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C00C_{00}C00​ is an eigenvector of Tt2\mathbf T_t^2Tt2​ with eigenvalue NNN

Proved
NaculichRegge.tt2_C00_eigen

by Lucas · Sep 25, 2026 · Mathlib 0df444a (Lean v4.33.1)

color-algebramathematical-physicsscattering-amplitudes

The tree-level ttt-channel colour factor is an eigenvector of the ttt-channel Casimir: Tt2C00=N C00\mathbf T_t^2C_{00}=N\,C_{00}Tt2​C00​=NC00​. In the paper this is T1⋅T4C00=−12NC00\mathbf T_1\cdot\mathbf T_4C_{00}=-\tfrac12NC_{00}T1​⋅T4​C00​=−21​NC00​ (eq. (4.2)) combined with Tt2=2N+2T1⋅T4\mathbf T_t^2=2N+2\mathbf T_1\cdot\mathbf T_4Tt2​=2N+2T1​⋅T4​ (eq. (4.7)); here it is stated for the matrix of eq. (4.15).

Preamble
import Definitions.Def_NaculichRegge_TraceBasis

open Polynomial
Formal statement
namespace NaculichRegge

/-- Naculich, eqs. (4.2), (4.7): `C₀₀` is an eigenvector of `𝐓_t²` with eigenvalue `N`. -/
theorem tt2_C00_eigen : Tt2.mulVec C00 = (X : ℂ[X]) • C00 := by sorry

end NaculichRegge
Source
S. G. Naculich, "All-loop-orders relation between Regge limits of N = 4 SYM and N = 8 supergravity four-point amplitudes", arXiv:2012.00030v2, https://arxiv.org/abs/2012.00030, pp. 11–13, eqs. (4.2), (4.7), (4.15)
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The statement asserts the equality of colour vectors

Tt2 C00=N⋅C00,\mathbf T_t^2\,C_{00}=N\cdot C_{00},Tt2​C00​=N⋅C00​,

i.e. the matrix Tt2\mathbf T_t^2Tt2​ applied to C00=(1,0,−1,0,0,0)TC_{00}=(1,0,-1,0,0,0)^TC00​=(1,0,−1,0,0,0)T equals (N,0,−N,0,0,0)T(N,0,-N,0,0,0)^T(N,0,−N,0,0,0)T, as vectors of polynomials in NNN with complex coefficients. It has no hypotheses.

Definitions used. Throughout, NNN denotes the polynomial variable XXX of C[X]\mathbb{C}[X]C[X]; a colour vector is a column vector v=(v1,…,v6)∈C[X]6v=(v_1,\dots,v_6)\in\mathbb{C}[X]^6v=(v1​,…,v6​)∈C[X]6 (component vjv_jvj​ is the coefficient of the trace-basis element c[j]c[j]c[j]), and a colour operator is a 6×66\times 66×6 matrix over C[X]\mathbb{C}[X]C[X] acting on column vectors by matrix–vector multiplication. Tt2\mathbf T_t^2Tt2​ and Ts−u2\mathbf T_{s-u}^2Ts−u2​ are the two fixed matrices

Tt2=(N0000−102N010100N−1000202N00−20−2000020002N),Ts−u2=(−N2000−1−12000−1201200N21210012N00−101000−2−1000−N),\mathbf T_t^2=\begin{pmatrix}N&0&0&0&0&-1\\0&2N&0&1&0&1\\0&0&N&-1&0&0\\0&2&0&2N&0&0\\-2&0&-2&0&0&0\\0&2&0&0&0&2N\end{pmatrix},\qquad \mathbf T_{s-u}^2=\begin{pmatrix}-\tfrac N2&0&0&0&-1&-\tfrac12\\0&0&0&-\tfrac12&0&\tfrac12\\0&0&\tfrac N2&\tfrac12&1&0\\0&1&2&N&0&0\\-1&0&1&0&0&0\\-2&-1&0&0&0&-N\end{pmatrix},Tt2​=​N000−20​02N0202​00N0−20​01−12N00​000000​−110002N​​,Ts−u2​=​−2N​000−1−2​00010−1​002N​210​0−21​21​N00​−101000​−21​21​000−N​​,

C00=(1,0,−1,0,0,0)TC_{00}=(1,0,-1,0,0,0)^{T}C00​=(1,0,−1,0,0,0)T, and PPP ("crossing") is the permutation matrix exchanging coordinates 1↔31\leftrightarrow 31↔3 and 4↔64\leftrightarrow 64↔6 and fixing 2,52,52,5. With [A,B]=AB−BA[A,B]=AB-BA[A,B]=AB−BA, the Regge colour factor CikC_{ik}Cik​ is OikC00O_{ik}C_{00}Oik​C00​, where OikO_{ik}Oik​ is: the identity if i=0i=0i=0 (for every kkk); otherwise (Ts−u2)i(\mathbf T_{s-u}^2)^i(Ts−u2​)i if k=ik=ik=i; otherwise adTt2 i−1(Ts−u2)\mathrm{ad}_{\mathbf T_t^2}^{\,i-1}(\mathbf T_{s-u}^2)adTt2​i−1​(Ts−u2​) if k=1k=1k=1; otherwise adTs−u2 i−2([Tt2,Ts−u2])\mathrm{ad}_{\mathbf T_{s-u}^2}^{\,i-2}([\mathbf T_t^2,\mathbf T_{s-u}^2])adTs−u2​i−2​([Tt2​,Ts−u2​]) if k=i−1k=i-1k=i−1 (here i−2i-2i−2 is truncated at 000); and the zero matrix in all other cases. A pair (i,k)(i,k)(i,k) is admissible if (i,k)=(0,0)(i,k)=(0,0)(i,k)=(0,0), or (i,k)=(1,1)(i,k)=(1,1)(i,k)=(1,1), or i=2i=2i=2 and k∈{1,2}k\in\{1,2\}k∈{1,2}, or i≥3i\ge 3i≥3 and k∈{1,i−1,i}k\in\{1,i-1,i\}k∈{1,i−1,i}; RℓR_\ellRℓ​ is the finite set of admissible pairs with i≤ℓi\le\elli≤ℓ and k≤ℓk\le\ellk≤ℓ.

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