Research-Stack/lean_binned/BinnedFormalizations.lean
allaun 475f6319ea chore(repo): push local 768-commit branch state onto clean remote baseline
This squashes all local history (768 commits) onto the scrubbed PR #90
baseline. Individual commits were lost during filter-repo corruption;
the working tree content is preserved intact.

Build: N/A (working tree state only)
2026-06-15 22:46:50 -05:00

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import Mathlib
/- Original: z = 1/a -/
theorem eq_dc1663f465de629e (a : ) (z : ) : z = 1/a := by
omega
/- Original: N = {1, 2 -/
theorem eq_4a18ceaf3888bba3 (N : ) : N = {1 ∧ 2 := by
omega
/- Original: k ≥ 2 where 1 x = (1 x , -/
theorem eq_0085761c3512ef7e (k : ) (where : ) (x : ) : k ≥ 2 where 1 x = (1 x , := by
omega
/- Original: T = 2 (3 -/
theorem eq_5681ee9bcf0fa212 (T : ) : T = 2 (3 := by
omega
/- Original: b = 1a -/
theorem eq_3ed31f1ae076490c (a : ) (b : ) : b = 1-a := by
omega
/- Original: is = 12 s -/
theorem eq_db937c0f244fb14f (is : ) (s : ) : is = 12 - s := by
omega
/- Original: ZkRT =⇒ ZUCS(1),k -/
theorem eq_840155af33c6593a (ZUCS : ) (ZkRT : ) (k : ) : ZkRT =⇒ ZUCS(1) ∧ k := by
omega
/- Original: a ≤ b, we set [a, b] = {k ∈ ZP | a ≤ k ≤ b} -/
theorem eq_45aae6731480405b (ZP : ) (a : ) (b : ) (k : ) (set : ) (we : ) : a ≤ b ∧ we set [a ∧ b] = {k ∈ ZP | a ≤ k ≤ b} := by
omega
/- Original: Htx = y)g(y) (1 -/
theorem eq_0d0a8db0702e6227 (Htx : ) (g : ) (y : ) : Htx = y)g(y) (1 := by
omega
/- Original: b = (4 -/
theorem eq_165389a1b0e1fa3a (b : ) : b = (4 := by
omega
/- Original: ess ≤ λα · eP (ϕ) < eP (ϕ) , and the SRB measure µ+ = µϕ(u) has absolutely continuous conditional measures along unstable manifolds -/
theorem eq_40ce41ef24bab64a (SRB : ) (absolutely : ) (along : ) (conditional : ) (continuous : ) (eP : ) (ess : ) (has : ) (manifolds : ) (measure : ) (measures : ) (the : ) (u : ) (unstable : ) (µ : ) (µϕ : ) (λα : ) (ϕ : ) : ess ≤ λα * eP (ϕ) < eP (ϕ) , ∧ the SRB measure µ+ = µϕ(u) has absolutely continuous conditional measures along unstable manifolds := by
omega
/- Original: l ≥ 0, with C = (M (2 + 2CvM ))2M -/
theorem eq_41846a6477bb5031 (C : ) (CvM : ) (M : ) (l : ) : l ≥ 0 ∧ with C = (M (2 + 2CvM ))2M := by
omega
/- Original: Ep = q -/
theorem eq_a3304dc6002ba5ff (Ep : ) (q : ) : Ep = q := by
omega
/- Original: N = ±1 -/
theorem eq_4873edfda3319bb7 (N : ) : N = ±1 := by
omega
/- Original: M = M P -/
theorem eq_5c60d8b2b41be060 (M : ) (P : ) : M = M P := by
omega
/- Original: M = 2 -/
theorem eq_5897ae98de4b014b (M : ) : M = 2 := by
omega
/- Original: SR = 1 + 0 -/
theorem eq_f3229308596f7e0f (SR : ) : SR = 1 + 0 := by
