The Polyakov action in conformal gauge

Proved

PolyakovAction.conformal_gauge_action

by Lucas · Oct 1, 2026 · Mathlib 0df444a (Lean v4.33.1)

mathematical-physicsstring-theory

In conformal gauge, $h_{ab}=\eta_{ab}=\mathrm{diag}(1,-1)$ , the Polyakov action becomes

S=\frac T2\int d^2\sigma\,\sqrt{-\eta}\,\eta^{ab}g_{\mu\nu}(X)\partial_aX^\mu\partial_bX^\nu=\frac T2\int d^2\sigma\,\big(\dot X^2-X'^2\big),

where $\dot X^2=g_{\mu\nu}\dot X^\mu\dot X^\nu$ , $X'^2=g_{\mu\nu}X'^\mu X'^\nu$ , $\dot X=\partial_\tau X$ , $X'=\partial_\sigma X$ .

Formalization Note. The identity holds for any target metric $g$ and region $U$ ; the gauge-fixing step itself (using diffeomorphisms and Weyl rescalings to reach $\eta$ ) is not part of this statement.

Preamble

import Mathlib
import Definitions.Def_PolyakovAction_Defs

open MeasureTheory Filter Asymptotics
open scoped Matrix Topology

Formal statement

namespace PolyakovAction

theorem conformal_gauge_action {D : ℕ} (T : ℝ) (g : Spacetime D → Matrix (Fin D) (Fin D) ℝ)
    (X : Worldsheet → Spacetime D) (U : Set Worldsheet) :
    polyakovAction T g (fun _ => minkowskiMetric 2) X U
      = T / 2 * ∫ σ in U, (inducedMetric g X σ 0 0 - inducedMetric g X σ 1 1) := by sorry

end PolyakovAction

Source

Wikipedia, "Polyakov action", revision oldid=1292212311 (https://en.wikipedia.org/w/index.php?title=Polyakov_action&oldid=1292212311)

Read-back

What the Lean code literally says, in plain math · Aristotle (Harmonic)

Non-blind read-back — not independent testimony. This read-back was written by the same agent (Aristotle, by Harmonic) that drafted the Lean statements of this proposal, at the account owner's explicit instruction. Its author knew the source material and the intended meaning of the code while writing it, so it is not a blind audit and must not be mistaken for independent testimony. Reviewers should compare it against the Lean code themselves.

Throughout, $\sigma=(\sigma^0,\sigma^1)\in\mathbb R^2$ is a worldsheet point (index $0$ is $\tau$ , index $1$ is $\sigma$ ), $X:\mathbb R^2\to\mathbb R^D$ is the embedding, $\partial_a X^\mu(\sigma)$ is the $\mu$ -th component of the Fréchet derivative of $X$ at $\sigma$ applied to the $a$ -th standard basis vector (it is $0$ wherever $X$ is not differentiable), $G_{ab}(\sigma)=\sum_{\mu,\nu} g_{\mu\nu}(X(\sigma))\,\partial_aX^\mu\,\partial_bX^\nu$ is the induced metric, $h^{ab}$ denotes the entries of the matrix inverse $(h_{ab})^{-1}$ (Mathlib's inverse, which is the zero matrix when $\det h=0$ ), and $\sqrt{\cdot}$ is the real square root, which returns $0$ on negative inputs. The Polyakov density is $\mathcal L_P=\sqrt{-\det h}\,\sum_{a,b}h^{ab}G_{ab}$ , the Polyakov action on a set $U$ is $S_P[U]=\frac T2\int_U\mathcal L_P\,d^2\sigma$ (Lebesgue measure; Bochner integral, equal to $0$ if the integrand is not integrable on $U$ ), and the Nambu–Goto action is $S_{NG}[U]=T\int_U\sqrt{-\det G}\,d^2\sigma$ . The stress–energy tensor is $T_{ab}=T\big(G_{ab}-\tfrac12 h_{ab}\sum_{c,d}h^{cd}G_{cd}\big)$ , and $\eta^{(n)}=\mathrm{diag}(1,-1,\dots,-1)$ is the $n\times n$ Minkowski matrix.

Statement. For every $D$ , real $T$ , target metric $g$ , map $X$ and set $U$ :

S_P\big(T,g,\,\sigma\mapsto\eta^{(2)},\,X,\,U\big)=\frac T2\int_U\big(G_{00}(\sigma)-G_{11}(\sigma)\big)\,d^2\sigma,

where $\eta^{(2)}=\mathrm{diag}(1,-1)$ and $G_{00}=\sum g_{\mu\nu}(X)\partial_0X^\mu\partial_0X^\nu$ , $G_{11}=\sum g_{\mu\nu}(X)\partial_1X^\mu\partial_1X^\nu$ (index $0=\tau$ , $1=\sigma$ ).

Human review

Endorsed by Shuze Chen · Oct 8, 2026
Confirmed by the moderator at approval.
Endorsed by Lucas · Oct 8, 2026
Confirmed by the mission captain (proposal self-audit).

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