Unit 11, lesson 83

Expected shortfall and coherent risk

Defines expected shortfall as a quantile integral that handles atoms, derives its threshold and dual envelope representations, proves that it is a coherent risk measure and explains why tail estimates remain uncertain.

  • Video 83
  • Attribution and tail risk measures

A loss is 0 with probability 0.9, 10 with probability 0.08 and 30 with probability 0.02, so its 95 percent value at risk is 10. What is the average loss over the worst 5 percent of probability? All of the mass at 30 belongs to that tail, but only 0.03 of the 0.08 at 10 does, so the answer has to count part of an atom. Expected shortfall is that average. This lesson defines it as an integral of quantiles, derives its threshold and dual envelope representations, proves that it is a coherent risk measure, unlike VaR, and explains why an exact formula does not make a tail estimate certain.

Key terms

Expected shortfall

Definition Let LL be an integrable loss, so that E[∣L∣]<∞\mathbb{E}[\lvert L \rvert] < \infty, with larger positive values worse, and let α∈(0,1)\alpha \in (0, 1). With the lower quantiles qu(L)=VaR⁡u(L)q_u(L) = \operatorname{VaR}_u(L) of Value at risk and quantile estimation, the expected shortfall at level α\alpha is

ES⁡α(L)=11−α∫α1qu(L) du.\operatorname{ES}_{\alpha}(L) = \frac{1}{1 - \alpha}\int_{\alpha}^{1} q_u(L)\,du .

It is a finite amount in currency units, as the next card shows. Because u↦quu \mapsto q_u is nondecreasing, ES⁡α(L)≥VaR⁡α(L)\operatorname{ES}_{\alpha}(L) \ge \operatorname{VaR}_{\alpha}(L), and because ∫01qu du=E[L]\int_0^1 q_u\,du = \mathbb{E}[L], the average over the top part of the levels is at least the overall average, ES⁡α(L)≥E[L]\operatorname{ES}_{\alpha}(L) \ge \mathbb{E}[L]. When LL has no atom at qαq_{\alpha}, the tail {L>qα}\{L > q_{\alpha}\} has probability exactly 1−α1 - \alpha and ES⁡α(L)=E[L∣L>qα]=E[L∣L≥qα]\operatorname{ES}_{\alpha}(L) = \mathbb{E}[L \mid L > q_{\alpha}] = \mathbb{E}[L \mid L \ge q_{\alpha}]. With an atom at the quantile both conditional means can differ from ES, because ES always averages exactly 1−α1 - \alpha of probability. Some texts call this quantity conditional value at risk or average value at risk.

In plain words Expected shortfall is the average loss over the worst 1−α1 - \alpha of probability. It averages a share of probability, not a set of loss values, so when one loss value straddles the cutoff only the needed part of its probability is counted.

Example For the opening loss, qu=0q_u = 0 for u≤0.9u \le 0.9, qu=10q_u = 10 for 0.9<u≤0.980.9 < u \le 0.98 and qu=30q_u = 30 for u>0.98u > 0.98, so

ES⁡0.95(L)=0.03⋅10+0.02⋅300.05=0.90.05=18.\begin{aligned} &\operatorname{ES}_{0.95}(L) \\[0.4em] &\quad = \frac{0.03 \cdot 10 + 0.02 \cdot 30}{0.05} \\[0.4em] &\quad = \frac{0.9}{0.05} = 18 . \end{aligned}

The mean of the losses strictly above VaR is 3030, and the mean of the losses at or above VaR is (0.08⋅10+0.02⋅30)/0.1=14(0.08 \cdot 10 + 0.02 \cdot 30)/0.1 = 14. Neither is 1818, because the first leaves out the part of the atom at 1010 that lies in the tail and the second includes all of it.

Quantile integral

Definition The quantile integral can be evaluated through the quantile representation of LL. If UU is uniform on (0,1)(0, 1), then qU(L)q_U(L) has the law of LL, because qu≤ℓq_u \le \ell holds exactly when u≤FL(ℓ)u \le F_L(\ell). Let q=qα(L)q = q_{\alpha}(L) and p=P(L>q)p = \mathbb{P}(L > q). For α<u≤FL(q)\alpha < u \le F_L(q) the quantile equals qq, and qu>qq_u > q exactly when u>FL(q)u > F_L(q), so

