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Pseudoregulus Type in Projective Geometry

Updated 7 July 2026
  • Pseudoregulus type is a classical family of maximum scattered Fq-linear sets defined on PG(1,q^t) and extended to higher dimensions, characterized by models like Frobenius graphs.
  • The concept is rigorously analyzed via projection, field reduction, and ring geometry, ensuring detailed descriptions of equivalence, rigidity, and transversal structures.
  • Its applications span translation planes, semifields, hyperovals, and MRD codes, establishing it as a benchmark for newer scattered linear set constructions.

Searching arXiv for recent and foundational papers on pseudoregulus type linear sets, scattered polynomials, and related translation planes. Pseudoregulus type denotes the classical family of maximum scattered Fq\mathbb F_q-linear sets that first appears on the projective line PG(1,qt)\mathrm{PG}(1,q^t) and extends to higher-dimensional spaces PG(2n−1,qt)\mathrm{PG}(2n-1,q^t). In the line case, it is represented by Frobenius-graph models such as {(λ,λq)qt:λ∈Fqt∗}\{(\lambda,\lambda^q)_{q^t}:\lambda\in \mathbb F_{q^t}^\ast\}; in the higher-dimensional case, it is characterized by a large family of pairwise disjoint weight-tt lines together with exactly two transversal (n−1)(n-1)-spaces. Across the literature, pseudoregulus type is the prototype against which later families of scattered linear sets, scattered polynomials, translation planes, and rank-metric constructions are measured (Lunardon et al., 2012, Casarino et al., 2022).

1. Classical definition and standard models

On PG(1,qt)\mathrm{PG}(1,q^t), a linear set of pseudoregulus type is, up to projective equivalence, the standard scattered set

L={(λ,λq)qt:λ∈Fqt∗}.L=\{(\lambda,\lambda^q)_{q^t}:\lambda\in\mathbb F_{q^t}^\ast\}.

Equivalent formulations replace xqx^q by xqνx^{q^\nu} with PG(1,qt)\mathrm{PG}(1,q^t)0, or by the monomial

PG(1,qt)\mathrm{PG}(1,q^t)1

with PG(1,qt)\mathrm{PG}(1,q^t)2 chosen so that

PG(1,qt)\mathrm{PG}(1,q^t)3

The associated linear set is then

PG(1,qt)\mathrm{PG}(1,q^t)4

and after a projective change of coordinates all such sets are projectively equivalent (Casarino et al., 2022, Csajbók et al., 2015).

In this line setting, pseudoregulus type is a maximum scattered PG(1,qt)\mathrm{PG}(1,q^t)5-linear set of rank PG(1,qt)\mathrm{PG}(1,q^t)6. The standard model has exactly two transversal points, namely PG(1,qt)\mathrm{PG}(1,q^t)7 and PG(1,qt)\mathrm{PG}(1,q^t)8 (Csajbók et al., 2015). For PG(1,qt)\mathrm{PG}(1,q^t)9, the prototype is

PG(2n−1,qt)\mathrm{PG}(2n-1,q^t)0

and the corresponding linear set PG(2n−1,qt)\mathrm{PG}(2n-1,q^t)1 is explicitly identified as pseudoregulus type (Csajbók et al., 2017).

In higher dimension, the notion is defined on PG(2n−1,qt)\mathrm{PG}(2n-1,q^t)2. A scattered PG(2n−1,qt)\mathrm{PG}(2n-1,q^t)3-linear set PG(2n−1,qt)\mathrm{PG}(2n-1,q^t)4 of rank PG(2n−1,qt)\mathrm{PG}(2n-1,q^t)5 is of pseudoregulus type if there exist

