Notation by work
Hilbert 12: contracting ambient torsion
All notation · Glossary · Source coverage
196 symbol spellings in 133 mathematical passages across 3 selected source files. Subscripts and superscripts have their own entries alongside their base symbols.
The same symbol can have several meanings here. A passage classified as a definition may define another part of its expression. Read the linked context before assigning a meaning.
All 196 entries are available below.
+Use in source · 31 passages
Search aliases: +
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 15
ω^2+ω+1=0, β^3=7, ε=2-β, ρ=ε^-1=β^2+2β+4.
Exact mathematical passage
\omega^2+\omega+1=0,\quad \beta^3=7,\quad \varepsilon=2-\beta,\quad \rho=\varepsilon^{-1}=\beta^2+2\beta+4.
=Use in source · 77 passages
Search aliases: =
Use in source · H12_Ambient_Torsion_README.md, line 5
This research package continues the pure cubic experiment K= Q(β), β^3=7.
Exact mathematical passage
K=\mathbb Q(\beta)
AUse in source · 3 passages
Search aliases: A
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 155
A_0=4k+5ℓ+j, B_0=4ℓ+5j, C_0=4j,
Exact mathematical passage
A_0=4k+5\ell+j,\qquad B_0=4\ell+5j,\qquad C_0=4j,
aUse in source · 9 passages
Search aliases: a
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 45
q_a(z)=fracθ_0(z;a)^5θ_0(5z;5a).
Exact mathematical passage
q_a(z)=\frac{\theta_0(z;a)^5}{\theta_0(5z;5a)}.
A_0Use in source · 3 passages
Search aliases: A_0
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 155
A_0=4k+5ℓ+j, B_0=4ℓ+5j, C_0=4j,
Exact mathematical passage
A_0=4k+5\ell+j,\qquad B_0=4\ell+5j,\qquad C_0=4j,
a_0Use in source · 1 passage
Search aliases: a_0
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 385
The covector a_0=(1,0,0)^T, corresponding to the oriented complementary pairing with w, has an orbit of length **21** under this matrix. Its first three iterates are
Exact mathematical passage
a_0=(1,0,0)^T
a_xUse in source · 1 passage
Search aliases: a_x
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 208
Let d_x=(a_x,b_x,c_x)^T be the integer carry vector from Section 3. At stage m, the carry is d_x,m=R^m-1d_x∈ Z^3. Set W_x,m=ρ^m-1z_T x. By the arithmetic transport formula,
Exact mathematical passage
d_x=(a_x,b_x,c_x)^T
a_{x,m}Use in source · 2 passages
Search aliases: a_x,m
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 210
ρ^m z_x=W_x,m+a_x,mτ+b_x,mσ+c_x,m.
Exact mathematical passage
\rho^m z_x=W_{x,m}+a_{x,m}\tau+b_{x,m}\sigma+c_{x,m}.
BUse in source · 3 passages
Search aliases: B
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 155
A_0=4k+5ℓ+j, B_0=4ℓ+5j, C_0=4j,
Exact mathematical passage
A_0=4k+5\ell+j,\qquad B_0=4\ell+5j,\qquad C_0=4j,
bUse in source · 6 passages
Search aliases: b
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 169
ρ z_k,ℓ,j= z_k',ℓ',j'+aτ+bσ+c
Exact mathematical passage
\boxed{ \rho z_{k,\ell,j}= z_{k',\ell',j'}+a\tau+b\sigma+c }
B_0Use in source · 3 passages
Search aliases: B_0
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 155
A_0=4k+5ℓ+j, B_0=4ℓ+5j, C_0=4j,
Exact mathematical passage
A_0=4k+5\ell+j,\qquad B_0=4\ell+5j,\qquad C_0=4j,
b_xUse in source · 1 passage
Search aliases: b_x
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 208
Let d_x=(a_x,b_x,c_x)^T be the integer carry vector from Section 3. At stage m, the carry is d_x,m=R^m-1d_x∈ Z^3. Set W_x,m=ρ^m-1z_T x. By the arithmetic transport formula,
Exact mathematical passage
d_x=(a_x,b_x,c_x)^T
b_{x,m}Use in source · 2 passages
Search aliases: b_x,m
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 210
ρ^m z_x=W_x,m+a_x,mτ+b_x,mσ+c_x,m.
Exact mathematical passage
\rho^m z_x=W_{x,m}+a_{x,m}\tau+b_{x,m}\sigma+c_{x,m}.
\bmodUse in source · 2 passages
Search aliases: bmod
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 167
Write (k',ℓ',j')=(A_0,B_0,C_0)bmod7. Then
Exact mathematical passage
(k',\ell',j')=(A_0,B_0,C_0)\bmod7
CUse in source · 9 passages
Search aliases: C
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 155
A_0=4k+5ℓ+j, B_0=4ℓ+5j, C_0=4j,
Exact mathematical passage
A_0=4k+5\ell+j,\qquad B_0=4\ell+5j,\qquad C_0=4j,
cUse in source · 4 passages
Search aliases: c
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 169
ρ z_k,ℓ,j= z_k',ℓ',j'+aτ+bσ+c
Exact mathematical passage
\boxed{ \rho z_{k,\ell,j}= z_{k',\ell',j'}+a\tau+b\sigma+c }
C_0Use in source · 3 passages
Search aliases: C_0
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 155
A_0=4k+5ℓ+j, B_0=4ℓ+5j, C_0=4j,
Exact mathematical passage
A_0=4k+5\ell+j,\qquad B_0=4\ell+5j,\qquad C_0=4j,
C_mUse in source · 1 passage
Search aliases: C_m
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 364
f_m(x)=C_m(x)f_m-1(Tx), x∈ V.
Exact mathematical passage
f_m(x)=C_m(x)f_{m-1}(Tx),\qquad x\in V.
C_{\mathrm{pol}}Use in source · 1 passage
Search aliases: C_pol mathrm
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 348
Im(C_polU_Γ^3)=0
Exact mathematical passage
\operatorname{Im}(C_{\mathrm{pol}}U_\Gamma^3)=0
C_{T^{-m}x}^{(m)}Use in source · 1 passage
Search aliases: C_T^-mx^(m)
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 246
F(z_x)=ε^2 ∏_m=1^∞ (C_T^-mx^(m))^-1.
Exact mathematical passage
\boxed{ F(z_x)=\varepsilon^2 \prod_{m=1}^{\infty} \left(C_{T^{-m}x}^{(m)}\right)^{-1}. }
c_xUse in source · 1 passage
Search aliases: c_x
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 208
Let d_x=(a_x,b_x,c_x)^T be the integer carry vector from Section 3. At stage m, the carry is d_x,m=R^m-1d_x∈ Z^3. Set W_x,m=ρ^m-1z_T x. By the arithmetic transport formula,
Exact mathematical passage
d_x=(a_x,b_x,c_x)^T
c_{x,m}Use in source · 1 passage
Search aliases: c_x,m
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 210
ρ^m z_x=W_x,m+a_x,mτ+b_x,mσ+c_x,m.
Exact mathematical passage
\rho^m z_x=W_{x,m}+a_{x,m}\tau+b_{x,m}\sigma+c_{x,m}.
C_x^{(m)}Use in source · 3 passages
Search aliases: C_x^(m)
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 227
C_x^(m)= P(q_t^-1;b_x,m,W_x,m,σ) P(q_σ;a_x,m,W_x,m+b_x,mσ,τ).
Exact mathematical passage
\boxed{ C_x^{(m)}= \mathcal P(q_t^{-1};b_{x,m},W_{x,m},\sigma)\, \mathcal P(q_\sigma;a_{x,m},W_{x,m}+b_{x,m}\sigma,\tau). }
dUse in source · 2 passages
Search aliases: d
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 208
Let d_x=(a_x,b_x,c_x)^T be the integer carry vector from Section 3. At stage m, the carry is d_x,m=R^m-1d_x∈ Z^3. Set W_x,m=ρ^m-1z_T x. By the arithmetic transport formula,
Exact mathematical passage
d_x=(a_x,b_x,c_x)^T
d_xUse in source · 2 passages
Search aliases: d_x
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 208
Let d_x=(a_x,b_x,c_x)^T be the integer carry vector from Section 3. At stage m, the carry is d_x,m=R^m-1d_x∈ Z^3. Set W_x,m=ρ^m-1z_T x. By the arithmetic transport formula,
Exact mathematical passage
d_x=(a_x,b_x,c_x)^T
d_{x,m}Use in source · 1 passage
Search aliases: d_x,m
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 208
Let d_x=(a_x,b_x,c_x)^T be the integer carry vector from Section 3. At stage m, the carry is d_x,m=R^m-1d_x∈ Z^3. Set W_x,m=ρ^m-1z_T x. By the arithmetic transport formula,
Exact mathematical passage
d_{x,m}=R^{m-1}d_x\in\mathbb Z^3
\detUse in source · 1 passage
Search aliases: det
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 124
Since δ,η,ξ are the images of u/7,v/7,w/7, and det[u v w]=1, the 343 labels represent all of tfrac17Λ/Λ. Here this is torsion of the rank-three lattice quotient, not a claim that the nondiscrete rank-three quotient is an ordinary elliptic curve.
Exact mathematical passage
\det[u\ v\ w]=1
eUse in source · 3 passages
Search aliases: e
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 262
L_t,σ(z)=-5∑_substackm≥1 5nmid m fracP^m e^2π imz-Q^m e^-2π imz m(1-P^m)(1-Q^m), P=e^2π it, Q=e^2π iσ.
