For sample means of Poisson random variables of mean , the cumulant-generating function is . Its Legendre-Fenchel transform is the displayed good rate function, with , and is infinite for . Near its zero, . This local quadratic explains the Poisson moderate deviation principle.
For independent and identically distributed exponential random variables of rate , the sample mean has large-deviation speed and the displayed good rate function, infinite for . The cumulant-generating function is for . Its Legendre-Fenchel transform has maximizing parameter . For , sending gives infinite cost. The cost has its unique zero at and diverges at both ends of its positive domain.
For independent unit-rate exponential random variables, the cumulant-generating function is for . Its Legendre transform of a cumulant-generating function is for and infinite otherwise. The Cramér theorem gives the upper-tail logarithmic rate for , and zero for . At the mean threshold the infima on both the open and closed upper half-lines are zero; below the mean the strong law of large numbers applies.
For independent identically distributed real variables with everywhere finite cumulant-generating function, let be the mean. If and , then for each . The Legendre transform of a cumulant-generating function is finite at , and a positive exponential parameter gives strictly greater cost at . A Chernoff bound for the farther tail divided by the Cramér theorem lower estimate at decays exponentially. The support condition both ensures positive conditioning probabilities and avoids a vacuous conditioning event.
Exponential tilting by replaces a law by
Under the tilted law, the mean is whenever the derivative exists.
Suppose for all . Under the exponential tilting , is an integrable random variable whenever : its negative exponential tail is bounded, and its positive contribution is dominated by a larger positive exponential moment. Differentiation under the integral sign gives the displayed mean. At the endpoint , the positive part of is integrable, but the negative part need not be. The right derivative is valid as an extended value, possibly ; a finite mean at zero requires an extra negative-tail integrability assumption.

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