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3.2. Conclusiones del estudio de mercado
In this section we detail the dynamic copula modelling framework first developed by Schu- bert and Schönbucher (2001).
Assume we have
n
obligors and recall in Chapter 4 (Note 3) we demonstrated how a con- ditionally independent framework could be constructed. For obligorsi
∈ {1, . . . , n}
we determined that default times could be constructed as:τ
i= inf{t∈R
+:
Z
t0
˜
where
ζ
i are random variables with uniform distribution on[0,1]
. In Chapter 4 (Note 3) weassumed these random variables were mutually independent, here we relax this assump- tion. Moreover in the models subsequently considered in Chapter 4 we assumed that
(˜λ
it
)
t≥0were deterministic, in this chapter we take
(˜λ
it)
t≥0 to beF−adapted
continuous stochasticprocesses.
We will use the notation
λ
and˜λ
to denote intensities in the setting where we have full information on the default times of all obligors and the setting where we only have informa- tion on a specific obligor respectively. The process(˜λ
it
)
t≥0 will be shown to be the intensityof obligor
i
in the setting where we only have information about the occurrence (or not) of default of obligori. For this reason Schubert and Schönbucher (2001) call
(˜λ
it
)
t≥0 thepseudo intensity of obligor
i. We will subsequently denote the intensity of obligors defined
on the filtration that contains the default information of all obligors by(λ
it
)
t≥0. We call thisintensity thefull intensity.
In this chapter the setup of Note 3 (Chapter 4) will enable us to generate spread dynamics using stochastic intensities. Although it is feasible to correlate the processes
(˜λ
it
)
t≥0 inorder to induce some level of default correlation, we will not do this. Default dependence is generated by the joint distribution of
ζ
i∀i∈ {1, . . . , n}
using a copula function.This setup works well because a dependence structure is completely characterised by a cop- ula function. By Sklar’s theorem (Theorem 15 in Chapter 4), the use of a copula function does not affect the marginal distribution of default times. Hence in this setup the calibra- tion of single obligor intensities are not affected by the default dependence relationship between obligors as it is given by a copula. This is important as it allows for efficient multi- obligor modelling. In contrast, in Chapter 4 (Section 4.2), we showed that when one tries to describe the default dependence relationship between obligors by correlating intensities the calibration of the volatility parameter is affected.
5.1.1
The full intensity of an obligor
Recall the definition of the enlarged filtration:
G=F∨D,
where
D= (D
t)
t≥0,D
t=∨
ni=1D
tiandD
itis the smallest sigma-algebra containing informationabout the default of an obligor
i∈ {1, . . . , n}
at timet≥0
.G
contains information about thedefault of all obligors. We can also define a smaller filtration:
˜
where
D
i= (D
ti)
t≥0.G˜
contains information about the default of only obligori.
• The filtration
G˜
is the one we used in Chapter 3, where only one obligor was consid-ered.
• The filtration
G
is the one used in Chapter 4 and includes information on the defaulttimes of all obligors. We call this filtration thefull filtration.
Under
G˜
we have established in Chapter 3 (Section 3.4.1) that the intensity of obligori
isthe
F−adapted
process(˜λ
it)
t≥0 in Note 3 (Chapter 4).We now consider the default intensity of obligor
i
under the full filtration,G
, where we havedefault information about all obligors.
Assumption 5.1. LetU
={ζ
1, . . . , ζ
n}
. UnderG
,Uis distributed with ann−dimensional
copula which is twice differentiable. We call the copula function forUthe threshold copula, denoted by
C
T.RecallUis independent of
F
.Theorem 18. Let
(λ
it)
t≥0 be the intensity of obligori
underG
, then∀t≥0
, If no defaultshave occured, we have:
• The intensity of obligor
i
is:λ
it= ˜λ
ite− Rt 0˜λisds ∂ ∂xiC
T(x
1, . . . , x
n)
C
T(x
1, . . . , x
n)
,
(5.1.2) wherex
i=
e− Rt 0λ˜ i sds∀i∈ {1, . . . , n}
.• The dynamics of the intensity of obligor
i
is:dλ
itλ
it=
dλ˜
it˜
λ
i t+
λ
it1−
C
xixiC
C
2 xi−˜λ
itdt−dN
i+
nX
j=1,j6=iC
xixjC
C
xiC
xj−1
dN
j−λ
jtdt
,
(5.1.3) whereC
=C
T(x
1, . . . , x
n)
,C
xi denotes the partial derivative ofC
with respect to thei
th argument,C
xixj is the second order partial derivative with respect to the
i
th and
j
thargument,N
i is the point process of obligori
.Proof. See propositions 4.3 and 4.7 in Schubert and Schönbucher (2001).
