The Elliptical Quartic Exponential Distribution An Annular Distribution Obtained via Maximum Entropy Christopher K I Williams

2025-05-06 0 0 233.84KB 6 页 10玖币
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The Elliptical Quartic Exponential Distribution: An
Annular Distribution Obtained via Maximum Entropy
Christopher K I Williams
School of Informatics, University of Edinburgh, UK
October 11, 2022
Abstract
This paper describes the Elliptical Quartic Exponential distribution in RD, obtained via
a maximum entropy construction by imposing second and fourth moment constraints. I
discuss relationships to related work, analytical expressions for the normalization constant
and the entropy, and the conditional and marginal distributions.
The maximum entropy construction allows the specification of a probability distribution in
terms of constraints, see e.g., Cover and Thomas (1991, ch. 12). Consider a radially symmetric
zero-mean distribution in RDwith r2=xTx. Constraints are imposed on the variance E[r2] =
c2and on E[r4] = c4; the latter implies a constraint on the “variance of the variance”. The
intuition behind the construction here is that if this “variance of the variance” is small then the
distribution should be similar to an annulus at some radius R. We define an annular distribution
to be one where the distribution as a function of ris unimodal with the mode away from zero.
The maximum entropy construction gives
p(x) = 1
ZD(λ1, λ2)exp λ1xTxλ2(xTx)2,(1)
where ZD(λ1, λ2)is the normalization constant in RD. We require λ2>0so that the distri-
bution is normalizable. λ1>0produces an annular distribution, while for λ10the density
decays monotonically from r= 0.
Consider the exponential term in eq. 1 as a function of rfor λ1>0. By differentiation we
have at the maximum that 2λ1r4λ2r3= 0. Let the value of rat which the maximum is
reached be denoted by R. Hence λ2=λ1/(2R2). By setting λ1=α/R2for α > 0, we have
p(x) = 1
ZD(α, R)exp αxTx
R2(xTx)2
2R4.(2)
As αincreases the thickness of the ring decreases. A plot of p(x)in 2D with R= 1 and α= 8
is shown in Figure 1.
1
arXiv:2210.04221v1 [stat.ME] 9 Oct 2022
Figure 1: A plot of the annular distribution in 2D for R= 1 and α= 8.
The distribution can clearly be shifted to a non-zero mean µand xTxcan transformed
to xTΣ1xfor some SPD matrix Σ. I term the distribution in eq. 1 under this transformation
the Elliptical Quartic Exponential distribution, by analogy with the Elliptical Gamma distribution
discussed below; both have elliptical contours.
Below I discuss related work, analytical expressions for the normalization constant and
the entropy, and the conditional and marginal distributions of the Elliptical Quartic Exponential
distribution.
1.1 Related work
Fisher (1922) discussed univariate probability densities having the form p(x)exp(Qk(x)),
where Qk(x) = Pk
q=1 αqxq, with keven and αk>0. Matz (1978) discusses the case
with k= 4 known as the quartic exponential distribution, and the special case of p(x)
exp(βx2γx4)with γ > 0and βunrestricted in sign; this is termed the symmetric quartic
exponential distribution. The quartic exponential distribution can be obtained via maximum
entropy considerations given the first four moments, see e.g., Zellner and Highfield (1988).
In the multivariate case, Urzúa (1997) considers p(x)exp(Q(x)). If Q(x)is a poly-
nomial of degree kin Ddimensions, it can be written as Q(x) = Pk
q=1 Q(q)(x), where each
Q(q)(x)is a homogeneous polynomial of degree q, i.e.
Q(q)(x) = Xα(q)
j1...jD
D
Y
i=1
xji
i,(3)
with the summation taken over all non-negative integer D-tuples (j1, . . . , jD)such that j1+
. . . +jD=q. This is known as the multivariate quartic exponential distribution. The maximum
2
摘要:

TheEllipticalQuarticExponentialDistribution:AnAnnularDistributionObtainedviaMaximumEntropyChristopherKIWilliamsSchoolofInformatics,UniversityofEdinburgh,UKOctober11,2022AbstractThispaperdescribestheEllipticalQuarticExponentialdistributioninRD,obtainedviaamaximumentropyconstructionbyimposingsecondand...

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