AN INTRODUCTION TO EXTREME ORDER
STATISTICS AND ACTUARIAL APPLICATIONS
2004 ERM Symposium, Chicago April 26, 2004
Sessions CS 1E, 2E, 3E:
Extreme Value Forum
H. N. Nagaraja (hnn@stat.ohio-state.edu) Ohio State University, Columbus
Hour 1: ORDER STATISTICS - BASIC THEORY & ACTUARIAL
EXAMPLES
Hour 2: EXTREME VALUES - BASIC MODELS
Hour 3: EXTREME VALUES - INFERENCE AND APPLICATIONS
Hour 1: ORDER STATISTICS - BASIC THEORY & ACTUARIAL
EXAMPLES
1. Exact Distributions of Order Statistics
• Uniform Parent
• Exponential
• Normal
• Gumbel
2. Order Statistics Related Quantities of Actuarial In- terest
• Last Survivor Policy
• Multiple Life Annuities
• Percentiles and VaR (Value at Risk)
• Tail Probabilities
• Conditional Tail Expectation (CTE)
• Exceedances and Mean Excess Function 3. Large Sample Distribution of Order Statistics
• Central Order Statistics (Central Percentiles)
• Extreme Order Statistics
• Intermediate Order Statistics
4. Sum of top order statistics & sample CTE 5. Data Examples and Model Fitting
• Nationwide Data
• Danish Fire-loss Data
• Missouri Flood level Data
• Venice Sea Level Data
Hour 2: EXTREME VALUES - BASIC MODELS
1. Limit Distributions For the Maximum
• Fr´echet
• Weibull
• Gumbel (or the extreme-value)
2. Generalized Extreme Value (GEV) Distribution 3. Limit Distributions for the Other Upper Extremes 4. Limit Distributions for the Minimum
5. Exceedances - Generalized Pareto Distribution (GPD) 6. Examples
Hour 3: EXTREME VALUES - INFERENCE AND APPLICATIONS
1. GEV Distribution- Maximum Likelihood Estimates 2. Blocked Maxima Approach
3. Inference based on top k extremes
• Pickands’ Estimator
• Hills Estimator
• Estimating High Quantiles
4. GPD and Estimates Based on Exceedances 5. General Diagnostic Plots
• QQ Plot
• Empirical Mean Excess Function Plot 6. Examples
7. General Remarks 8. Software Resources 9. References
Hour 1
1 Exact Distribution of An Order Statistic If the random variables X1, ..., Xn are arranged in order of magnitude and then written as
X(1) ≤ · · · ≤ X(n),
we call X(i) the ith order statistic (i = 1, ..., n). We as- sume Xi to be statistically independent and identically distributed - a random sample from a continuous pop- ulation with cumulative distribution function (cdf) F (x) and probability density function (pdf) f (x).
CDF and PDF of Xr
F(r)(x) = Pr{X(r) ≤ x}
=
Xn i=r
µn i
¶
Fi(x)[1 − F (x)]n−i Minimum : F(1)(x) = 1 − [1 − F (x)]n Maximum : F(n)(x) = [F (x)]n
f(r)(x) = n!
(r − 1)!(n − r)!Fr−1(x)[1 − F (x)]n−rf (x).
Standard Uniform Parent – PDFs f (x) = 1, 0 ≤ x ≤ 1.
0 1 2 3 4 5
pdf at x
0.2 0.4 0.6 0.8 1
x
Figure 1: The probability density function (pdf) of the standard uniform population and the pdfs of the first, second, third, fourth and largest order statistics from a random sample of size 5.
Standard Uniform Parent – CDFs
F (x) = x, 0 ≤ x ≤ 1.
E(X(r)) = r
n + 1; V ar(X(r)) = r(n − r + 1) (n + 1)2 .
0 0.2 0.4 0.6 0.8 1
cdf at x
0.2 0.4 0.6 0.8 1
x
Figure 2: The cumulative distribution function (cdf) of the standard uniform population and the cdfs of the first (minimum), third (me- dian), and the largest (maximum) order statistics from a random sample of size 5.
Standard Normal Parent – PDFs f (x; µ, σ) = 1
√2πσ exp{− 1
2σ2(x−µ)2}, −∞ < x < ∞.
Here µ is the mean and σ is the standard deviation.
Standard Normal: µ = 0; σ = 1.
−4 −2 0 2 4
0.00.20.40.60.8
x
Probability Density Function
1 5
2 4
3
Figure 3: The pdf of the standard normal population and the pdfs of the first, second, third, fourth and the largest order statistics from a random sample of size 5.
Standard Normal Parent – PDFs of the Maxima
−4 −2 0 2 4 6
0.00.20.40.60.81.01.2
x
Probability Density Function
10 50
100 200
Figure 4: The pdf of the standard normal parent and the pdfs of the maximum from random samples of size n = 10, 50, 100, 200.
Standard Exponential Parent – PDFs f (x; λ) = λ exp{−λx}, 0 ≤ x < ∞.
