TheoremBase

The ZkZ_k are replaced by the YkY_k one at a time; at each step a second-order Taylor expansion around the sum of the other terms, independent of the replaced pair, cancels the first- and second-order terms in expectation, and the remainders are bounded by a2a^2 g; the steps telescope.

Proof

Integrability. Let k∈[n]k\in[n] and X∈{Yk,Zk}X\in\{Y_{k},Z_{k}\}. Then g(X)=min⁑{M2X2,12M3a∣X∣3}g(X)=\min\{M_{2}X^{2},\tfrac12M_{3}a|X|^{3}\} is a random variable (here and below, the functions y↦M2y2y\mapsto M_{2}y^{2}, y↦12M3a∣y∣3y\mapsto\tfrac12M_{3}a|y|^{3} and yβ†¦βˆ£y∣y\mapsto|y| on R\mathbb{R} exist by Maps and Relations Given by Formulas (i), sums, products and Borel functions of measurable real functions are measurable, and finite sums in R\mathbb{R} are rearranged and compared termwise: Arithmetic of Measurable Real- and [0,∞]-Valued Maps (i), Arithmetic of Measurable Real- and [0,∞]-Valued Maps (ii), Measurable Maps: Generators, Composition, Continuous Maps, Restrictions, and Criteria for Real- and [0,∞]-Valued Maps (iv), Random Vectors: Coordinates, Functions, Pairs and Almost-Sure Equality (ii), Finite Sums in a Commutative Ring and in an Ordered Field: Distributivity, Differences, Telescoping, Constant Terms, Comparison and the Triangle Inequality (i), Finite Sums in a Commutative Ring and in an Ordered Field: Distributivity, Differences, Telescoping, Constant Terms, Comparison and the Triangle Inequality (v)), and 0≀g(X)≀M2X20\le g(X)\le M_{2}X^{2}, since M2β‰₯∣fβ€²β€²(0)∣β‰₯0M_{2}\ge|f''(0)|\ge0 and likewise M3β‰₯0M_{3}\ge0. As X∈L2(P)X\in\mathcal{L}^{2}(P), X2X^{2} is integrable (Rules for Expectations, Variances and Covariances (vii)), so g(X)g(X) is integrable (Linearity and Monotonicity of the Lebesgue Integral, and the Integrability Criterion (v)). This proves (i).

Interpolating sums. Let U0=aβˆ‘k=1nZkU_{0}=a\sum_{k=1}^{n}Z_{k} and, recursively,

Uj=Ujβˆ’1+aYjβˆ’aZj(j∈[n]),U_{j}=U_{j-1}+aY_{j}-aZ_{j}\qquad(j\in[n]),

and let Vj=Ujβˆ’1βˆ’aZjV_{j}=U_{j-1}-aZ_{j} for j∈[n]j\in[n] (j↦Ujj\mapsto U_{j} is a function on {0,1,…,n}\{0,1,\dots,n\} by Iterating a Binary Operation along a Finite List (i), applied to sums in RΞ©\mathbb{R}^{\Omega}; j↦Vjj\mapsto V_{j} is one on [n][n], and j↦Ef(Uj)j\mapsto\mathbb{E}f(U_{j}) one on {0,1,…,n}\{0,1,\dots,n\}, by Maps and Relations Given by Formulas (i)). These are random variables, and for j∈[n]j\in[n]

Uj=Vj+aYj,Ujβˆ’1=Vj+aZj.U_{j}=V_{j}+aY_{j},\qquad U_{j-1}=V_{j}+aZ_{j}.

