2018), while for filled-in Julia sets associated to cc60 there are four principal 3D-slice classes when cc61 is even and eight or nine when cc62 is odd, depending on cc63 and cc64 (Charles et al., 2 May 2025). In homological topology, a first-quadrant multicomplex is a bigraded module

cc65

with maps

cc66

satisfying

cc67

and the Morse–Bott multicomplex combines singular cubical chains and Morse chains in the same multicomplex (Hurtubise, 2012).

This suggests that the qualifier “configuration” is not a generic synonym for multicomplex structures, but a designation for a particular liaison-theoretic and Gröbner-theoretic specialization framework. Within that framework, the main significance of the theory is that it transfers combinatorial data from a cc68-multicomplex to a projective configuration while retaining controlled initial ideals, explicit primary decompositions, Cohen–Macaulayness, glicci behavior, and the graded Betti numbers of the originating Artinian monomial ideal (Klein et al., 14 Jul 2025).

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