∫α1qu du=q (FL(q)−α)+E[L 1{L>q}].\begin{aligned} &\int_{\alpha}^{1} q_u\,du = q\,\bigl(F_L(q) - \alpha\bigr) \\[0.4em] &\qquad + \mathbb{E}\bigl[L\,\mathbf{1}_{\{L > q\}}\bigr] . \end{aligned}

The last term is finite because LL is integrable. The weight FL(q)−α=1−α−pF_L(q) - \alpha = 1 - \alpha - p is the part of the atom at qq that the tail needs, and it lies between 00 and P(L=q)\mathbb{P}(L = q) because P(L<q)≤α≤FL(q)\mathbb{P}(L < q) \le \alpha \le F_L(q). Dividing by 1−α1 - \alpha and using E[(L−q)+]=E[L 1{L>q}]−qp\mathbb{E}[(L - q)^{+}] = \mathbb{E}[L\,\mathbf{1}_{\{L > q\}}] - qp gives

ES⁡α(L)=q+E[(L−q)+]1−α.\begin{aligned} &\operatorname{ES}_{\alpha}(L) \\[0.4em] &\quad = q + \frac{\mathbb{E}\bigl[(L - q)^{+}\bigr]}{1 - \alpha} . \end{aligned}

In plain words The worst 1−α1 - \alpha of probability consists of all the probability strictly above the quantile plus just enough of the atom at the quantile to fill the share. The last formula uses the quantile as a baseline for the whole tail and adds the expected excess of the losses beyond it, scaled to the size of the tail.

Example For the opening loss at α=0.95\alpha = 0.95, the quantile is q=10q = 10, the tail takes all 0.020.02 at 3030 and FL(10)−0.95=0.03F_L(10) - 0.95 = 0.03 of the atom at 1010, and the formula gives 10+0.02⋅20/0.05=10+8=1810 + 0.02 \cdot 20/0.05 = 10 + 8 = 18. At α=0.9\alpha = 0.9 the quantile is 00, since FL(0)=0.9F_L(0) = 0.9, so no part of the atom at 00 is needed and

ES⁡0.9(L)=0.08⋅10+0.02⋅300.1=14.\begin{aligned} &\operatorname{ES}_{0.9}(L) \\[0.4em] &\quad = \frac{0.08 \cdot 10 + 0.02 \cdot 30}{0.1} \\[0.4em] &\quad = 14 . \end{aligned}

Here ES equals the mean of the losses strictly above VaR, because FL(q)=αF_L(q) = \alpha.

Threshold representation

Definition For an integrable loss LL, a level α∈(0,1)\alpha \in (0, 1) and a real threshold zz, put

G(z)=z+E[(L−z)+]1−α.G(z) = z + \frac{\mathbb{E}\bigl[(L - z)^{+}\bigr]}{1 - \alpha} .

Then GG is finite and convex, its minimizers are exactly the zz with

P(L<z)≤α≤P(L≤z),\mathbb{P}(L < z) \le \alpha \le \mathbb{P}(L \le z),

a closed interval that contains qα(L)q_{\alpha}(L), and

ES⁡α(L)=min⁡z∈RG(z).\operatorname{ES}_{\alpha}(L) = \min_{z \in \mathbb{R}} G(z) .

For the proof, the map z↦(ℓ−z)+z \mapsto (\ell - z)^{+} is convex for each ℓ\ell, so GG is convex. The one-sided difference quotients of (ℓ−z)+(\ell - z)^{+} in zz are bounded by 11 in absolute value, so dominated convergence moves the one-sided derivatives inside the expectation,

G+′(z)=1−P(L>z)1−α,G−′(z)=1−P(L≥z)1−α.\begin{aligned} G'_{+}(z) &= 1 - \frac{\mathbb{P}(L > z)}{1 - \alpha}, \\[0.4em] G'_{-}(z) &= 1 - \frac{\mathbb{P}(L \ge z)}{1 - \alpha}. \end{aligned}

A point minimizes a convex function exactly when G−′(z)≤0≤G+′(z)G'_{-}(z) \le 0 \le G'_{+}(z), which is the displayed quantile condition. The lower quantile satisfies it, and the previous card gives G(qα)=ES⁡α(L)G(q_{\alpha}) = \operatorname{ES}_{\alpha}(L). The minimizer need not be unique, since the condition holds on a whole interval when FLF_L equals α\alpha across a gap between loss values, but every minimizer gives the same value. For nn equally weighted scenarios whose losses Li(w)L_i(w) are affine in the portfolio weights ww, the problem

min⁡z, u, w  z+1n(1−α)∑i=1nui,\min_{z,\,u,\,w}\; z + \frac{1}{n(1 - \alpha)}\sum_{i=1}^{n} u_i ,

subject to ui≥Li(w)−zu_i \ge L_i(w) - z and ui≥0u_i \ge 0 for every scenario and to linear constraints on ww, is a linear program. At an optimum each uiu_i equals (Li(w)−z)+(L_i(w) - z)^{+}, so its optimal value, when it exists, is the smallest scenario ES over the allowed portfolios, found without sorting the losses of every trial portfolio.

