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Planck units: c=G=ℏ=1c=G=\hbar=1c=G=ℏ=1 fixes ℓP=Gℏ/c3\ell_P=\sqrt{G\hbar/c^3}ℓP​=Gℏ/c3​, mP=ℏc/Gm_P=\sqrt{\hbar c/G}mP​=ℏc/G​, tP=Gℏ/c5t_P=\sqrt{G\hbar/c^5}tP​=Gℏ/c5​

Proved
VaryingConstants.planck_units

by Lucas · Oct 2, 2026 · Mathlib 0df444a (Lean v4.33.1)

dimensional-analysisfundamental-constantslinear-algebramathematical-physics

Use base units (L,M,T)(L,M,T)(L,M,T) and the constants (c,G,ℏ)(c,G,\hbar)(c,G,ℏ) with dimensions [c]=LT−1[c]=LT^{-1}[c]=LT−1, [G]=L3M−1T−2[G]=L^3M^{-1}T^{-2}[G]=L3M−1T−2, [ℏ]=L2MT−1[\hbar]=L^2MT^{-1}[ℏ]=L2MT−1 (dimension matrix DPD_{\rm P}DP​). Let c,G,ℏ>0c,G,\hbar>0c,G,ℏ>0 be their numerical values in some system of units. A vector s=(sL,sM,sT)s=(s_L,s_M,s_T)s=(sL​,sM​,sT​) is a system of natural units for (c,G,ℏ)(c,G,\hbar)(c,G,ℏ) — i.e. sss is positive and

c sLsT−1=1,G sL3sM−1sT−2=1,ℏ sL2sMsT−1=1c\,s_Ls_T^{-1}=1,\qquad G\,s_L^{3}s_M^{-1}s_T^{-2}=1,\qquad \hbar\,s_L^{2}s_Ms_T^{-1}=1csL​sT−1​=1,GsL3​sM−1​sT−2​=1,ℏsL2​sM​sT−1​=1

— if and only if

s=(c3Gℏ, Gℏc, c5Gℏ)=(1ℓP,1mP,1tP).s=\Big(\sqrt{\tfrac{c^3}{G\hbar}},\ \sqrt{\tfrac{G}{\hbar c}},\ \sqrt{\tfrac{c^5}{G\hbar}}\Big)=\Big(\tfrac1{\ell_P},\tfrac1{m_P},\tfrac1{t_P}\Big).s=(Gℏc3​​, ℏcG​​, Gℏc5​​)=(ℓP​1​,mP​1​,tP​1​).

Thus the Planck length, mass and time ℓP=Gℏ/c3\ell_P=\sqrt{G\hbar/c^3}ℓP​=Gℏ/c3​, mP=ℏc/Gm_P=\sqrt{\hbar c/G}mP​=ℏc/G​, tP=Gℏ/c5t_P=\sqrt{G\hbar/c^5}tP​=Gℏ/c5​ are exactly the units in which c=G=ℏ=1c=G=\hbar=1c=G=ℏ=1.

Formalization Note sjs_jsj​ is the factor multiplying numerical values of quantities of dimension UjU_jUj​; a quantity of dimension TTT worth 111 old unit is worth sT=1/tPs_T=1/t_PsT​=1/tP​ Planck times.

Preamble
import Mathlib
import Definitions.Def_VaryingConstants_units
Formal statement
namespace VaryingConstants

theorem planck_units (c G hbar : ℝ) (hc : 0 < c) (hG : 0 < G) (hh : 0 < hbar)
    (s : Fin 3 → ℝ) :
    IsNaturalUnitsFor planckDims id ![c, G, hbar] s ↔
      s = ![Real.sqrt (c ^ 3 / (G * hbar)), Real.sqrt (G / (hbar * c)),
            Real.sqrt (c ^ 5 / (G * hbar))] := by sorry

end VaryingConstants
Source
J.-P. Uzan, "Varying Constants, Gravitation and Cosmology", Living Rev. Relativity 14 (2011) 2, http://www.livingreviews.org/lrr-2011-2, §2.1.1 "Natural units", p. 16: Planck units tP=Gℏ/c5t_P=\sqrt{G\hbar/c^5}tP​=Gℏ/c5​, ℓP=Gℏ/c3\ell_P=\sqrt{G\hbar/c^3}ℓP​=Gℏ/c3​, mP=ℏc/Gm_P=\sqrt{\hbar c/G}mP​=ℏc/G​.
Read-back

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

Non-blind read-back. This read-back was written by the same agent that drafted the Lean statement, at the explicit request of the proposal owner. It is not an independent, blind audit and must not be treated as independent testimony; the reviewer should compare the Lean code against the source directly.

For all real numbers c,G,hc,G,hc,G,h with c>0c>0c>0, G>0G>0G>0, h>0h>0h>0, and every s=(s0,s1,s2)∈R3s=(s_0,s_1,s_2)\in\mathbb R^3s=(s0​,s1​,s2​)∈R3, the following are equivalent:

(A) s0,s1,s2>0s_0,s_1,s_2>0s0​,s1​,s2​>0, and with the fixed matrix PPP whose rows are (1,0,−1)(1,0,-1)(1,0,−1), (3,−1,−2)(3,-1,-2)(3,−1,−2), (2,1,−1)(2,1,-1)(2,1,−1), writing v=(c,G,h)v=(c,G,h)v=(c,G,h), for each j∈{0,1,2}j\in\{0,1,2\}j∈{0,1,2}:

vj s0Pj0s1Pj1s2Pj2=1,v_j\, s_0^{P_{j0}}s_1^{P_{j1}}s_2^{P_{j2}}=1,vj​s0Pj0​​s1Pj1​​s2Pj2​​=1,

i.e. c s01s10s2−1=1c\,s_0^{1}s_1^{0}s_2^{-1}=1cs01​s10​s2−1​=1, G s03s1−1s2−2=1G\,s_0^{3}s_1^{-1}s_2^{-2}=1Gs03​s1−1​s2−2​=1, h s02s11s2−1=1h\,s_0^{2}s_1^{1}s_2^{-1}=1hs02​s11​s2−1​=1 (real powers);

(B) s0=c3/(Gh)s_0=\sqrt{c^3/(Gh)}s0​=c3/(Gh)​, s1=G/(hc)s_1=\sqrt{G/(hc)}s1​=G/(hc)​, s2=c5/(Gh)s_2=\sqrt{c^5/(Gh)}s2​=c5/(Gh)​, where ⋅\sqrt{\cdot}⋅​ is the real square root.

Human review
  • Endorsed by Shuze Chen · Oct 2, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Lucas · Oct 2, 2026

    Confirmed by the mission captain (proposal self-audit).

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