Exercise [2.1.5] Let > 0 and pick K = K( ) finite such that if k ≥ K then r(k) ≤ . Applying the Cauchy-Schwarz inequality for Xi −EXi and Xj −EXj we have that Cov(Xi, Xj) ≤ [Var(Xi)Var(Xj)] ≤ r(0) <∞ for all i, j. Thus, breaking the double sum in Var(Sn) = ∑n i,j=1 Cov(Xi, Xj) into {(i, j) : |i − j| < K} and {(i, j) : |i− j| ≥ K} gives the bound Var(Sn) ≤ 2Knr(0) + n . Dividing by n we see that...

The constant γ in the strengthened Cauchy-Bunyakowskii-Schwarz inequality is a basic tool for the construction of two-level and multilevel preconditioning matrices. Therefore many authors consider estimates or computations of this quantity. In this paper the bilinear form arising from 3D linear elasticity problems is considered on a polyhedron. The cosine of the abstract angle between multileve...

This paper follows the recent discussion on the sparse solution recovery with quasi-norms `q, q ∈ (0, 1) when the sensing matrix possesses a Restricted Isometry Constant δ2k (RIC). Our key tool is an improvement on a version of “the converse of a generalized Cauchy-Schwarz inequality” extended to the setting of quasi-norm. We show that, if δ2k ≤ 1/2, any minimizer of the lq minimization, at lea...

Quantum photonics offers much promise for the development of new technologies. The ability to control the interaction of light and matter at the level of single quantum excitations is a prerequisite for the construction of potentially powerful devices. Here we use the rotational levels of a room temperature ensemble of hydrogen molecules to couple two distinct optical modes at the single photon...

Exercise [2.1.5] Let > 0 and pick K = K( ) finite such that if k ≥ K then r(k) ≤ . Applying the Cauchy-Schwarz inequality for Xi −EXi and Xj −EXj we have that Cov(Xi, Xj) ≤ [Var(Xi)Var(Xj)] ≤ r(0) <∞ for all i, j. Thus, breaking the double sum in Var(Sn) = ∑n i,j=1 Cov(Xi, Xj) into {(i, j) : |i − j| < K} and {(i, j) : |i− j| ≥ K} gives the bound Var(Sn) ≤ 2Knr(0) + n . Dividing by n we see that...

1. Introductory remarks 1 2. Energy and area 3 3. Exact Lagrangian submanifolds and the non-squeezing theorem 7 4. Sobolev spaces 9 5. The linear Cauchy–Riemann operator 20 5.1. Proof of the Calderón–Zygmund Theorem for p , 2 26 6. Local properties of J-holomorphic curves 30 6.1. Smoothness 31 6.2. The Carleman Similarity Principle and its applications 35 6.3. Isolation of intersection points a...

The time dependence of nonclassical correlations is investigated for two fields (1,2) generated by an ensemble of cold cesium atoms via the protocol of Duan et al. [Nature (London) 414, 413 (2001)]]. The correlation function R(t1,t2) for the ratio of cross to autocorrelations for the (1,2) fields at times (t1,t2) is found to have a maximum value R(max=292+/-57, which significantly violates the ...

H ·H := ̆ h = fg : f, g ∈ H ̄ = H ←↩ H is the product space of H2, by inner/outer factorization and Cauchy-Schwarz inequality. It is interesting, then, to find the dual space of H1. C. Fefferman [7] proved that, under the H2 paring (with some care), (H2 ·H2)∗ = (H1)∗ = BMO∩H(D) is the space of the analytic functions with bounded mean oscillation. The definition of BMO, born out of a problem in el...

Rays are classes of an equivalence relation on a module V over supertropical semiring. They provide version convex geometry, supported by ‘supertropical trigonometry’ and compatible with quasilinearity, in which the CS-ratio takes role Cauchy–Schwarz inequality. CS-functions that emerge from useful tool helps to understand variety quasilinear stars ray space Ray(V). In particular, these functio...

We use the intrinsic area to define a distance on space of homothety classes convex bodies in $n$-dimensional Euclidean space, which makes it isometric subset infinite dimensional hyperbolic space. The ambient Lorentzian structure is an extension form bodies, and Alexandrov–Fenchel inequality interpreted as reversed Cauchy–Schwarz inequality. deduce that similarity has proper geodesic with curv...