The Yeast Ca2+-ATPases and Ca2+/H+ Exchangers of the Secretory Pathway and Their Regulation

Lévy Distributions for One-Dimensional Analysis of the Bose–Einstein Correlations

“…The similar situation is observed for nucleus-nucleus collisions: estimations for parameters of exponential function Ω C derived with (6) agree with corresponding experimental results mostly within 1σ, but the coincidence is achieved within 2σ for R C in both the Pb + Pb collisions at √ s N N = 17.3 GeV [24] and the O + Ag reactions at √ s N N = 19.4 GeV [28]. The estimations of 1D BEC parameters λ C , R C obtained for p + p with help of (7) are in qualitative agreement with corresponding experimental results [25] even for the case of unusually large chaoticity. Thus the system of equations ( 6) provides quite reasonable estimations for parameters for exponential function based on the a priori known values of 1D BEC observables for Gaussian function in various strong interaction processes at all available experimental energies.…”

“…Account the relation R G ≤ R C / √ π and properties of the functions exp(−x 2 ), erf(x) allows us to simplify Eqs. (7) to the system…”

“…the estimations within the present paper for set of Gaussian parameters {λ G , R G } agree with the results of the WA98 experiment [24] within 2σ. But there is qualitative agreement only between results of calculations with help of (7) and experimental data for p + p collisions [25]. Perhaps, this discrepancy is dominated by some features of experiment provided unusually large values of chaoticity for both the exponential and the Gaussian parameterizations of 1D CF C 2 (q).…”

“…The quite reasonable fit is achieved with this parametrization of two-pion CF in various types of multiparicle production processes [1]. But unfortunately power-law fits are absent for high-statistics modern experimental data so far [7]. On the other hand the stable (on Lévy) distributions [8] are one of the most promising tools for studies of fractal-like space-time extent of emission region.…”

“…The thin dotted lines are the ultimate levels for R1 (a,b) and λ1 (c,d) calculated with (3) for given values of the α1 and the set of parameters {α2, λ2, R2} for second Lévy parametrization. Dependence of 1D BEC radius (a,b) and strength of correlations (c,d) for Gaussian parametrization on low q1 (a,c) and high q2 (b,d) limits of integration in the system of equations(7) for fixed values of the parameters for exponential parametrization: λC = π/2 and RC = √ π fm. The solid lines correspond to the indicated values of the q2 for q1-dependence (a,c) and to shown values of the q1 for q2-dependence (b,d).…”