omega
/- Original: S = nK -/
theorem eq_ee1806e38c2e138f (S : ) (nK : ) : S = nK := by
omega
/- Original: j = ∅ -/
theorem eq_c1a65b020b4cbca9 (j : ) : j = ∅ := by
omega
/- Original: r>0  r∈Z+ 12 e0= (∂ ψe ψ) (B -/
theorem eq_3cbd19f4716d6d25 (B : ) (Z : ) (e0 : ) (r : ) (ψ : ) (ψe : ) : r>0  r∈Z+ 12 e0= (∂ ψe ψ) (B := by
omega
/- Original: m ≥ 0, we multiply the equation for m by m2 , with m = max(0, m) and integrate in space and time -/
theorem eq_250c08e8451f986b (by : ) (equation : ) (for : ) (integrate : ) (m : ) (m2 : ) (multiply : ) (space : ) (the : ) (time : ) (we : ) : m ≥ 0, we multiply the equation for m by m2- , with m- = max(0, -m) ∧ integrate in space and time := by
omega
/- Original: qi = T pi -/
theorem eq_16394787daa75309 (T : ) (pi : ) (qi : ) : qi = T pi := by
omega
/- Original: g = 1 -/
theorem eq_ff52deca30009dcd (g : ) : g = -1 := by
omega
/- Original: q = 0, Eq -/
theorem eq_32ab2ff729514bc2 (Eq : ) (q : ) : q = 0 ∧ Eq := by
omega
/- Original: P = ci P -/
theorem eq_86c1193b23361384 (P : ) (ci : ) : P = ci P := by
omega
/- Original: C = √12 -/
theorem eq_b0211e5bfd10d843 (C : ) : C = √12 := by
omega
/- Original: TV = 0 -/
theorem eq_45c6d0f7052c61f2 (TV : ) : TV = 0 := by
omega
/- Original: u = F u† -/
theorem eq_2e12c41db0bb746d (F : ) (u : ) : u = F u† := by
omega
/- Original: q > 1 and t := b/q < 1 -/
theorem eq_acdbf6dbfe3926e8 (b : ) (q : ) (t : ) : q > 1 and t := b/q < 1 := by
omega
/- Original: cTglob = (10 -/
theorem eq_2577f85be9648be4 (cTglob : ) : cTglob = (10 := by
omega
/- Original: ruf = r⋄ and Ω2uf = 4D(r⋄ ; M, ϱ) on R(1, uf , 1, ∞), where r⋄ is as in Lemma 4 -/
theorem eq_0a5b6d95dadfc3e2 (D : ) (Lemma : ) (M : ) (R : ) (as : ) (is : ) (on : ) (r : ) (ruf : ) (uf : ) (where : ) (ϱ : ) (Ω2uf : ) : ruf = r⋄ ∧ Ω2uf = 4D(r⋄ ; M, ϱ) on R(1, uf , 1, ∞), where r⋄ is as in Lemma 4 := by
omega
/- Original: V = V1 + V2 , where ( V1 = χ(|x| < r)V (x), |V1 (x)| ⩽ Cr2d ⟨x⟩D , (3 -/
theorem eq_2ddaee8030fa39eb (Cr2d : ) (D : ) (V : ) (V1 : ) (V2 : ) (r : ) (where : ) (x : ) (χ : ) : V = V1 + V2 ∧ where ( V1 = χ(|x| < r)V (x) ∧ |V1 (x)| ⩽ Cr2d ⟨x⟩-D ∧ (3 := by
omega
/- Original: p =I ⊗ Φp + ϵI ⊗ Wp,Φ ϵ2 Source0,p + O(ϵ3 ) (3 -/
theorem eq_d2028815ba9b7371 (I : ) (O : ) (Source0 : ) (Wp : ) (p : ) (Φ : ) (Φp : ) (ϵ2 : ) (ϵ3 : ) (ϵI : ) : p =I ⊗ Φp + ϵI ⊗ Wp ∧ Φ - ϵ2 Source0 ∧ p + O(ϵ3 ) (3 := by
omega
/- Original: x = 21 , and the previous identities imply  y (k) 12 = 0, k = 0, 1, 2, 3 -/
theorem eq_410dfb7a851615f8 (identities : ) (imply : ) (k : ) (previous : ) (the : ) (x : ) (y : ) : x = 21 , ∧ the previous identities imply  y (k) 12 = 0, k = 0, 1, 2, 3 := by