Exact mathematical passage
L_{t,\sigma}(z)=-5\sum_{\substack{m\ge1\\5\nmid m}} \frac{P^m e^{2\pi imz}-Q^m e^{-2\pi imz}} {m(1-P^m)(1-Q^m)},\qquad P=e^{2\pi it},\ Q=e^{2\pi i\sigma}.
e^{-2\pi i nq z}Use in source · 1 passage
Search aliases: e^-2π i nq z pi
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 297
-5∑_substackq≥1 5nmid nq fracP^q e^2π i nq z-Q^q e^-2π i nq z q(1-P^q)(1-Q^q).
Exact mathematical passage
-5\sum_{\substack{q\ge1\\5\nmid nq}} \frac{P^q e^{2\pi i nq z}-Q^q e^{-2\pi i nq z}} {q(1-P^q)(1-Q^q)}.
e^{-2\pi imz}Use in source · 1 passage
Search aliases: e^-2π imz pi
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 262
L_t,σ(z)=-5∑_substackm≥1 5nmid m fracP^m e^2π imz-Q^m e^-2π imz m(1-P^m)(1-Q^m), P=e^2π it, Q=e^2π iσ.
Exact mathematical passage
L_{t,\sigma}(z)=-5\sum_{\substack{m\ge1\\5\nmid m}} \frac{P^m e^{2\pi imz}-Q^m e^{-2\pi imz}} {m(1-P^m)(1-Q^m)},\qquad P=e^{2\pi it},\ Q=e^{2\pi i\sigma}.
e^{2\pi i nq z}Use in source · 1 passage
Search aliases: e^2π i nq z pi
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 297
-5∑_substackq≥1 5nmid nq fracP^q e^2π i nq z-Q^q e^-2π i nq z q(1-P^q)(1-Q^q).
Exact mathematical passage
-5\sum_{\substack{q\ge1\\5\nmid nq}} \frac{P^q e^{2\pi i nq z}-Q^q e^{-2\pi i nq z}} {q(1-P^q)(1-Q^q)}.
e^{2\pi i/7}Use in source · 1 passage
Search aliases: e^2π i/7 pi
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 330
Fix the oriented seventh-root phase ζ_7=e^2π i/7. The additive character against the top dual direction is
Exact mathematical passage
\zeta_7=e^{2\pi i/7}
e^{2\pi imz}Use in source · 1 passage
Search aliases: e^2π imz pi
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 262
L_t,σ(z)=-5∑_substackm≥1 5nmid m fracP^m e^2π imz-Q^m e^-2π imz m(1-P^m)(1-Q^m), P=e^2π it, Q=e^2π iσ.
Exact mathematical passage
L_{t,\sigma}(z)=-5\sum_{\substack{m\ge1\\5\nmid m}} \frac{P^m e^{2\pi imz}-Q^m e^{-2\pi imz}} {m(1-P^m)(1-Q^m)},\qquad P=e^{2\pi it},\ Q=e^{2\pi i\sigma}.
e^{2\pi it}Use in source · 1 passage
Search aliases: e^2π it pi
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 262
L_t,σ(z)=-5∑_substackm≥1 5nmid m fracP^m e^2π imz-Q^m e^-2π imz m(1-P^m)(1-Q^m), P=e^2π it, Q=e^2π iσ.
Exact mathematical passage
L_{t,\sigma}(z)=-5\sum_{\substack{m\ge1\\5\nmid m}} \frac{P^m e^{2\pi imz}-Q^m e^{-2\pi imz}} {m(1-P^m)(1-Q^m)},\qquad P=e^{2\pi it},\ Q=e^{2\pi i\sigma}.
e^{2\pi i\sigma}Use in source · 1 passage
Search aliases: e^2π iσ pi sigma
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 262
L_t,σ(z)=-5∑_substackm≥1 5nmid m fracP^m e^2π imz-Q^m e^-2π imz m(1-P^m)(1-Q^m), P=e^2π it, Q=e^2π iσ.
Exact mathematical passage
L_{t,\sigma}(z)=-5\sum_{\substack{m\ge1\\5\nmid m}} \frac{P^m e^{2\pi imz}-Q^m e^{-2\pi imz}} {m(1-P^m)(1-Q^m)},\qquad P=e^{2\pi it},\ Q=e^{2\pi i\sigma}.
\mathrm{ell}Use in source · 1 passage
Search aliases: ell mathrm
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 30
F(z)=fracΓ_ell(z;τ,σ)^5 Γ_ell(5z;5τ,5σ), U_Γ=F(z_0).
Exact mathematical passage
F(z)=\frac{\Gamma_{\mathrm{ell}}(z;\tau,\sigma)^5} {\Gamma_{\mathrm{ell}}(5z;5\tau,5\sigma)},\qquad U_\Gamma=F(z_0).
\expUse in source · 1 passage
Search aliases: exp
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 356
Let V=( Z/7)^3, ζ=exp(2π i/7), and let F be the ordinary finite Fourier transform
Exact mathematical passage
\zeta=\exp(2\pi i/7)
FUse in source · 11 passages
Search aliases: F
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 30
F(z)=fracΓ_ell(z;τ,σ)^5 Γ_ell(5z;5τ,5σ), U_Γ=F(z_0).
Exact mathematical passage
F(z)=\frac{\Gamma_{\mathrm{ell}}(z;\tau,\sigma)^5} {\Gamma_{\mathrm{ell}}(5z;5\tau,5\sigma)},\qquad U_\Gamma=F(z_0).
\mathbb FUse in source · 1 passage
Search aliases: F mathbb
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 90
Because R^3-I≠0, the order of R in GL_3( F_7) is exactly 21. Its one-dimensional eigenline has scalar action 4, of order three. Thus the order-three torsion packet is the semisimple slice of a nonsemisimple order-21 arithmetic operator.
Exact mathematical passage
\mathrm{GL}_3(\mathbb F_7)
\mathcal FUse in source · 1 passage
Search aliases: F mathcal
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 356
Let V=( Z/7)^3, ζ=exp(2π i/7), and let F be the ordinary finite Fourier transform
Exact mathematical passage
\mathcal F
fUse in source · 5 passages
Search aliases: f
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 204
f_x^(m)=F(ρ^m z_x), m≥0.
Exact mathematical passage
f_x^{(m)}=F(\rho^m z_x),\qquad m\ge0.
\mathbb F_7Use in source · 1 passage
Search aliases: F_7 mathbb
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 90
Because R^3-I≠0, the order of R in GL_3( F_7) is exactly 21. Its one-dimensional eigenline has scalar action 4, of order three. Thus the order-three torsion packet is the semisimple slice of a nonsemisimple order-21 arithmetic operator.
Exact mathematical passage
\mathrm{GL}_3(\mathbb F_7)
f_mUse in source · 1 passage
Search aliases: f_m
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 364
f_m(x)=C_m(x)f_m-1(Tx), x∈ V.
Exact mathematical passage
f_m(x)=C_m(x)f_{m-1}(Tx),\qquad x\in V.
f_{m-1}Use in source · 1 passage
Search aliases: f_m-1
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 364
f_m(x)=C_m(x)f_m-1(Tx), x∈ V.
Exact mathematical passage
f_m(x)=C_m(x)f_{m-1}(Tx),\qquad x\in V.
f_{T x}^{(m-1)}Use in source · 1 passage
Search aliases: f_T x^(m-1)
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 237
f_x^(m)=C_x^(m) f_T x^(m-1).
Exact mathematical passage
\boxed{f_x^{(m)}=C_x^{(m)} f_{T x}^{(m-1)}.}
f_x^{(m)}Use in source · 3 passages
Search aliases: f_x^(m)
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 204
f_x^(m)=F(ρ^m z_x), m≥0.
Exact mathematical passage
f_x^{(m)}=F(\rho^m z_x),\qquad m\ge0.
GUse in source · 1 passage
Search aliases: G
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 326
G_H=0 · 0 · 1 0 · 1 · 0 1 · 0 · 0.
Exact mathematical passage
G_H=\begin{pmatrix}0&0&1\\0&1&0\\1&0&0\end{pmatrix}.
gUse in source · 1 passage
Search aliases: g
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 216
P(g;n,w,h)= ∏_r=0^n-1g(w+rh), · n>0, 1, · n=0, ∏_r=n^-1g(w+rh)^-1, · n<0.
Exact mathematical passage
\mathcal P(g;n,w,h)= \begin{cases} \prod_{r=0}^{n-1}g(w+rh),&n>0,\\ 1,&n=0,\\ \prod_{r=n}^{-1}g(w+rh)^{-1},&n<0. \end{cases}
G_HUse in source · 1 passage
Search aliases: G_H
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 326
G_H=0 · 0 · 1 0 · 1 · 0 1 · 0 · 0.
Exact mathematical passage
G_H=\begin{pmatrix}0&0&1\\0&1&0\\1&0&0\end{pmatrix}.
\mathrm{GL}Use in source · 1 passage
Search aliases: GL mathrm
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 90
Because R^3-I≠0, the order of R in GL_3( F_7) is exactly 21. Its one-dimensional eigenline has scalar action 4, of order three. Thus the order-three torsion packet is the semisimple slice of a nonsemisimple order-21 arithmetic operator.
Exact mathematical passage
\mathrm{GL}_3(\mathbb F_7)
\mathrm{GL}_3Use in source · 1 passage
Search aliases: GL_3 mathrm
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 90
Because R^3-I≠0, the order of R in GL_3( F_7) is exactly 21. Its one-dimensional eigenline has scalar action 4, of order three. Thus the order-three torsion packet is the semisimple slice of a nonsemisimple order-21 arithmetic operator.