In plain words The threshold form treats the cutoff as a variable. Pay a trial threshold in full and add the expected excess above it, scaled by 1/(1−α)1/(1 - \alpha). This overstates the tail average unless the threshold is a quantile, where the two pieces add up to ES exactly.

Example For the opening loss at α=0.95\alpha = 0.95 the objective takes the values G(0)=28G(0) = 28, G(5)=23G(5) = 23, G(10)=18G(10) = 18, G(20)=24G(20) = 24 and G(30)=30G(30) = 30. At z=10z = 10 the one-sided derivatives are G−′(10)=1−0.1/0.05=−1G'_{-}(10) = 1 - 0.1/0.05 = -1 and G+′(10)=1−0.02/0.05=0.6G'_{+}(10) = 1 - 0.02/0.05 = 0.6, so 1010 is the unique minimizer, at a kink of GG, and the minimum is 1818. At α=0.9\alpha = 0.9 the distribution function equals 0.90.9 on [0,10)[0, 10), every zz in [0,10][0, 10] satisfies the condition, and G(0)=G(5)=G(10)=14G(0) = G(5) = G(10) = 14.

Dual envelope representation

Definition Let Zα\mathcal{Z}_{\alpha} be the set of random variables ZZ on the same probability space with 0≤Z≤1/(1−α)0 \le Z \le 1/(1 - \alpha) almost surely and E[Z]=1\mathbb{E}[Z] = 1. For an integrable loss LL and α∈(0,1)\alpha \in (0, 1),

ES⁡α(L)=sup⁡Z∈ZαE[ZL],\operatorname{ES}_{\alpha}(L) = \sup_{Z \in \mathcal{Z}_{\alpha}} \mathbb{E}[ZL] ,

and the supremum is attained. Each Z∈ZαZ \in \mathcal{Z}_{\alpha} is the density dQ/dPd\mathbb{Q}/d\mathbb{P} of a probability measure Q\mathbb{Q} that multiplies probabilities by factors between 00 and 1/(1−α)1/(1 - \alpha), so ES is the largest expected loss over these reweightings. For the upper bound, take any Z∈ZαZ \in \mathcal{Z}_{\alpha} and any real zz. Because E[Z]=1\mathbb{E}[Z] = 1, Z≥0Z \ge 0 and Z≤1/(1−α)Z \le 1/(1 - \alpha),

E[ZL]=z+E[Z(L−z)]≤z+E[Z(L−z)+]≤z+E[(L−z)+]1−α,\begin{aligned} \mathbb{E}[ZL] &= z + \mathbb{E}\bigl[Z(L - z)\bigr] \\[0.4em] &\le z + \mathbb{E}\bigl[Z(L - z)^{+}\bigr] \\[0.4em] &\le z + \frac{\mathbb{E}\bigl[(L - z)^{+}\bigr]}{1 - \alpha} , \end{aligned}

and the choice z=qαz = q_{\alpha} gives E[ZL]≤ES⁡α(L)\mathbb{E}[ZL] \le \operatorname{ES}_{\alpha}(L). For attainment, let q=qαq = q_{\alpha} and set Z∗=1/(1−α)Z^{*} = 1/(1 - \alpha) on {L>q}\{L > q\}, Z∗=0Z^{*} = 0 on {L<q}\{L < q\} and, when P(L=q)>0\mathbb{P}(L = q) > 0, Z∗=βZ^{*} = \beta on {L=q}\{L = q\} with

β=1−α−P(L>q)(1−α) P(L=q).\beta = \frac{1 - \alpha - \mathbb{P}(L > q)}{(1 - \alpha)\,\mathbb{P}(L = q)} .