omega
/- Original: t ≥ 0 into X tn X X tn X etΓ β(x) = [Γn β](x) β(y) γ (n) (y, x) =: β(y)γt (y, x) -/
theorem eq_069f772cfae3e2f6 (X : ) (etΓ : ) (into : ) (n : ) (t : ) (tn : ) (x : ) (y : ) (Γn : ) (β : ) (γ : ) (γt : ) : t ≥ 0 into X tn X X tn X etΓ β(x) = [Γn β](x) β(y) γ (n) (y ∧ x) =: β(y)γt (y ∧ x) := by
omega
/- Original: j=a1 h i a,b=1, -/
theorem eq_3994fe06c226dbed (a : ) (b : ) (h : ) (i : ) (j : ) : j=a-1 h i a ∧ b=1 := by
omega
/- Original: ux = ux P u + 2 2     1 2 1 2 1 2 2 2 = ux P+ u + ux + h(u) P u + ux + h(u) + u2 2 2 2 + h(u) λ(t)ux -/
theorem eq_7ba3cc2c96fdf78f (P : ) (h : ) (t : ) (u : ) (u2 : ) (ux : ) (λ : ) : ux = - ux - P * u + 2 2     1 2 1 2 1 2 2 2 = - ux - P+ * u + ux + h(u) - P- * u + ux + h(u) + u2 2 2 2 + h(u) - λ(t)ux := by
omega
/- Original: k = 4πkG σ0 C0 and χ is the Euler characteristic, i -/
theorem eq_8fa7c2d3a5dadce7 (C0 : ) (Euler : ) (characteristic : ) (i : ) (is : ) (k : ) (the : ) (πkG : ) (σ0 : ) (χ : ) : k = 4πkG σ0 C0 ∧ χ is the Euler characteristic, i := by
omega
/- Original: k=1 ≤ ∞ X eC3 N δ -/
theorem eq_089337bb135cc24e (C3 : ) (N : ) (X : ) (e : ) (k : ) (δ : ) : k=1 ≤ ∞ X e-C3 N δ := by
omega
/- Original: m = O((n2 + n log δ 1 )/ε2 ) copies of ρunsqueezed to get outcomes v1 , · · · , v2m ∈ R2n -/
theorem eq_b13ac6b3013ec125 (O : ) (R2n : ) (copies : ) (get : ) (m : ) (n : ) (n2 : ) (of : ) (outcomes : ) (to : ) (v1 : ) (v2m : ) (δ : ) (ε2 : ) (ρunsqueezed : ) : m = O((n2 + n log δ -1 )/ε2 ) copies of ρunsqueezed to get outcomes v1 ∧ * * * ∧ v2m ∈ R2n := by
omega
/- Original: DE = 16i + 16λ4 , then E cannot be the zero polynomial, so we must have A = 0 -/
theorem eq_6b1aad59341606ce (A : ) (DE : ) (E : ) (be : ) (cannot : ) (have : ) (i : ) (must : ) (polynomial : ) (so : ) (the : ) (we : ) (zero : ) (λ4 : ) : DE = -16i + 16λ4 ∧ then E cannot be the zero polynomial ∧ so we must have A = 0 := by
omega
/- Original: H = µ10 B), while boundary conditions are naturally expressed with the inclusion map i : ∂Ω → Ω and its pullback action on forms -/
theorem eq_2a1f22b692aa87c9 (B : ) (H : ) (action : ) (are : ) (boundary : ) (conditions : ) (expressed : ) (forms : ) (i : ) (inclusion : ) (its : ) (map : ) (naturally : ) (on : ) (pullback : ) (the : ) (while : ) (µ10 : ) (Ω : ) : H = µ10 B), while boundary conditions are naturally expressed with the inclusion map i : ∂Ω → Ω ∧ its pullback action on forms := by
omega
/- Original: C ≤ γ dte + γ dte e N −∞ = 1+ Z ∞ dteγt Pr(gk E[gk ] ≥ t) 0 0 √ 2πγC N e γ2 C 2 2 -/