Exact mathematical passage
\mathrm{GL}_3(\mathbb F_7)
HUse in source · 4 passages
Search aliases: H
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 94
H=4 · -4 · 15 -4 · 1 · 0 15 · 0 · 0, M^T H=HM,
Exact mathematical passage
H=\begin{pmatrix}4&-4&15\\-4&1&0\\15&0&0\end{pmatrix},\qquad M^T H=HM,
hUse in source · 1 passage
Search aliases: h
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 216
P(g;n,w,h)= ∏_r=0^n-1g(w+rh), · n>0, 1, · n=0, ∏_r=n^-1g(w+rh)^-1, · n<0.
Exact mathematical passage
\mathcal P(g;n,w,h)= \begin{cases} \prod_{r=0}^{n-1}g(w+rh),&n>0,\\ 1,&n=0,\\ \prod_{r=n}^{-1}g(w+rh)^{-1},&n<0. \end{cases}
IUse in source · 4 passages
Search aliases: I
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 63
Let N=M-2Ipmod7. Then N^3=0 and N^2≠0. Define
Exact mathematical passage
N=M-2I\pmod7
iUse in source · 4 passages
Search aliases: i
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 262
L_t,σ(z)=-5∑_substackm≥1 5nmid m fracP^m e^2π imz-Q^m e^-2π imz m(1-P^m)(1-Q^m), P=e^2π it, Q=e^2π iσ.
Exact mathematical passage
L_{t,\sigma}(z)=-5\sum_{\substack{m\ge1\\5\nmid m}} \frac{P^m e^{2\pi imz}-Q^m e^{-2\pi imz}} {m(1-P^m)(1-Q^m)},\qquad P=e^{2\pi it},\ Q=e^{2\pi i\sigma}.
\operatorname{Im}Use in source · 1 passage
Search aliases: Im operatorname
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 348
Im(C_polU_Γ^3)=0
Exact mathematical passage
\operatorname{Im}(C_{\mathrm{pol}}U_\Gamma^3)=0
JUse in source · 1 passage
Search aliases: J
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 346
A successful next theorem would compute a character-sensitive, correctly based analytic transport and prove that its arithmetic evaluation agrees with the oriented Gauss/Jacobi coordinate J=2+3ω. The fixed desired scalar identity remains
Exact mathematical passage
J=2+3\omega
jUse in source · 20 passages
Search aliases: j
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 119
z_k,ℓ,j=z_0+kδ+ℓη+jξ, k,ℓ,j∈{0,…,6}.
Exact mathematical passage
\boxed{z_{k,\ell,j}=z_0+k\delta+\ell\eta+j\xi,\qquad k,\ell,j\in\{0,\ldots,6\}.}
j'Use in source · 2 passages
Search aliases: j'
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 167
Write (k',ℓ',j')=(A_0,B_0,C_0)bmod7. Then
Exact mathematical passage
(k',\ell',j')=(A_0,B_0,C_0)\bmod7
KUse in source · 1 passage
Search aliases: K
Use in source · H12_Ambient_Torsion_README.md, line 5
This research package continues the pure cubic experiment K= Q(β), β^3=7.
Exact mathematical passage
K=\mathbb Q(\beta)
kUse in source · 17 passages
Search aliases: k
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 117
The seven-point packet has arguments z_0+kδ. The first refinement consists of z_0+kδ+ℓη, with 49 labels. The full ambient packet is
Exact mathematical passage
z_0+k\delta
k'Use in source · 2 passages
Search aliases: k'
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 167
Write (k',ℓ',j')=(A_0,B_0,C_0)bmod7. Then
Exact mathematical passage
(k',\ell',j')=(A_0,B_0,C_0)\bmod7
LUse in source · 2 passages
Search aliases: L
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 262
L_t,σ(z)=-5∑_substackm≥1 5nmid m fracP^m e^2π imz-Q^m e^-2π imz m(1-P^m)(1-Q^m), P=e^2π it, Q=e^2π iσ.
Exact mathematical passage
L_{t,\sigma}(z)=-5\sum_{\substack{m\ge1\\5\nmid m}} \frac{P^m e^{2\pi imz}-Q^m e^{-2\pi imz}} {m(1-P^m)(1-Q^m)},\qquad P=e^{2\pi it},\ Q=e^{2\pi i\sigma}.
L_{t,\sigma}Use in source · 2 passages
Search aliases: L_t,σ sigma
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 262
L_t,σ(z)=-5∑_substackm≥1 5nmid m fracP^m e^2π imz-Q^m e^-2π imz m(1-P^m)(1-Q^m), P=e^2π it, Q=e^2π iσ.
Exact mathematical passage
L_{t,\sigma}(z)=-5\sum_{\substack{m\ge1\\5\nmid m}} \frac{P^m e^{2\pi imz}-Q^m e^{-2\pi imz}} {m(1-P^m)(1-Q^m)},\qquad P=e^{2\pi it},\ Q=e^{2\pi i\sigma}.
\lfloorUse in source · 1 passage
Search aliases: lfloor
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 161
q_1=lfloor A_0/7rfloor, q_2=lfloor B_0/7rfloor, q_3=lfloor C_0/7rfloor.
Exact mathematical passage
q_1=\lfloor A_0/7\rfloor,\quad q_2=\lfloor B_0/7\rfloor,\quad q_3=\lfloor C_0/7\rfloor.
MUse in source · 3 passages
Search aliases: M
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 54
M=0 · 1 · 0 -4 · 2 · 15 -1 · 0 · 4, R=M^-1=8 · -4 · 15 1 · 0 · 0 2 · -1 · 4.
Exact mathematical passage
M=\begin{pmatrix}0&1&0\\-4&2&15\\-1&0&4\end{pmatrix},\qquad R=M^{-1}=\begin{pmatrix}8&-4&15\\1&0&0\\2&-1&4\end{pmatrix}.
mUse in source · 15 passages
Search aliases: m
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 204
f_x^(m)=F(ρ^m z_x), m≥0.
Exact mathematical passage
f_x^{(m)}=F(\rho^m z_x),\qquad m\ge0.
M^{-1}Use in source · 1 passage
Search aliases: M^-1
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 54
M=0 · 1 · 0 -4 · 2 · 15 -1 · 0 · 4, R=M^-1=8 · -4 · 15 1 · 0 · 0 2 · -1 · 4.
Exact mathematical passage
M=\begin{pmatrix}0&1&0\\-4&2&15\\-1&0&4\end{pmatrix},\qquad R=M^{-1}=\begin{pmatrix}8&-4&15\\1&0&0\\2&-1&4\end{pmatrix}.
M^TUse in source · 1 passage
Search aliases: M^T
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 94
H=4 · -4 · 15 -4 · 1 · 0 15 · 0 · 0, M^T H=HM,
Exact mathematical passage
H=\begin{pmatrix}4&-4&15\\-4&1&0\\15&0&0\end{pmatrix},\qquad M^T H=HM,
\midUse in source · 2 passages
Search aliases: mid
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 279
N_nF(z)= F(nz), · 5nmid n, 1, · 5mid n.
Exact mathematical passage
\boxed{ \mathcal N_nF(z)= \begin{cases}F(nz),&5\nmid n,\\1,&5\mid n.\end{cases} }
NUse in source · 8 passages
Search aliases: N
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 63
Let N=M-2Ipmod7. Then N^3=0 and N^2≠0. Define
Exact mathematical passage
N=M-2I\pmod7
\mathcal NUse in source · 3 passages
Search aliases: N mathcal
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 271
N_n F(z)= ∏_u=1-n^0∏_v=0^n-1∏_j=0^n-1 F(z+fracut+vσ+jn).
Exact mathematical passage
\mathcal N_n F(z)= \prod_{u=1-n}^{0}\prod_{v=0}^{n-1}\prod_{j=0}^{n-1} F\left(z+\frac{ut+v\sigma+j}{n}\right).
nUse in source · 15 passages
Search aliases: n
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 214
For an integer n, define the oriented finite product
Exact mathematical passage
n
N^2Use in source · 4 passages
Search aliases: N^2
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 63
Let N=M-2Ipmod7. Then N^3=0 and N^2≠0. Define
Exact mathematical passage
N^2\ne0
N^3Use in source · 1 passage
Search aliases: N^3
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 63
Let N=M-2Ipmod7. Then N^3=0 and N^2≠0. Define
Exact mathematical passage
N^3=0
\mathcal N_7Use in source · 1 passage
Search aliases: N_7 mathcal
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 307
N_7F(1/3)=F(7/3)=F(1/3)=U_Γ.
Exact mathematical passage
\boxed{\mathcal N_7F(1/3)=F(7/3)=F(1/3)=U_\Gamma.}
\mathcal N_nUse in source · 2 passages
Search aliases: N_n mathcal
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 271
N_n F(z)= ∏_u=1-n^0∏_v=0^n-1∏_j=0^n-1 F(z+fracut+vσ+jn).
Exact mathematical passage
\mathcal N_n F(z)= \prod_{u=1-n}^{0}\prod_{v=0}^{n-1}\prod_{j=0}^{n-1} F\left(z+\frac{ut+v\sigma+j}{n}\right).
\nmidUse in source · 6 passages
Search aliases: nmid
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 262
L_t,σ(z)=-5∑_substackm≥1 5nmid m fracP^m e^2π imz-Q^m e^-2π imz m(1-P^m)(1-Q^m), P=e^2π it, Q=e^2π iσ.
Exact mathematical passage
L_{t,\sigma}(z)=-5\sum_{\substack{m\ge1\\5\nmid m}} \frac{P^m e^{2\pi imz}-Q^m e^{-2\pi imz}} {m(1-P^m)(1-Q^m)},\qquad P=e^{2\pi it},\ Q=e^{2\pi i\sigma}.
