Adjustment coefficient 2026-10-06
The adjustment coefficient is a positive root of in the classical risk model. When the moment-generating function is finite at , the process is a continuous-time martingale. It yields the Lundberg inequality and, under the relevant tilted integrability, the Cramér–Lundberg ruin asymptotic.
For positive claims with finite variance and , the classical risk model has ruin probability one from any finite capital. At claim times, surplus increments are independent copies of with mean . Negative mean sends their partial sums to minus infinity by the strong law of large numbers. At zero mean, the increments have finite nonzero variance. For every fixed , the central limit theorem gives limiting probability of a partial sum below . The probability of unboundedness below is therefore at least ; as a tail event it has probability zero or one by the Kolmogorov zero-one law, and hence one.
In the classical risk model with positive relative safety loading and adjustment coefficient , tilting the ruin defective renewal equation gives a proper renewal equation. The key renewal theorem yields . The constant is positive if the denominator is finite and zero if it is infinite; the claim-size density provides the nonarithmetic hypothesis.
In a classical risk model, before the first claim at time , available capital is . A claim of size leaves future survival probability by the Markov property. Integrating over the independent first-arrival exponential distribution and claim density gives .
Lundberg inequality 2026-10-06
For a classical risk model with adjustment coefficient , the ultimate ruin probability from capital satisfies . Stop the exponential continuous-time martingale at ruin or a finite horizon, bound its value on the ruin event, and then increase the horizon.
Use for the premium income rate, reserving later for the smaller exponential decay rate. In the classical risk model, the surplus is
Here is the relative safety loading. The aggregate claims form a Compound Poisson process. Define , so ruin occurs when . By independent increments and the exponential formula for a marked Poisson sum,
Thus is a nonnegative continuous-time martingale with , because the adjustment coefficient makes the exponent vanish.
Let . Apply the optional stopping theorem at the bounded stopping time . On , , so
Letting increase proves the Lundberg inequality and the unscaled limit:
For the precise asymptotic, put
The given exponential integral identity makes a probability density. Multiplying the given defective renewal equation by turns it into the ordinary renewal equation
For clarity, the version of the key renewal theorem used here is: if the interarrival law is nonarithmetic, has mean , and is directly Riemann integrable, the locally bounded solution of this renewal equation satisfies . The infinite-mean version gives zero for nonnegative directly Riemann integrable .
All the hypotheses can be checked here. The density gives a nonarithmetic distribution. The Tonelli theorem gives
Furthermore
Thus is continuous and integrable, and . On a mesh of width , the difference between its upper and lower sums is at most ; its upper sum is at most . This proves direct Riemann integrability rather than assuming it. Also by the Lundberg inequality, so the solution is locally bounded. Its renewal representation is , where and ; the residual after iteration tends to zero on compact intervals because sums of positive interarrivals tend to infinity.
Writing , the tilted interarrival expected value is . The key renewal theorem gives the Cramér–Lundberg ruin asymptotic
If , the same formula is interpreted as . A positive finite asymptotic constant requires ; this extra integrability is not explicitly stated in the paper.
For the final two-exponential case, evaluate the defective renewal equation at zero:
One can identify the adjustment coefficient without silently assuming . For , set
It is finite and positive. Integrating the nonnegative terms of the defective renewal equation, using the Tonelli theorem, first shows that is finite and then gives
As , because . By monotone convergence theorem, . The integrated tail distribution in the classical risk model has density , so by the tail integral formula for moments. Hence solves the adjustment equation, and its stipulated uniqueness implies . Finally the displayed form of gives the remaining constants
In particular the decay exponent and the coefficient do not affect or . The in these final answers is the printed decay rate, not .
Relative safety loading 2026-10-06
If the expected claim outflow per unit time is , the relative safety loading is . Positive loading means expected premium income exceeds expected claim outflow. This is the net profit condition in the classical risk model.
In a classical risk model with positive relative safety loading, zero initial capital has ultimate survival probability , where is the claim-arrival rate, the claim expected value and the premium rate. It depends on the claim law through its mean alone. It is not the event of never receiving a claim: premium accumulates between arrivals.