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Measurement of inelastic, single- and double-diffraction cross sections in proton–proton collisions at the LHC with ALICE

机译:用ALICE测量LHC在质子-质子碰撞中的非弹性,单衍射和双衍射截面

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Measurements of cross sections of inelastic and diffractive processes in proton–proton collisions at LHC energies were carried out with the ALICE detector. The fractions of diffractive processes in inelastic collisions were determined from a study of gaps in charged particle pseudorapidity distributions: for single diffraction (diffractive mass MX<200 GeV/c2) (sigma_{mathrm{SD}}/sigma_{mathrm {INEL}} = 0.21 pm 0.03, 0.20^{+0.07}_{-0.08}), and (0.20^{+0.04}_{-0.07}), respectively at centre-of-mass energies (sqrt{s} = 0.9, 2.76mbox{, and }7~mbox{TeV}); for double diffraction (for a pseudorapidity gap Δη>3) σDD/σINEL=0.11±0.03,0.12±0.05, and (0.12^{+0.05}_{-0.04}), respectively at (sqrt{s} = 0.9, 2.76mbox{, and }7~mbox{TeV}). To measure the inelastic cross section, beam properties were determined with van der Meer scans, and, using a simulation of diffraction adjusted to data, the following values were obtained: (sigma_{mathrm{INEL}} = 62.8^{+2.4}_{-4.0} (mathrm{model}) pm1.2 (mathrm{lumi}))?mb at (sqrt{s} = 2.76 mbox{TeV}) and (73.2^{+2.0}_{-4.6} (mathrm{model}) pm2.6 (mathrm{lumi})~mbox{mb}) at (sqrt{s} = 7 mbox{TeV}). The single- and double-diffractive cross sections were calculated combining relative rates of diffraction with inelastic cross sections. The results are compared to previous measurements at proton–antiproton and proton–proton colliders at lower energies, to measurements by other experiments at the LHC, and to theoretical models.
机译:用ALICE检测器测量LHC能量下质子-质子碰撞中非弹性和衍射过程的横截面。通过研究带电粒子假快速分布中的间隙来确定非弹性碰撞中的衍射过程分数:对于单衍射(衍射质量MX <200 GeV / c2)(sigma_ {mathrm {SD}} / sigma_ {mathrm {INEL}}分别在质心能量处(sqrt {s} = 0.9,2.76)= 0.21 pm 0.03,0.20 ^ {+ 0.07} _ {-0.08})和(0.20 ^ {+ 0.04} _ {-0.07}) mbox {和} 7〜mbox {TeV});分别用于(sqrt {s} = 0.9,2.76)的双衍射(对于伪快速间隙Δη> 3)σDD/σINEL= 0.11±0.03,0.12±0.05和(0.12 ^ {+ 0.05} _ {-0.04}) mbox {和} 7〜mbox {TeV})。为了测量非弹性横截面,使用van der Meer扫描确定了梁的性能,并使用调整为数据的衍射模拟获得了以下值:(sigma_ {mathrm {INEL}} = 62.8 ^ {+ 2.4} _ {-4.0}(mathrm {model})pm1.2(mathrm {lumi}))?mb at(sqrt {s} = 2.76 mbox {TeV})and(73.2 ^ {+ 2.0} _ {-4.6}(mathrm {model})pm2.6(mathrm {lumi})〜mbox {mb}),位于(sqrt {s} = 7 mbox {TeV})。结合相对衍射率和非弹性横截面计算出单衍射和双衍射截面。将结果与以前在较低能量下质子-反质子和质子-质子对撞机上的测量结果,大型强子对撞机上其他实验的测量结果以及理论模型进行了比较。

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