OUse in source · 1 passage
Search aliases: O
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 242
As ρ^m z_x→0, all f_x^(m)→ F(0)=ε^2. Every multiplier is nonzero at the chosen arguments, and C_x^(m)=1+O(|ρ|^m-1).
Exact mathematical passage
C_x^{(m)}=1+O(|\rho|^{m-1})
PUse in source · 3 passages
Search aliases: P
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 262
L_t,σ(z)=-5∑_substackm≥1 5nmid m fracP^m e^2π imz-Q^m e^-2π imz m(1-P^m)(1-Q^m), P=e^2π it, Q=e^2π iσ.
Exact mathematical passage
L_{t,\sigma}(z)=-5\sum_{\substack{m\ge1\\5\nmid m}} \frac{P^m e^{2\pi imz}-Q^m e^{-2\pi imz}} {m(1-P^m)(1-Q^m)},\qquad P=e^{2\pi it},\ Q=e^{2\pi i\sigma}.
\mathcal PUse in source · 2 passages
Search aliases: P mathcal
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 216
P(g;n,w,h)= ∏_r=0^n-1g(w+rh), · n>0, 1, · n=0, ∏_r=n^-1g(w+rh)^-1, · n<0.
Exact mathematical passage
\mathcal P(g;n,w,h)= \begin{cases} \prod_{r=0}^{n-1}g(w+rh),&n>0,\\ 1,&n=0,\\ \prod_{r=n}^{-1}g(w+rh)^{-1},&n<0. \end{cases}
P^{-(n-1)q}Use in source · 1 passage
Search aliases: P^-(n-1)q
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 288
∑_u=1-n^0P^qu =P^-(n-1)qfrac1-P^nq1-P^q, ∑_v=0^n-1Q^qv =frac1-Q^nq1-Q^q.
Exact mathematical passage
\sum_{u=1-n}^{0}P^{qu} =P^{-(n-1)q}\frac{1-P^{nq}}{1-P^q},\qquad \sum_{v=0}^{n-1}Q^{qv} =\frac{1-Q^{nq}}{1-Q^q}.
P^mUse in source · 1 passage
Search aliases: P^m
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 262
L_t,σ(z)=-5∑_substackm≥1 5nmid m fracP^m e^2π imz-Q^m e^-2π imz m(1-P^m)(1-Q^m), P=e^2π it, Q=e^2π iσ.
Exact mathematical passage
L_{t,\sigma}(z)=-5\sum_{\substack{m\ge1\\5\nmid m}} \frac{P^m e^{2\pi imz}-Q^m e^{-2\pi imz}} {m(1-P^m)(1-Q^m)},\qquad P=e^{2\pi it},\ Q=e^{2\pi i\sigma}.
P^{nq}Use in source · 1 passage
Search aliases: P^nq
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 288
∑_u=1-n^0P^qu =P^-(n-1)qfrac1-P^nq1-P^q, ∑_v=0^n-1Q^qv =frac1-Q^nq1-Q^q.
Exact mathematical passage
\sum_{u=1-n}^{0}P^{qu} =P^{-(n-1)q}\frac{1-P^{nq}}{1-P^q},\qquad \sum_{v=0}^{n-1}Q^{qv} =\frac{1-Q^{nq}}{1-Q^q}.
P^qUse in source · 2 passages
Search aliases: P^q
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 288
∑_u=1-n^0P^qu =P^-(n-1)qfrac1-P^nq1-P^q, ∑_v=0^n-1Q^qv =frac1-Q^nq1-Q^q.
Exact mathematical passage
\sum_{u=1-n}^{0}P^{qu} =P^{-(n-1)q}\frac{1-P^{nq}}{1-P^q},\qquad \sum_{v=0}^{n-1}Q^{qv} =\frac{1-Q^{nq}}{1-Q^q}.
P^{qu}Use in source · 1 passage
Search aliases: P^qu
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 288
∑_u=1-n^0P^qu =P^-(n-1)qfrac1-P^nq1-P^q, ∑_v=0^n-1Q^qv =frac1-Q^nq1-Q^q.
Exact mathematical passage
\sum_{u=1-n}^{0}P^{qu} =P^{-(n-1)q}\frac{1-P^{nq}}{1-P^q},\qquad \sum_{v=0}^{n-1}Q^{qv} =\frac{1-Q^{nq}}{1-Q^q}.
\pmodUse in source · 5 passages
Search aliases: pmod
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 63
Let N=M-2Ipmod7. Then N^3=0 and N^2≠0. Define
Exact mathematical passage
N=M-2I\pmod7
\mathrm{pol}Use in source · 1 passage
Search aliases: pol mathrm
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 348
Im(C_polU_Γ^3)=0
Exact mathematical passage
\operatorname{Im}(C_{\mathrm{pol}}U_\Gamma^3)=0
QUse in source · 3 passages
Search aliases: Q
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 262
L_t,σ(z)=-5∑_substackm≥1 5nmid m fracP^m e^2π imz-Q^m e^-2π imz m(1-P^m)(1-Q^m), P=e^2π it, Q=e^2π iσ.
Exact mathematical passage
L_{t,\sigma}(z)=-5\sum_{\substack{m\ge1\\5\nmid m}} \frac{P^m e^{2\pi imz}-Q^m e^{-2\pi imz}} {m(1-P^m)(1-Q^m)},\qquad P=e^{2\pi it},\ Q=e^{2\pi i\sigma}.
\mathbb QUse in source · 1 passage
Search aliases: Q mathbb
Use in source · H12_Ambient_Torsion_README.md, line 5
This research package continues the pure cubic experiment K= Q(β), β^3=7.
Exact mathematical passage
K=\mathbb Q(\beta)
qUse in source · 10 passages
Search aliases: q
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 37
F(z+1)=F(z), F(z+τ)=q_σ(z)F(z), F(z+σ)=q_t(z)^-1F(z),
Exact mathematical passage
F(z+1)=F(z),\qquad F(z+\tau)=q_\sigma(z)F(z),\qquad F(z+\sigma)=q_t(z)^{-1}F(z),
Q^mUse in source · 1 passage
Search aliases: Q^m
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 262
L_t,σ(z)=-5∑_substackm≥1 5nmid m fracP^m e^2π imz-Q^m e^-2π imz m(1-P^m)(1-Q^m), P=e^2π it, Q=e^2π iσ.
Exact mathematical passage
L_{t,\sigma}(z)=-5\sum_{\substack{m\ge1\\5\nmid m}} \frac{P^m e^{2\pi imz}-Q^m e^{-2\pi imz}} {m(1-P^m)(1-Q^m)},\qquad P=e^{2\pi it},\ Q=e^{2\pi i\sigma}.
Q^{nq}Use in source · 1 passage
Search aliases: Q^nq
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 288
∑_u=1-n^0P^qu =P^-(n-1)qfrac1-P^nq1-P^q, ∑_v=0^n-1Q^qv =frac1-Q^nq1-Q^q.
Exact mathematical passage
\sum_{u=1-n}^{0}P^{qu} =P^{-(n-1)q}\frac{1-P^{nq}}{1-P^q},\qquad \sum_{v=0}^{n-1}Q^{qv} =\frac{1-Q^{nq}}{1-Q^q}.
Q^qUse in source · 2 passages
Search aliases: Q^q
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 288
∑_u=1-n^0P^qu =P^-(n-1)qfrac1-P^nq1-P^q, ∑_v=0^n-1Q^qv =frac1-Q^nq1-Q^q.
Exact mathematical passage
\sum_{u=1-n}^{0}P^{qu} =P^{-(n-1)q}\frac{1-P^{nq}}{1-P^q},\qquad \sum_{v=0}^{n-1}Q^{qv} =\frac{1-Q^{nq}}{1-Q^q}.
Q^{qv}Use in source · 1 passage
Search aliases: Q^qv
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 288
∑_u=1-n^0P^qu =P^-(n-1)qfrac1-P^nq1-P^q, ∑_v=0^n-1Q^qv =frac1-Q^nq1-Q^q.
Exact mathematical passage
\sum_{u=1-n}^{0}P^{qu} =P^{-(n-1)q}\frac{1-P^{nq}}{1-P^q},\qquad \sum_{v=0}^{n-1}Q^{qv} =\frac{1-Q^{nq}}{1-Q^q}.
q_1Use in source · 2 passages
Search aliases: q_1
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 161
q_1=lfloor A_0/7rfloor, q_2=lfloor B_0/7rfloor, q_3=lfloor C_0/7rfloor.
Exact mathematical passage
q_1=\lfloor A_0/7\rfloor,\quad q_2=\lfloor B_0/7\rfloor,\quad q_3=\lfloor C_0/7\rfloor.
q_2Use in source · 2 passages
Search aliases: q_2
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 161
q_1=lfloor A_0/7rfloor, q_2=lfloor B_0/7rfloor, q_3=lfloor C_0/7rfloor.
Exact mathematical passage
q_1=\lfloor A_0/7\rfloor,\quad q_2=\lfloor B_0/7\rfloor,\quad q_3=\lfloor C_0/7\rfloor.
q_3Use in source · 2 passages
Search aliases: q_3
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 161
q_1=lfloor A_0/7rfloor, q_2=lfloor B_0/7rfloor, q_3=lfloor C_0/7rfloor.
Exact mathematical passage
q_1=\lfloor A_0/7\rfloor,\quad q_2=\lfloor B_0/7\rfloor,\quad q_3=\lfloor C_0/7\rfloor.
q_aUse in source · 1 passage
Search aliases: q_a
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 45
q_a(z)=fracθ_0(z;a)^5θ_0(5z;5a).
