Abstract
AbstractWe consider the limiting process that arises at the hard edge of Muttalib–Borodin ensembles. This point process depends on $$\theta > 0$$
θ
>
0
and has a kernel built out of Wright’s generalized Bessel functions. In a recent paper, Claeys, Girotti and Stivigny have established first and second order asymptotics for large gap probabilities in these ensembles. These asymptotics take the form $$\begin{aligned} {\mathbb {P}}(\text{ gap } \text{ on } [0,s]) = C \exp \left( -a s^{2\rho } + b s^{\rho } + c \ln s \right) (1 + o(1)) \qquad \text{ as } s \rightarrow + \infty , \end{aligned}$$
P
(
gap
on
[
0
,
s
]
)
=
C
exp
-
a
s
2
ρ
+
b
s
ρ
+
c
ln
s
(
1
+
o
(
1
)
)
as
s
→
+
∞
,
where the constants $$\rho $$
ρ
, a, and b have been derived explicitly via a differential identity in s and the analysis of a Riemann–Hilbert problem. Their method can be used to evaluate c (with more efforts), but does not allow for the evaluation of C. In this work, we obtain expressions for the constants c and C by employing a differential identity in $$\theta $$
θ
. When $$\theta $$
θ
is rational, we find that C can be expressed in terms of Barnes’ G-function. We also show that the asymptotic formula can be extended to all orders in s.
Funder
European Research Council
Vetenskapsrådet
Ruth and Nils-Erik Stenbäck foundation
Publisher
Springer Science and Business Media LLC
Subject
Mathematical Physics,Statistical and Nonlinear Physics
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