Here mean = std. dev. = 1/λ; Std. Exponential: λ = 1.
Moments for the Max:
E(X(n)) ≈ log(n) − 0.5772; V ar(X(n)) ≈ π2/6 ≈ 1.64.
0 1 2 3 4
0.00.20.40.60.81.01.2
x
Probability Density Function
16
17
18
19
20
Figure 5: The pdfs of the standard exponential parent and those of the top 5 order statistics from a random sample of size 20.
Standard Gumbel Parent – PDFs
F (x; a, b) = exp{− exp[−(x − µ)/σ]}, −∞ < x < ∞.
Interesting Fact: X(n) is Gumbel with µ and σ/n.
Standard Gumbel: µ = 0, σ = 1;
E(X) = −γ(Euler’s constant) ≈ −0.5772;
Variance = π2/6.
−2 0 2 4 6
0.00.20.40.60.8
x
Probability Density Function
48
49
50
Figure 6: The pdfs of the standard Gumbel parent and those of the top 3 order statistics from a random sample of size n = 50.
2 Order Statistics Related Quantities of Actuarial Interest
Last Survivor Policy and Multiple Life Annuities
(a) Last Survivor Policy: Distribution of the Max- imum; of interest will be the mean, standard deviation and percentiles of the distribution.
(b) Multiple Life Annuities: Distribution of the rth order statistic from a sample of size n; say the third to die out of five.
Percentiles and VaR (Value at Risk)
Upper pth percentile of the Distribution of X. Here X could be the random variable corresponding to profits and losses (P&L) or returns on a financial instrument over a certain time horizon. Let
xp = F−1(1 − p),
where F−1 is the inverse cdf or the quantile function.
If p = 0.25, or p = .05 say – central order statistics, p = 0.01 or p = 0.001 – extreme order statistics. VaR = Value-at-Risk is generally an extreme percentile.
Exceedances and Tail Probabilities
Exceedance is an event that an observation from the population of X exceeds a given threshold c. Probability exceeding or below a certain threshold c; probability of ruin.
Pr(X > c).
When c is an extreme threshold, we need EVT.
Conditional Tail Expectation (CTE)
Suppose the top 100p% of the population are selected and one is interested in the average of the selected group.
E(X|X > xp) = µp = 1 p
Z ∞
xp
xf (x)dx.
Mean Excess Function
Suppose c is the threshold and the interest is the av- erage excess above it.
E(X − c|X > c) = m(c) = 1 1 − F (c)
Z ∞
c
(x − c)f (x)dx
= 1
1 − F (c) Z ∞
c
[1 − F (x)]dx.
3 Large Sample Distribution of Order Statis- tics
• Central Order Statistics (Central Percentiles)
• Extreme Order Statistics
• Intermediate Order Statistics
The asymptotic theory of order statistics is concerned with the distribution of Xr:n, suitably standardized, as n approaches ∞. If r/n ≈ p, fundamentally different results are obtained according as
(a) 0 < p < 1 (central or quantile case) (b) r or n − r is held fixed (extreme case)
(c) p = 0 or 1, with r = r(n) (intermediate case).
In Cases (a) and (c) the limit distribution is generally normal. In case (b), it is one of the three extreme-value distributions, or a member of the family of Generalized Extreme Value (GEV) distributions.
Central Case
Result 1. Let 0 < p < 1, and assume r ≈ np, and 0 < f (F−1(p)) < ∞. Then the asymptotic distri- bution of
n12(Xr:n − F−1(p)) is normal with zero mean and variance
p(1 − p) [f (F−1(p))]2.
• With 0 < p1 < p2 < 1,
³
n12(Xr1:n − F−1(p1)), n12(Xr2:n − F−1(p2))
´ is bivariate normal with correlations
p1(1 − p2) p2(1 − p1).
• These limiting means, variances and correlations can be used to approximate the moments of central order statistics.
• One can use this result to estimate and find confi- dence intervals for central percentiles.
• One can find the large sample distribution of, e.g., the sample interquartile range (IQR).
Intermediate Case
Result 2. Suppose the upper-tail of F satisfies some smoothness conditions (von Mises conditions).
As r → ∞ and r/n → 0, with pn = r/n, nf (xpn)r−12 (Xn−r+1:n − zpn) is asymptotically standard normal.
• xp is the upper pth quantile.
• There are 3 types of von Mises conditions - tied to EVT.
• Here and in the quantile case, one can obtain local estimates of the pdf f using neighboring order statis- tics.
Upper and Lower Extremes
None of the limit distributions is normal. There are 3 families of distributions that generate the limit distribu- tions for the upper extremes, and for the lower extremes.
• A nonsymmetric parent can have different types of limit distributions for the max. and min.
• The limit distribution for the kth maximum is related to, but different from that of the maximum.
Example. Consider a random sample from a stan- dard exponential population. That is,
Pr(X ≤ x) = 1 − exp(−x), x ≥ 0.
