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Hilbert 12: contracting ambient torsion

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196 symbol spellings in 133 mathematical passages across 3 selected source files. Subscripts and superscripts have their own entries alongside their base symbols.

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+Use in source · 31 passages

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=Use in source · 77 passages

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AUse in source · 3 passages

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aUse in source · 9 passages

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A_0Use in source · 3 passages

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a_0Use in source · 1 passage

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a_xUse in source · 1 passage

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  • 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

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BUse in source · 3 passages

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bUse in source · 6 passages

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B_0Use in source · 3 passages

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b_xUse in source · 1 passage

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  • 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

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\bmodUse in source · 2 passages

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CUse in source · 9 passages

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cUse in source · 4 passages

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C_0Use in source · 3 passages

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C_mUse in source · 1 passage

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C_{\mathrm{pol}}Use in source · 1 passage

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C_{T^{-m}x}^{(m)}Use in source · 1 passage

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c_xUse in source · 1 passage

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  • 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

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C_x^{(m)}Use in source · 3 passages

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  • 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

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  • 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

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  • 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

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  • 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

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  • 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

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  • 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

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  • 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

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  • 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

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  • 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

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e^{2\pi imz}Use in source · 1 passage

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  • 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

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  • 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

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  • 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

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\expUse in source · 1 passage

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FUse in source · 11 passages

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\mathbb FUse in source · 1 passage

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  • 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

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fUse in source · 5 passages

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\mathbb F_7Use in source · 1 passage

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  • 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

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f_{m-1}Use in source · 1 passage

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f_{T x}^{(m-1)}Use in source · 1 passage

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f_x^{(m)}Use in source · 3 passages

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GUse in source · 1 passage

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gUse in source · 1 passage

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  • 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

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\mathrm{GL}Use in source · 1 passage

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  • 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

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  • 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

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hUse in source · 1 passage

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  • 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

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iUse in source · 4 passages

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  • 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

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JUse in source · 1 passage

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  • 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

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j'Use in source · 2 passages

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KUse in source · 1 passage

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kUse in source · 17 passages

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k'Use in source · 2 passages

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LUse in source · 2 passages

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  • 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

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  • 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

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MUse in source · 3 passages

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  • 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

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M^{-1}Use in source · 1 passage

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  • 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

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\midUse in source · 2 passages

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NUse in source · 8 passages

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\mathcal NUse in source · 3 passages

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nUse in source · 15 passages

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N^2Use in source · 4 passages

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N^3Use in source · 1 passage

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\mathcal N_7Use in source · 1 passage

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\mathcal N_nUse in source · 2 passages

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\nmidUse in source · 6 passages

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  • 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

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PUse in source · 3 passages

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  • 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

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  • 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

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  • 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

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  • 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

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  • 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

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  • 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

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  • 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

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\mathrm{pol}Use in source · 1 passage

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QUse in source · 3 passages

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  • 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

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qUse in source · 10 passages

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  • 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

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  • 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

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  • 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

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  • 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

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q_2Use in source · 2 passages

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q_aUse in source · 1 passage

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q_tUse in source · 1 passage

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q_t^{-1}Use in source · 1 passage

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  • 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

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RUse in source · 7 passages

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  • 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

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  • 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

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R^3Use in source · 2 passages

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R^7Use in source · 1 passage

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R^{m-1}Use in source · 1 passage

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  • 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

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\squareUse in source · 1 passage

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  • 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

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tUse in source · 8 passages

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T^{-m}Use in source · 2 passages

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UUse in source · 5 passages

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uUse in source · 15 passages

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U_\GammaUse in source · 4 passages

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VUse in source · 5 passages

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vUse in source · 14 passages

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WUse in source · 3 passages

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  • 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

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W_{x,m}Use in source · 3 passages

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  • 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

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\widehat C_mUse in source · 1 passage

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\widehat fUse in source · 2 passages

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\widehat f_mUse in source · 1 passage

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\widehat f_{m-1}Use in source · 1 passage

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xUse in source · 15 passages

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\mathbb ZUse in source · 6 passages

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  • 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

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\mathbb Z^3Use in source · 1 passage

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  • 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

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z_{k',\ell',j'}Use in source · 1 passage

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z_{k,\ell,j}Use in source · 4 passages

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z_{T x}Use in source · 1 passage

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  • 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

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|Use in source · 2 passages

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|^{m-1}Use in source · 1 passage

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\cdotUse in source · 4 passages

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\betaUse in source · 5 passages

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\GammaUse in source · 5 passages

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\deltaUse in source · 7 passages

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\varepsilonUse in source · 6 passages

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  • 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

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\zeta^{a\cdot x}Use in source · 1 passage

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\zeta_7Use in source · 1 passage

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\zeta_7^{3(4k+5\ell+j)}Use in source · 1 passage

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\etaUse in source · 6 passages

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\LambdaUse in source · 6 passages

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  • 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

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  • 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

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\piUse in source · 4 passages

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  • 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

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\rho^mUse in source · 3 passages

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\rho^{m-1}Use in source · 1 passage

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  • 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

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\tauUse in source · 13 passages

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\psiUse in source · 2 passages

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\omegaUse in source · 3 passages

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\ldotsUse in source · 1 passage

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\ellUse in source · 16 passages

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\ell'Use in source · 2 passages

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\toUse in source · 2 passages

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\inUse in source · 6 passages

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\prodUse in source · 4 passages

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  • 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

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\prod_{j=0}^{n-1}Use in source · 1 passage

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\prod_{m=1}^{\infty}Use in source · 1 passage

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\prod_{r=0}^{n-1}Use in source · 1 passage

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  • 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

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  • 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

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\prod_{v=0}^{n-1}Use in source · 1 passage

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\sumUse in source · 5 passages

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  • 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

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\sum_{\substack{m\ge1\\5\nmid m}}Use in source · 1 passage

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  • 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

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  • 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

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  • 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

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  • 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

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\inftyUse in source · 1 passage

Search aliases: ∞ infty

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\neUse in source · 4 passages

Search aliases: ≠ ne

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  • 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

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\langleUse in source · 2 passages

Search aliases: ⟨ langle

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  • 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

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  • 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

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  • 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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