The quantile inequalities P(L>q)≤1−α≤P(L≥q)\mathbb{P}(L > q) \le 1 - \alpha \le \mathbb{P}(L \ge q) give 0≤β≤1/(1−α)0 \le \beta \le 1/(1 - \alpha). Then E[Z∗]=1\mathbb{E}[Z^{*}] = 1, and E[Z∗L]\mathbb{E}[Z^{*}L] is the tail-mass formula of the quantile integral card divided by 1−α1 - \alpha, which is ES. Without an atom at qq one has P(L>q)=1−α\mathbb{P}(L > q) = 1 - \alpha, and the upper tail alone carries the weight.

In plain words Think of ZZ as a stress reweighting of the states. It keeps total probability equal to one and may multiply the probability of any state by a factor between zero and 1/(1−α)1/(1 - \alpha). The most damaging reweighting puts the full factor on the losses above the quantile, a partial factor on the cutoff atom so that the probabilities still add to one, and zero elsewhere. Its expected loss is ES.

Example For the opening loss at α=0.95\alpha = 0.95 the cap is 2020. The construction gives weight 2020 to the loss 3030, weight β=0.03/(0.05⋅0.08)=7.5\beta = 0.03/(0.05 \cdot 0.08) = 7.5 to the loss 1010 and weight 00 to the loss 00. Then E[Z∗]=0.02⋅20+0.08⋅7.5=1\mathbb{E}[Z^{*}] = 0.02 \cdot 20 + 0.08 \cdot 7.5 = 1, and the reweighted probabilities are 0.40.4 on 3030 and 0.60.6 on 1010, so E[Z∗L]=0.4⋅30+0.6⋅10=18\mathbb{E}[Z^{*}L] = 0.4 \cdot 30 + 0.6 \cdot 10 = 18. The feasible weight Z=10Z = 10 on both losses 1010 and 3030 gives only 1414, the mean at or above VaR, and a grid search over all feasible weights on the three states finds no value above 1818.

Coherent risk measure

Definition Let ρ\rho assign a real number to every integrable loss on a fixed probability space, with losses positive when adverse. It is a coherent risk measure if, for all integrable LL, L1L_1 and L2L_2, every constant cc and every λ≥0\lambda \ge 0,

L1≤L2  ⟹  ρ(L1)≤ρ(L2),ρ(L+c)=ρ(L)+c,ρ(λL)=λ ρ(L),ρ(L1+L2)≤ρ(L1)+ρ(L2),\begin{gathered} L_1 \le L_2 \implies \rho(L_1) \le \rho(L_2), \\[0.4em] \rho(L + c) = \rho(L) + c, \\[0.4em] \rho(\lambda L) = \lambda\,\rho(L), \\[0.4em] \rho(L_1 + L_2) \le \rho(L_1) + \rho(L_2), \end{gathered}

where L1≤L2L_1 \le L_2 holds almost surely. These are monotonicity, translation equivariance, positive homogeneity and subadditivity. In the profit and loss convention X=−LX = -L, translation reads ρ(X+m)=ρ(X)−m\rho(X + m) = \rho(X) - m, since a sure gain lowers risk. Expected shortfall is coherent, and each property follows from the dual envelope with one set Zα\mathcal{Z}_{\alpha} for every loss. Monotonicity holds because every ZZ is nonnegative, translation because E[Z(L+c)]=E[ZL]+c\mathbb{E}[Z(L + c)] = \mathbb{E}[ZL] + c, and positive homogeneity because E[ZλL]=λ E[ZL]\mathbb{E}[Z\lambda L] = \lambda\,\mathbb{E}[ZL] with λ≥0\lambda \ge 0. For subadditivity, every Z∈ZαZ \in \mathcal{Z}_{\alpha} gives

E[Z(L1+L2)]=E[ZL1]+E[ZL2]≤ES⁡α(L1)+ES⁡α(L2),\begin{aligned} &\mathbb{E}[Z(L_1 + L_2)] \\[0.4em] &\quad = \mathbb{E}[ZL_1] + \mathbb{E}[ZL_2] \\[0.4em] &\quad \le \operatorname{ES}_{\alpha}(L_1) + \operatorname{ES}_{\alpha}(L_2), \end{aligned}

and the supremum over ZZ on the left is ES⁡α(L1+L2)\operatorname{ES}_{\alpha}(L_1 + L_2). No independence or distributional assumption enters, because one set of weights serves every loss. VaR has the first three properties but not the fourth, as the previous lesson shows.

In plain words A coherent measure ranks a loss that is larger in every state as riskier, adds a sure loss one for one, scales with position size and never charges a combined book more than the sum of its parts. Coherence is a property of the measure. It says nothing about whether the loss distribution fed into it is correct.