Then, for large n X(n) − log(n) ≈ Gumbel with location parameter 0 and scale 1. That is,
Pr(X(n)−log(n) ≤ x) ≈ exp[− exp(−x)], for all real x.
In contrast, the sample minimum is exactly Exponential with mean 1/n without any location shift. That is,
Pr(X(1) ≤ x) = 1 − exp(−nx), x ≥ 0.
Other Upper Extremes
Pr(X(n−k)−log(n) ≤ x) ≈ exp[− exp(−x)]
Xk j=0
exp(−jx) j! . Other Lower Extremes
Pr(nX(k) ≤ x) ≈ 1 − exp(−x) Xk
j=0
(x)j
j! , x ≥ 0.
4 Sum of top order statistics & sample CTE Suppose we are interested in estimating the CTE µp = E(X|X > xp) where xp is the upper pth quantile and p is not very small (say 5%) and let k/n ≈ p. Define the sample CTE as
Dk = 1 k
Xn j=n−k+1
X(j). Result 3. For large n,
√k(Dk − µp) ≈ N(0, σp2 + p(xp − µp)2).
where σp2 = V ar(X|X > xp).
• On the right, xp, µp and σp2 can be estimated from the sample using the sample quantile X(n−k), Dk and SD2 , the sample variance of the top k order statistics.
• The CTE and Mean Excess Function are related.
E(X|X > c) = c + m(c).
5 Data Examples and Model Fitting
Capital Requirements Data
Data Source: Steve Craighead, Nationwide Insurance, Columbus Values are negatives of the cap-requirements
-10000000 30000000 60000000
-10000000 0 10000000 20000000 30000000 40000000 50000000 60000000 70000000 80000000 90000000
.001 .01 .05.10 .25 .50 .75 .90.95 .99 .999
-4 -3 -2 -1 0 1 2 3 4
Normal Quantile Plot
Quantiles
100.0% maximum 89490993
99.5% 36103098
97.5% 11807434
90.0% 2782728.4
75.0% quartile 207245.65
50.0% median -2.094e+6
25.0% quartile -3.8605e6
10.0% -5.1367e6
2.5% -6.5963e6
0.5% -8.0968e6
0.0% minimum -9.133e+6
Moments
Mean -1.0354e6
Std Dev 5983789.7
Std Err Mean 189318.73
upper 95% Mean -663845.7 lower 95% Mean -1.4069e6
N 999
Bivariate Fit of mexf By (-capreq)_lag1
10000000 20000000 30000000
mexf
19
Danish Fire Insurance Claims Data Data Source: http://www.math.ethz.ch/~mcneil/
(Alexander McNeil Swiss Federal Institute of Technology) Original Source: Rytgaard (ASTIN Bulletin)
0 100 200
Loss-in-DKM 01/01/1978 01/01/1980 01/01/1982 01/01/1984 01/01/1986 01/01/1988 01/01/1990 01/01/1992
Date
0 10 20 30 40 50 60
Quantiles (Note: Top 3 values were excl.)
100.0% maximum 65.707
99.5% 32.402
97.5% 15.921
90.0% 5.506
75.0% quartile 2.964
50.0% median 1.775
25.0% quartile 1.321
10.0% 1.113
2.5% 1.020
0.5% 1.000
0.0% minimum 1.000
Moments (Top 3 excl.)
Mean 3.1308527
Std Dev 4.6580174
Std Err Mean 0.1001319
upper 95% Mean 3.3272175 lower 95% Mean 2.9344879
N 2164
Bivariate Fit of mexf By loss_lag1
0 20 40 60 70 90 110 120
mexf
0 10 20 30 40 50 60 70 80 90100 120 140 loss_lag1
Missouri River Annual Maximum Flow Data for the Towns of Boonville and Hermann
Data Source: US Army Corp of Engineers
-100000 0 100000 200000 300000 400000 500000 600000 700000 800000 900000 1000000 1100000
Boonville
1880 1900 1920 1940 1960 1980 2000 Year
0 100000 200000 300000 400000 500000 600000 700000 800000 900000 1000000 1100000
Hermann
1880 1900 1920 1940 1960 1980 2000 Year
0 100000 200000 300000 400000 500000 600000 700000 800000 900000 1000000
Extreme-Value and Normal fits for Boonville
100000 200000 300000 400000 500000 600000 700000 800000 900000 1000000
Extreme Value Fit for Hermann
0 100000 200000 300000 400000 500000 600000 700000 800000 900000 1000000
Boonville
100000 300000 500000 700000 900000 Hermann
Pearson Correlation
Boonv ille Hermann
1.0000 0.8936
0.8936 1.0000 Boonv ille Hermann
Venice Annual Extreme Sea level Readings (1931-1981) Data Source: Reiss and Thomas (1997); XTREMES software.