Finite sums of random variables are evaluated pointwise, (aβˆ‘k=1nZk)(Ο‰)=aβˆ‘k=1nZk(Ο‰)\bigl(a\sum_{k=1}^{n}Z_{k}\bigr)(\omega)=a\sum_{k=1}^{n}Z_{k}(\omega) for Ο‰βˆˆΞ©\omega\in\Omega, by the uniqueness in Iterating a Binary Operation along a Finite List (i). For fixed j∈[n]j\in[n], let mjm_{j} be the function on [n][n] with mj(l)=aYlm_{j}(l)=aY_{l} for l<jl<j, mj(j)=0m_{j}(j)=0 and mj(l)=aZlm_{j}(l)=aZ_{l} for l>jl>j (Maps and Relations Given by Formulas (i)), and let sj=βˆ‘l=1jβˆ’1aZls_{j}=\sum_{l=1}^{j-1}aZ_{l} be the partial sum over l<jl<j (Iterated Operations: Finite Sums and Finite Products (iii), Iterated Operations: Finite Sums and Finite Products (ii)). Telescoping the recursion (Finite Sums in a Commutative Ring and in an Ordered Field: Distributivity, Differences, Telescoping, Constant Terms, Comparison and the Triangle Inequality (iii), Finite Sums in a Commutative Ring and in an Ordered Field: Distributivity, Differences, Telescoping, Constant Terms, Comparison and the Triangle Inequality (ii), Finite Sums in a Commutative Ring and in an Ordered Field: Distributivity, Differences, Telescoping, Constant Terms, Comparison and the Triangle Inequality (i)) gives Ujβˆ’1=U0βˆ’sj+βˆ‘l=1jβˆ’1aYlU_{j-1}=U_{0}-s_{j}+\sum_{l=1}^{j-1}aY_{l}, and hence Vj=Ujβˆ’1βˆ’aZj=βˆ‘l=1nmj(l)V_{j}=U_{j-1}-aZ_{j}=\sum_{l=1}^{n}m_{j}(l); for j=1j=1 the recursion is not used, since V1=U0βˆ’aZ1V_{1}=U_{0}-aZ_{1} directly. Evaluated at each Ο‰\omega, this is the closed form: for j∈[n]j\in[n] and Ο‰βˆˆΞ©\omega\in\Omega,

Vj(Ο‰)=a(βˆ‘k=1jβˆ’1Yk(Ο‰)+βˆ‘k=j+1nZk(Ο‰)),Un=aβˆ‘k=1nYk,V_{j}(\omega)=a\Bigl(\sum_{k=1}^{j-1}Y_{k}(\omega)+\sum_{k=j+1}^{n}Z_{k}(\omega)\Bigr),\qquad U_{n}=a\sum_{k=1}^{n}Y_{k},

empty sums being 00.

The sum VjV_{j} is independent of YjY_{j} and of ZjZ_{j}. Fix j∈[n]j\in[n], let Jj=[2n]βˆ–{j,n+j}J_{j}=[2n]\setminus\{j,n+j\} and let Hj=Οƒ(⋃i∈JjΟƒ(Wi))\mathcal{H}_{j}=\sigma\bigl(\bigcup_{i\in J_{j}}\sigma(W_{i})\bigr). The family (Οƒ(Wi))i∈[2n](\sigma(W_{i}))_{i\in[2n]} is independent (Independence of Events and of Random Elements (ii)), so by Independence of Οƒ-Algebras: Ο€-Systems, Grouping and Pairs (iii), applied to the disjoint index sets JjJ_{j} and {j}\{j\}, and to JjJ_{j} and {n+j}\{n+j\}, together with Independence of Οƒ-Algebras: Ο€-Systems, Grouping and Pairs (iv), Hj\mathcal{H}_{j} is independent of Οƒ(Yj)\sigma(Y_{j}) and of Οƒ(Zj)\sigma(Z_{j}) (the Οƒ\sigma-algebra generated by Οƒ(Wi)\sigma(W_{i}) being Οƒ(Wi)\sigma(W_{i}) itself). Every WiW_{i} with i∈Jji\in J_{j} is Hj\mathcal{H}_{j}-measurable (The Οƒ-Algebra Generated by Measurable Functions into Metric Spaces (ii)), hence so is VjV_{j}, by its closed form, and Οƒ(Vj)βŠ†Hj\sigma(V_{j})\subseteq\mathcal{H}_{j} (The Οƒ-Algebra Generated by Measurable Functions into Metric Spaces (i)). The product formula of Independence of Classes of Events and of Οƒ-Algebras (iii) for Hj\mathcal{H}_{j} and Οƒ(Yj)\sigma(Y_{j}) holds in particular on Οƒ(Vj)\sigma(V_{j}), so VjV_{j} and YjY_{j} are independent (Independence of Events and of Random Elements (iii)), and likewise VjV_{j} and ZjZ_{j}. Since fβ€²f' and fβ€²β€²f'' are differentiable, they are continuous (The Increment Form of the Derivative, and Differentiability Implies Continuity (ii), R\mathbb{R} being an interval by Basic Facts about Intervals of the Real Line (i)) and hence Borel, as is y↦y2y\mapsto y^{2}; so, by Independent Random Elements: Preimages, Functions and Blocks (iv), for X∈{Yj,Zj}X\in\{Y_{j},Z_{j}\}

fβ€²(Vj)Β andΒ XΒ areΒ independent,fβ€²β€²(Vj)Β andΒ X2Β areΒ independent.f'(V_{j})\text{ and }X\text{ are independent},\qquad f''(V_{j})\text{ and }X^{2}\text{ are independent}.