Example Take the independent exposures AA and BB of the previous lesson, each losing 100100 with probability 0.040.04. At 9595 percent their VaR is 00 and ES⁡0.95(A)=0+0.04⋅100/0.05=80\operatorname{ES}_{0.95}(A) = 0 + 0.04 \cdot 100/0.05 = 80, and the same holds for BB. The sum has VaR 100100 and

ES⁡0.95(A+B)=100+0.0016⋅1000.05=103.2,\begin{aligned} &\operatorname{ES}_{0.95}(A + B) \\[0.4em] &\quad = 100 + \frac{0.0016 \cdot 100}{0.05} = 103.2 , \end{aligned}

below 80+80=16080 + 80 = 160, whereas the VaRs were 00, 00 and 100100. If B=AB = A, the sum is 2A2A and ES⁡0.95(2A)=160\operatorname{ES}_{0.95}(2A) = 160, so the bound is attained for identical exposures.

Tail estimation

Definition For nn equally weighted losses with order statistics L(1)≤⋯≤L(n)L_{(1)} \le \dots \le L_{(n)} and k=⌈nα⌉k = \lceil n\alpha \rceil, the ES of the empirical law satisfies

n(1−α) ES⁡^α=(k−nα) L(k)+∑i=k+1nL(i),\begin{aligned} &n(1 - \alpha)\,\widehat{\operatorname{ES}}_{\alpha} \\[0.4em] &\quad = (k - n\alpha)\,L_{(k)} \\[0.4em] &\qquad + \sum_{i = k + 1}^{n} L_{(i)} , \end{aligned}

which is the quantile integral of the empirical distribution, with the fractional weight (k−nα)/n(k - n\alpha)/n on the cutoff observation. When nαn\alpha is an integer it is the mean of the n(1−α)n(1 - \alpha) largest losses. The formula is exact for the sample, but as an estimate of the ES of the loss distribution it is uncertain. About n(1−α)n(1 - \alpha) observations determine it, they set both the cutoff and the severity of the tail, and a single new large loss can move it far. Dependence and changing volatility change its sampling behavior further. If E[L+]=∞\mathbb{E}[L^{+}] = \infty, the quantile integral diverges and ES⁡α(L)=∞\operatorname{ES}_{\alpha}(L) = \infty at every level, although every VaR is finite. A heavy tail of gains alone does not make ES infinite, although the derivations above assumed E[∣L∣]<∞\mathbb{E}[\lvert L \rvert] < \infty. Extreme value models extend a tail beyond the data, but they add assumptions about severity that the sample cannot confirm. Statistical theory for ES estimators is beyond this lesson.

In plain words Computing the tail average of a sample is exact arithmetic, but the tail of a sample is thin. A few observations decide the answer, so the estimate can move a lot from one sample to the next, and losses larger than any in the sample do not enter it at all.

Example For the twenty constructed losses of the previous lesson, nα=19n\alpha = 19 at 9595 percent, so the empirical ES is the single largest loss, 4040, and at 9090 percent it is (25+40)/2=32.5(25 + 40)/2 = 32.5. Adding the loss 100100 gives n=21n = 21, k=20k = 20 and k−nα=0.05k - n\alpha = 0.05, so

ES⁡^0.95=0.05⋅40+1001.05≈97.14,\begin{aligned} \widehat{\operatorname{ES}}_{0.95} &= \frac{0.05 \cdot 40 + 100}{1.05} \\[0.4em] &\approx 97.14 , \end{aligned}

while the empirical VaR moved only from 2525 to 4040. For constructed losses that are independent and normal with mean 00 and standard deviation 1010, the 97.597.5 percent ES is 10 φ(1.96)/0.025≈23.3810\,\varphi(1.96)/0.025 \approx 23.38, with Φ−1(0.975)≈1.96\Phi^{-1}(0.975) \approx 1.96. In a simulation of 100000100000 samples of size 250250, with about 66 observations per sample beyond the cutoff, the empirical ES averaged about 23.0523.05 with a standard deviation of about 2.002.00. With samples of size 10001000 it averaged about 23.2923.29 with a standard deviation of about 1.011.01.