Similar results can be found for the case where defaults have occurred, see Schubert and Schönbucher (2001). A few important points arise from Theorem 18:
• Under
G
the intensity of obligori
still depends on(˜λ
it)
t≥0. However, now, the addi-tional information from
ζ
j∀j∈ {1, . . . , n}&j6=i
is incorporated.• Consider the case of two obligors. Let us assume
ζ
1andζ
2(as given in Note 3 (Chapter4)) have perfect positive dependence. If obligor 1 has not defaulted, then by Note 3 this implies that the realisation of
ζ
1 was not high, as no default has been triggerede.g. e−R0tλ˜
i
sds
> ζ
1 holds. As a result of perfect positive correlation, we have that
ζ
1=
ζ
2. Henceζ
2 is also not high, meaning it is less likely obligor 2 has defaulted.This is the effect that comes through when the intensity of obligor
i
is considered in the full filtration: the conditional value ofζ
1 influences directly the full intensity ofobligor 2. • Let:
π
ij=
C
xixjC
C
xiC
xj−1
.
Schönbucher (2003a) shows that
π
ij is positive if and only if there is locally positivedependence between obligors
j
andi. Hence in the case of positive dependence
between obligors we haveπ
ij>0∀i, j
∈ {1, . . . , n}
. From Theorem 18 we can considerthe influence of obligor
j
on obligori, withj6=i:
– If obligor
j
has not defaulted thendN
j= 0
and the only influence from obligorj
is
−π
ijλ
jt<0
. Hence, in the case of no default of obligorj
the intensity of obligori
reduces. This is what we expect.– If obligor
j
has defaulted thendN
j= 1
and the influence from obligorj
is to addπ
ij>0
to the intensity of obligorj. Again a desired feature.
– Therefore default contagion feeds naturally into this model setup. When there is positive correlation in the quantities
ζ
i∀i∈ {1, . . . , n}
, then upon a default of anobligor, all other obligors’ full intensities increase leading to greater chances of further defaults.
5.1.2
The survival and threshold copula
In this sub-section we make a connection between the threshold copula and a copula called the survival copula. Recall that the threshold copula was the copula that described the relationship between quantities
ζ
i∀i∈ {1, . . . , n}
and was denoted byC
T.Now consider the conditional survival functions,
Q
i(t, t
i)∀i∈ {1, . . . , n}
, defined in Chapterτ
1, . . . , τ
ncan be denoted by:S(t
1, . . . , t
n) =Q(τ
1> t
1, . . . , τ
n> t
n|F
t).
(5.1.4)By Sklar’s theorem (Theorem 15) we have:
S(t
1, . . . , t
n) =C
S(Q
1(0, t
1), . . . , Q
n(0, t
n)).
(5.1.5)C
Sis called the survival copula. Jouanin et al. (2001) provide the following important result:Proposition 19. The relationship between
C
T andC
S is given,∀t≥0
, by:C
S(Q
1(t, t
1), . . . , Q
n(t, t
n)) =E[C
T(
e− Rt1 t ˜λ1sds, . . . ,
e− Rtn t ˜λ n s ds)|F
t],
(5.1.6)where the notation
(˜λ
it)
t≥0refers to the intensity of obligori
with respect to the filtrationG˜
that contains default information only about obligor
i
.Proof. See Jouanin et al. (2001).
We note that