theorem eq_2ceef993fadb8617 (C : ) (E : ) (N : ) (Pr : ) (Z : ) (dte : ) (dteγt : ) (e : ) (gk : ) (t : ) (γ : ) (γ2 : ) (πγC : ) : C ≤ γ dte + γ dte e N -∞ = 1+ Z ∞ dteγt Pr(gk - E[gk ] ≥ t) 0 0 √ 2πγC N e γ2 C 2 2 := by
omega
/- Original: G = (V, E) be a connected, locally finite, infinite graph -/
theorem eq_2927625930f9ceca (E : ) (G : ) (V : ) (a : ) (be : ) (connected : ) (finite : ) (graph : ) (infinite : ) (locally : ) : G = (V ∧ E) be a connected ∧ locally finite ∧ infinite graph := by
omega
/- Original: S = [M T M] and T = [MSM ], and AT = [MM ] -/
theorem eq_b2589194317b5375 (AT : ) (M : ) (MM : ) (MSM : ) (S : ) (T : ) : S = [M* T M] ∧ T = [MSM* ], and AT = [MM* ] := by
omega
/- Original: j = OK (aK N ), when s j ∈ J(N aN ), N aN Kd -/
theorem eq_3b5cf8d2d4956d3c (J : ) (K : ) (Kd : ) (N : ) (OK : ) (a : ) (aN : ) (j : ) (s : ) (when : ) : j = OK (a-K N ) ∧ when s - j ∈ J-(N - aN ) ∧ N - aN Kd := by
omega
/- Original: i=k (97) 1 lim inf lnq pk (X0n1 ) ≥ Hq,k -/
theorem eq_e5af0670d5ebda22 (Hq : ) (X0n : ) (i : ) (inf : ) (k : ) (lim : ) (lnq : ) (pk : ) : i=k (97) 1 lim inf - lnq pk (X0n-1 ) ≥ Hq ∧ k := by
omega
/- Original: q = N1 ∥m∥2 depends on m, we have ∂i q = 2m N -/
theorem eq_526b05d361948008 (N : ) (N1 : ) (depends : ) (have : ) (i : ) (m : ) (on : ) (q : ) (we : ) : q = N1 ∥m∥2 depends on m ∧ we have ∂i q = 2m N := by
omega
/- Original: di=1 |i⟩⟨i|A + |d⟩⟨d|A , trHB (|V0 ⟩⟩⟨⟨V0 |) = P (1 ε2 ) di=1 |i⟩⟨i|A , if d is odd , if d is even so trHB (|V0 ⟩⟩⟨⟨V0 |) ≤ IA -/
theorem eq_2fd8a5739608720e (A : ) (IA : ) (P : ) (V0 : ) (d : ) (di : ) (even : ) (i : ) (is : ) (odd : ) (so : ) (trHB : ) (ε2 : ) : di=1 |i⟩⟨i|A + |d⟩⟨d|A ∧ trHB (|V0 ⟩⟩⟨⟨V0 |) = P (1 - ε2 ) di=1 |i⟩⟨i|A ∧ if d is odd ∧ if d is even so trHB (|V0 ⟩⟩⟨⟨V0 |) ≤ IA := by
omega
/- Original: i=0 τ (35) which satisfies T (A) ∈ gTI for all A and T (A) = A for all A ∈ gTI -/
theorem eq_d725a0ae5e609f46 (A : ) (T : ) (all : ) (for : ) (gTI : ) (i : ) (satisfies : ) (which : ) (τ : ) : i=0 τ (35) which satisfies T (A) ∈ gTI for all A ∧ T (A) = A for all A ∈ gTI := by
omega
/- Original: M ≥ g independent branches: Cmulti = M · (CR + Cprep ) + O(N M 2 ) -/
theorem eq_ee0fe7334f580135 (CR : ) (Cmulti : ) (Cprep : ) (M : ) (N : ) (O : ) (branches : ) (g : ) (independent : ) : M ≥ g independent branches: Cmulti = M * (CR + Cprep ) + O(N M 2 ) := by
omega
/- Original: E = π2 (T M ) E-mail: jorge -/
theorem eq_347dab94660d5126 (E : ) (M : ) (T : ) (jorge : ) (mail : ) (π2 : ) : E = π2* (T * M ) * E-mail: jorge := by
omega
/- Original: Q = L ⋉ U , where L = LI = Q ∩ Θ(Q) -/
theorem eq_772db3539479dd4b (L : ) (LI : ) (Q : ) (U : ) (where : ) (Θ : ) : Q = L ⋉ U ∧ where L = LI = Q ∩ Θ(Q) := by
omega
