“…This is also Lemma 1 of Salmassi [41]. Our statement of Proposition 2.1 corrects the constants c 1 and c 2 given by Merkes and Salmassi [34]. Figure 1 shows Ai(z) (black) and m term approximations to Ai(z) based on Proposition 2.1 with m = 25 (green), 125 (magenta), and 500 (blue).…”
Section: Chernoff's Density Is Log-concavesupporting
confidence: 76%
“…1 is given by Merkes and Salmassi [34]; see their Lemma 1, page 211. This is also Lemma 1 of Salmassi [41].…”
Section: Chernoff's Density Is Log-concavementioning
confidence: 97%
“…Theorem 2.2 (Schoenberg, 1951). A necessary and sufficient condition for a (density) function g(x), −∞ < x < ∞, to be a PF ∞ (density) function is that the reciprocal of its bilateral Laplace transform (i.e., Fourier) be an entire function of the form where [34]; see their Lemma 1, page 211. This is also Lemma 1 of Salmassi [41].…”
Section: Chernoff's Density Is Log-concavementioning
We show that the density of Z = argmax{W (t) − t2}, sometimes known as Chernoff’s density, is log-concave. We conjecture that Chernoff’s density is strongly log-concave or “super-Gaussian”, and provide evidence in support of the conjecture.
“…This is also Lemma 1 of Salmassi [41]. Our statement of Proposition 2.1 corrects the constants c 1 and c 2 given by Merkes and Salmassi [34]. Figure 1 shows Ai(z) (black) and m term approximations to Ai(z) based on Proposition 2.1 with m = 25 (green), 125 (magenta), and 500 (blue).…”
Section: Chernoff's Density Is Log-concavesupporting
confidence: 76%
“…1 is given by Merkes and Salmassi [34]; see their Lemma 1, page 211. This is also Lemma 1 of Salmassi [41].…”
Section: Chernoff's Density Is Log-concavementioning
confidence: 97%
“…Theorem 2.2 (Schoenberg, 1951). A necessary and sufficient condition for a (density) function g(x), −∞ < x < ∞, to be a PF ∞ (density) function is that the reciprocal of its bilateral Laplace transform (i.e., Fourier) be an entire function of the form where [34]; see their Lemma 1, page 211. This is also Lemma 1 of Salmassi [41].…”
Section: Chernoff's Density Is Log-concavementioning
We show that the density of Z = argmax{W (t) − t2}, sometimes known as Chernoff’s density, is log-concave. We conjecture that Chernoff’s density is strongly log-concave or “super-Gaussian”, and provide evidence in support of the conjecture.
“…Below we give two proofs based on the infinite product representation of Ai(x). In [5] we used the latter to obtain the radius of univalence of Ai(z). The following lemma summarizes all that we need.…”
“…. over square wells can probably be achieved by representing the characteristic determinant ∆(E) in (54) via Hadamar product representation of the Airy functions [53] as a spectral determinant of Bethe-ansatz type [16,29,54] and studying it by similar cocycle functional equations as in Ref. [55].…”
It is shown that the α 2 −dynamo of Magnetohydrodynamics, the hydrodynamic Squire equation as well as an interpolation model of PT −symmetric Quantum Mechanics are closely related as spectral problems in Krein spaces. For the α 2 −dynamo and the PT −symmetric model the strong similarities are demonstrated with the help of a 2 × 2 operator matrix representation, whereas the Squire equation is re-interpreted as a rescaled and Wick-rotated PT −symmetric problem. Based on recent results on the Squire equation the spectrum of the PT −symmetric interpolation model is analyzed in detail and the Herbst limit is described as spectral singularity.
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