Song–Zhang v2: summable budgets and starting depths
Part of the second version of Song–Zhang, Chapter Song–Zhang, second version: technical estimates ; the reading order is on the full proofs page.
Overview. This develops the finite-chain argument for
Proposition 9.4 , corresponding to Propositions 9.23–9.25
of Song & Zhang, 2026 . The scalar threshold and degree-sum
arguments are combined with the independently reconstructed finite-chain
block theorem and the near-unit depth/outer-round lemmas from the small-loss
dossier to close the full profile induction.
Dependencies. Use Definition 9.1 ,
Proposition 9.1 , and the functions and scalar lemmas in
Proposition 9.3 . In particular W i = t ˉ ∘ χ ˉ ∘ i W_i=\bar t\circ\bar\chi^{\circ i} W i = t ˉ ∘ χ ˉ ∘ i
and L r = ℓ r / ϱ \mathcal L_r=\ell_r/\varrho L r = ℓ r / ϱ . All laws below are centered regular
log-concave measures with covariance at most I I I . No BKL result or KLS
conclusion is used.
The disjoint-degree moment estimate and the full finite-chain block
realization are proved in Proposition 10.2 . Their
constants do not depend on the number of retained coefficient majorants.
Paying the growing depth thresholds ¶ Let
α i = 2 − i 16 , R i = ⌈ C R α i − 12 ⌉ , S i = 1 + B ∑ l < i 2 − l , A i = A 0 exp ( C A ∑ l < i α l ) . \alpha_i={2^{-i}\over16},\quad R_i=\lceil C_R\alpha_i^{-12}\rceil,
\quad S_i=1+B\sum_{l<i}2^{-l},\quad
A_i=A_0\exp\left(C_A\sum_{l<i}\alpha_l\right). α i = 16 2 − i , R i = ⌈ C R α i − 12 ⌉ , S i = 1 + B l < i ∑ 2 − l , A i = A 0 exp ( C A l < i ∑ α l ) . For fixed C , p ≥ 1 C,p\geq1 C , p ≥ 1 there is b C , p b_{C,p} b C , p independent of i i i with
W i ( C α i − p ) ≤ 4 + b C , p 2 − i . W_i(C\alpha_i^{-p})\leq4+b_{C,p}2^{-i}. W i ( C α i − p ) ≤ 4 + b C , p 2 − i . For fixed C R , C C_R,C C R , C there is b b b such that for all real x ≥ 1 x\geq1 x ≥ 1 ,
W i ( R i + ⌈ C t ( x ) ⌉ ) ≤ W i ( x ) + b 2 − i . W_i(R_i+\lceil Ct(x)\rceil)\leq W_i(x)+b2^{-i}. W i ( R i + ⌈ Ct ( x )⌉) ≤ W i ( x ) + b 2 − i . Since α i − 1 = 16 ⋅ 2 i \alpha_i^{-1}=16\cdot2^i α i − 1 = 16 ⋅ 2 i , the fixed-power inequality for W i W_i W i
first gives
W i ( C 1 6 p ( 2 i ) p ) ≤ W i ( 2 i ) + b C 1 6 p , p 4 − i . W_i(C16^p(2^i)^p)\leq W_i(2^i)+b_{C16^p,p}4^{-i}. W i ( C 1 6 p ( 2 i ) p ) ≤ W i ( 2 i ) + b C 1 6 p , p 4 − i . The Lipschitz bound at the fixed point four gives
W i ( 2 i ) ≤ 4 + 4 − i − 1 ( 2 i − 4 ) + W_i(2^i)\leq4+4^{-i-1}(2^i-4)_+ W i ( 2 i ) ≤ 4 + 4 − i − 1 ( 2 i − 4 ) + , including i = 0 i=0 i = 0 .
This proves the first assertion. Since α i − 12 ≥ 1 \alpha_i^{-12}\geq1 α i − 12 ≥ 1 ,
R i ≤ ( C R + 1 ) α i − 12 R_i\leq(C_R+1)\alpha_i^{-12} R i ≤ ( C R + 1 ) α i − 12 . Apply the sum estimate to
R i + ⌈ C t ( x ) ⌉ R_i+\lceil Ct(x)\rceil R i + ⌈ Ct ( x )⌉ . Its first term is at most 4 + b 1 2 − i 4+b_12^{-i} 4 + b 1 2 − i
by the first assertion. The second is at most
W i ( x ) + b 2 4 − i W_i(x)+b_24^{-i} W i ( x ) + b 2 4 − i , since t ( x ) ≤ C ′ ( x + 1 ) ≤ 2 C ′ x t(x)\leq C'(x+1)\leq2C'x t ( x ) ≤ C ′ ( x + 1 ) ≤ 2 C ′ x and
⌈ C t ( x ) ⌉ ≤ C ′ ′ x \lceil Ct(x)\rceil\leq C''x ⌈ Ct ( x )⌉ ≤ C ′′ x . Because W i ( x ) ≥ 4 W_i(x)\geq4 W i ( x ) ≥ 4 , taking
the maximum and paying the one sum error proves the claim.
