modified struve function (Struve Labs)
90
Structured Review
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modified struve function
Modified Struve Function, supplied by Struve Labs, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
https://www.bioz.com/product/struve+function+k0/modified+struve+function/pmc08791053-91-106-106
Average 90 stars, based on 1 article reviews
Modified Struve Function, supplied by Struve Labs, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
https://www.bioz.com/product/struve+function+k0/modified+struve+function/pmc08791053-91-106-106
Average 90 stars, based on 1 article reviews
modified struve function - by Bioz Stars,
2026-11
90/100 stars
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other:Article Title: X-ray powder diffraction in education. Part II. Intensity of a powder pattern Article Snippet: A reasonable approximation for an absorption correction factor has been given by Sabine et al. (1998 ): with The absorption factors A L at the Laue conditionand A B at the Bragg conditionare given by and B n ( z ) is the the modified Bessel function of the first kind, which for integer n is defined as The modified Article Title: Integral-equation approach to resonances in circular two-layer flows around an island with bottom topography Article Snippet: This paper presents an integral-equation approach to the linear instability problem of two-layer quasi-geostrophic flows around circular islands with radial offshore bottom slope.. The flows are composed of concentric uniform potential-vorticity (PV) rings in each layer, with the PV of each ring being opposite in sign.. The study extends an earlier similar barotropic model and focuses on the degree to which the topographic waves resonate with the deformation waves at the rings’ peripheries. Modification:Article Title: Discrete Lebedev’s index transforms Article Snippet: .. II, Entries 2.16.3.1, 2.16.3.6) (1.4)an = 2 cosh( n∕2) ∫ ∞ 0 Kin∕2(y) [ Iin∕2(y) + I−in∕2(y) ] f (y)dy, n ∈ N, (1.5)an = 1 2 ∫ ∞ 0 K2 in∕2 (y)f (y)dy, n ∈ N, (1.6)f (x) = π 2 ∞∑ n=1 an cosh(πn∕2) Kin∕2(x) [ Iin∕2(x) + I−in∕2(x) ] , x > 0, (1.7)f (x) = 1 2 ∞∑ n=1 anK 2 in∕2 (x), x > 0. (1.8)Kν(z) = ∫ ∞ 0 e−z cosh(u) cosh(νu)du, Rez > 0, Article Title: Discrete Lebedev’s index transforms Article Snippet: .. 1 3 Noting the integral representation for the modified Article Title: On the Distribution of the Information Density of Gaussian Random Vectors: Explicit Formulas and Tight Approximations Article Snippet: .. To begin with, we define two functions appearing in the series representations ( ) and , which involve the modified Bessel function K α of second kind and order α and the modified Article Title: Run-and-tumble particles in two dimensions: Marginal position distributions Article Snippet: .. For this purpose, we rewrite Eq. (77) in terms of the Cartesian coordinates as P (x, y, t ) = e−γ t [ δ( √ x2 + y2 − v0t ) 2π √ x2 + y2 + γ e ( γ v0 √ v20 t 2−x2−y2 ) 2πv0 √ v20t 2 − x2 − y2 (v0t − √ x2 + y2) ] . (78) The marginal distribution of x is obtained by integrating over y, P(x, t ) = ∫ ∞−∞ dy P (x, y, t ), which yields P(x, t ) = e−γ t [ γ 2v0 ( L0 ( γ v0 W (x) ) + I0( γv0 W (x)) ) + 1 πW (x) ] (79) where W (x) = √ v20t 2 − x2 ; I0 is the the modified Bessel func- tion of the first kind, and L0 is the modified Article Title: Spatial vibrations suppressing resonant tunneling Article Snippet: The dynamics of resonant tunneling via a spatially oscillating narrow well is investigated.. The well generates a quasiresonance state, which can trap the incoming particles.. Four spectral regimes are found: (1) the adiabatic regime, when the vibrations’ frequency is lower than the spectral width of the resonance. Article Title: Flow around topological defects in active nematic films Article Snippet: .. The y -component vanishes due to symmetry considerations, and the x -component is given by 3.1 u x a ( 0 ) = 2 |