50 100 150 200
max1
1920 1930 1940 1950 1960 1970 1980 1990 y ear
Highest Annual level
70 80 90 100 110 120 130 140 150
max2
1920 1930 1940 1950 1960 1970 1980 1990 y ear
Second Best Annual level
60 80 100 120 140 160 180 200
max1
1930 1940 1950 1960 1970 1980 1990 y ear
max1 = -990.0706 + 0.5673303 year
60 80 100 120 140 160 180
Extreme Value Fit for mod.max1
Pairwise Pearson Correlations
max1 max2 max3 max4 max5 max6
1.0000 0.8103 0.7746 0.6724 0.6741 0.6685
0.8103 1.0000 0.9455 0.9145 0.8872 0.8626
0.7746 0.9455 1.0000 0.9524 0.9208 0.8901
0.6724 0.9145 0.9524 1.0000 0.9662 0.9253
0.6741 0.8872 0.9208 0.9662 1.0000 0.9682
0.6685 0.8626 0.8901 0.9253 0.9682 1.0000
max1 max2 max3 max4 max5 max6
Hour 2: EXTREME VALUES - BASIC MODELS
1 Sample Maximum
For an arbitrary parent distribution, Xn:n, the largest in a random sample of n from a population with cdf F (x), even after suitable standardization, may not possess a limiting distribution.
Result 3. If F (x) is such that (X(n) − an)/bn has a limit distribution for large n, then the limiting cdf must be one of just three types:
(Fr´echet) G1(x; α) = 0 x ≤ 0, α > 0,
= exp(−x−α) x > 0;
(Weibull) G2(x; α) = exp [−(−x)α] x ≤ 0, α > 0,
= 1 x > 0;
(Gumbel) G3(x) = exp¡
−e−x¢
− ∞ < x < ∞.
(1)
Notes
• For a given parent cdf F there can be only one type of G.
• Norming constants an and bn need to be estimated from the data and formulas depend on the type of G and parent cdf F . Convenient choices are given below in Result 4.
• For the sample minimum, the limit distributions are similar and have one-to-one relationship with the family in (1).
• necessary and sufficient conditions for each of the 3 possibilities are known and are very technical. They depend on the right-tail thickness of F .
• For many insurance applications, the right-tail is Pareto like resulting in limiting Fr´echet distribution.
• Simpler sufficient conditions are available for contin- uous distributions.
• There are parent cdfs for which no (nondegenerate) limit distribution exists for the max.
Formulas for Norming Constants For the Maximum Result 4. The location shift an and scale shift bn are
(i) an = 0 and bn = x1/n if G = G1
(ii)an = F−1(1) and bn = F−1(1) − x1/n if G = G2 (iii) an = x1/n and bn = E(X − an|X > an) ≈ [nf (an)]−1 if G = G3
Domains For Common Distributions
Fr´echet: F has infinite upper limit.
Cauchy; Pareto; Burr; Stable with index < 2; Loggamma.
Weibull: F Bounded Above.
Uniform; Power law (upper end); Beta.
Gumbel: Bounded or unbounded F .
Exponential; Weibull; Gamma; Normal; Benktander-type I and type II.
An Example: Pareto Distribution
Suppose the cdf is
F (x) = 1 − x−α, x ≥ 1, α > 0.
Then
Pr(X(n) ≤ n1/αx) ≈ exp{−x−α} for all x > 0.
Note: The α of the limit distribution of the maximum is the α of the parent distribution representing the tail thickness.
Another Example Suppose the cdf is
F (x) = 1 − (log(x))−1, x ≥ e.
Then you cannot normalize X(n) so that we get a nonde- generate limit distribution.
2 Generalized Extreme-Value Distribution The Gk in (1) are members of the family of generalized extreme-value (GEV) distributions
Gξ(y; µ, σ) =
exp
h
−(1 + ξy−µσ )−1ξ i
, 1 + ξy−µσ > 0, ξ 6= 0, exp¡
−e−[(y−µ)/σ]¢
, −∞ < y < ∞, ξ = 0.
(2) ξ is the shape, µ is the location and σ is the scale pa- rameter.
Connections
G1(y; α) when ξ > 0 , σ = 1, µξ = 1 and α = 1/ξ, G2(y; α) when ξ < 0, σ = 1, and α = −1/ξ
G3(y) when ξ = 0, σ = 1 and µ = 0.
Moments of GEV
Take µ = 0, σ = 1.
When ξ 6= 0,
Mean = 1
ξ [Γ(1 − ξ) − 1] , ξ < 1;
Variance = 1 ξ2
£Γ(1 − 2ξ) − Γ2(1 − ξ)¤
, ξ < 1/2;
Mode = 1 ξ
£(1 + ξ)−ξ − 1¤ .
When ξ = 0, we have the Gumbel distribution and Mean = γ = 0.5772.. = Euler’s constant;
Variance = π2/6; Mode = 0.
Quantile Function of GEV
Take µ = 0, σ = 1.
When ξ 6= 0,
G−1ξ (q) = 1 ξ
©[− log(q)]−ξ − 1ª
For the Gumbel cdf, G−10 (q) = − log[− log(q)].
