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Multivariate Regularly Varying Copulas

Updated 8 July 2026
  • Multivariate regularly varying copulas are defined by anisotropic tail behavior, where operator tail densities capture varying rates of extremal dependence across dimensions.
  • They decompose joint operator regular variation into a dependence component from the copula’s tail density and a marginal component from univariate regular variation.
  • The operator framework facilitates explicit modeling with examples like Liouville and Archimedean copulas, aiding analysis in fields such as finance and insurance.

Searching arXiv for the cited papers and closely related work on operator tail dependence and multivariate regularly varying copulas. arxiv_search query: "Operator Tail Densities of Multivariate Copulas (Li, 22 Dec 2025)" Multivariate regularly varying copulas are copulas whose extremal dependence is described by regular variation under possibly anisotropic scaling. In the operator framework, the key object is the operator tail density of the copula, which records how the copula density behaves near a tail corner when different coordinates approach that corner at different regularly varying rates. This yields a decomposition of multivariate operator regular variation into a dependence component carried by the copula and a marginal component carried by univariate regular variation. In this formulation, a multivariate distribution is operator-regularly-varying if and only if, roughly, its copula has an appropriate operator tail density and its marginals are regularly varying with compatible indices (Li, 22 Dec 2025).

1. Conceptual and mathematical setting

Classical multivariate regular variation starts from a nonnegative random vector X=(X1,,Xd)X=(X_1,\dots,X_d) with distribution FF. One asks whether there exists a univariate regularly varying function UU such that

P(XtB)U(t)μ(B)\frac{\mathbb{P}(X\in tB)}{U(t)}\to \mu(B)

for relatively compact Borel sets BR+d{0}B\subset \mathbb{R}_+^d\setminus\{0\} bounded away from $0$. This uses a scalar scaling factor tt, and is therefore most natural when the marginals are tail-equivalent.

Operator regular variation replaces scalar norming by matrix norming. For a real d×dd\times d matrix EE, one defines

tE=exp(Elogt).t^E=\exp(E\log t).

The framework developed for multivariate regularly varying copulas restricts to diagonal matrices

FF0

so that

FF1

This allows different coordinates to scale at different power rates. For a diagonal operator-regularly-varying mapping FF2, one has the representation

FF3

with each FF4 slowly varying.

At the density level, the central notion is an operator-regularly-varying density. If FF5 has density FF6, then

FF7

means that for some operator-regularly-varying mapping FF8,

FF9

locally uniformly on UU0, where UU1. The limit UU2 satisfies the operator homogeneity relation

UU3

Copulas enter through Sklar’s representation. For continuous marginals UU4, the copula is

UU5

and the survival copula UU6 corresponds to UU7. Upper-orthant limits of UU8 near UU9 correspond to lower-orthant limits of P(XtB)U(t)μ(B)\frac{\mathbb{P}(X\in tB)}{U(t)}\to \mu(B)0 near P(XtB)U(t)μ(B)\frac{\mathbb{P}(X\in tB)}{U(t)}\to \mu(B)1. This operator scaling viewpoint makes it possible to treat non tail-equivalent marginals without forcing a single radial normalization (Li, 22 Dec 2025).

2. Operator tail densities of copulas

The defining dependence object is the operator tail density of a copula. Let P(XtB)U(t)μ(B)\frac{\mathbb{P}(X\in tB)}{U(t)}\to \mu(B)2 have density P(XtB)U(t)μ(B)\frac{\mathbb{P}(X\in tB)}{U(t)}\to \mu(B)3. For a tail-order vector P(XtB)U(t)μ(B)\frac{\mathbb{P}(X\in tB)}{U(t)}\to \mu(B)4 with P(XtB)U(t)μ(B)\frac{\mathbb{P}(X\in tB)}{U(t)}\to \mu(B)5, the upper tail density is the locally uniform limit

P(XtB)U(t)μ(B)\frac{\mathbb{P}(X\in tB)}{U(t)}\to \mu(B)6

where P(XtB)U(t)μ(B)\frac{\mathbb{P}(X\in tB)}{U(t)}\to \mu(B)7 and P(XtB)U(t)μ(B)\frac{\mathbb{P}(X\in tB)}{U(t)}\to \mu(B)8. The lower tail density is defined as the upper tail density of the survival copula, equivalently by

