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Strong CR Tournaments in Determinant Theory

Updated 8 July 2026
  • Strong CR tournaments are tournaments defined using determinant layers where each subtournament’s determinant is strictly bounded, ensuring rigidity via switching and transitive blowups.
  • They are characterized by CR-associated vertices and extension rules, with canonical templates like the Lₙ family serving as irreducible building blocks in the determinant layer Dₖ.
  • Their structure implies that any tournament containing a basic strong CR tournament is switching equivalent to a transitive blowup, preserving the determinant-bound property.

Strong CR tournaments are a class of tournaments introduced in the determinant-based study of skew-adjacency matrices. In this setting, if TT is a tournament with skew-adjacency matrix STS_T, the determinant of TT is det(T):=det(ST)\det(T):=\det(S_T), and for a positive odd integer kk one considers the class Dk\mathcal D_k of tournaments all of whose subtournaments have determinant at most k2k^2. A CR tournament is a tournament in DkDk2\mathcal D_k\setminus \mathcal D_{k-2} whose one-vertex extensions preserve the determinant bound only in the “CR-associated” directions; a strong CR tournament is a CR tournament for which every $1$-transitive blowup is again a CR tournament. The central role of strong CR tournaments is that, for a basic strong CR tournament HH, every tournament STS_T0 containing a subtournament switching isomorphic to STS_T1 remains in the same determinant layer STS_T2 if and only if STS_T3 is switching equivalent to a transitive blowup of STS_T4 (Zeng et al., 10 Aug 2025).

1. Determinant framework and switching structure

A tournament is an orientation of the complete graph: for every two distinct vertices STS_T5, exactly one of STS_T6 or STS_T7 holds. If STS_T8 is an STS_T9-tournament with vertex ordering TT0, its adjacency matrix is

TT1

and its skew-adjacency matrix is

TT2

The determinant of a tournament is

TT3

This does not depend on the chosen vertex ordering. The determinant is TT4 for tournaments of odd order, while for even order it is the square of an odd integer (Zeng et al., 10 Aug 2025).

For a positive odd integer TT5,

TT6

The layer

TT7

consists of tournaments whose subtournament determinants are all TT8, and for which at least one subtournament has determinant exactly TT9. The convention

det(T):=det(ST)\det(T):=\det(S_T)0

is also used.

Switching is fundamental. Given det(T):=det(ST)\det(T):=\det(S_T)1, the switch of det(T):=det(ST)\det(T):=\det(S_T)2 with respect to det(T):=det(ST)\det(T):=\det(S_T)3 is obtained by reversing all arcs between det(T):=det(ST)\det(T):=\det(S_T)4 and det(T):=det(ST)\det(T):=\det(S_T)5. Two tournaments are switching equivalent if one is obtained from the other by such a switch. Determinant and membership in det(T):=det(ST)\det(T):=\det(S_T)6 are invariant under switching. A tournament det(T):=det(ST)\det(T):=\det(S_T)7 is switching isomorphic to det(T):=det(ST)\det(T):=\det(S_T)8 if some switch of det(T):=det(ST)\det(T):=\det(S_T)9 is isomorphic to kk0.

Blowups provide the main constructive operation. If kk1 has vertices kk2, and kk3 are tournaments, the blowup

kk4

is obtained by replacing kk5 by kk6, and orienting all edges between kk7 and kk8 according to the arc kk9 in Dk\mathcal D_k0. If each Dk\mathcal D_k1 is transitive and Dk\mathcal D_k2, this is the transitive Dk\mathcal D_k3-blowup of Dk\mathcal D_k4, denoted

Dk\mathcal D_k5

A Dk\mathcal D_k6-transitive blowup means exactly one Dk\mathcal D_k7 and all others are Dk\mathcal D_k8. A key inherited fact is that

Dk\mathcal D_k9

and hence

k2k^20

2. CR tournaments, basic tournaments, and strong CR tournaments

The paper introduces CR-associated vertices as the local mechanism governing admissible one-vertex extensions. For vertices k2k^21 in a tournament k2k^22, they are covertices if they have identical orientation to every other vertex, and revertices if they have opposite orientation to every other vertex. Formally, when k2k^23,

k2k^24

for covertices, and

k2k^25

for revertices, where k2k^26 if k2k^27, and k2k^28 otherwise. If two vertices are covertices or revertices, they are CR-associated (Zeng et al., 10 Aug 2025).

