Absolute-error loss 2026-10-05
The loss for estimating a real parameter by . Its risk of a decision rule is the corresponding expected value. Unlike squared-error loss, its pointwise size is a metric, so the triangle inequality gives a direct overlap version of the Le Cam two-point lemma.
If each claim includes an independent expense , replace its payment law by the convolution of independent random variables . Its moment-generating function is and its expected value is . Keeping the relative safety loading fixed therefore changes the premium rate as well. The new coefficient solves , within the common finite-transform domain.
Angular momentum of a radial function times a linear polynomial Created 2026-10-05 Updated 2026-10-07
Orbital angular momentum operators annihilate a radial multiplier . Their squared sum sends every degree-one homogeneous polynomial to times that polynomial, so a nonzero normalizable state has angular momentum quantum number . With real and real coefficients, its third-component expected value is zero by angular symmetry, though it need not be an eigenstate of that component.
Suppose and . The breadth-first exploration of a binomial random graph has deterministic drift up to steps. Its weighted martingale has variance . For , the Doob L2 maximal inequality makes its maximum smaller than with high probability. Then throughout , giving a graph component of order .
For the upper expectation bound, let . The dominating binomial branching process has branching survival probability by the binomial branching survival correction. Its branching process conditioned on extinction has mean and total-progeny expected value . Therefore . Since and , this yields the matching upper bound. Controlling rare large components is necessary to conclude an expected value asymptotic from a typical-size statement.
Best response 2026-10-03
A best response is a strategy that maximizes a player's expected payoff when the other players' strategies are held fixed.
Branching process conditioned on extinction 2026-10-07
Let be the branching extinction probability of a Galton-Watson process with offspring probability generating function . Conditional on extinction, the probability of children is multiplied by : every child's descendants must also become extinct. Hence the new probability generating function is and its mean is . If , the total progeny of a branching process has conditional expected value , and unconditionally . The Markov inequality gives a finite-total-progeny tail bound without discarding the survival mass.
Bühlmann credibility premium Created 2026-10-06 Updated 2026-10-07
Cameron-Martin theorem for a Gaussian measure Created 2026-10-05 Updated 2026-10-06
For with injective covariance operator of a Gaussian measure, its translated law is an equivalent probability measure to if and only if , the Cameron-Martin space of a Gaussian measure. For such ,The series has mean-square convergence and converges almost surely under , with normal distribution . Its exponential density has expected value one by the moment-generating function of a normal distribution. Finite-dimensional projections give the formula by ratios of multivariate normal densities; convergence of these likelihood ratios gives the infinite-dimensional result. The expression is only formal when the sample is outside . For , translation gives mutually singular measures.
Capped geometric waiting time 2026-10-07
For a positive-integer geometric distribution with , the capped time has masses for and at . The last mass includes all later arrivals, not only . Its probability generating function and expected value areThe expectation follows either by differentiating the PGF or summing the tail probabilities up to .
Caro-Wei bound 2026-10-06
For a finite simple graph, . Randomly order its vertices and retain each vertex preceding all its graph neighbours. This gives an independent set with the first expression as its expected value. The second inequality is the Cauchy-Schwarz inequality.
Centered truncation of a Wigner matrix 2026-10-07
Truncate the unscaled entries of a Wigner matrix at a fixed threshold and subtract their expected values. The difference between original and truncated entries is with , so its variance is bounded by . The centering term cannot be discarded for an asymmetric entry law.
Claim count distribution 2026-10-07
The probability distribution of the nonnegative integer number of claims over a specified accounting period. Its probability generating function determines the count probabilities. A Poisson distribution gives equal count expected value and variance; a Poisson mixture allows heterogeneity in the underlying risk intensity.
Concentration inequality Created 2026-09-24 Updated 2026-09-24
A concentration inequality bounds the probability that a random variable differs substantially from a typical value such as its expected value or median.
Convergence in L1 2026-10-05
Convergence in L1 means that the expected value of the absolute error tends to zero. It implies convergence in probability and convergence of expected values.
Credibility estimate 2026-10-07
A credibility estimate combines a risk's individual experience with population information. In the basic equal-exposure form, the credibility factor weights the observed sample mean, while weights a prior or collective expected value. The Bühlmann credibility premium is the best affine estimate under mean squared error; an exact Bayesian posterior mean can also have this form, as in the natural conjugate credibility identity.
Credibility factor Created 2026-10-06 Updated 2026-10-07
The credibility factor in the Bühlmann model is the weight placed on the sample mean after observations. The remaining weight is placed on the population expected value. More experience or larger variance of hypothetical means increases ; larger expected process variance decreases it.
Cumulant 2026-10-05
The th cumulant is the coefficient of in the cumulant-generating function. The first two cumulants are the expected value and variance; the third is the third central moment.
Curie–Weiss model Created 2026-10-05 Updated 2026-10-06
The zero-field ferromagnetic Curie–Weiss model is an Ising model on spins with an equal interaction between every pair. For and , its normalized probability mass function is . The partition function sums these weights over all configurations. The square includes constant diagonal terms; these affect only normalization. Spin inversion symmetry makes every spin's expected value zero, while grouping configurations by their spin magnetization givesHere , .