3 Limit Distributions of the top Extremes kth Order Statistic
Result 5.If F (x) is such that (X(n) − an)/bn has a limiting cdf G, then, for a fixed k, the limiting cdf of (X(n−k+1) − an)/bn is of the form:
G(k)(x) = G(x) Xk−1
j=0
[− log G(x)]j
j! .
Notes
• The same G and the same set of norming constants work.
• The form of G(k)(x) has a Poisson partial sum form.
Pareto Example Contd.
Suppose the cdf is
F (x) = 1 − x−α, x ≥ 1, α > 0.
Then
Pr(X(n−k+1) ≤ n1/αx) ≈ exp{−x−α} Xk−1
j=0
x−jα j!
for all x > 0.
Limiting Joint Distribution of the top kth Order Statistics
Result 6. If (X(n) − an)/bn has limiting cdf G and g is the pdf of G then the k-dimensional vector
µX(n) − an
bn , . . . , X(n−k+1) − an bn
¶
(3) has a limit distribution with joint pdf
g(1,...,k)(w1, . . . , wk) = G(wk) Yk
i=1
g(wi)
G(wi), w1 > · · · > wk. (4) Pareto Example Contd.
Suppose the cdf is
F (x) = 1 − x−α, x ≥ 1, α > 0.
Then ³
X(n)/n1/α, . . . , X(n−k+1)/n1/α
´ has limiting joint pdf
g(1,...,k)(w1, . . . , wk) = exp{−w−αk } Yk
i=1
α wα+1i , for all w1 > · · · > wk > 0.
Notes
• Result 6 is useful for making inference when only the top k observations are available.
• The joint density in (4) will involve the location, scale and shape parameters associated with the General- ized Extreme Value Distribution of interest.
• Methods of Maximum Likelihood or Moments for the Estimation of the parameters will involve this joint density.
Discrete Parent Populations
While the results hold, no familiar discrete distribu- tion is in the domain of maximal attraction (or minimal attraction).
4 Limiting Distribution of the Sample Mini- mum
Result similar to Result 3 holds for the asymptotic dis- tribution of the standardized minimum, (X(1) − a∗n)/b∗n.
Result 7.The three possible limiting cdfs for the minimum are as follows:
G∗1(x; α) = 1 − exp£
−(−x)−α¤
x ≤ 0, α > 0,
= 1 x > 0;
G∗2(x; α) = 0 x ≤ 0, α > 0, (5)
= 1 − exp(−xα) x > 0;
G∗3(x) = 1 − exp (−ex) − ∞ < x < ∞.
Clearly, G∗i(x) = 1 − Gi(−x), i = 1, 2, 3. where Gi is given by (1).
Notes
• Here G∗2(x; α) is the real Weibull distribution!
• Norming constants can be obtained using Result 4 with appropriate modifications.
• Instead of dealing with the sample minimum from X one can see it as the negative of the maximum from
−X. Thus need to know only the upper extremes well.
Pareto Example Contd.
Suppose the cdf is
F (x) = 1 − x−α, x ≥ 1, α > 0.
Then
P (X(1) > x) = [1 − F (x)]n = x−nα, x ≥ 1.
So
P {n(X(1) − 1) > y} = [1 + y
n]−nα, y ≥ 0.
This approaches exp(−yα) as n increases. So the limiting cdf is G∗2(x; α).
Joint Limiting Distribution of Max and Min.
Any “lower” extreme X(r) is asymptotically indepen- dent of any “upper” extreme X(n+1−k). This result is very useful for finding the limiting distributions of statis- tics such as the range and the midrange.
5 Distributions of Exceedances and the Gen- eralized Pareto Distribution (GPD)
When F is unbounded to the right, there is an inter- esting connection between the limit distribution for X(n) for large n and the limit behavior as t → ∞ of stan- dardized excess life (X − a(t))/b(t), conditioned on the event {X > t}.
Balkema and de Haan (1974), and Pickands (1975) characterize the family of limiting distributions for the excess life.
Result 8. For a nondegenerate cdf H(x) if
t→∞lim Pr
½X − a(t)
b(t) > x¯
¯X > t
¾
= 1 − H(x) then H(x) is a Pareto-type cdf having the form
Hξ(x) =
1 − (1 + ξx)−1ξ, x ≥ 0, if ξ > 0 1 − e−x, x ≥ 0, if ξ = 0
(6)
if and only if Pr
µX(n) − an
bn ≤ x
¶
→ Gξ(x)
where Gξ is the GEV cdf given in (2) with the same shape parameter ξ ≥ 0.
Moments of GPD When ξ 6= 0,
Mean = 1
1 − ξ, ξ < 1;
Variance = £
(1 − 2ξ)(1 − ξ)2¤−1
, ξ < 1/2;
Mode = 1 ξ
£(1 + ξ)−ξ − 1¤ .
Mean Excess Function = E(X−t|X > t) = 1 + ξt
1 − ξ , ξ < 1.
When ξ = 0, we have the standard exponential distri- bution and
Mean = Standard Deviation = 1 = Mean Excess Function.
Quantile Function of GPD When ξ 6= 0,
Hξ−1(q) = 1 ξ
©(1 − q)−ξ − 1ª .