PG(2n−1,qt)\mathrm{PG}(2n-1,q^t)6

pairwise disjoint lines PG(2n−1,qt)\mathrm{PG}(2n-1,q^t)7 with weight PG(2n−1,qt)\mathrm{PG}(2n-1,q^t)8, and exactly two PG(2n−1,qt)\mathrm{PG}(2n-1,q^t)9-dimensional subspaces {(λ,λq)qt:λ∈Fqt∗}\{(\lambda,\lambda^q)_{q^t}:\lambda\in \mathbb F_{q^t}^\ast\}0, disjoint from {(λ,λq)qt:λ∈Fqt∗}\{(\lambda,\lambda^q)_{q^t}:\lambda\in \mathbb F_{q^t}^\ast\}1, such that each {(λ,λq)qt:λ∈Fqt∗}\{(\lambda,\lambda^q)_{q^t}:\lambda\in \mathbb F_{q^t}^\ast\}2 meets both {(λ,λq)qt:λ∈Fqt∗}\{(\lambda,\lambda^q)_{q^t}:\lambda\in \mathbb F_{q^t}^\ast\}3 and {(λ,λq)qt:λ∈Fqt∗}\{(\lambda,\lambda^q)_{q^t}:\lambda\in \mathbb F_{q^t}^\ast\}4. The family {(λ,λq)qt:λ∈Fqt∗}\{(\lambda,\lambda^q)_{q^t}:\lambda\in \mathbb F_{q^t}^\ast\}5 is the {(λ,λq)qt:λ∈Fqt∗}\{(\lambda,\lambda^q)_{q^t}:\lambda\in \mathbb F_{q^t}^\ast\}6-pseudoregulus, and {(λ,λq)qt:λ∈Fqt∗}\{(\lambda,\lambda^q)_{q^t}:\lambda\in \mathbb F_{q^t}^\ast\}7 are the transversal spaces (Lunardon et al., 2012).

2. Geometric characterizations via projection, field reduction, and ring geometry

A central characterization realizes pseudoregulus type as a projection of a canonical subgeometry. Let {(λ,λq)qt:λ∈Fqt∗}\{(\lambda,\lambda^q)_{q^t}:\lambda\in \mathbb F_{q^t}^\ast\}8 be a canonical subgeometry of {(λ,λq)qt:λ∈Fqt∗}\{(\lambda,\lambda^q)_{q^t}:\lambda\in \mathbb F_{q^t}^\ast\}9, let tt0 be a tt1-subspace disjoint from tt2, and let tt3 be a line disjoint from tt4. Then

tt5

is a scattered linear set of pseudoregulus type precisely when there exists a generator tt6 of the subgroup of tt7 fixing tt8 pointwise such that

tt9

with (n−1)(n-1)0 not contained in the span of any hyperplane of (n−1)(n-1)1. Equivalently, there exist an imaginary point (n−1)(n-1)2 and such a generator (n−1)(n-1)3 for which

(n−1)(n-1)4

and the orbit (n−1)(n-1)5 spans the ambient space (Csajbók et al., 2015). In the line case (n−1)(n-1)6, the same vertex criterion is commonly written as

(n−1)(n-1)7

or

(n−1)(n-1)8

for a generator (n−1)(n-1)9 of the pointwise stabilizer of the canonical subgeometry (Grimaldi et al., 2024).

Field reduction gives a second description. For a pseudoregulus-type linear set in PG(1,qt)\mathrm{PG}(1,q^t)0, the field-reduced image lies on the hypersurface

PG(1,qt)\mathrm{PG}(1,q^t)1

where PG(1,qt)\mathrm{PG}(1,q^t)2. This hypersurface is partitioned by PG(1,qt)\mathrm{PG}(1,q^t)3-spaces

PG(1,qt)\mathrm{PG}(1,q^t)4

and the field-reduction image of the pseudoregulus-type linear set is one such PG(1,qt)\mathrm{PG}(1,q^t)5. The same objects also appear as exterior splashes of canonical subgeometries on exterior lines (Csajbók et al., 2015).