/- Original: B = B(x, 4r) of radius 4r > 0 that is contained inside of B (k) ∩ S c -/
theorem eq_7f3b54e3d118c8d5 (B : ) (S : ) (c : ) (contained : ) (inside : ) (is : ) (k : ) (of : ) (r : ) (radius : ) (that : ) (x : ) : B = B(x ∧ 4r) of radius 4r > 0 that is contained inside of B (k) ∩ S c := by
omega
/- Original: u = 1 + cn(ϕ, m) = and hence cn(ϕK , m) = 2 , 1 + x2 (1 x2 ) -/
theorem eq_cc987483e73ebf5c (cn : ) (hence : ) (m : ) (u : ) (x2 : ) (ϕ : ) (ϕK : ) : u = 1 + cn(ϕ, m) = ∧ hence cn(ϕK , m) = 2 , 1 + x2 (1 - x2 ) := by
omega
/- Original: n ≥ 1, we set     k X X n Gn := F ⊗ Gn , where Gn := σ X :0≤k ≤2 1 -/
theorem eq_aa3fd0e09ced1b7f (F : ) (Gn : ) (X : ) (k : ) (n : ) (set : ) (we : ) (where : ) (σ : ) : n ≥ 1, we set     k X X n Gn := F ⊗ Gn , where Gn := σ X :0≤k ≤2 -1 := by
omega
/- Original: XB > qn | E(B)) = P(XRκk > qn ) -/
theorem eq_710b5f57b38d8dae (B : ) (E : ) (P : ) (XB : ) (XRκ : ) (k : ) (qn : ) : XB > qn | E(B)) = P(XRκ-k > qn ) := by
omega
/- Original: N ≥ 0 to see that fk+ (N ) ≤ C sup Assume that gm −−−−−→ 0 hence q = 0 -/
theorem eq_682a7c79a2c07abc (Assume : ) (C : ) (N : ) (fk : ) (gm : ) (hence : ) (q : ) (see : ) (sup : ) (that : ) (to : ) : N ≥ 0 to see that fk+ (N ) ≤ C sup Assume that gm -----→ 0 hence q = 0 := by
omega
/- Original: K< is the cone given by  K< = (H(e))e∈En,d | L(e) < L(e ) if e, e satisfy condition (2)(b)(ii) of Definition 4 -/
theorem eq_bc1cdbda2c7b279f (Definition : ) (En : ) (H : ) (K : ) (L : ) (b : ) (by : ) (condition : ) (cone : ) (d : ) (e : ) (given : ) (ii : ) (is : ) (of : ) (satisfy : ) (the : ) : K< is the cone given by  K< = (H(e))e∈En ∧ d | L(e) < L(e ) if e ∧ e satisfy condition (2)(b)(ii) of Definition 4 := by
omega
/- Original: dS = Γo Z ji± nΓi dS = 0 Γi hold -/
theorem eq_094035ea8dbecdbc (Z : ) (dS : ) (hold : ) (ji : ) (nΓi : ) (Γi : ) (Γo : ) : dS = Γo Z ji± nΓi dS = 0 Γi hold := by
omega
/- Original: m =p n=1 1 1 K L   (3 -/
theorem eq_cf28a9fb490522ae (K : ) (L : ) (m : ) (n : ) (p : ) : m =p n=1 1 1 K L   (3 := by
omega
/- Original: n≥1 γ1 ,··· ,γn ∈PL N A∩(γ1 ···γn )̸=∅ n Y φn (γ1 , -/
theorem eq_cdd78fef1b6ac967 (A : ) (N : ) (PL : ) (Y : ) (n : ) (γ1 : ) (γn : ) (φn : ) : n≥1 γ1 ∧ *** ∧ γn ∈PL N A∩(γ1 ***γn )̸=∅ n Y φn (γ1 := by
omega
/- Original: e = 1, ηm = 1, ηf = 1 -/
theorem eq_10fc93294da04990 (e : ) (ηf : ) (ηm : ) : e = -1 ∧ ηm = 1 ∧ ηf = -1 := by
omega
/- Original: e = R+ (Γ)1 Γ, Γ e2 = R+ (Γ2 )1 Γ2 -/
theorem eq_b9b5adde4c75eb99 (R : ) (e : ) (e2 : ) (Γ : ) (Γ2 : ) : e = R+ (Γ)-1 Γ ∧ Γ e2 = R+ (Γ2 )-1 Γ2 := by
omega
/- Original: R = RU(a), pushing both sides through the MPS tensors should give the same virtual operators on the boundary -/