P(XtB)U(t)μ(B)\frac{\mathbb{P}(X\in tB)}{U(t)}\to \mu(B)9

This definition allows coordinatewise approach to the tail corner at different rates. When all BR+d{0}B\subset \mathbb{R}_+^d\setminus\{0\}0, it reduces to the classical tail density of Li and Wu (2013). When all BR+d{0}B\subset \mathbb{R}_+^d\setminus\{0\}1 equal a common value, it reduces to the “tail order” notion in Li and Hua (2015). In operator notation, if BR+d{0}B\subset \mathbb{R}_+^d\setminus\{0\}2, then the tail density is quasihomogeneous: BR+d{0}B\subset \mathbb{R}_+^d\setminus\{0\}3

This homogeneity is the copula analogue of the operator homogeneity satisfied by the limiting joint density BR+d{0}B\subset \mathbb{R}_+^d\setminus\{0\}4. It turns the copula tail density into a margin-free tail descriptor that is adapted to anisotropic scaling rather than scalar scaling. Under continuity of the copula density near the tail corner and local uniform convergence, the limit function is continuous on the interior of BR+d{0}B\subset \mathbb{R}_+^d\setminus\{0\}5, with extension to the cone closure by continuity. A plausible implication is that operator tail densities play the same structural role for anisotropic extremal dependence that ordinary tail densities play in the scalar case, but now on cones endowed with operator homogeneity (Li, 22 Dec 2025).

3. Decomposition of operator multivariate regular variation

The main structural result is a two-way decomposition linking joint operator regular variation, copula tail densities, and marginal regular variation.

First, if a density is operator-regularly-varying, then the corresponding distribution is operator-regularly-varying in the measure sense. If BR+d{0}B\subset \mathbb{R}_+^d\setminus\{0\}6, then for Borel sets BR+d{0}B\subset \mathbb{R}_+^d\setminus\{0\}7,

BR+d{0}B\subset \mathbb{R}_+^d\setminus\{0\}8

where BR+d{0}B\subset \mathbb{R}_+^d\setminus\{0\}9 and $0$0. For nonnegative $0$1, this implies that the $0$2-th marginal is regularly varying with tail index $0$3.

Second, operator regular variation of the joint density implies existence of a copula tail density. If $0$4 has ultimately non-increasing density $0$5, copula density $0$6, and

$0$7

then the upper tail density $0$8 exists, and the limiting density of the joint law is recovered from it by

$0$9

where

tt0

This writes the joint tail density as a transformed copula tail density multiplied by a Jacobian term. The copula contributes the dependence-only part; the Jacobian carries the marginal power-tail exponents.

Third, the reverse implication requires a compatibility condition. Suppose tt1 has upper tail density tt2, with tt3, and suppose the marginals have densities tt4. If

tt5

then the joint density is operator-regularly-varying: tt6 with

tt7

In this sense, a multivariate regularly varying copula is a copula whose tail density, together with compatible regularly varying marginals, determines an operator-regularly-varying joint law. Conversely, any operator-regularly-varying joint density induces an order-tt8 copula tail density. If compatibility fails, the paper states that one can still analyze the extremes via copula tail densities and marginal regular variation, but the neat operator-MRV representation fails. This marks compatibility as a structural rather than merely technical condition (Li, 22 Dec 2025).

4. Relation to exponent functions and non-standard regular variation

Operator tail densities are closely related to operator exponent functions. For a copula tt9 with tail-order vector d×dd\times d0, the upper operator exponent function is defined by

d×dd\times d1

For copulas with continuous density, the exponent function and the operator tail density are related by

d×dd\times d2

where d×dd\times d3. Under differentiability,

d×dd\times d4

Thus the tail dependence measure generated by the exponent function has density d×dd\times d5 on d×dd\times d6.

This density–measure relation extends the earlier operator-tail-dependence framework. In that framework, one defines lower and upper operator exponent functions d×dd\times d7 and d×dd\times d8, and lower and upper operator tail dependence functions d×dd\times d9 and EE0, for a positive-definite matrix EE1. When EE2 is diagonal, these functions are homogeneous under EE3, and if EE4, the operator construction reduces to standard copula tail dependence with common scaling order (Li, 2016).

