Archimedean Weight and Pointwise Bounds #
Defines the archimedean weight w(t) = exp(t/2) / (2 sinh t) for t > 0 and proves
key estimates: positivity, sinh t ≥ t, w(t) ≤ exp(t/2)/(2t), the cancellation
identity 2 exp(-t/2) w(t) = 1/sinh(t), tail bound 1/sinh(t) < 4 exp(-t) for t ≥ 1,
and integrability of correction terms.
Reference: lamportform.tex, Section 2, lines 329–332, 399–416.
The archimedean weight function #
Auxiliary lemmas #
Positivity and basic bounds #
The archimedean weight is positive for t > 0.
w(t) ≤ exp(t/2) / (2t) for t > 0, using sinh t ≥ t.
Estimates for the tail integral #
Bound on the correction integrand #
Integrability estimates #
The tail integrand 1/sinh t is integrable on (2L, ∞) for L ≥ 1/2.
By comparison with 4 exp(-t) (from one_div_sinh_lt_four_exp_neg)
which is integrable on (2L, ∞) (from integrableOn_exp_neg_Ioi).
Reference: lamportform.tex, Step 7.2.
The correction integrand 2(exp(-t/2) - 1) w(t) is integrable on (0, 2L].
By correction_integrand_bound, the integrand is bounded by exp(t/2)/2
for each t, and on Ioc 0 (2L) we have t ≤ 2L, so t/2 ≤ L and hence
exp(t/2) ≤ exp(L). Thus the integrand is uniformly bounded by exp(L)/2
on this finite-measure set.
Reference: lamportform.tex, Step 8.2.
The map t ↦ ‖G̃ - S_t G̃‖² is measurable as a function of t.
This is a prerequisite for the outer integral in the energy decomposition
to type-check. Follows from measurability of translationOp in t and
measurability of the Lebesgue integral.
Archimedean energy integrand #
The archimedean energy integrand:
w(t) * ‖G̃ - S_t G̃‖² as an ENNReal-valued function of t.
This is the integrand in the archimedean energy decomposition.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The archimedean energy integral on (0, 2L):
∫₀^{2L} w(t) ‖G̃ - S_t G̃‖² dt.
Equations
- ConnesLean.archEnergyIntegral G L = ∫⁻ (t : ℝ) in Set.Ioo 0 (2 * L), ConnesLean.archEnergyIntegrand G L t
Instances For
The archimedean constant #
The archimedean constant c_∞(λ):
c_∞(λ) = -(log 4π + γ) + ∫₀^{2L} 2(e^{-t/2} - 1) w(t) dt + ∫_{2L}^∞ 2 e^{-t/2} w(t) dt,
where L = log cutoffLambda.
This definition matches the expression used in lamportform.tex (Steps 7.2, 8.2, and 9, around line ~420); analytic convergence of the two integrals is treated there and in subsequent lemmas.
Equations
- One or more equations did not get rendered due to their size.