The order of operations matters: applying Lipschitz directly to R i R_i R i
would multiply 4 − i 4^{-i} 4 − i by a quantity of order 2 12 i 2^{12i} 2 12 i .
The universal constants A 0 , C A , C R , B A_0,C_A,C_R,B A 0 , C A , C R , B can be chosen so that every integer
i ≥ 0 i\geq0 i ≥ 0 , every integer r ≥ R i r\geq R_i r ≥ R i , and every law in the stated regular
class with curvature at least a I aI a I , a > 0 a>0 a > 0 , satisfy
A ≤ A i [ W i ( r ) + S i ] 1 / 3 L r ( a − 1 ) 2 . \mathcal A\leq A_i[W_i(r)+S_i]^{1/3}\mathcal L_r(a^{-1})^2. A ≤ A i [ W i ( r ) + S i ] 1/3 L r ( a − 1 ) 2 . Furthermore A i ≤ A 0 e C A / 8 A_i\leq A_0e^{C_A/8} A i ≤ A 0 e C A /8 and S i ≤ 1 + 2 B S_i\leq1+2B S i ≤ 1 + 2 B .
This is Proposition 9.4 .
Retaining caps and closing the analytic induction ¶ Suppose the profile has been established through stage i i i , and define
r l ( x ) = max { R l , ⌈ C r t ( x ) ⌉ + ⌈ D r / α l ⌉ } ( 0 ≤ l ≤ i ) . r_l(x)=\max\{R_l,\lceil C_rt(x)\rceil+\lceil D_r/\alpha_l\rceil\}
\quad(0\leq l\leq i). r l ( x ) = max { R l , ⌈ C r t ( x )⌉ + ⌈ D r / α l ⌉} ( 0 ≤ l ≤ i ) . The static transfer Proposition 10.1 gives the fixed valid coefficient
majorants
H l ( x ) 2 = min { G ∗ ( x ) 2 , e 3 α l A l [ W l ( r l ( x ) ) + S l ] 1 / 3 } . H_l(x)^2=\min\{G_*(x)^2,
e^{3\alpha_l}A_l[W_l(r_l(x))+S_l]^{1/3}\}. H l ( x ) 2 = min { G ∗ ( x ) 2 , e 3 α l A l [ W l ( r l ( x )) + S l ] 1/3 } . Here G ∗ G_* G ∗ is the universal original coefficient majorant; its validity
comes from the preceding height-reduction argument, not from KLS.
Indeed take Γ 2 = A l [ W l ( r l ( d ) ) + S l ] 1 / 3 / ϱ 2 \Gamma^2=A_l[W_l(r_l(d))+S_l]^{1/3}/\varrho^2 Γ 2 = A l [ W l ( r l ( d )) + S l ] 1/3 / ϱ 2 at the
fixed depth r l ( d ) r_l(d) r l ( d ) . It is at least one after a fixed choice of A 0 A_0 A 0 .
The all-law profile gives the transfer hypothesis at that depth; burn-in
bounds L r l ( d ) ( d ) 2 \mathcal L_{r_l(d)}(d)^2 L r l ( d ) ( d ) 2 and ( 1 + r l ( d ) − 2 ) 2 (1+r_l(d)^{-2})^2 ( 1 + r l ( d ) − 2 ) 2 by
e α l e^{\alpha_l} e α l each, leaving room in the displayed e 3 α l e^{3\alpha_l} e 3 α l .
No comparison with C P C_P C P or continuity of the supremum defining
A \mathcal A A is used. Once extracted, these majorants are retained unchanged.
For an additional 0 < ϵ ≤ α i 0<\epsilon\leq\alpha_i 0 < ϵ ≤ α i , use
K l = ⌈ L α l − 2 ⌉ K_l=\lceil L\alpha_l^{-2}\rceil K l = ⌈ L α l − 2 ⌉ through l = i l=i l = i ,
K i + 1 = ⌈ L ϵ − 2 ⌉ K_{i+1}=\lceil L\epsilon^{-2}\rceil K i + 1 = ⌈ L ϵ − 2 ⌉ , and
Ξ l = ⌈ 4 C d e g α l − 1 K l + 1 ⌉ \Xi_l=\lceil4C_{\rm deg}\alpha_l^{-1}K_{l+1}\rceil Ξ l = ⌈ 4 C deg α l − 1 K l + 1 ⌉ .