Exact mathematical passage
q_a(z)=\frac{\theta_0(z;a)^5}{\theta_0(5z;5a)}.
q_tUse in source · 1 passage
Search aliases: q_t
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 37
F(z+1)=F(z), F(z+τ)=q_σ(z)F(z), F(z+σ)=q_t(z)^-1F(z),
Exact mathematical passage
F(z+1)=F(z),\qquad F(z+\tau)=q_\sigma(z)F(z),\qquad F(z+\sigma)=q_t(z)^{-1}F(z),
q_t^{-1}Use in source · 1 passage
Search aliases: q_t^-1
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 227
C_x^(m)= P(q_t^-1;b_x,m,W_x,m,σ) P(q_σ;a_x,m,W_x,m+b_x,mσ,τ).
Exact mathematical passage
\boxed{ C_x^{(m)}= \mathcal P(q_t^{-1};b_{x,m},W_{x,m},\sigma)\, \mathcal P(q_\sigma;a_{x,m},W_{x,m}+b_{x,m}\sigma,\tau). }
q_\sigmaUse in source · 2 passages
Search aliases: q_σ sigma
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 37
F(z+1)=F(z), F(z+τ)=q_σ(z)F(z), F(z+σ)=q_t(z)^-1F(z),
Exact mathematical passage
F(z+1)=F(z),\qquad F(z+\tau)=q_\sigma(z)F(z),\qquad F(z+\sigma)=q_t(z)^{-1}F(z),
RUse in source · 7 passages
Search aliases: R
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 54
M=0 · 1 · 0 -4 · 2 · 15 -1 · 0 · 4, R=M^-1=8 · -4 · 15 1 · 0 · 0 2 · -1 · 4.
Exact mathematical passage
M=\begin{pmatrix}0&1&0\\-4&2&15\\-1&0&4\end{pmatrix},\qquad R=M^{-1}=\begin{pmatrix}8&-4&15\\1&0&0\\2&-1&4\end{pmatrix}.
rUse in source · 1 passage
Search aliases: r
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 216
P(g;n,w,h)= ∏_r=0^n-1g(w+rh), · n>0, 1, · n=0, ∏_r=n^-1g(w+rh)^-1, · n<0.
Exact mathematical passage
\mathcal P(g;n,w,h)= \begin{cases} \prod_{r=0}^{n-1}g(w+rh),&n>0,\\ 1,&n=0,\\ \prod_{r=n}^{-1}g(w+rh)^{-1},&n<0. \end{cases}
R^{21}Use in source · 1 passage
Search aliases: R^21
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 85
R^3-I=2N+5N^2pmod7, R^7=4Ipmod7, R^21=Ipmod7.
Exact mathematical passage
R^3-I=2N+5N^2\pmod7,\qquad R^7=4I\pmod7,\qquad R^{21}=I\pmod7.
R^3Use in source · 2 passages
Search aliases: R^3
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 85
R^3-I=2N+5N^2pmod7, R^7=4Ipmod7, R^21=Ipmod7.
Exact mathematical passage
R^3-I=2N+5N^2\pmod7,\qquad R^7=4I\pmod7,\qquad R^{21}=I\pmod7.
R^7Use in source · 1 passage
Search aliases: R^7
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 85
R^3-I=2N+5N^2pmod7, R^7=4Ipmod7, R^21=Ipmod7.
Exact mathematical passage
R^3-I=2N+5N^2\pmod7,\qquad R^7=4I\pmod7,\qquad R^{21}=I\pmod7.
R^{m-1}Use in source · 1 passage
Search aliases: R^m-1
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 208
Let d_x=(a_x,b_x,c_x)^T be the integer carry vector from Section 3. At stage m, the carry is d_x,m=R^m-1d_x∈ Z^3. Set W_x,m=ρ^m-1z_T x. By the arithmetic transport formula,
Exact mathematical passage
d_{x,m}=R^{m-1}d_x\in\mathbb Z^3
\rfloorUse in source · 1 passage
Search aliases: rfloor
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 161
q_1=lfloor A_0/7rfloor, q_2=lfloor B_0/7rfloor, q_3=lfloor C_0/7rfloor.
Exact mathematical passage
q_1=\lfloor A_0/7\rfloor,\quad q_2=\lfloor B_0/7\rfloor,\quad q_3=\lfloor C_0/7\rfloor.
\squareUse in source · 1 passage
Search aliases: square
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 303
When 5nmid n, the condition 5nmid nq is exactly 5nmid q, giving L_t,σ(nz). When 5mid n, no terms remain and the logarithm is zero. Exponentiating proves the equality in the convergence region. Meromorphic continuation gives the stated identities. square
Exact mathematical passage
\square
TUse in source · 14 passages
Search aliases: T
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 65
u=(1,2,4)^T, v=(0,1,2)^T, w=(0,0,1)^T.
Exact mathematical passage
u=(1,2,4)^T,\quad v=(0,1,2)^T,\quad w=(0,0,1)^T.
tUse in source · 8 passages
Search aliases: t
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 22
τ=fracβ^2+2β15, σ=-fracβ+215, t=-τ, z_0=frac13.
Exact mathematical passage
\tau=\frac{\beta^2+2\beta}{15},\qquad \sigma=-\frac{\beta+2}{15},\qquad t=-\tau, \quad z_0=\frac13.
T^{-m}Use in source · 2 passages
Search aliases: T^-m
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 246
F(z_x)=ε^2 ∏_m=1^∞ (C_T^-mx^(m))^-1.
Exact mathematical passage
\boxed{ F(z_x)=\varepsilon^2 \prod_{m=1}^{\infty} \left(C_{T^{-m}x}^{(m)}\right)^{-1}. }
T^{-T}Use in source · 2 passages
Search aliases: T^-T
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 370
widehat f_m(a)=frac1343∑_b∈ V widehat C_m(a-b) widehat f_m-1(T^-Tb).
Exact mathematical passage
\boxed{ \widehat f_m(a)=\frac1{343}\sum_{b\in V} \widehat C_m(a-b)\,\widehat f_{m-1}(T^{-T}b). }
UUse in source · 5 passages
Search aliases: U
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 30
F(z)=fracΓ_ell(z;τ,σ)^5 Γ_ell(5z;5τ,5σ), U_Γ=F(z_0).
Exact mathematical passage
F(z)=\frac{\Gamma_{\mathrm{ell}}(z;\tau,\sigma)^5} {\Gamma_{\mathrm{ell}}(5z;5\tau,5\sigma)},\qquad U_\Gamma=F(z_0).
uUse in source · 15 passages
Search aliases: u
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 65
u=(1,2,4)^T, v=(0,1,2)^T, w=(0,0,1)^T.
Exact mathematical passage
u=(1,2,4)^T,\quad v=(0,1,2)^T,\quad w=(0,0,1)^T.
U_\GammaUse in source · 4 passages
Search aliases: U_Γ Gamma
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 30
F(z)=fracΓ_ell(z;τ,σ)^5 Γ_ell(5z;5τ,5σ), U_Γ=F(z_0).
Exact mathematical passage
F(z)=\frac{\Gamma_{\mathrm{ell}}(z;\tau,\sigma)^5} {\Gamma_{\mathrm{ell}}(5z;5\tau,5\sigma)},\qquad U_\Gamma=F(z_0).
U_\Gamma^3Use in source · 1 passage
Search aliases: U_Γ^3 Gamma
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 348
Im(C_polU_Γ^3)=0
Exact mathematical passage
\operatorname{Im}(C_{\mathrm{pol}}U_\Gamma^3)=0
VUse in source · 5 passages
Search aliases: V
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 202
Let x=(k,ℓ,j)∈ V=( Z/7)^3 and z_x=z_k,ℓ,j. Define
Exact mathematical passage
x=(k,\ell,j)\in V=(\mathbb Z/7)^3
vUse in source · 14 passages
Search aliases: v
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 65
u=(1,2,4)^T, v=(0,1,2)^T, w=(0,0,1)^T.
Exact mathematical passage
u=(1,2,4)^T,\quad v=(0,1,2)^T,\quad w=(0,0,1)^T.
WUse in source · 3 passages
Search aliases: W
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 208
Let d_x=(a_x,b_x,c_x)^T be the integer carry vector from Section 3. At stage m, the carry is d_x,m=R^m-1d_x∈ Z^3. Set W_x,m=ρ^m-1z_T x. By the arithmetic transport formula,
Exact mathematical passage
W_{x,m}=\rho^{m-1}z_{T x}
wUse in source · 16 passages
Search aliases: w
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 65
u=(1,2,4)^T, v=(0,1,2)^T, w=(0,0,1)^T.
Exact mathematical passage
u=(1,2,4)^T,\quad v=(0,1,2)^T,\quad w=(0,0,1)^T.
W_{x,m}Use in source · 3 passages
Search aliases: W_x,m
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 208
Let d_x=(a_x,b_x,c_x)^T be the integer carry vector from Section 3. At stage m, the carry is d_x,m=R^m-1d_x∈ Z^3. Set W_x,m=ρ^m-1z_T x. By the arithmetic transport formula,
Exact mathematical passage
W_{x,m}=\rho^{m-1}z_{T x}
\widehat CUse in source · 1 passage
Search aliases: widehat C widehat
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 370
widehat f_m(a)=frac1343∑_b∈ V widehat C_m(a-b) widehat f_m-1(T^-Tb).
