The mean squared distance between two independent copies and nonzero-variance bounds #
Let f be a square-integrable function, with values in a real Hilbert space, on a finite measure
space (α, μ). Then
∫∫ ‖f x - f y‖² dμ(x) dμ(y) = 2 (μ(α) ∫ ‖f‖² dμ - ‖∫ f dμ‖²).
For a probability measure the right-hand side is twice the variance ∫ ‖f‖² dμ - ‖∫ f dμ‖² of
f, the trace of its covariance: the mean squared distance between two independent samples of f
is twice its variance. Expanding ‖u - v‖² = ‖u‖² + ‖v‖² - 2 ⟪u, v⟫, the cross term integrates
to ‖∫ f dμ‖² because the two coordinates are integrated separately.
This identity is what turns the strong-convexity remainder of an interaction energy along a transport plan, an integral over pairs of transported pairs, into the variance of the displacement.
The file also records the elementary bound of the mean of a real function by the square root of
its second moment (the nonnegativity of its variance), together with two consequences of nonzero
variance Var[X; μ] ≠ 0: strict positivity of the expectation of an ℝ≥0-valued random variable
on a finite measure space, and nondegeneracy μ {ω | X ω = 0} < 1 of a real-valued random
variable on a probability space.
Main statements #
MeasureTheory.MemLp.integrable_norm_sub_sq_prod: forf ∈ L²(μ)and a finite measureμ, the function(x, y) ↦ ‖f x - f y‖²is integrable forμ ⊗ μ.TauCeti.integral_norm_sub_sq_prod: the identity above.MeasureTheory.integral_le_sqrt_integral_sq: on a probability space, the mean of a real square-integrable function is at most the square root of its second moment, which is the nonnegativity of its variance.MeasureTheory.MeasurePreserving.evariance_fun_comp: the variance is invariant under composition with a measure-preserving measurable embedding.ProbabilityTheory.tendsto_variance_of_tendsto_eLpNorm_sub: variance is continuous under L² convergence on a finite measure space.TauCeti.Probability.evariance_integral_prod_leandTauCeti.Probability.evariance_prod_le: product-variance bounds for averages and products.TauCeti.Probability.variance_weighted_coordinate_sumandTauCeti.Probability.measure_weighted_coordinate_sum_sub_mean_ge: variance and Chebyshev bounds for weighted sums of pairwise independent variables.TauCeti.integral_coe_pos_of_variance_ne_zero: on a finite measure space, anℝ≥0-valued random variable with nonzero variance has strictly positive expectation.TauCeti.measure_setOf_eq_zero_lt_one_of_variance_ne_zero: on a probability space, a real-valued random variable with nonzero variance satisfiesμ {ω | X ω = 0} < 1.
The variance is continuous under L² convergence on a finite measure space.
For a square-integrable function f on a finite measure space, (x, y) ↦ ‖f x - f y‖² is
integrable for the product of the measure with itself.
On a probability space, the mean of a square-integrable function is at most the square root of its second moment.
The mean squared distance between two independent copies. For a square-integrable function
f with values in a real Hilbert space and a finite measure μ,
∫∫ ‖f x - f y‖² dμ(x) dμ(y) = 2 (μ(α) ∫ ‖f‖² dμ - ‖∫ f dμ‖²). For a probability measure this is
twice the variance of f.
A nonnegative random variable on a finite measure space with nonzero variance has strictly positive real expectation.
On a probability space, a real-valued random variable with nonzero variance is not almost surely zero.
The variance is invariant under composition with a measure-preserving measurable embedding.
The variance of a weighted sum of pairwise independent square-integrable variables.
Chebyshev's bound for a weighted sum of pairwise independent variables.
Jensen's inequality for the variance of an average: the variance of the average over the second coordinate is at most the average over the second coordinate of the variances in the first coordinate.
The two-factor Efron--Stein inequality.
The variance of f in coordinate i, with the other coordinates frozen at x, is a
measurable function of x.