Check yourself

  1. For the opening loss, which is 00, 1010 or 3030 with probabilities 0.90.9, 0.080.08 and 0.020.02, compute the 97.597.5 percent VaR and ES from the tail masses, from the threshold formula and from the dual weights.
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The distribution function is 0.90.9 at 00 and 0.980.98 at 1010, so the 97.597.5 percent VaR is 1010. The tail of probability 0.0250.025 takes all 0.020.02 at 3030 and 0.0050.005 of the atom at 1010, which contribute 0.02⋅30=0.60.02 \cdot 30 = 0.6 and 0.005⋅10=0.050.005 \cdot 10 = 0.05, so

ES⁡0.975=0.6+0.050.025=0.650.025=26.\begin{aligned} \operatorname{ES}_{0.975} &= \frac{0.6 + 0.05}{0.025} \\[0.4em] &= \frac{0.65}{0.025} = 26 . \end{aligned}

The threshold formula at q=10q = 10 gives 10+0.02⋅20/0.025=10+16=2610 + 0.02 \cdot 20/0.025 = 10 + 16 = 26. The cap of the dual weights is 4040, the loss 3030 gets weight 4040 and the atom at 1010 gets β=0.005/(0.025⋅0.08)=2.5\beta = 0.005/(0.025 \cdot 0.08) = 2.5. These weights satisfy 0.02⋅40+0.08⋅2.5=10.02 \cdot 40 + 0.08 \cdot 2.5 = 1, and the reweighted expectation is 0.8⋅30+0.2⋅10=260.8 \cdot 30 + 0.2 \cdot 10 = 26.

  1. For the independent exposures AA and BB that each lose 100100 with probability 0.040.04, a colleague measures tail risk by the mean of the losses at or above the 9595 percent VaR. Compute this measure for AA, for BB and for A+BA + B, and compare it with ES.
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Each exposure has VaR 00, and every state has a loss at or above 00, so the colleague’s measure is the plain mean E[A]=0.04⋅100=4\mathbb{E}[A] = 0.04 \cdot 100 = 4, and the same for BB. The sum has VaR 100100, the states at or above it have probability 0.0768+0.0016=0.07840.0768 + 0.0016 = 0.0784, and they contribute 0.0768⋅100=7.680.0768 \cdot 100 = 7.68 and 0.0016⋅200=0.320.0016 \cdot 200 = 0.32 to the expectation, so

E[A+B∣A+B≥100]=7.68+0.320.0784≈102.04,\begin{aligned} &\mathbb{E}[A + B \mid A + B \ge 100] \\[0.4em] &\quad = \frac{7.68 + 0.32}{0.0784} \\[0.4em] &\quad \approx 102.04 , \end{aligned}

which exceeds 4+4=84 + 4 = 8, so this measure is not subadditive. It averages over probability 11 for each exposure and 0.07840.0784 for the sum instead of over 0.050.05 in each case. ES gives 8080, 8080 and 103.2103.2, which satisfies subadditivity. The two measures agree whenever the event of losses at or above VaR has probability exactly 1−α1 - \alpha, for example when the distribution function is continuous.

  1. A constructed loss has P(L>x)=1/x\mathbb{P}(L > x) = 1/x for x≥1x \ge 1. Find its 9999 percent VaR and ES, and do the same for P(L>x)=1/x2\mathbb{P}(L > x) = 1/x^2. Which hypothesis of the lesson fails in the first case, and what would the empirical ES of a sample from it report?
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In the first case F(x)=1−1/xF(x) = 1 - 1/x, so qu=1/(1−u)q_u = 1/(1 - u) and VaR⁡0.99=100\operatorname{VaR}_{0.99} = 100. The quantile integral

∫0.991du1−u=∞,\int_{0.99}^{1} \frac{du}{1 - u} = \infty ,

so ES is infinite. The hypothesis that fails is integrability, since E[L]=1+∫1∞x−1 dx=∞\mathbb{E}[L] = 1 + \int_1^{\infty} x^{-1}\,dx = \infty. In the second case qu=(1−u)−1/2q_u = (1 - u)^{-1/2}, so VaR⁡0.99=10\operatorname{VaR}_{0.99} = 10 and

ES⁡0.99=20.010.01=20.\begin{aligned} \operatorname{ES}_{0.99} &= \frac{2\sqrt{0.01}}{0.01} \\[0.4em] &= 20 . \end{aligned}

Every sample is finite, so the empirical ES of a sample from the first law is always a finite number, and it tends to grow without bound as the sample grows. A finite estimate is therefore no evidence that ES is finite. In the second case ES is finite, but E[L2]=∞\mathbb{E}[L^2] = \infty, so the usual standard error formula for an average does not apply to the tail losses.

How this lesson connects