Notation can vary slightly here.
In [7, 10], Xue and Zhao-Yamada introduce the notations of a-thin (with respect to the Schrödinger operator (mathit{Sch}_{a})) at a point and a-rarefied sets at infinity (with respect to the Schrödinger operator (mathit{Sch}_{a})), which generalized the earlier notations obtained by Miyamoto, Hoshida, Brelot (see [11 14]).
In [5], Long-Gao-Deng introduce the notations of a-thin (with respect to the Schrödinger operator Sch a ) at a point, a-polar set (with respect to the Schrödinger operator Sch a ) and a-minimal thin sets at infinity (with respect to the Schrödinger operator Sch a ), which generalized earlier notations obtained by Brelot and Miyamoto (see [7, 8]).
In [7], Long et al. introduced the notations of a-thin (with respect to the Schrödinger operator Sch a ) at a point, a-polar set (with respect to the Schrödinger operator Sch a ) and a-rarefied sets at infinity (with respect to the Schrödinger operator Sch a ), which generalized earlier notations obtained by Brelot and Miyamoto (see [8, 9]).
Under the longstanding policy of the testing service, his results were mailed out with the notation, "Scores obtained under special conditions".
The matrix notation is obtained by letting (mathbf {G} = [ mathbf {g}_{1}, ldots, mathbf {g}_{K} ] in mathbb {C}^{M times K}) be the precoding matrix and (mathbf {s} = [s_{1}, ldots, s_{K}]^{text {tiny T}} sim mathcal {CN}(mathbf {0}_{Ktimes 1},mathbf {I}_{ K} ) be the vector containing all UT data symbols.
In 2005, in [15], the authors presented a new notation and obtained their abstract results by means of the methods introduced in [10] to deal with 2D Navier-Stokes equations with a normal external force in (L_{mathrm{loc}}^{2}(mathbb{R},L^{2})) which is translation bounded but not translation compact.
The 5-grade notation was obtained using the formula: L = 5- LogMAR.
The physical interpretation of l VUT (and the origin of its notation) is obtained by recalling that t convection is the time it takes for the temperature to return to its steady state value, after a short heating pulse, in the absence of heat conduction.
Based on these notations, Beardon obtained the following two main theorems.