For the Exponential cdf, H0−1(q) = − log(1 − q).
Note
In addition to the shape parameter ξ the GPD has one more parameter, namely the scale parameter σ.
Hour 3: INFERENCE FOR EXTREME VALUE MODELS
1 Generalized Extreme Value Distribution Let Y be a random variable having a generalized extreme- value (GEV) distribution with shape parameter ξ, loca- tion parameter µ and scale parameter σ. The cdf is (see (2))
Gξ(y; µ, σ) =
exp
h
−(1 + ξy−µσ )−1ξ i
, 1 + ξy−µσ > 0, ξ 6= 0, exp¡
−e−[(y−µ)/σ]¢
, −∞ < y < ∞, ξ = 0.
The pdf is
gξ(y; µ, σ) =
1
σGξ(y; µ, σ)(1 + ξy−µσ )−1ξ,
ξ(y − µ) > −σ, ξ 6= 0,
1
σ exp¡
−e−[(y−µ)/σ]¢
e−[(y−µ)/σ],
−∞ < y < ∞, ξ = 0.
(7)
1.1 Maximum Likelihood Method
• For a given data (Y1, . . . , Ym) whose joint likelihood L (i.e., probability density function) is known but for an unknown parameter θ, we choose the parameter value such that the likelihood L is maximized.
• It is generally chosen by looking at the first deriva- tives with respect to θ (if θ represents a multiparam- eter) of the logarithm of the likelihood (log L) and equating to 0 and solving for θ. That is,
∂ log L
∂θ = 0
is solved and the solutions are checked to see which one corresponds to the largest possible value for the likelihood L.
• This general recipe produces estimates called Maxi- mum Likelihood Estimates (MLE) (say ˆθ) that have good large-sample properties under “regularity con- ditions”.
• One condition is that the range of the data is free of the unknown parameter we are trying to estimate (GEV with ξ 6= 0 is a “nonregular situation”.)
• In particular, if m is the sample size and m is large,
generally, √
m(ˆθ − θ) ≈ N(0, σθ2)
where σθ2 is related to the average Fisher information in the sample.
• This variance σθ2 can be estimated by the reciprocal of
− 1 m
∂2log L
∂θ2
¯¯
¯¯
θ=ˆθ
Example. If we have a random sample of size m from an exponential distribution with pdf
f (y; θ) = 1
θ exp{−y/θ}, y ≥ 0, the log-likelihood is given by
log L(θ) = −m log(θ) − 1 θ
Xm i=1
yi.
Differentiating this with respect to θ and equating to 0 we get only one solution namely,
θ = y,ˆ
the sample mean. Var(Y ) = θ2 and this is the recipro- cal of the Fisher information per observation. We know (central limit theorem) that
√m(ˆθ − θ) ≈ N(0, θ2).
2 Blocked Maxima Approach
Suppose we have a LARGE sample of size n from a dis- tribution with cdf F whose sample maximum is in the domain of maximal attraction. We are interested in the large percentiles and upper tails of F .
Suppose we can divide the total sample into m nonover- lapping blocks each of size r where r itself is big (say over 100). Note that n = m · r. Let Y1 be the largest in the first block,..., Ym be the largest of the mth block. Then Y1, . . . , Ym behaves like a random sample from the GEV distribution with pdf g(y) given by (7).
Note: If we know that F is in the domain of attraction of Gumbel, then ξ = 0 and hence we will have one less parameter and we will satisfy the regularity conditions for nice properties for the MLE to hold. We will consider it first.
Gumbel Distribution
From (7) we can write the joint pdf of Y1, . . . , Ym. The log-likelihood, log L(µ, σ) will be
−m log σ − Xm
i=1
µyi − µ σ
¶
− Xm
i=1
exp
½
−
µyi − µ σ
¶¾ .
We differentiate this with respect to µ and σ and ob- tain two equations. Solving iteratively using numerical techniques, we obtain the MLE (ˆµ, ˆσ). If m is large, the vector is approximately normally distributed with mean (µ, σ) and covariance matrix
1 m
6σ2 π2
Ãπ2
6 + (1 − γ)2 (1 − γ)
(1 − γ) 1
!
where γ is the Euler’s constant 0.5772... This can be used to provide confidence intervals for the parameter es- timates.
GEV Distribution
The log-likelihood for the GEV parameters is given by
−m log σ −(1 + 1ξ)Pm
i=1log£
1 + ξ¡y
i−µ σ
¢¤
−Pm
i=1
£1 + ξ ¡y
i−µ σ
¢¤−1/ξ ,
provided ξ(yi − µ) > −σ for i = 1, . . . , m. Since the range depends on the unknown parameters, the MLEs may not have the usual nice properties.
Smith (1985)
• When ξ > −0.5, MLEs have the usual properties.
• −1 < ξ ≤ −0.5: MLEs are generally obtainable but do not have the standard asymptotic properties.
• ξ < −1: MLEs are unlikely to be obtainable from numerical techniques- likelihood is too bumpy.
