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    Application of27Al NMR techniques to structure determination in solids

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    Measurement of the total cross section and ρ\rho -parameter from elastic scattering in pp collisions at s=13\sqrt{s}=13 TeV with the ATLAS detector

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    International audienceIn a special run of the LHC with ÎČ⋆=2.5\beta ^{\star } = 2.5 km, proton–proton elastic-scattering events were recorded at s=13\sqrt{s} = 13 TeV with an integrated luminosity of 340~\upmu {\text {b}}^{-1} using the ALFA subdetector of ATLAS in 2016. The elastic cross section was measured differentially in the Mandelstam t variable in the range from −t=2.5⋅10−4-t = 2.5 \cdot 10^{-4} GeV2^{2} to −t=0.46-t = 0.46 GeV2^{2} using 6.9 million elastic-scattering candidates. This paper presents measurements of the total cross section σtot\sigma _{\text {tot}}, parameters of the nuclear slope, and the ρ\rho -parameter defined as the ratio of the real part to the imaginary part of the elastic-scattering amplitude in the limit t→0t \rightarrow 0. These parameters are determined from a fit to the differential elastic cross section using the optical theorem and different parameterizations of the t-dependence. The results for σtot\sigma _{\text {tot}} and ρ\rho are σtot(pp→X)=104.7±1.1   mb ,ρ=0.098±0.011.\begin{aligned} \sigma _{\text {tot}}(pp\rightarrow X) = 104.7 \pm 1.1 \; \text{ mb },\quad \rho = 0.098 \pm 0.011 . \end{aligned}The uncertainty in σtot\sigma _{\text {tot}} is dominated by the luminosity measurement, and in ρ\rho by imperfect knowledge of the detector alignment and by modelling of the nuclear amplitude
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