For l < i l<i l < i , geometric margins give
Ξ l ≤ C α l − 3 \Xi_l\leq C\alpha_l^{-3} Ξ l ≤ C α l − 3 and
r l ( Ξ l ) ≤ C ′ α l − 12 r_l(\Xi_l)\leq C'\alpha_l^{-12} r l ( Ξ l ) ≤ C ′ α l − 12 . Therefore
W l ( r l ( Ξ l ) ) ≤ 4 + b o l d 2 − l . W_l(r_l(\Xi_l))\leq4+b_{\rm old}2^{-l}. W l ( r l ( Ξ l )) ≤ 4 + b old 2 − l . Taking B ≥ b o l d B\geq b_{\rm old} B ≥ b old pays this error from the very next increment
of S S S , and C A ≥ 4 C_A\geq4 C A ≥ 4 gives, for l < i l<i l < i ,
( 1 + α l ) H l ( Ξ l ) 2 ≤ A i ( 4 + S i ) 1 / 3 . (1+\alpha_l)H_l(\Xi_l)^2\leq A_i(4+S_i)^{1/3}. ( 1 + α l ) H l ( Ξ l ) 2 ≤ A i ( 4 + S i ) 1/3 . Indeed log ( 1 + α l ) + 3 α l ≤ 4 α l \log(1+\alpha_l)+3\alpha_l\leq4\alpha_l log ( 1 + α l ) + 3 α l ≤ 4 α l and
A i / A l ≥ e C A α l A_i/A_l\geq e^{C_A\alpha_l} A i / A l ≥ e C A α l . This is a maximum bound on each
retained floor, so the number of floors does not enter.
For 0 < ϵ ≤ α i 0<\epsilon\le\alpha_i 0 < ϵ ≤ α i , every j ≥ 1 j\ge1 j ≥ 1 , odd Q ≥ Q ϵ Q\ge Q_\epsilon Q ≥ Q ϵ ,
and r ≥ max { R i , ⌈ C b t ( Q ) ⌉ + ⌈ C b ′ / ϵ ⌉ } r\ge\max\{R_i,\lceil C_bt(Q)\rceil+\lceil C_b'/\epsilon\rceil\} r ≥ max { R i , ⌈ C b t ( Q )⌉ + ⌈ C b ′ / ϵ ⌉} ,
A ≤ e 16 α i + 24 ϵ j A i max { t j ( Q ) , D i } 1 / 3 ( r + 1 ) 1 / Q L r ( a − 1 ) 2 , D i = W i ( ϵ − 1 ) + S i + b p r e 4 − i . \mathcal A\le e^{16\alpha_i+24\epsilon j}A_i
\max\{t_j(Q),D_i\}^{1/3}(r+1)^{1/Q}\mathcal L_r(a^{-1})^2,
\qquad D_i=W_i(\epsilon^{-1})+S_i+b_{\rm pre}4^{-i}. A ≤ e 16 α i + 24 ϵ j A i max { t j ( Q ) , D i } 1/3 ( r + 1 ) 1/ Q L r ( a − 1 ) 2 , D i = W i ( ϵ − 1 ) + S i + b pre 4 − i . Apply Lemma 10.12 with V = W i V=W_i V = W i , m = i m=i m = i ,
δ = α i \delta=\alpha_i δ = α i , A = A i A=A_i A = A i and S = S i S=S_i S = S i . The newest cap is the
H i H_i H i already extracted above. The earlier floors were bounded
individually above by A i ( 4 + S i ) 1 / 3 A_i(4+S_i)^{1/3} A i ( 4 + S i ) 1/3 , which is exactly the
retained-floor hypothesis of that lemma. The original-seed floor is
constant: K 0 = ⌈ C c u t α 0 − 2 ⌉ K_0=\lceil C_{\rm cut}\alpha_0^{-2}\rceil K 0 = ⌈ C cut α 0 − 2 ⌉ is fixed.
Increase A 0 A_0 A 0 once to bound C 0 G ∗ ( 16 K 0 ) 2 C_0G_*(16K_0)^2 C 0 G ∗ ( 16 K 0 ) 2 and C 0 C_0 C 0 .
The finite-chain theorem is applied with N = i + 1 ≥ 1 N=i+1\ge1 N = i + 1 ≥ 1 ; its constants
are independent of i i i . Finally S i ≤ 1 + 2 B S_i\le1+2B S i ≤ 1 + 2 B , so one universal
b p r e b_{\rm pre} b pre serves every i i i . The outer-round proof supplies the
coefficient return, initialization, and full terminal-depth induction;
none of these is inferred from the block construction alone.