• If ξ ≤ −0.5, we have a short bounded upper tail for F - not encountered; Fr´echet has ξ > 0.
• ( ˆξ, ˆµ, ˆσ) is asymptotically normal with mean (ξ, µ, σ) and the covariance matrix can be approximated us- ing the inverse of the observed Fisher information matrix.
Large Quantile Estimation
Let zp be the upper pth quantile of the GEV. Then its estimate is given by
ˆ zp =
ˆ µ − ˆσˆ
ξ(1 − ypξˆ), if ˆξ 6= 0 ˆ
µ − ˆσ log(yp), if ξ = 0 (Gumbel),
where yp = − log(1 − p) is the upper pth quantile of the standard exponential population. Confidence inter- val for this percentile estimate can be computed using
the covariance matrix of the MLEs of the individual pa- rameters and linear approximations.
What we need are the estimates of the large quantiles of F . Suppose
F (xp0) = 1−p0 or Fr(xp0) = Pr(X(r) ≤ xp0) = (1−p0)r. Then with p = 1 − (1 − p0)r we have
ˆ
xp0 = ˆzp
given above. For example, suppose we need to estimate 99.5th (= 1 − p0) percentile of the parent population and we have used blocks of size 100. Then p = 1 − (0.995)100 ≈ 0.39 and we use this percentile estimate ˆz.39.
Tail Probability Estimation
Pr(X > c) = 1 − F (c)
= 1 − [Fr(c)]1/r
≈ 1 − [Gξ(c; µ, σ)]1/r.
Use the estimates of ξ, µ, and σ in the above formula to estimate the tail probability for the population.
3 Inference Using Top k Order Statistics Suppose n is large, but not large enough to make blocks of subsamples of substantial size. One can think of using the top k order statistics. If k is small when compared to n, one can use the joint pdf given in Result 6, namely,
g(yk) Yk
i=1
g(yi)
G(yi), y1 > · · · > yk
where g and G correspond to the GEV distribution. Thus, the likelihood will be
exp (
−
·
1 + ξ(yi − µ σ )
¸−1
ξ
) k Y
i=1
1 σ
·
1 + ξ(yi − µ σ )
¸−1
ξ−1
, where ξ(yi − µ) > −σ, i = 1, . . . , k. Using this like- lihood, one can obtain the MLEs of ξ, µ, σ. These esti- mates can be used to estimate the high percentiles of F by using p = 1 − (1 − p0)n and the ˆzp given earlier.
Remarks
• If we have data of top k order statistics from several blocks, say m, then we use the product of these like- lihoods and determine the MLEs using the combined likelihood.
• How large k can we take? A tricky question. Larger k means decreased standard error of the estimators, but increased bias as we move away from G towards F . Typically one increases k and looks at a plot of the estimates of the parameters; when they stabilize, one stops.
Quick Estimators of ξ
(a) Hill’s (1975) Estimator
• Assume ξ > 0 (Fr´echet type). This means upper limit of F is infinite.
ξˆH = 1 k
Xn i=n−k+1
log(X(i)) − log(X(n−k)).
• This is the mean excess function for the log(X) val- ues! log(X) values are defined for X > 0 and this is the case for the upper extremes from large samples.
• The Hill estimator is also asymptotically normal.
• This is the MLE of ξ assuming µ = 0 and σ = 1.
The MLE of α = 1/ ˆξ.
• Choice of k is determined by the examination of the plot of (k, ˆξH(k)).
(b) Pickands’ Estimator
• Works for any ξ real.
ξˆP = 1
log 2log
½ X(n−k+1) − X(n−2k+1) X(n−2k+1) − X(n−4k+1)
¾ .
• Here k is large but k/n is small.
• Choice of k is determined by the examination of the plot of (k, ˆξP(k)).
Remark
There are other estimators that are refinements of Hill’s and Pickands’. They have explicit forms and hence com- putation is easy, but there are no clear preferences.
4 Generalized Pareto Distribution – Estimates Based on Exceedances
Let t be the threshold and we use only the Xi that exceed t. Then, for t large, the exceedances Y ∗ = X −t have cdfs that can be approximated by a Pareto-type cdf having the form
Hξ(y; σ) =
1 − (1 + ξyσ)−1ξ, y > 0; ξy > −σ, if ξ 6= 0 1 − e−y/σ, y ≥ 0, if ξ = 0
(8) If there are k exceedances above t, say y1∗, . . . , yk∗, the MLEs of ξ and σ are obtained by using the log-likelihood
−k log(σ) − (1 + 1 ξ)
Xk i=1
log(1 + ξyi∗ k )
and for the case ξ = 0 we have the MLE based on the exponential distribution.
• The variance covariance matrix of ( ˆξ, ˆσ) is approxi- mated by using the inverse of the sample Fisher in- formation matrix.