Let k2k^29, and let DkDk2\mathcal D_k\setminus \mathcal D_{k-2}0 specify the orientations between DkDk2\mathcal D_k\setminus \mathcal D_{k-2}1 and DkDk2\mathcal D_k\setminus \mathcal D_{k-2}2. Write DkDk2\mathcal D_k\setminus \mathcal D_{k-2}3 for the enlarged tournament. Then DkDk2\mathcal D_k\setminus \mathcal D_{k-2}4 is a CR vertex for DkDk2\mathcal D_k\setminus \mathcal D_{k-2}5 with DkDk2\mathcal D_k\setminus \mathcal D_{k-2}6 if in DkDk2\mathcal D_k\setminus \mathcal D_{k-2}7 there exists some DkDk2\mathcal D_k\setminus \mathcal D_{k-2}8 such that DkDk2\mathcal D_k\setminus \mathcal D_{k-2}9 and $1$0 are CR-associated. Otherwise $1$1 is a non-CR vertex.

This leads to the main definitions. Let $1$2.

  • If $1$3 is a $1$4-tournament, a $1$5-tournament, or a diamond, it is a trivial CR tournament.
  • Otherwise, $1$6 is a CR tournament if for every non-CR way of adding a new vertex $1$7, the resulting tournament leaves $1$8:

$1$9

Equivalently, for HH0,

HH1

A tournament HH2 of order HH3 is basic if it has no pair of CR-associated vertices. A CR tournament HH4 is a strong CR tournament if every HH5-transitive blowup of HH6 is also a CR tournament. A basic CR tournament is both basic and CR, and a basic strong CR tournament is both basic and strong CR.

These notions are switching invariant: CR-associated relation, being a CR tournament, being a strong CR tournament, and being basic are all invariant under switching, and hence under switching isomorphism. This makes switching equivalence the natural ambient equivalence relation for the theory.

3. Structural characterization of basic strong CR tournaments

The central theorem states that strong CR tournaments are precisely the templates whose transitive blowups exhaust the determinant layer inside their containment class. Let HH7 denote the class of tournaments containing a subtournament switching isomorphic to HH8. Then for odd HH9 and a basic tournament STS_T00, the following are equivalent:

  1. STS_T01 is a strong CR tournament;
  2. all transitive blowups of STS_T02 are CR tournaments;

3.

STS_T03

This is the paper’s main characterization theorem (Zeng et al., 10 Aug 2025).

A basic strong CR tournament therefore acts as a rigid extremal template for the layer STS_T04. If STS_T05 contains a subtournament switching isomorphic to STS_T06, then no additional structure beyond transitive blowup is permitted while staying inside the same determinant bound.

The basicness assumption is essential. If a tournament is not basic, then after switching it is a STS_T07-transitive blowup of a smaller tournament. Thus basic tournaments are the irreducible cores of the theory. The paper also proves that in a basic tournament, a newly added CR vertex can be CR-associated with at most one original vertex, and if STS_T08 is a transitive blowup of a basic tournament STS_T09, then adding a non-CR vertex cannot accidentally produce something switching equivalent to a transitive blowup of STS_T10. This suggests that the basic/strong CR distinction isolates the exact point at which blowup rigidity becomes canonical.

4. The canonical family STS_T11 and the determinant layers STS_T12

For STS_T13, STS_T14 is the STS_T15-tournament with vertices STS_T16 such that STS_T17 is transitive with

STS_T18

and STS_T19 alternates against those vertices: STS_T20 Thus STS_T21 is transitive, STS_T22 is a diamond, and for even STS_T23,

STS_T24

The paper proves two decisive facts: for even STS_T25, STS_T26 is a basic strong CR tournament; and all STS_T27 are strong CR tournaments (Zeng et al., 10 Aug 2025). Even STS_T28 are basic, while odd STS_T29 are strong CR but not basic. This matters because even STS_T30 provide the irreducible templates to which the main characterization theorem applies directly.