Exact mathematical passage
\boxed{ \widehat f_m(a)=\frac1{343}\sum_{b\in V} \widehat C_m(a-b)\,\widehat f_{m-1}(T^{-T}b). }
\widehat C_mUse in source · 1 passage
Search aliases: widehat C_m widehat
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 370
widehat f_m(a)=frac1343∑_b∈ V widehat C_m(a-b) widehat f_m-1(T^-Tb).
Exact mathematical passage
\boxed{ \widehat f_m(a)=\frac1{343}\sum_{b\in V} \widehat C_m(a-b)\,\widehat f_{m-1}(T^{-T}b). }
\widehat fUse in source · 2 passages
Search aliases: widehat f widehat
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 358
widehat f(a)=∑_x∈ Vζ^a· xf(x), a∈ V.
Exact mathematical passage
\widehat f(a)=\sum_{x\in V}\zeta^{a\cdot x}f(x),\qquad a\in V.
\widehat f_mUse in source · 1 passage
Search aliases: widehat f_m widehat
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 370
widehat f_m(a)=frac1343∑_b∈ V widehat C_m(a-b) widehat f_m-1(T^-Tb).
Exact mathematical passage
\boxed{ \widehat f_m(a)=\frac1{343}\sum_{b\in V} \widehat C_m(a-b)\,\widehat f_{m-1}(T^{-T}b). }
\widehat f_{m-1}Use in source · 1 passage
Search aliases: widehat f_m-1 widehat
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 370
widehat f_m(a)=frac1343∑_b∈ V widehat C_m(a-b) widehat f_m-1(T^-Tb).
Exact mathematical passage
\boxed{ \widehat f_m(a)=\frac1{343}\sum_{b\in V} \widehat C_m(a-b)\,\widehat f_{m-1}(T^{-T}b). }
xUse in source · 15 passages
Search aliases: x
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 202
Let x=(k,ℓ,j)∈ V=( Z/7)^3 and z_x=z_k,ℓ,j. Define
Exact mathematical passage
x=(k,\ell,j)\in V=(\mathbb Z/7)^3
\mathbb ZUse in source · 6 passages
Search aliases: Z mathbb
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 50
The previously established zero-anchor normalization is F(0)=ε^2≠0. The divisor support is contained in Λ_5= Zτ+ Zσ+tfrac15 Z. These analytic facts are inherited inputs, not freshly formalized in Lean here.
Exact mathematical passage
\Lambda_5=\mathbb Z\tau+\mathbb Z\sigma+\tfrac15\mathbb Z
zUse in source · 23 passages
Search aliases: z
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 22
τ=fracβ^2+2β15, σ=-fracβ+215, t=-τ, z_0=frac13.
Exact mathematical passage
\tau=\frac{\beta^2+2\beta}{15},\qquad \sigma=-\frac{\beta+2}{15},\qquad t=-\tau, \quad z_0=\frac13.
\mathbb Z^3Use in source · 1 passage
Search aliases: Z^3 mathbb
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 208
Let d_x=(a_x,b_x,c_x)^T be the integer carry vector from Section 3. At stage m, the carry is d_x,m=R^m-1d_x∈ Z^3. Set W_x,m=ρ^m-1z_T x. By the arithmetic transport formula,
Exact mathematical passage
d_{x,m}=R^{m-1}d_x\in\mathbb Z^3
z_0Use in source · 7 passages
Search aliases: z_0
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 22
τ=fracβ^2+2β15, σ=-fracβ+215, t=-τ, z_0=frac13.
Exact mathematical passage
\tau=\frac{\beta^2+2\beta}{15},\qquad \sigma=-\frac{\beta+2}{15},\qquad t=-\tau, \quad z_0=\frac13.
z_{k',\ell',j'}Use in source · 1 passage
Search aliases: z_k',ℓ',j' ell
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 169
ρ z_k,ℓ,j= z_k',ℓ',j'+aτ+bσ+c
Exact mathematical passage
\boxed{ \rho z_{k,\ell,j}= z_{k',\ell',j'}+a\tau+b\sigma+c }
z_{k,\ell,j}Use in source · 4 passages
Search aliases: z_k,ℓ,j ell
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 119
z_k,ℓ,j=z_0+kδ+ℓη+jξ, k,ℓ,j∈{0,…,6}.
Exact mathematical passage
\boxed{z_{k,\ell,j}=z_0+k\delta+\ell\eta+j\xi,\qquad k,\ell,j\in\{0,\ldots,6\}.}
z_{T x}Use in source · 1 passage
Search aliases: z_T x
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 208
Let d_x=(a_x,b_x,c_x)^T be the integer carry vector from Section 3. At stage m, the carry is d_x,m=R^m-1d_x∈ Z^3. Set W_x,m=ρ^m-1z_T x. By the arithmetic transport formula,
Exact mathematical passage
W_{x,m}=\rho^{m-1}z_{T x}
z_xUse in source · 5 passages
Search aliases: z_x
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 202
Let x=(k,ℓ,j)∈ V=( Z/7)^3 and z_x=z_k,ℓ,j. Define
Exact mathematical passage
z_x=z_{k,\ell,j}
|Use in source · 2 passages
Search aliases: |
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 20
Choose the complex embedding β=7^1/3ω^2, so |ρ|<1. Put
Exact mathematical passage
|\rho|<1
|^{m-1}Use in source · 1 passage
Search aliases: |^m-1
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 242
As ρ^m z_x→0, all f_x^(m)→ F(0)=ε^2. Every multiplier is nonzero at the chosen arguments, and C_x^(m)=1+O(|ρ|^m-1).
Exact mathematical passage
C_x^{(m)}=1+O(|\rho|^{m-1})
\cdotUse in source · 4 passages
Search aliases: · cdot
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 145
343=1+2·3+16·21.
Exact mathematical passage
\boxed{343=1+2\cdot3+16\cdot21.}
\betaUse in source · 5 passages
Search aliases: β beta
Use in source · H12_Ambient_Torsion_README.md, line 5
This research package continues the pure cubic experiment K= Q(β), β^3=7.
Exact mathematical passage
K=\mathbb Q(\beta)
\beta^2Use in source · 2 passages
Search aliases: β^2 beta
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 15
ω^2+ω+1=0, β^3=7, ε=2-β, ρ=ε^-1=β^2+2β+4.
Exact mathematical passage
\omega^2+\omega+1=0,\quad \beta^3=7,\quad \varepsilon=2-\beta,\quad \rho=\varepsilon^{-1}=\beta^2+2\beta+4.
\beta^3Use in source · 2 passages
Search aliases: β^3 beta
Use in source · H12_Ambient_Torsion_README.md, line 5
This research package continues the pure cubic experiment K= Q(β), β^3=7.
Exact mathematical passage
\beta^3=7
\GammaUse in source · 5 passages
Search aliases: Γ Gamma
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 30
F(z)=fracΓ_ell(z;τ,σ)^5 Γ_ell(5z;5τ,5σ), U_Γ=F(z_0).
Exact mathematical passage
F(z)=\frac{\Gamma_{\mathrm{ell}}(z;\tau,\sigma)^5} {\Gamma_{\mathrm{ell}}(5z;5\tau,5\sigma)},\qquad U_\Gamma=F(z_0).
\Gamma_{\mathrm{ell}}Use in source · 1 passage
Search aliases: Γ_ell Gamma mathrm
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 30
F(z)=fracΓ_ell(z;τ,σ)^5 Γ_ell(5z;5τ,5σ), U_Γ=F(z_0).
Exact mathematical passage
F(z)=\frac{\Gamma_{\mathrm{ell}}(z;\tau,\sigma)^5} {\Gamma_{\mathrm{ell}}(5z;5\tau,5\sigma)},\qquad U_\Gamma=F(z_0).
\deltaUse in source · 7 passages
Search aliases: δ delta
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 111
δ=fracτ+2σ+47, η=fracσ+27, ξ=frac17.
Exact mathematical passage
\delta=\frac{\tau+2\sigma+4}{7},\qquad \eta=\frac{\sigma+2}{7},\qquad \xi=\frac17.
\varepsilonUse in source · 6 passages
Search aliases: ε varepsilon
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 15
ω^2+ω+1=0, β^3=7, ε=2-β, ρ=ε^-1=β^2+2β+4.
Exact mathematical passage
\omega^2+\omega+1=0,\quad \beta^3=7,\quad \varepsilon=2-\beta,\quad \rho=\varepsilon^{-1}=\beta^2+2\beta+4.
\varepsilon^{-1}Use in source · 1 passage
Search aliases: ε^-1 varepsilon
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 15
ω^2+ω+1=0, β^3=7, ε=2-β, ρ=ε^-1=β^2+2β+4.
Exact mathematical passage
\omega^2+\omega+1=0,\quad \beta^3=7,\quad \varepsilon=2-\beta,\quad \rho=\varepsilon^{-1}=\beta^2+2\beta+4.
\varepsilon^2Use in source · 3 passages
Search aliases: ε^2 varepsilon
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 49
The previously established zero-anchor normalization is F(0)=ε^2≠0. The divisor support is contained in Λ_5= Zτ+ Zσ+tfrac15 Z. These analytic facts are inherited inputs, not freshly formalized in Lean here.
Exact mathematical passage
F(0)=\varepsilon^2\ne0
\zetaUse in source · 5 passages
Search aliases: ζ zeta
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 330
Fix the oriented seventh-root phase ζ_7=e^2π i/7. The additive character against the top dual direction is
Exact mathematical passage
\zeta_7=e^{2\pi i/7}
\zeta^{a\cdot x}Use in source · 1 passage
Search aliases: ζ^a· x zeta cdot
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 358
widehat f(a)=∑_x∈ Vζ^a· xf(x), a∈ V.