One replacement. For v,h∈Rv,h\in\mathbb{R} let

R(v,h)=f(v+h)βˆ’f(v)βˆ’fβ€²(v)hβˆ’12fβ€²β€²(v)h2.R(v,h)=f(v+h)-f(v)-f'(v)h-\tfrac12f''(v)h^{2}.

By A Bound on the Second-Order Taylor Remainder by the Second and Third Derivatives (i) and a>0a>0, for all v,y∈Rv,y\in\mathbb{R},

∣R(v,ay)βˆ£β‰€min⁑{M2a2y2,12M3a3∣y∣3}=a2g(y).|R(v,ay)|\le\min\bigl\{M_{2}a^{2}y^{2},\tfrac12M_{3}a^{3}|y|^{3}\bigr\}=a^{2}g(y).

Fix j∈[n]j\in[n] and X∈{Yj,Zj}X\in\{Y_{j},Z_{j}\}, and write V=VjV=V_{j}. Pointwise on Ω\Omega,

f(V+aX)=f(V)+a fβ€²(V)X+12a2fβ€²β€²(V)X2+R(V,aX).f(V+aX)=f(V)+a\,f'(V)X+\tfrac12a^{2}f''(V)X^{2}+R(V,aX).

The random variables f(V+aX)f(V+aX), f(V)f(V), fβ€²(V)f'(V) and fβ€²β€²(V)f''(V) are integrable, being Borel functions of random variables bounded by MM (Rules for Expectations, Variances and Covariances (ii), Linearity and Monotonicity of the Lebesgue Integral, and the Integrability Criterion (v); ff is continuous by The Increment Form of the Derivative, and Differentiability Implies Continuity (ii), R\mathbb{R} being an interval by Basic Facts about Intervals of the Real Line (i)). Moreover XX is integrable with EX=0\mathbb{E}X=0, and X2X^{2} is integrable with E[X2]=1\mathbb{E}[X^{2}]=1. By the independence just shown and Expectations and Variances of Independent Random Variables (i), fβ€²(V)Xf'(V)X and fβ€²β€²(V)X2f''(V)X^{2} are integrable and

E[fβ€²(V)X]=Efβ€²(V) EX=0,E[fβ€²β€²(V)X2]=Efβ€²β€²(V) E[X2]=Efβ€²β€²(V).\mathbb{E}[f'(V)X]=\mathbb{E}f'(V)\,\mathbb{E}X=0,\qquad\mathbb{E}[f''(V)X^{2}]=\mathbb{E}f''(V)\,\mathbb{E}[X^{2}]=\mathbb{E}f''(V).

So R(V,aX)R(V,aX) is integrable, being a linear combination of the integrable terms above, and by linearity (Rules for Expectations, Variances and Covariances (iii))

Ef(V+aX)=Ef(V)+12a2 Efβ€²β€²(V)+ER(V,aX).\mathbb{E}f(V+aX)=\mathbb{E}f(V)+\tfrac12a^{2}\,\mathbb{E}f''(V)+\mathbb{E}R(V,aX).

Taking X=YjX=Y_{j} and X=ZjX=Z_{j} and subtracting, the first two terms cancel:

Ef(Uj)βˆ’Ef(Ujβˆ’1)=ER(Vj,aYj)βˆ’ER(Vj,aZj).\mathbb{E}f(U_{j})-\mathbb{E}f(U_{j-1})=\mathbb{E}R(V_{j},aY_{j})-\mathbb{E}R(V_{j},aZ_{j}).