• Let zp be the upper pth percentile of Hξ(y; σ). Then an estimate of the upper pth percentile of F is given
by
ˆ
xp = t + σˆ ξˆ
(µPr{X > t}
p
¶ξˆ
− 1 )
where we assume Pr{X > t} > p and Pr{X > t} is estimated by the sample proportion exceeding t.
• Choice of the threshold t - how close the exceedances are modeled by the Generalized Pareto distribution.
• Such data are called Peaks Over Threshold (POT) data.
5 General Diagnostic Plots
5.1 QQ plots
Plots of Sample Order Statistics against the Quantiles of the fitted/hypothesized distribution. Generally
¡X(i), F−1(n+1i )¢
for i = 1, . . . , n, is plotted. Sometimes (i − 12)/n is used in place of n+1i . Linear trend indicates good fit.
5.2 Mean Excess Function Plots
Plots of (k, en(k)), k = 1, 2, ... that tell us how close the data agrees with the assumed distribution. Here en(k) is the sample mean excess function
en(k) = 1 k
Xn i=n−k+1
X(i) − X(n−k) = Dk − X(n−k).
5.3 Plots for Choosing the top k Order Statistics
Plots of (k, ˆθ(k)) where ˆθ(k) is the estimate of the param- eter θ based on top k order statistics; it is accompanied by standard errors of the estimate. Used to examine the trade-off characteristics between bias and variance, and choose k for making inference.
6 General Remarks
1. The distribution of the maximum of a Poisson num- ber of IID excesses over a high threshold is a GEV.
(Crucial for stop-loss treaties.)
2. Relaxing Model Assumptions- Adjusting for Trend.
3. Stationarity with mild dependence structures.
4. Non-identical but independent, with no dominating distribution.
5. Linear processes (ARMA etc.)
7 Examples
Extreme Sea Levels in Venice Data Largest annual sea levels from 1931-1981.
a) Maxima of blocks of n = 365 days.
b) Scatterplot and Adjusting for trend.
c) Fitting GEV.
d) Estimating large percentile for 2005.
Reference: Ferreiras article in Reiss and Thomas (1997);
XTREMES software.
8 Computational/Software Resources
• XTREMES.
A free-standing software that comes with Reiss and Thomas’ book (academic edition- with limited data capacity). Professional edition is also available. Web- site:
http://www.xtremes.math.uni-siegen.de/xtremes/
• Alexander McNeil’s Website:
http://www.math.ethz.ch/ mcneil/software.html Has free software attachment that works with S-PLUS.
• http://www.maths.bris.ac.uik/ masgc/ismev/summary.html Associated with Coles’ book.
9 References
1. Arnold B. C., Balakrishnan N., and Nagaraja, H. N.
(1992). A First Course in Order Statistics. John Wiley, New York.
An elementary introduction to Order Statistics.
2. Balkema, A. A. and de Haan, L. (1974). Residual lifetime at great age. Annals of Probability 2, 792- 804.
3. Cebri´an, A. C., Denuit, M., and Lambert, P. (2003).
Generalized Pareto fit to the Society of Actuaries’
Large Claims Database. North American Actuarial Journal 7, No. 3, 18-36.
Shows how the GPD model outperforms parametric counter parts for this data set.
4. Coles, S. (2001). An Introduction to Statistical Modeling of Extreme Values. Springer Verlag, Lon- don.
A truly enjoyable applied introduction to extremes;
an excellent starting point. Has S-Plus codes and help to run them. Has two data examples from fi- nance.
5. Craighead, S. (2004). Personal communication - Cap- ital Requirements Data.
6. David H. A. and Nagaraja, H. N. (2003). Order Statistics, Third Edition. John Wiley, New York.
An encyclopedic reference - a dense treatment.
7. Embrechts P., Kl¨uppelberg C., and Mikosch, T. (1997).
Modelling Extremal Events for Insurance and Fi- nance. Springer Verlag, Berlin.
A compendium of theory and applications - requires a strong mathematical background; has examples from Insurance and Finance.
8. Hill, B. M. (1975). A simple general approach to inference about the tail of a distribution. Annals of Statistics 3, 1163-1174.
9. McNeil, A. J. Webpage: http://www.math.ethz.ch/ mc- neil/
An excellent resource for software, datasets, and pa- pers.
10. McNeil, A. J. (1996). Estimating the tails of loss severity distributions using extreme value theory. (his webpage)
11. Nagaraja, H. N., Choudhary, P.K., and Matalas, N.
(2002). Number of records in a bivariate sample with application to Missouri river flood data. Methodol-
ogy and Computing in Applied Probability 4, 377- 392.
12. Pickands, J. (1975). Statistical inference using ex- treme order statistics. Annals of Statistics 3, 119- 131.
13. Reiss R.-D. and Thomas, M. (1997). Statistical Anal- ysis of Extreme Values. Birkh¨auser Verlag, Basel, Switzerland.
XTREMES software comes with the book.
14. SAS JMP software, Version 5.1. (2003). SAS Insti- tute, Cary NC.
15. Smith, R. L. (1985). Maximum likelihood estimation in a class of non-regular cases. Biometrika 72, 67- 90.