Exact mathematical passage
\widehat f(a)=\sum_{x\in V}\zeta^{a\cdot x}f(x),\qquad a\in V.
\zeta_7Use in source · 1 passage
Search aliases: ζ_7 zeta
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 330
Fix the oriented seventh-root phase ζ_7=e^2π i/7. The additive character against the top dual direction is
Exact mathematical passage
\zeta_7=e^{2\pi i/7}
\zeta_7^{3(4k+5\ell+j)}Use in source · 1 passage
Search aliases: ζ_7^3(4k+5ℓ+j) zeta ell
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 338
ψ_w(T(k,ℓ,j))=ζ_7^3(4k+5ℓ+j).
Exact mathematical passage
\boxed{\psi_w(T(k,\ell,j))=\zeta_7^{3(4k+5\ell+j)}.}
\zeta_7^{3k}Use in source · 1 passage
Search aliases: ζ_7^3k zeta
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 332
ψ_w(k,ℓ,j)=ζ_7^3k.
Exact mathematical passage
\boxed{\psi_w(k,\ell,j)=\zeta_7^{3k}.}
\etaUse in source · 6 passages
Search aliases: η eta
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 111
δ=fracτ+2σ+47, η=fracσ+27, ξ=frac17.
Exact mathematical passage
\delta=\frac{\tau+2\sigma+4}{7},\qquad \eta=\frac{\sigma+2}{7},\qquad \xi=\frac17.
\thetaUse in source · 1 passage
Search aliases: θ theta
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 45
q_a(z)=fracθ_0(z;a)^5θ_0(5z;5a).
Exact mathematical passage
q_a(z)=\frac{\theta_0(z;a)^5}{\theta_0(5z;5a)}.
\theta_0Use in source · 1 passage
Search aliases: θ_0 theta
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 45
q_a(z)=fracθ_0(z;a)^5θ_0(5z;5a).
Exact mathematical passage
q_a(z)=\frac{\theta_0(z;a)^5}{\theta_0(5z;5a)}.
\LambdaUse in source · 6 passages
Search aliases: Λ Lambda
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 50
The previously established zero-anchor normalization is F(0)=ε^2≠0. The divisor support is contained in Λ_5= Zτ+ Zσ+tfrac15 Z. These analytic facts are inherited inputs, not freshly formalized in Lean here.
Exact mathematical passage
\Lambda_5=\mathbb Z\tau+\mathbb Z\sigma+\tfrac15\mathbb Z
\Lambda_5Use in source · 4 passages
Search aliases: Λ_5 Lambda
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 50
The previously established zero-anchor normalization is F(0)=ε^2≠0. The divisor support is contained in Λ_5= Zτ+ Zσ+tfrac15 Z. These analytic facts are inherited inputs, not freshly formalized in Lean here.
Exact mathematical passage
\Lambda_5=\mathbb Z\tau+\mathbb Z\sigma+\tfrac15\mathbb Z
\xiUse in source · 5 passages
Search aliases: ξ xi
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 111
δ=fracτ+2σ+47, η=fracσ+27, ξ=frac17.
Exact mathematical passage
\delta=\frac{\tau+2\sigma+4}{7},\qquad \eta=\frac{\sigma+2}{7},\qquad \xi=\frac17.
\piUse in source · 4 passages
Search aliases: π pi
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 262
L_t,σ(z)=-5∑_substackm≥1 5nmid m fracP^m e^2π imz-Q^m e^-2π imz m(1-P^m)(1-Q^m), P=e^2π it, Q=e^2π iσ.
Exact mathematical passage
L_{t,\sigma}(z)=-5\sum_{\substack{m\ge1\\5\nmid m}} \frac{P^m e^{2\pi imz}-Q^m e^{-2\pi imz}} {m(1-P^m)(1-Q^m)},\qquad P=e^{2\pi it},\ Q=e^{2\pi i\sigma}.
\rhoUse in source · 12 passages
Search aliases: ρ rho
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 15
ω^2+ω+1=0, β^3=7, ε=2-β, ρ=ε^-1=β^2+2β+4.
Exact mathematical passage
\omega^2+\omega+1=0,\quad \beta^3=7,\quad \varepsilon=2-\beta,\quad \rho=\varepsilon^{-1}=\beta^2+2\beta+4.
\rho^mUse in source · 3 passages
Search aliases: ρ^m rho
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 204
f_x^(m)=F(ρ^m z_x), m≥0.
Exact mathematical passage
f_x^{(m)}=F(\rho^m z_x),\qquad m\ge0.
\rho^{m-1}Use in source · 1 passage
Search aliases: ρ^m-1 rho
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 208
Let d_x=(a_x,b_x,c_x)^T be the integer carry vector from Section 3. At stage m, the carry is d_x,m=R^m-1d_x∈ Z^3. Set W_x,m=ρ^m-1z_T x. By the arithmetic transport formula,
Exact mathematical passage
W_{x,m}=\rho^{m-1}z_{T x}
\sigmaUse in source · 18 passages
Search aliases: σ sigma
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 22
τ=fracβ^2+2β15, σ=-fracβ+215, t=-τ, z_0=frac13.
Exact mathematical passage
\tau=\frac{\beta^2+2\beta}{15},\qquad \sigma=-\frac{\beta+2}{15},\qquad t=-\tau, \quad z_0=\frac13.
\tauUse in source · 13 passages
Search aliases: τ tau
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 22
τ=fracβ^2+2β15, σ=-fracβ+215, t=-τ, z_0=frac13.
Exact mathematical passage
\tau=\frac{\beta^2+2\beta}{15},\qquad \sigma=-\frac{\beta+2}{15},\qquad t=-\tau, \quad z_0=\frac13.
\psiUse in source · 2 passages
Search aliases: ψ psi
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 332
ψ_w(k,ℓ,j)=ζ_7^3k.
Exact mathematical passage
\boxed{\psi_w(k,\ell,j)=\zeta_7^{3k}.}
\psi_wUse in source · 2 passages
Search aliases: ψ_w psi
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 332
ψ_w(k,ℓ,j)=ζ_7^3k.
Exact mathematical passage
\boxed{\psi_w(k,\ell,j)=\zeta_7^{3k}.}
\omegaUse in source · 3 passages
Search aliases: ω omega
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 15
ω^2+ω+1=0, β^3=7, ε=2-β, ρ=ε^-1=β^2+2β+4.
Exact mathematical passage
\omega^2+\omega+1=0,\quad \beta^3=7,\quad \varepsilon=2-\beta,\quad \rho=\varepsilon^{-1}=\beta^2+2\beta+4.
\omega^2Use in source · 2 passages
Search aliases: ω^2 omega
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 15
ω^2+ω+1=0, β^3=7, ε=2-β, ρ=ε^-1=β^2+2β+4.
Exact mathematical passage
\omega^2+\omega+1=0,\quad \beta^3=7,\quad \varepsilon=2-\beta,\quad \rho=\varepsilon^{-1}=\beta^2+2\beta+4.
\ldotsUse in source · 1 passage
Search aliases: … ldots
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 119
z_k,ℓ,j=z_0+kδ+ℓη+jξ, k,ℓ,j∈{0,…,6}.
Exact mathematical passage
\boxed{z_{k,\ell,j}=z_0+k\delta+\ell\eta+j\xi,\qquad k,\ell,j\in\{0,\ldots,6\}.}
\ellUse in source · 16 passages
Search aliases: ℓ ell
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 117
The seven-point packet has arguments z_0+kδ. The first refinement consists of z_0+kδ+ℓη, with 49 labels. The full ambient packet is
Exact mathematical passage
z_0+k\delta+\ell\eta
\ell'Use in source · 2 passages
Search aliases: ℓ' ell
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 167
Write (k',ℓ',j')=(A_0,B_0,C_0)bmod7. Then
Exact mathematical passage
(k',\ell',j')=(A_0,B_0,C_0)\bmod7
\toUse in source · 2 passages
Search aliases: → to
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 241
As ρ^m z_x→0, all f_x^(m)→ F(0)=ε^2. Every multiplier is nonzero at the chosen arguments, and C_x^(m)=1+O(|ρ|^m-1).
Exact mathematical passage
\rho^m z_x\to0
\inUse in source · 6 passages
Search aliases: ∈ in
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 119
z_k,ℓ,j=z_0+kδ+ℓη+jξ, k,ℓ,j∈{0,…,6}.
Exact mathematical passage
\boxed{z_{k,\ell,j}=z_0+k\delta+\ell\eta+j\xi,\qquad k,\ell,j\in\{0,\ldots,6\}.}
\prodUse in source · 4 passages
Search aliases: ∏ prod
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 216
P(g;n,w,h)= ∏_r=0^n-1g(w+rh), · n>0, 1, · n=0, ∏_r=n^-1g(w+rh)^-1, · n<0.
Exact mathematical passage
\mathcal P(g;n,w,h)= \begin{cases} \prod_{r=0}^{n-1}g(w+rh),&n>0,\\ 1,&n=0,\\ \prod_{r=n}^{-1}g(w+rh)^{-1},&n<0. \end{cases}
\prod_{(u,v,j)\ne(0,0,0)}Use in source · 1 passage
Search aliases: ∏_(u,v,j)≠(0,0,0) prod ne
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 313
∏_(u,v,j)≠(0,0,0) F(frac13+fracut+vσ+j7)=1.
Exact mathematical passage
\boxed{ \prod_{(u,v,j)\ne(0,0,0)} F\left(\frac13+\frac{ut+v\sigma+j}{7}\right)=1. }
\prod_{j=0}^{n-1}Use in source · 1 passage
Search aliases: ∏_j=0^n-1 prod
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 271
N_n F(z)= ∏_u=1-n^0∏_v=0^n-1∏_j=0^n-1 F(z+fracut+vσ+jn).