The stage-zero profile follows from the initialization proved in the
small-loss dossier with W 0 = t ˉ W_0=\bar t W 0 = t ˉ ; its proof does not require the
constant branch of W ^ \widehat W W . Increase A 0 , C R A_0,C_R A 0 , C R once accordingly.
Use the realized outer-round estimate above at each subsequent stage. For a
prescribed r ≥ R i + 1 r\geq R_{i+1} r ≥ R i + 1 let j = κ ( r ) j=\kappa(r) j = κ ( r ) ,
ϵ = α i / ( j + 1 ) \epsilon=\alpha_i/(j+1) ϵ = α i / ( j + 1 ) , and take the least odd Q Q Q at least
max { Q ϵ , α i − 1 log ( r + 1 ) } \max\{Q_\epsilon,\alpha_i^{-1}\log(r+1)\} max { Q ϵ , α i − 1 log ( r + 1 )} .
The polynomial threshold calculation in the small-loss argument proves
Q ≤ r Q\leq r Q ≤ r and that this r r r is admissible, with a universal choice of C R C_R C R .
Consequently t ∘ j ( Q ) ≤ 3 < D i t^{\circ j}(Q)\leq3<D_i t ∘ j ( Q ) ≤ 3 < D i ,
( r + 1 ) 1 / Q ≤ e α i (r+1)^{1/Q}\leq e^{\alpha_i} ( r + 1 ) 1/ Q ≤ e α i , and ϵ j ≤ α i \epsilon j\leq\alpha_i ϵ j ≤ α i .
Use the product inequality and j + 1 ≤ χ ( r ) j+1\leq\chi(r) j + 1 ≤ χ ( r ) to obtain
W i ( ϵ − 1 ) ≤ max { W i ( χ ( r ) ) , W i ( α i − 1 ) } + b 4 − i ≤ W i + 1 ( r ) + b r e t 2 − i . \begin{split}
W_i(\epsilon^{-1})
&\leq\max\{W_i(\chi(r)),W_i(\alpha_i^{-1})\}+b4^{-i}\\
&\leq W_{i+1}(r)+b_{\rm ret}2^{-i}.
\end{split} W i ( ϵ − 1 ) ≤ max { W i ( χ ( r )) , W i ( α i − 1 )} + b 4 − i ≤ W i + 1 ( r ) + b ret 2 − i . The last step uses threshold absorption, W i + 1 ≥ 4 W_{i+1}\geq4 W i + 1 ≥ 4 , and
W i ∘ χ ˉ = W i + 1 W_i\circ\bar\chi=W_{i+1} W i ∘ χ ˉ = W i + 1 . Choose
B ≥ b r e t + b p r e B\geq b_{\rm ret}+b_{\rm pre} B ≥ b ret + b pre in addition to its earlier requirement.
Then D i ≤ W i + 1 ( r ) + S i + 1 D_i\leq W_{i+1}(r)+S_{i+1} D i ≤ W i + 1 ( r ) + S i + 1 . The total multiplicative loss is
at most e 41 α i e^{41\alpha_i} e 41 α i , so C A ≥ 42 C_A\geq42 C A ≥ 42 covers it.
This proves the next profile. All choices are universal: the dependence
of b p r e b_{\rm pre} b pre and the threshold-absorption constants on B B B is at
most C log ( e + B ) C\log(e+B) C log ( e + B ) , because S ∗ = 1 + 2 B S_*=1+2B S ∗ = 1 + 2 B changes only the fixed
high-height cutoff, and that cutoff enters a fixed-power height bound.
Thus choose B B B to satisfy B ≥ C log ( e + B ) B\ge C\log(e+B) B ≥ C log ( e + B ) and all the finitely
many earlier lower bounds; then freeze it before the induction.
The realized recurrences satisfy
∑ l < i α l ≤ 1 / 8 , ∑ l < i 2 − l ≤ 2 , \sum_{l<i}\alpha_l\leq1/8,\qquad
\sum_{l<i}2^{-l}\leq2, l < i ∑ α l ≤ 1/8 , l < i ∑ 2 − l ≤ 2 , and therefore the stated bounds on A i , S i A_i,S_i A i , S i . Together with the preceding finite induction, these sums prove the
claimed bounded-amplitude profiles.
Fences respected. Uniform admissibility is paid before choosing each
depth; no estimate for a growing starting depth is suppressed. No
uniform coefficient bound is inferred from the target or from BKL.
Song, Z., & Zhang, X. (2026). An O(1) Bound for the KLS Constant . https://arxiv.org/abs/2610.01447v2