Abstract

The TOTEM collaboration has measured the elastic proton-proton differential cross section dσ/dt{\rm d}σ/{\rm d}t at s=13\sqrt{s}=13 TeV LHC energy using dedicated β∗=90β^{*}=90 m beam optics. The Roman Pot detectors were inserted to 10σσ distance from the LHC beam, which allowed the measurement of the range [0.04[0.04 GeV2^{2};4; 4 GeV2^{2}]] in four-momentum transfer squared ∣t∣|t|. The efficient data acquisition allowed to collect about 109^{9} elastic events to precisely measure the differential cross-section including the diffractive minimum (dip), the subsequent maximum (bump) and the large-∣t∣|t| tail. The average nuclear slope has been found to be B=(20.40±0.002stat±0.01syst) B=(20.40 \pm 0.002^{\rm stat} \pm 0.01^{\rm syst})~GeV−2^{-2} in the ∣t∣|t|-range 0.04 0.04~GeV2^{2} to 0.2 0.2~GeV2^{2}. The dip position is ∣tdip∣=(0.47±0.004stat±0.01syst) |t_{\rm dip}|=(0.47 \pm 0.004^{\rm stat} \pm 0.01^{\rm syst})~GeV2^{2}. The differential cross section ratio at the bump vs. at the dip R=1.77±0.01statR=1.77\pm0.01^{\rm stat} has been measured with high precision. The series of TOTEM elastic pp measurements show that the dip is a permanent feature of the pp differential cross-section at the TeV scale.

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