Condition on the claim count, defining the empty sum to be zero. Independence gives . By the law of total expectation,
For nonnegative claims this also follows from Tonelli theorem; for signed claims finite and ensure integrability. Conditional independence likewise gives
This random-sum transform identity holds wherever the composed series is finite, or as an extended nonnegative expectation. It is not permission to use an algebraic continuation outside the convergence domain.
For the zero-based geometric distribution, summing the geometric series gives
The exponential distribution of mean has for . Therefore
The stricter bound is necessary: the geometric series requires . At and above that series diverges; at and above even one claim has an infinite transform. Thus the displayed rational expression represents the moment-generating function only on its stated domain.
Since all claims are strictly positive, exactly when , so . Splitting the transform gives
Uniqueness of the moment-generating function identifies a mixture distribution with a zero atom of weight and an exponential positive component of weight and rate . In particular,
The density integrates to , not one. One can also verify it directly: conditional on , the sum has Erlang distribution density . Multiplying by and summing over gives , the same density. This is the zero-based geometric sum of exponential variables.
Under excess of loss reinsurance, the ceded amount for each claim is , and the monthly reduction is their random sum. The tail integral formula for moments gives
Conditioning on again yields
The retained payment is ; it is generally not .
Under aggregate stop loss reinsurance, the reduction is . The aggregate tail is for , so
The prefactor is positive. Equality with the per-claim recovery is equivalent to , giving the unique reinsurance retention
This is the relation for equal expected recoveries from excess of loss and stop loss; since , the aggregate reinsurance retention exceeds the individual reinsurance retention. These are reductions in claim payouts, before any reinsurance premium is deducted.
Write , with , and differentiate :
Using and gives
Thus the first three cumulants are the mean, variance and third central moment. A finite moment-generating function near zero justifies these differentiations. For positive claims with only three finite ordinary moments, the same calculations are valid as left derivatives at zero of the logarithm of the Laplace transform of a nonnegative random variable; positive exponential moments are not needed for the resulting moment identities.
For the independent Poisson distribution count, the random-sum transform identity gives
Consequently the compound Poisson distribution has
These are raw severity moments, not severity cumulants.
The printed gamma density uses rate , not scale. Direct integration against gives
Therefore the required matching equations for the shifted gamma distribution are
For and nonzero positive claims with finite , these equations give positive and the unique solution
This is the three-cumulant shifted gamma approximation. In particular, its skewness equals , the skewness of .
The competing normal approximation to a compound Poisson aggregate is
To justify its large-count limit, let be the claim characteristic function. For fixed severity law with , its expansion is . The characteristic function of is
Thus it converges in distribution to a standard normal distribution as .
The normal approximation is simple, uses only , and works well in the centre when the count is large and standardized skewness is small. It imposes symmetry, whereas positive compound-Poisson claims have positive third cumulant. The shifted-gamma approximation reproduces that third cumulant and can better describe moderate right skewness. It requires a finite and reliably known third moment, and matching three cumulants alone does not guarantee accurate extreme tails.
Neither continuous approximation reproduces the genuine atom , which matters at small . The normal distribution also assigns probability to negative losses. The gamma approximation is bounded below by , but its fitted shift need not be nonnegative: exponential claims of mean give , so it too can assign mass to negative losses. If , it instead excludes some genuinely possible small losses. These support and atom discrepancies prevent either approximation from being a universal replacement for the exact aggregate law.
For the Poisson process of claims and relative safety loading , the premium rate in the classical risk model is . Dividing the adjustment coefficient equation by explains why the arrival rate cancels. Interpret as the upper endpoint of the finite moment-generating function domain, so for and its stated divergence occurs at that endpoint.
Set . Then
Differentiation is valid inside the finite-transform domain, and its positive neighbourhood gives finite moments of every order. Thus is strictly convex and negative just to the right of zero. If , divergence of makes at the endpoint. If , choose with ; then , which eventually exceeds every linear function. Again . The intermediate value theorem gives a positive zero.
There is at most one positive zero: strict convexity and make the secant slope strictly increasing for . It starts at and crosses zero exactly once. Hence
This proves the secant-slope existence criterion for an adjustment coefficient in the present setting.
Put . For , the positive remainder of the exponential series gives . Apply it to and take expectations:
Dividing by yields
Keeping the cubic term similarly gives
The polynomial is strictly increasing for , is negative at zero and tends to infinity. Let be its unique positive zero. The last inequality says , so
Finally, , whence . Monotonicity gives . Thus the requested upper bounds can in fact be sharpened to the strict ordering . The bounds themselves need not lie in the finite-transform domain; the argument only evaluates the actual transform at and polynomial moments elsewhere. These are polynomial moment bounds for the adjustment coefficient.
For rate- exponential distribution claims,
The positive root satisfies after dividing out , so
The cubic-bound equation reduces to , selecting the displayed positive root. In particular , as required by the transform domain, for every .
A credibility estimate combines a risk's observed experience with collective or prior information, typically as . The credibility factor is the weight assigned to the individual experience: more reliable or more extensive data generally increases it. Bayesian credibility treats the risk parameter as random with a prior distribution and predicts future claims by averaging the conditional claim mean under its posterior distribution. Under squared-error loss this posterior predictive mean is optimal. It need not be an affine combination in every Bayesian model; the Poisson-gamma conjugacy calculation below yields that credibility form exactly, rather than as a best-linear approximation.
Let . The conditional joint likelihood function of the observed counts is
The prior is a gamma distribution with shape two and rate . Multiplication by its density gives the unnormalized posterior density . Normalizing with the gamma function yields
Thus Poisson-gamma conjugacy gives . Conditional on and the past data, the next count has mean , so the law of total expectation gives
With and prior mean , this is exactly
Here , , and the credibility factor increases to one as the number of observed years grows. The denominator uses the prior rate and total exposure ; it does not add two to the exposure when adding the prior shape.
Given , the sum of the independent yearly counts is : their probability generating functions multiply to . Averaging this conditional law over the prior gives the mixed Poisson distribution
The likelihood for the full vector depends on only through , so is a sufficient statistic; conditioning on the total or on the full observed vector gives the same posterior for .
For an event of positive probability , the posterior density is proportional to . Put . Its mean is . The future count has conditional mean , so
This is the posterior mean from adjacent mixed Poisson probabilities. Both probabilities refer to the same -year exposure; the numerator is not a probability for . For a proper prior and , the integrals defining this posterior mean are finite because is bounded on .
Insert the shape-two gamma prior into the integral from part (ii). The gamma function integral gives
Therefore has a negative binomial distribution with shape two and success probability , using the failures-before-two-successes convention. This is the Poisson-gamma mixture. The identity verifies that the probabilities sum to one.
Its adjacent probability ratio is
Substituting in the posterior formula gives
exactly the estimate from part (i). The equality is required by sufficiency, and the direct computation confirms that the two negative-binomial and gamma parameter conventions have been used consistently.

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