A third characterization uses the projective line over the endomorphism ring PG(1,qt)\mathrm{PG}(1,q^t)6. If a scattered linear set PG(1,qt)\mathrm{PG}(1,q^t)7 corresponds to a point PG(1,qt)\mathrm{PG}(1,q^t)8, then PG(1,qt)\mathrm{PG}(1,q^t)9 is of pseudoregulus type if and only if there exists a projectivity L={(λ,λq)qt:λ∈Fqt∗}.L=\{(\lambda,\lambda^q)_{q^t}:\lambda\in\mathbb F_{q^t}^\ast\}.0 of L={(λ,λq)qt:λ∈Fqt∗}.L=\{(\lambda,\lambda^q)_{q^t}:\lambda\in\mathbb F_{q^t}^\ast\}.1 such that

L={(λ,λq)qt:λ∈Fqt∗}.L=\{(\lambda,\lambda^q)_{q^t}:\lambda\in\mathbb F_{q^t}^\ast\}.2

Equivalently, pseudoregulus type is exactly the case in which the two rulings arising from L={(λ,λq)qt:λ∈Fqt∗}.L=\{(\lambda,\lambda^q)_{q^t}:\lambda\in\mathbb F_{q^t}^\ast\}.3 are projectively interchangeable in the ring-geometric model (Havlicek et al., 2016).

3. Equivalence, orbit structure, and rigidity

On L={(λ,λq)qt:λ∈Fqt∗}.L=\{(\lambda,\lambda^q)_{q^t}:\lambda\in\mathbb F_{q^t}^\ast\}.4, all linear sets of pseudoregulus type are L={(λ,λq)qt:λ∈Fqt∗}.L=\{(\lambda,\lambda^q)_{q^t}:\lambda\in\mathbb F_{q^t}^\ast\}.5-equivalent, so the family is projectively uniform (Csajbók et al., 2015, Csajbók et al., 2015). This projective uniformity does not collapse the finer semilinear orbit structure. For a pseudoregulus-type maximum scattered linear set L={(λ,λq)qt:λ∈Fqt∗}.L=\{(\lambda,\lambda^q)_{q^t}:\lambda\in\mathbb F_{q^t}^\ast\}.6, the L={(λ,λq)qt:λ∈Fqt∗}.L=\{(\lambda,\lambda^q)_{q^t}:\lambda\in\mathbb F_{q^t}^\ast\}.7-class is

L={(λ,λq)qt:λ∈Fqt∗}.L=\{(\lambda,\lambda^q)_{q^t}:\lambda\in\mathbb F_{q^t}^\ast\}.8

where L={(λ,λq)qt:λ∈Fqt∗}.L=\{(\lambda,\lambda^q)_{q^t}:\lambda\in\mathbb F_{q^t}^\ast\}.9 is Euler’s totient function (Casarino et al., 2022). In the higher-dimensional family of pseudoregulus type in xqx^q0, projective equivalence is controlled by the companion automorphism of the defining semilinear map, up to inversion, and there are

xqx^q1

projective orbits for xqx^q2, xqx^q3 (Lunardon et al., 2012).

The family is rigid, but not in the strongest possible sense. For xqx^q4 or xqx^q5, a pseudoregulus-type linear set on xqx^q6 can be obtained as the projection of two different canonical subgeometries xqx^q7 from the same center xqx^q8 to the same axis, while no ambient collineation xqx^q9 satisfies

xqνx^{q^\nu}0

Accordingly, the existence of an ambient collineation between projecting configurations is not a necessary condition for equivalence of the projected linear sets in general; the exact criterion is the paper’s condition (A) (Csajbók et al., 2015).

This combination of projective uniqueness and semilinear multiplicity is one of the distinctive features of pseudoregulus type. It explains why the family is simultaneously the most symmetric scattered family and a nontrivial source of inequivalent defining subspaces.

4. Position in the classification of maximum scattered linear sets

In the classification of maximum scattered linear sets on projective lines, pseudoregulus type is the baseline family. For xqνx^{q^\nu}1, the complete classification states that the only maximum scattered xqνx^{q^\nu}2-linear sets are those of pseudoregulus type and those of Lunardon–Polverino type. Every maximum scattered set is projectively equivalent to

xqνx^{q^\nu}3

with xqνx^{q^\nu}4; the case xqνx^{q^\nu}5 is exactly pseudoregulus type (Csajbók et al., 2017).