The same line of work shows that copulas with operator tail dependence, combined with regularly varying univariate margins, generate a rich class of non-standard multivariate regularly varying distributions. Conversely, under orthant continuity and regularly varying margins, the copula of a non-standard multivariate regularly varying distribution has an upper operator exponent function, and under mild conditions this reduces to standard tail dependence of order 1. This clarifies an important point: anisotropic multivariate regular variation need not imply non-standard copula scaling at the observable copula level. The paper on operator tail densities makes the same point in a density-based form by showing that an operator-regularly-varying joint density induces an order-EE5 copula tail density after the marginal powers are absorbed into the change of variables. This suggests that much of the anisotropy may be transferred from the copula scale to the marginal scale unless one studies finer cones or hidden regimes (Li, 22 Dec 2025).

5. Representative model classes and explicit constructions

A particularly instructive example is provided by Liouville copulas. A nonnegative random vector EE6 has a Liouville distribution if, up to normalization,

EE7

with EE8 and

EE9

Although the associated Liouville copula

tE=exp(Elogt).t^E=\exp(E\log t).0

does not have a closed-form expression, it admits an explicit operator tail density. If tE=exp(Elogt).t^E=\exp(E\log t).1, then the Liouville density is operator-regularly-varying, and the induced copula tail density takes the form

tE=exp(Elogt).t^E=\exp(E\log t).2

with

tE=exp(Elogt).t^E=\exp(E\log t).3

In the symmetric case tE=exp(Elogt).t^E=\exp(E\log t).4 and tE=exp(Elogt).t^E=\exp(E\log t).5,

tE=exp(Elogt).t^E=\exp(E\log t).6

The example shows that explicit tail dependence may be available even when the copula itself is analytically intractable (Li, 22 Dec 2025).

A second relevant class is the Laplace-generated multivariate Archimedean copulas. For

tE=exp(Elogt).t^E=\exp(E\log t).7

the extremal regime depends on whether the generator tE=exp(Elogt).t^E=\exp(E\log t).8 is regularly varying, slowly varying, or rapidly varying. If tE=exp(Elogt).t^E=\exp(E\log t).9 with FF00, then

FF01

If FF02, then

FF03

If FF04 and satisfies the stated asymptotic condition, then a higher-order tail dependence function exists: FF05 This classification shows that first-order multivariate regular variation corresponds to the heavy-tailed case, while higher-order tail orders arise for rapidly varying generators (Li, 2024).

A third class is the max-stable / multivariate extreme-value construction based on independent unit Fréchet factors: FF06 Its copula is

FF07

This is a max-stable copula, and the associated stable tail dependence function is

FF08

The model provides a discrete-spectral, max-linear construction of multivariate regularly varying copulas with prescribed pairwise tail dependence coefficients

FF09

It therefore supplies an explicit constructive mechanism for regularly varying copulas in the extreme-value class (Ferreira, 2012).

6. Assumptions, scope, and open directions

The density-based characterization relies on explicit assumptions. For the direction from operator regular variation of the density to copula tail density, the density is assumed to be ultimately non-increasing. Densities and copula densities are assumed to exist, and continuity near the tail corner is used to guarantee existence and continuity of tail densities. The operator index matrix is restricted to a diagonal matrix with positive entries; the text notes that more general matrices are technically harder because the representation FF10 may fail. These are substantive constraints on the current theory rather than merely stylistic normalizations (Li, 22 Dec 2025).

The reverse characterization also depends critically on the compatibility condition linking the copula scaling functions FF11 to the marginal tails FF12. If the copula and marginals are not compatible, the resulting extremes may not be operator-regularly-varying, even though the copula tail dependence and the marginal regular variation remain analyzable. This separates the existence of a dependence descriptor from the existence of a full operator-MRV representation.

From a modeling viewpoint, the operator framework is designed for situations with non-equivalent marginal tails, such as those encountered in finance and insurance. It shows that once the marginal tail indices FF13 and the copula operator tail density FF14 are known, the operator tail density FF15, the corresponding tail measure, and the joint operator index matrix FF16 are determined. This suggests a workflow in which marginal tail indices are estimated first, copula tail orders and tail densities are estimated on transformed data, and compatibility is then assessed before reconstructing the joint tail law.

The present theory also points toward hidden multivariate regular variation. The Liouville discussion ends with the conjecture that nontrivial operator tail orders FF17 for copulas may arise in the analysis of hidden multivariate regular variation on sub-cones of FF18. A plausible implication is that the order-FF19 copula tail densities obtained from full-space operator-MRV laws may be only the first layer of a richer hierarchy of anisotropic tail objects, detectable only after restricting to finer cones or hidden regimes (Li, 22 Dec 2025).

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