theorem eq_3810af9531ba920b (MPS : ) (R : ) (RU : ) (a : ) (both : ) (boundary : ) (give : ) (on : ) (operators : ) (pushing : ) (same : ) (should : ) (sides : ) (tensors : ) (the : ) (through : ) (virtual : ) : R = RU(a) ∧ pushing both sides through the MPS tensors should give the same virtual operators on the boundary := by
omega
/- Original: ADM = HV take values from −∞ to ∞ due to this subtraction -/
theorem eq_90ae24f93c2aba19 (ADM : ) (HV : ) (due : ) (from : ) (subtraction : ) (take : ) (this : ) (to : ) (values : ) : ADM = HV take values from -∞ to ∞ due to this subtraction := by
omega
/- Original: i=1 where vi = |ei ⟩⟨ei+1 | for i = 1, -/
theorem eq_4b9a9d818949e851 (ei : ) (for : ) (i : ) (vi : ) (where : ) : i=1 where vi = |ei ⟩⟨ei+1 | for i = 1, := by
omega
/- Original: x > a, ψ− (x, k) = eikx , x < 0 -/
theorem eq_203a31a08446bc90 (a : ) (e : ) (ikx : ) (k : ) (x : ) (ψ : ) : x > a ∧ ψ- (x ∧ k) = e-ikx ∧ x < 0 := by
omega
/- Original: j = N, λ j,i = N -/
theorem eq_6dd2330a87fae20a (N : ) (i : ) (j : ) (λ : ) : j = N ∧ λ j ∧ i = -N := by
omega
/- Original: PLi = Li ⊗ t, TORAL CHERNSIMONS TQFT 31 be the toral MaslovKashiwara index of Proposition 2 -/
theorem eq_5032a7d91908ad76 (CHERN : ) (Kashiwara : ) (Li : ) (Maslov : ) (PLi : ) (Proposition : ) (SIMONS : ) (TORAL : ) (TQFT : ) (be : ) (index : ) (of : ) (t : ) (the : ) (toral : ) : PLi = Li ⊗ t ∧ TORAL CHERNSIMONS TQFT 31 be the toral MaslovKashiwara index of Proposition 2 := by
omega
/- Original: m = (2p + 3) -/
theorem eq_540e17d250b0af50 (m : ) (p : ) : m = (2p + 3) := by
omega
/- Original: X = H(P µ×µ X) -/
theorem eq_6c3ba7cc1fb845ce (H : ) (P : ) (X : ) (µ : ) : X = H(P µ*µ X) := by
omega
/- Original: b = 0, and Q b 1 Hilbert-Schmidt -/
theorem eq_3b6ae611d6b382ed (Hilbert : ) (Q : ) (Schmidt : ) (b : ) : b = 0, ∧ Q b - 1 Hilbert-Schmidt := by
omega
/- Original: j = 0), it is locally pure gauge -/
theorem eq_97721d62fd2a1ccb (gauge : ) (is : ) (it : ) (j : ) (locally : ) (pure : ) : j = 0) ∧ it is locally pure gauge := by
omega
/- Original: n = √ · 2n2 -/
theorem eq_5a5fbddb6b6a87a3 (n : ) : n = √ * 2n-2 := by
omega
/- Original: k = 2, as they need some refinement for general k-point correlation functions -/
theorem eq_4e29398f0be55f03 (as : ) (correlation : ) (for : ) (functions : ) (general : ) (k : ) (need : ) (point : ) (refinement : ) (some : ) (they : ) : k = 2 ∧ as they need some refinement for general k-point correlation functions := by
omega
/- Original: Qinst = -/
theorem eq_747a27fec4690e42 (Qinst : ) : Qinst = := by
omega
/- Original: t = 0) = 0) -/
