The real dilogarithm #
The dilogarithm Li₂ x = ∑_{n ≥ 1} xⁿ / n² on [-1, 1], its derivative -log(1 - x) / x, and the
classical functional equations obtained by differentiating and evaluating at an endpoint. Mathlib
has no polylogarithm.
Main definitions #
Dilog.Li₂: the real dilogarithm, as a power series.Dilog.rogersL: the Rogers dilogarithmL(x) = Li₂ x + ½ log x · log(1 - x).
Main results #
Dilog.Li₂_one:Li₂ 1 = π² / 6;Dilog.Li₂_neg_one:Li₂ (-1) = -π² / 12.Dilog.hasDerivAt_Li₂:Li₂′ x = -log(1 - x) / xfor0 < |x| < 1.Dilog.continuousOn_Li₂: continuity on[-1, 1].Dilog.Li₂_add_Li₂_one_sub: Euler's reflectionLi₂ x + Li₂ (1 - x) = π²/6 - log x · log (1 - x).Dilog.Li₂_one_half:Li₂ (1/2) = π²/12 - (log 2)²/2.Dilog.Li₂_landen: Landen's identityLi₂ x + Li₂ (x / (x - 1)) = -(log (1 - x))² / 2.Dilog.Li₂_sq: the duplication formulaLi₂ (x²) = 2 (Li₂ x + Li₂ (-x)).Dilog.Li₂_inv_goldenRatio_sq,Dilog.Li₂_inv_goldenRatio,Dilog.Li₂_neg_inv_goldenRatio: the values atφ⁻²,φ⁻¹and-φ⁻¹;Dilog.rogersL_inv_goldenRatio_sq:L(φ⁻²) = π²/15.Dilog.leeYang_effective_central_charge:L(φ⁻²) / L(1) = 2/5.
References #
- L. Lewin, Polylogarithms and Associated Functions, North-Holland, 1981.
- D. Zagier, The dilogarithm function, in Frontiers in Number Theory, Physics, and Geometry II, Springer, 2007, 3–65.
Li₂ 1 = π² / 6 — the Basel problem. Reindex ∑_{n≥0} 1/(n+1)² to hasSum_zeta_two
(∑_{n : ℕ} 1/n² = π²/6, whose n = 0 term is 0).
Li₂ is continuous on [-1, 1] (Weierstrass M-test: the series is dominated by
∑ 1/(n+1)² uniformly on the closed interval).
Euler's reflection identity for the dilogarithm on (0,1):
Li₂ x + Li₂ (1 - x) = π²/6 - log x · log (1 - x).
Proof: let F y := Li₂ y + Li₂ (1 - y) + log y · log (1 - y). Using hasDerivAt_Li₂
(and (Li₂ (1-·))' = log y/(1-y) by the chain rule), F' = 0 on (0,1), so F is constant
there (constant_of_has_deriv_right_zero on subintervals). Its limit as y → 0⁺ is
Li₂ 0 + Li₂ 1 + 0 = π²/6 by continuity of Li₂ on [-1,1] and
log y · log(1-y) = (log(1-y)/y)·(y·log y) → (-1)·0 = 0.
Landen's identity for the dilogarithm on (0, 1/2):
Li₂ x + Li₂ (x/(x-1)) = -log²(1-x) / 2.
For x ∈ (0, 1/2) the second argument x/(x-1) ∈ (-1, 0) stays inside the disc of
convergence of the defining power series; past x = 1/2 the identity requires analytic
continuation, which the series definition does not provide.
Proof: same scheme as the reflection identity — the combination
G y := Li₂ y + Li₂ (y/(y-1)) + log²(1-y)/2 has zero derivative on (0, 1/2) and tends
to 0 as y → 0⁺.
Golden-ratio evaluations #
The classical special values Li₂(1/φ²) = π²/15 − log²φ, Li₂(1/φ) = π²/10 − log²φ and
Li₂(−1/φ) = log²φ/2 − π²/15 (attributed to Landen; Lewin §1.4). The key golden facts are
1/φ + 1/φ² = 1 (so 1/φ² and 1/φ are a reflection pair) and
(1/φ²)/((1/φ²)−1) = −1/φ (so Landen's identity maps 1/φ² to −1/φ); together with the
duplication formula at 1/φ this gives a linear system — no five-term relation is needed.
Li₂(1/φ²) = π²/15 − log²φ (classical; Landen, cf. Lewin §1.4).
Li₂(1/φ) = π²/10 − log²φ (classical; Landen, cf. Lewin §1.4).
Li₂(−1/φ) = log²φ/2 − π²/15 (classical; Lewin §1.4).
The Rogers dilogarithm L(x) = Li₂(x) + ½·log x · log(1−x) (the natural
normalisation for 0 < x < 1; the log-product term removes the log² defects, so the
golden-ratio values become pure rational multiples of π²).
Instances For
L(1/φ²) = π²/15 — in physics terms: the effective central charge of the
Lee-Yang thermodynamic-Bethe-ansatz system is c_eff = L(1/φ²)/L(1) = (π²/15)/(π²/6) = 2/5,
the simplest TBA dilogarithm identity.
L(1/φ) = π²/10 (Landen).
Rogers' two-term golden identity L(1/φ) + L(1/φ²) = L(1) = π²/6 — the weight-2
"sum rule" behind the golden-ratio ladder (Rogers 1907).
The Lee–Yang effective central charge c_eff = L(1/φ²)/L(1) = 2/5, the simplest
thermodynamic-Bethe-ansatz dilogarithm identity.