For xqνx^{q^\nu}6, the projection model becomes the organizing principle. Every maximum scattered linear set is the projection of a canonical xqνx^{q^\nu}7-subgeometry xqνx^{q^\nu}8 from a plane xqνx^{q^\nu}9. If PG(1,qt)\mathrm{PG}(1,q^t)00 generates the cyclic group fixing PG(1,qt)\mathrm{PG}(1,q^t)01 pointwise and

PG(1,qt)\mathrm{PG}(1,q^t)02

then the abstract states that if PG(1,qt)\mathrm{PG}(1,q^t)03 and PG(1,qt)\mathrm{PG}(1,q^t)04 are not both points, the projected linear set is of pseudoregulus type. In the equivalent vertex language, pseudoregulus type is exactly the case

PG(1,qt)\mathrm{PG}(1,q^t)05

Once pseudoregulus type is excluded, the remaining cases split into LP type and a narrow residual case with PG(1,qt)\mathrm{PG}(1,q^t)06; exhaustive computation shows that for PG(1,qt)\mathrm{PG}(1,q^t)07 no new maximum scattered linear set exists (Lia et al., 31 Jul 2025).

At the level of scattered polynomials, pseudoregulus type is the monomial family

PG(1,qt)\mathrm{PG}(1,q^t)08

Recent work still treats this as one of the three known families that exist for infinitely many values of PG(1,qt)\mathrm{PG}(1,q^t)09 and PG(1,qt)\mathrm{PG}(1,q^t)10, alongside Lunardon–Polverino-type binomials and a family of quadrinomials (Giannoni et al., 14 Jan 2026). The same comparison appears in the study of new scattered quadrinomials, where pseudoregulus type is listed as family (i) among the previously known families for PG(1,qt)\mathrm{PG}(1,q^t)11 (Smaldore et al., 2024).

5. Translation planes, semifields, hyperovals, and MRD codes

Pseudoregulus type entered finite geometry in a decisive way through the construction of translation planes. Lunardon and Polverino started from a pseudoregulus-type scattered linear set in PG(1,qt)\mathrm{PG}(1,q^t)12 and performed a hyper-regulus replacement in the Desarguesian spread

PG(1,qt)\mathrm{PG}(1,q^t)13

This yields an André translation plane. In the later generalization to arbitrary scattered linearized polynomials, the paper explicitly notes that for PG(1,qt)\mathrm{PG}(1,q^t)14, the plane PG(1,qt)\mathrm{PG}(1,q^t)15 arising from the polynomial PG(1,qt)\mathrm{PG}(1,q^t)16 is exactly the André PG(1,qt)\mathrm{PG}(1,q^t)17-plane from the original construction, up to projective equivalence (Casarino et al., 2022). In the stabilizer-based analysis of scattered polynomials, pseudoregulus type is precisely the monomial case

PG(1,qt)\mathrm{PG}(1,q^t)18

with

PG(1,qt)\mathrm{PG}(1,q^t)19

and if PG(1,qt)\mathrm{PG}(1,q^t)20 is of pseudoregulus type then the associated translation plane PG(1,qt)\mathrm{PG}(1,q^t)21 is an André plane (Longobardi et al., 2022).

The family is also central in semifield geometry. In PG(1,qt)\mathrm{PG}(1,q^t)22, maximum scattered linear sets of pseudoregulus type are used to characterize the associated linear sets of Generalized Twisted Fields. In PG(1,qt)\mathrm{PG}(1,q^t)23, the corresponding pseudoregulus-type linear sets with transversal lines in the two reguli of the hyperbolic quadric PG(1,qt)\mathrm{PG}(1,q^t)24 characterize the Knuth semifields PG(1,qt)\mathrm{PG}(1,q^t)25 and PG(1,qt)\mathrm{PG}(1,q^t)26 (Lunardon et al., 2012).

Coding-theoretically, pseudoregulus type provides both reference examples and input data for new constructions. A new family of MRD codes is obtained by starting from maximum scattered linear sets of pseudoregulus type in PG(1,qt)\mathrm{PG}(1,q^t)27 and transferring the corresponding PG(1,qt)\mathrm{PG}(1,q^t)28-subspaces to PG(1,qt)\mathrm{PG}(1,q^t)29. For PG(1,qt)\mathrm{PG}(1,q^t)30 and suitable parameters, the resulting linear sets are maximum scattered and give new MRD codes with parameters PG(1,qt)\mathrm{PG}(1,q^t)31 for PG(1,qt)\mathrm{PG}(1,q^t)32 and PG(1,qt)\mathrm{PG}(1,q^t)33 for odd PG(1,qt)\mathrm{PG}(1,q^t)34 (Csajbók et al., 2017).