theorem eq_584ccf70dc2448ec (t : ) : t = 0) = 0) := by
omega
/- Original: KLk = KLk (g) is the full subcategory of b g-modules that satisfy the following properties -/
theorem eq_70d1ccc18e7340b6 (KLk : ) (b : ) (following : ) (full : ) (g : ) (is : ) (modules : ) (of : ) (properties : ) (satisfy : ) (subcategory : ) (that : ) (the : ) : KLk = KLk (g) is the full subcategory of b g-modules that satisfy the following properties := by
omega
/- Original: i ≥ 0, γ1 + γ2 + i = γ 1, and l1 + l2 = l -/
theorem eq_aa2457246f273f8f (i : ) (l : ) (l1 : ) (l2 : ) (γ : ) (γ1 : ) (γ2 : ) : i ≥ 0, γ1 + γ2 + i = γ - 1, ∧ l1 + l2 = l := by
omega
/- Original: f = λ0 (F ⊗ id)f , so (F ⊗ id)f =  -/
theorem eq_f08aae76038d585a (F : ) (f : ) (id : ) (so : ) (λ0 : ) : f = λ0 (F ⊗ id)f ∧ so (F ⊗ id)f =  := by
omega
/- Original: k = i term is shown in red horizontal lines -/
theorem eq_cbb575aa4c4bb9c0 (horizontal : ) (i : ) (is : ) (k : ) (lines : ) (red : ) (shown : ) (term : ) : k = i term is shown in red horizontal lines := by
omega
/- Original: N =1 where ψ̃ denotes the normalized LQG coherent state -/
theorem eq_e239715ab54a14e7 (LQG : ) (N : ) (coherent : ) (denotes : ) (normalized : ) (state : ) (the : ) (where : ) (ψ : ) : N =1 where ψ̃ denotes the normalized LQG coherent state := by
omega
/- Original: j=1 Therefore, we can apply Theorem 2 -/
theorem eq_43d1ba4864a0e012 (Theorem : ) (Therefore : ) (apply : ) (can : ) (j : ) (we : ) : j=1 Therefore ∧ we can apply Theorem 2 := by
omega
/- Original: A = *-alg(J) -/
theorem eq_8667a4abcdfb0e33 (A : ) (J : ) (alg : ) : A = *-alg(J) := by
omega
/- Original: dKdr = f1 drtt when e2ψ = f holds in vacuum -/
theorem eq_2eee55494a48e808 (dKdr : ) (drtt : ) (e2ψ : ) (f : ) (f1 : ) (holds : ) (vacuum : ) (when : ) : dKdr = f1 drtt when e2ψ = f holds in vacuum := by
omega
/- Original: s = 12 , similar to (3 -/
theorem eq_e73d75157c00b15f (s : ) (similar : ) (to : ) : s = 12 ∧ similar to (3 := by
omega
/- Original: I = Id is defined as in Subsection 2 -/
theorem eq_2309f4fa60e78526 (I : ) (Id : ) (Subsection : ) (as : ) (defined : ) (is : ) : I = Id is defined as in Subsection 2 := by
omega
/- Original: P = 1000 for 2-bead and 3-bead polymer molecules, and choose P = 1000, 2000, 5000, 10000 for 4-bead polymer molecules -/
theorem eq_e6bb6012128aeb31 (P : ) (bead : ) (choose : ) (for : ) (molecules : ) (polymer : ) : P = 1000 for 2-bead ∧ 3-bead polymer molecules, and choose P = 1000, 2000, 5000, 10000 for 4-bead polymer molecules := by
omega
/- Original: i = ais 1 Ks -/
theorem eq_dea3ec296a54c888 (Ks : ) (ais : ) (i : ) : i = ais 1 Ks := by
omega