Exact mathematical passage
\mathcal N_n F(z)= \prod_{u=1-n}^{0}\prod_{v=0}^{n-1}\prod_{j=0}^{n-1} F\left(z+\frac{ut+v\sigma+j}{n}\right).
\prod_{m=1}^{\infty}Use in source · 1 passage
Search aliases: ∏_m=1^∞ prod infty
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 246
F(z_x)=ε^2 ∏_m=1^∞ (C_T^-mx^(m))^-1.
Exact mathematical passage
\boxed{ F(z_x)=\varepsilon^2 \prod_{m=1}^{\infty} \left(C_{T^{-m}x}^{(m)}\right)^{-1}. }
\prod_{r=0}^{n-1}Use in source · 1 passage
Search aliases: ∏_r=0^n-1 prod
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 216
P(g;n,w,h)= ∏_r=0^n-1g(w+rh), · n>0, 1, · n=0, ∏_r=n^-1g(w+rh)^-1, · n<0.
Exact mathematical passage
\mathcal P(g;n,w,h)= \begin{cases} \prod_{r=0}^{n-1}g(w+rh),&n>0,\\ 1,&n=0,\\ \prod_{r=n}^{-1}g(w+rh)^{-1},&n<0. \end{cases}
\prod_{r=n}^{-1}Use in source · 1 passage
Search aliases: ∏_r=n^-1 prod
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 216
P(g;n,w,h)= ∏_r=0^n-1g(w+rh), · n>0, 1, · n=0, ∏_r=n^-1g(w+rh)^-1, · n<0.
Exact mathematical passage
\mathcal P(g;n,w,h)= \begin{cases} \prod_{r=0}^{n-1}g(w+rh),&n>0,\\ 1,&n=0,\\ \prod_{r=n}^{-1}g(w+rh)^{-1},&n<0. \end{cases}
\prod_{u=1-n}^{0}Use in source · 1 passage
Search aliases: ∏_u=1-n^0 prod
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 271
N_n F(z)= ∏_u=1-n^0∏_v=0^n-1∏_j=0^n-1 F(z+fracut+vσ+jn).
Exact mathematical passage
\mathcal N_n F(z)= \prod_{u=1-n}^{0}\prod_{v=0}^{n-1}\prod_{j=0}^{n-1} F\left(z+\frac{ut+v\sigma+j}{n}\right).
\prod_{v=0}^{n-1}Use in source · 1 passage
Search aliases: ∏_v=0^n-1 prod
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 271
N_n F(z)= ∏_u=1-n^0∏_v=0^n-1∏_j=0^n-1 F(z+fracut+vσ+jn).
Exact mathematical passage
\mathcal N_n F(z)= \prod_{u=1-n}^{0}\prod_{v=0}^{n-1}\prod_{j=0}^{n-1} F\left(z+\frac{ut+v\sigma+j}{n}\right).
\sumUse in source · 5 passages
Search aliases: ∑ sum
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 262
L_t,σ(z)=-5∑_substackm≥1 5nmid m fracP^m e^2π imz-Q^m e^-2π imz m(1-P^m)(1-Q^m), P=e^2π it, Q=e^2π iσ.
Exact mathematical passage
L_{t,\sigma}(z)=-5\sum_{\substack{m\ge1\\5\nmid m}} \frac{P^m e^{2\pi imz}-Q^m e^{-2\pi imz}} {m(1-P^m)(1-Q^m)},\qquad P=e^{2\pi it},\ Q=e^{2\pi i\sigma}.
\sum_{b\in V}Use in source · 1 passage
Search aliases: ∑_b∈ V sum in
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 370
widehat f_m(a)=frac1343∑_b∈ V widehat C_m(a-b) widehat f_m-1(T^-Tb).
Exact mathematical passage
\boxed{ \widehat f_m(a)=\frac1{343}\sum_{b\in V} \widehat C_m(a-b)\,\widehat f_{m-1}(T^{-T}b). }
\sum_{\substack{m\ge1\\5\nmid m}}Use in source · 1 passage
Search aliases: ∑_substackm≥1 5nmid m sum substack ge nmid
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 262
L_t,σ(z)=-5∑_substackm≥1 5nmid m fracP^m e^2π imz-Q^m e^-2π imz m(1-P^m)(1-Q^m), P=e^2π it, Q=e^2π iσ.
Exact mathematical passage
L_{t,\sigma}(z)=-5\sum_{\substack{m\ge1\\5\nmid m}} \frac{P^m e^{2\pi imz}-Q^m e^{-2\pi imz}} {m(1-P^m)(1-Q^m)},\qquad P=e^{2\pi it},\ Q=e^{2\pi i\sigma}.
\sum_{\substack{q\ge1\\5\nmid nq}}Use in source · 1 passage
Search aliases: ∑_substackq≥1 5nmid nq sum substack ge nmid
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 297
-5∑_substackq≥1 5nmid nq fracP^q e^2π i nq z-Q^q e^-2π i nq z q(1-P^q)(1-Q^q).
Exact mathematical passage
-5\sum_{\substack{q\ge1\\5\nmid nq}} \frac{P^q e^{2\pi i nq z}-Q^q e^{-2\pi i nq z}} {q(1-P^q)(1-Q^q)}.
\sum_{u=1-n}^{0}Use in source · 1 passage
Search aliases: ∑_u=1-n^0 sum
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 288
∑_u=1-n^0P^qu =P^-(n-1)qfrac1-P^nq1-P^q, ∑_v=0^n-1Q^qv =frac1-Q^nq1-Q^q.
Exact mathematical passage
\sum_{u=1-n}^{0}P^{qu} =P^{-(n-1)q}\frac{1-P^{nq}}{1-P^q},\qquad \sum_{v=0}^{n-1}Q^{qv} =\frac{1-Q^{nq}}{1-Q^q}.
\sum_{v=0}^{n-1}Use in source · 1 passage
Search aliases: ∑_v=0^n-1 sum
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 288
∑_u=1-n^0P^qu =P^-(n-1)qfrac1-P^nq1-P^q, ∑_v=0^n-1Q^qv =frac1-Q^nq1-Q^q.
Exact mathematical passage
\sum_{u=1-n}^{0}P^{qu} =P^{-(n-1)q}\frac{1-P^{nq}}{1-P^q},\qquad \sum_{v=0}^{n-1}Q^{qv} =\frac{1-Q^{nq}}{1-Q^q}.
\sum_{x\in V}Use in source · 1 passage
Search aliases: ∑_x∈ V sum in
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 358
widehat f(a)=∑_x∈ Vζ^a· xf(x), a∈ V.
Exact mathematical passage
\widehat f(a)=\sum_{x\in V}\zeta^{a\cdot x}f(x),\qquad a\in V.
\inftyUse in source · 1 passage
Search aliases: ∞ infty
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 246
F(z_x)=ε^2 ∏_m=1^∞ (C_T^-mx^(m))^-1.
Exact mathematical passage
\boxed{ F(z_x)=\varepsilon^2 \prod_{m=1}^{\infty} \left(C_{T^{-m}x}^{(m)}\right)^{-1}. }
\neUse in source · 4 passages
Search aliases: ≠ ne
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 49
The previously established zero-anchor normalization is F(0)=ε^2≠0. The divisor support is contained in Λ_5= Zτ+ Zσ+tfrac15 Z. These analytic facts are inherited inputs, not freshly formalized in Lean here.
Exact mathematical passage
F(0)=\varepsilon^2\ne0
\geUse in source · 4 passages
Search aliases: ≥ ge
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 204
f_x^(m)=F(ρ^m z_x), m≥0.
Exact mathematical passage
f_x^{(m)}=F(\rho^m z_x),\qquad m\ge0.
\langleUse in source · 2 passages
Search aliases: ⟨ langle
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 105
The essential duality is ⟨ u,w⟩_H=1 while ⟨ u,u⟩_H=⟨ u,v⟩_H=0 modulo seven. A stable linear subspace containing w also contains v=Nw and u=N^2w. Thus both the full unit action and this nontrivial socle-to-top pairing require the complete three-dimensional module.
Exact mathematical passage
\langle u,w\rangle_H=1
\rangleUse in source · 2 passages
Search aliases: ⟩ rangle
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 105
The essential duality is ⟨ u,w⟩_H=1 while ⟨ u,u⟩_H=⟨ u,v⟩_H=0 modulo seven. A stable linear subspace containing w also contains v=Nw and u=N^2w. Thus both the full unit action and this nontrivial socle-to-top pairing require the complete three-dimensional module.
Exact mathematical passage
\langle u,w\rangle_H=1
\rangle_HUse in source · 2 passages
Search aliases: ⟩_H rangle
Use in source · H12_Contracting_Ambient_Torsion_Research_Note.md, line 105
The essential duality is ⟨ u,w⟩_H=1 while ⟨ u,u⟩_H=⟨ u,v⟩_H=0 modulo seven. A stable linear subspace containing w also contains v=Nw and u=N^2w. Thus both the full unit action and this nontrivial socle-to-top pairing require the complete three-dimensional module.
Exact mathematical passage
\langle u,w\rangle_H=1
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- research/hilbert12-contracting-ambient-torsion/H12_Ambient_Torsion_README.md · 2 mathematical passages
- research/hilbert12-contracting-ambient-torsion/H12_Contracting_Ambient_Torsion_Research_Note.md · 131 mathematical passages
- research/hilbert12-contracting-ambient-torsion/H12_Full_Ambient_Torsion_Verification_Log.txt · 0 mathematical passages