These results unify earlier classifications of low determinant layers. Existing results had shown that for STS_T31, a tournament STS_T32 is switching equivalent to a transitive blowup of STS_T33. The strong CR theory yields a general higher-STS_T34 statement with a containment condition: if STS_T35 is odd and

STS_T36

then

STS_T37

This answers a question posed by Zeng and You.

The family STS_T38 is therefore not merely a source of examples. It is the canonical source of strong CR templates, and it explains why determinant layers can be governed by blowups of a single tournament once a switching-isomorphic copy of that tournament is present.

5. Proof architecture and technical mechanisms

The proof theory of strong CR tournaments combines switching, transitive blowups, and determinant identities. One foundational lemma states that if STS_T39 is a CR vertex for STS_T40, then some switch of STS_T41 is a STS_T42-transitive blowup of STS_T43. Since determinant and membership in STS_T44 are invariant under switching and preserved under transitive blowups, this gives

STS_T45

The difficult direction is to show that non-CR extensions force determinant STS_T46.

A second recurring mechanism is the interaction between blowups and determinant multiplication. For a transitive tournament STS_T47 of order STS_T48,

STS_T49

If a blowup STS_T50 has some non-transitive part STS_T51, then there is a subtournament with determinant STS_T52; in the special case where one part is a STS_T53-cycle and the others are singletons,

STS_T54

This shows why transitive blowups are the only blowups compatible with staying inside a fixed determinant layer.

For the proof that even STS_T55 are CR tournaments, the paper studies a non-CR extension STS_T56 through its skew-adjacency matrix. A key determinant identity is

STS_T57

A specialized corollary yields

STS_T58

for suitable STS_T59 and STS_T60. This reduces determinant comparison to arithmetic control of sign patterns.

The most technical part introduces a combinatorial matrix STS_T61 and row-sum parameters STS_T62 such that

STS_T63

Difference formulas for consecutive STS_T64 then show that if the extension pattern is non-CR, one of these determinants must exceed STS_T65. A plausible implication is that strong CR theory is driven less by global tournament structure than by an exact control of how sign-pattern perturbations propagate through skew-adjacency determinants.

6. Examples, neighboring usages of “CR,” and open problems

Several low-order examples anchor the theory. By definition, the STS_T66-tournament, the STS_T67-tournament, and the diamond are trivial CR tournaments. Every STS_T68-tournament is a CR tournament. The paper also checks directly that STS_T69 are strong CR tournaments for STS_T70, and in particular STS_T71 and STS_T72 are basic strong CR tournaments (Zeng et al., 10 Aug 2025).

The paper does not provide an example of a CR tournament that is not strong CR. After examining low-order cases, the authors found none, and they raise this as an open question. The explicit open problems include:

  1. Which CR tournaments are strong CR tournaments?
  2. Is every CR tournament a strong CR tournament?
  3. If not, find sufficient, necessary, or necessary-and-sufficient conditions for a CR tournament to be strong CR.
  4. For STS_T73, can one find finitely many basic tournaments STS_T74 such that

STS_T75

A common misconception is that “CR tournament” has a unique meaning across tournament theory. In fact, the same abbreviation appears elsewhere for the Condorcet Random model, a one-parameter upset model used in computational social choice. That literature does not define strong CR tournaments in the determinant-theoretic sense, and it treats “CR” as “Condorcet Random,” with upset probability STS_T76 and STS_T77 corresponding to the uniform random tournament (Mattei et al., 2016). Another nearby but distinct line studies strongly critical vertices in indecomposable tournaments, where “critical” and “strongly critical” refer to indecomposability rather than determinant layers; this is terminologically adjacent but mathematically separate (Rachid, 2023). This suggests that, in current usage, “strong CR tournament” is a specialized term of the determinant-and-switching framework, not a generic synonym for strong tournament structure.

In that framework, strong CR tournaments provide the rigid templates governing determinant-bounded classes through transitive blowups. Their defining feature is not strong connectivity, pancyclicity, or Erdős–Hajnal structure, but extension rigidity inside STS_T78: once a basic strong CR tournament appears, the only way to remain in the same determinant layer is to enlarge it by transitive blowup and switching equivalence.

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