A further application occurs in the André/Bruck–Bose representation of translation hyperovals. The affine point sets of translation hyperovals in PG(1,qt)\mathrm{PG}(1,q^t)35 are precisely those whose direction sets are scattered PG(1,qt)\mathrm{PG}(1,q^t)36-linear sets of pseudoregulus type in PG(1,qt)\mathrm{PG}(1,q^t)37 (D'haeseleer et al., 2019).

6. Generalizations and adjacent constructions

The most direct generalization is PG(1,qt)\mathrm{PG}(1,q^t)38-pseudoregulus type. In PG(1,qt)\mathrm{PG}(1,q^t)39, an PG(1,qt)\mathrm{PG}(1,q^t)40-linear set of rank PG(1,qt)\mathrm{PG}(1,q^t)41 is of PG(1,qt)\mathrm{PG}(1,q^t)42-pseudoregulus type if there exist

PG(1,qt)\mathrm{PG}(1,q^t)43

pairwise disjoint PG(1,qt)\mathrm{PG}(1,q^t)44-subspaces of weight PG(1,qt)\mathrm{PG}(1,q^t)45, together with exactly PG(1,qt)\mathrm{PG}(1,q^t)46 transversal PG(1,qt)\mathrm{PG}(1,q^t)47-spaces satisfying the incidence conditions of Definition 3.1. These objects arise by projecting a canonical subgeometry from the span of all but PG(1,qt)\mathrm{PG}(1,q^t)48 director spaces of a Desarguesian spread. Among them, the maximum PG(1,qt)\mathrm{PG}(1,q^t)49-scattered examples are exactly those whose associated exponent set is a Moore exponent set (Napolitano et al., 2020).

Pseudoregulus type also reappears in the one-sided theory of partially scattered polynomials. If PG(1,qt)\mathrm{PG}(1,q^t)50 and

PG(1,qt)\mathrm{PG}(1,q^t)51

then PG(1,qt)\mathrm{PG}(1,q^t)52 is PG(1,qt)\mathrm{PG}(1,q^t)53-PG(1,qt)\mathrm{PG}(1,q^t)54-partially scattered if and only if the associated PG(1,qt)\mathrm{PG}(1,q^t)55-linear set PG(1,qt)\mathrm{PG}(1,q^t)56 is of pseudoregulus type in PG(1,qt)\mathrm{PG}(1,q^t)57. In the same family, weak equivalence classes are governed by the exponent PG(1,qt)\mathrm{PG}(1,q^t)58, and there are exactly PG(1,qt)\mathrm{PG}(1,q^t)59 weak equivalence classes (Bartoli et al., 2021).

Recent papers constructing new scattered quadrinomials distinguish their families from pseudoregulus type rather than extending it. One paper proves that PG(1,qt)\mathrm{PG}(1,q^t)60 is never PG(1,qt)\mathrm{PG}(1,q^t)61-equivalent to a monomial PG(1,qt)\mathrm{PG}(1,q^t)62 of pseudoregulus type (Smaldore et al., 2024). Another compares the new quadrinomials PG(1,qt)\mathrm{PG}(1,q^t)63 with the classical benchmark families and shows geometrically that pseudoregulus type corresponds to vertex intersection number PG(1,qt)\mathrm{PG}(1,q^t)64, LP type to PG(1,qt)\mathrm{PG}(1,q^t)65, while the quadrinomial family has vertex intersection number at least PG(1,qt)\mathrm{PG}(1,q^t)66 (Giannoni et al., 14 Jan 2026).

Taken together, these developments show that pseudoregulus type remains the reference geometry in the subject: it is the uniquely rigid monomial family on PG(1,qt)\mathrm{PG}(1,q^t)67, the first case detected in vertex-based classification, the model for one-sided partial scatteredness, and the comparison orbit from which newer scattered families are separated.

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