Since ∣R(Vj,aX)βˆ£β‰€a2g(X)|R(V_{j},aX)|\le a^{2}g(X) pointwise, and g(X)g(X) is integrable by (i),

∣ER(Vj,aX)βˆ£β‰€E∣R(Vj,aX)βˆ£β‰€a2 Eg(X)|\mathbb{E}R(V_{j},aX)|\le\mathbb{E}|R(V_{j},aX)|\le a^{2}\,\mathbb{E}g(X)

(Rules for Expectations, Variances and Covariances (v), Rules for Expectations, Variances and Covariances (iv), Rules for Expectations, Variances and Covariances (iii)). Hence

∣Ef(Uj)βˆ’Ef(Ujβˆ’1)βˆ£β‰€a2(Eg(Yj)+Eg(Zj))(j∈[n]).\bigl|\mathbb{E}f(U_{j})-\mathbb{E}f(U_{j-1})\bigr|\le a^{2}\bigl(\mathbb{E}g(Y_{j})+\mathbb{E}g(Z_{j})\bigr)\qquad(j\in[n]).

Telescoping. Let dj=Ef(Ujβˆ’1)d_{j}=\mathbb{E}f(U_{j-1}) for j∈[n+1]j\in[n+1]; this is a function on [n+1][n+1], since k↦k+1k\mapsto k+1 maps {0,1,…,n}\{0,1,\dots,n\} onto [n+1][n+1], and for j∈[n]j\in[n] both jj and j+1j+1 lie in [n+1][n+1] (Intervals of Natural Numbers: Initial Segments, Adding One Element, Splitting and Shifting (iv), Intervals of Natural Numbers: Initial Segments, Adding One Element, Splitting and Shifting (ii)). By Finite Sums in a Commutative Ring and in an Ordered Field: Distributivity, Differences, Telescoping, Constant Terms, Comparison and the Triangle Inequality (iii),

Ef(Un)βˆ’Ef(U0)=dn+1βˆ’d1=βˆ‘j=1n(dj+1βˆ’dj)=βˆ‘j=1n(Ef(Uj)βˆ’Ef(Ujβˆ’1)).\mathbb{E}f(U_{n})-\mathbb{E}f(U_{0})=d_{n+1}-d_{1}=\sum_{j=1}^{n}(d_{j+1}-d_{j})=\sum_{j=1}^{n}\bigl(\mathbb{E}f(U_{j})-\mathbb{E}f(U_{j-1})\bigr).

Each term of this sum lies between βˆ’Ξ΄j-\delta_{j} and Ξ΄j\delta_{j}, where Ξ΄j=∣Ef(Uj)βˆ’Ef(Ujβˆ’1)∣\delta_{j}=\bigl|\mathbb{E}f(U_{j})-\mathbb{E}f(U_{j-1})\bigr|. Summing these bounds termwise, moving the sign through the sum and pulling out the factor a2a^{2} (Finite Sums in a Commutative Ring and in an Ordered Field: Distributivity, Differences, Telescoping, Constant Terms, Comparison and the Triangle Inequality (v), Finite Sums in a Commutative Ring and in an Ordered Field: Distributivity, Differences, Telescoping, Constant Terms, Comparison and the Triangle Inequality (ii), Finite Sums in a Commutative Ring and in an Ordered Field: Distributivity, Differences, Telescoping, Constant Terms, Comparison and the Triangle Inequality (i)), and using the bound of the previous step,

∣Ef(Un)βˆ’Ef(U0)βˆ£β‰€βˆ‘j=1nΞ΄jβ‰€βˆ‘j=1na2(Eg(Yj)+Eg(Zj))=a2βˆ‘j=1n(Eg(Yj)+Eg(Zj)).\bigl|\mathbb{E}f(U_{n})-\mathbb{E}f(U_{0})\bigr|\le\sum_{j=1}^{n}\delta_{j}\le\sum_{j=1}^{n}a^{2}\bigl(\mathbb{E}g(Y_{j})+\mathbb{E}g(Z_{j})\bigr)=a^{2}\sum_{j=1}^{n}\bigl(\mathbb{E}g(Y_{j})+\mathbb{E}g(Z_{j})\bigr).

As Un=aβˆ‘k=1nYkU_{n}=a\sum_{k=1}^{n}Y_{k} and U0=aβˆ‘k=1nZkU_{0}=a\sum_{k=1}^{n}Z_{k}, this is (ii).

Citations

Loading…

Dependencies

Uses0

Loading…

Comments

Log in to comment.

Loading…