Inclusive Bottom Production in $p \bar{p}$ Collisions at $\sqrt{s}$ = 1.8-TeV at D0 Central Detector Region

1995 ◽  
Author(s):  
Vitor Oguri
Keyword(s):  
Author(s):  
Kun Zhang ◽  
Miao He ◽  
Weidong Li ◽  
Jilei Xu

2016 ◽  
Vol 60 (4) ◽  
pp. 561-572 ◽  
Author(s):  
Zongyi Wang ◽  
◽  
Yuangqing Wang ◽  
Yuekun Heng ◽  
Xinxi Du ◽  
...  
Keyword(s):  

1991 ◽  
Vol 38 (2) ◽  
pp. 337-343
Author(s):  
V. Filippini ◽  
T.F. Liu ◽  
G. Maron ◽  
A. Masoni ◽  
G. Vedovato

2021 ◽  
Author(s):  
Kadir Ocalan

Abstract This paper presents high-accuracy predictions for the differential cross sections as a function of the key observable φ*η of the neutral-current Drell-Yan (DY) dilepton production in proton-proton (pp) collisions. The differential distributions for the φ*η are presented by using the state-of-the-art predictions from the combined calculations of fixed-order perturbative QCD corrections at next-to-next-to-leading order (NNLO) accuracy and resummation of large logarithmic terms at next-to-next-to-leading logarithmic (NNLL) and next-to-NNLL (N3LL) accuracies, i.e., NNLO+NNLL and NNLO+N3LL, respectively. The predicted distributions are reported for a thorough set of the DY dilepton invariant mass mll ranges, spanning a wide kinematic region of 50 < mll< 1000 GeV both near and away from the Z-boson mass peak, and rapidity yll ranges in the central detector acceptance region of |yll| < 2.4. The differential φ*η distributions in the wide mll and yll ranges offer stringent tests to assess the reliability of the predictions, where the mll and yll are closely correlated with the parton distribution functions (PDFs) of the incoming partons. The merged predictions through NNLO+N3LL are observed to provide good description of the 13 TeV pp collision data for the φ*η (including the dilepton transverse momentum pll T as well) distributions in almost the entire mll and yll ranges, apart from the intermediate- to high-φ*η region in the lowest mass range 50–76 GeV which is assessed to constitute a challenge for the presented predictions. The merged predictions at NNLO+N3LL are also reported at 14 TeV for the upcoming high-luminosity running era of the LHC, in which increasing amount of data is expected to require more accurate and precise theoretical description. The most recent PDF models MSHT20 and CT18 are tested for the first time in addition to the NNPDF3.1 exploiting the merged φ*η predictions.


2020 ◽  
Vol 4 (3) ◽  
pp. 362-371
Author(s):  
Xiaoyu Yang ◽  
Lei Yang ◽  
Wei He ◽  
Yatian Pei ◽  
Yuekun Heng ◽  
...  
Keyword(s):  

Author(s):  
Xiaoyu Yang ◽  
Yuekun Heng ◽  
Huafeng Li ◽  
Xiaoyan Ma ◽  
Wei He ◽  
...  
Keyword(s):  

2016 ◽  
Vol 40 (8) ◽  
pp. 086201
Author(s):  
Tao Lin ◽  
Zi-Yan Deng ◽  
Wei-Dong Li ◽  
Guo-Fu Cao ◽  
Zheng-Yun You ◽  
...  
Keyword(s):  

2016 ◽  
Vol 40 (2) ◽  
pp. 026001 ◽  
Author(s):  
Xin-Ying Li ◽  
Zi-Yan Deng ◽  
Liang-Jian Wen ◽  
Wei-Dong Li ◽  
Zheng-Yun You ◽  
...  

2019 ◽  
Vol 64 (7) ◽  
pp. 635
Author(s):  
M. Schever

The Jiangmen Underground Neutrino Observatory (JUNO) is a next generation multipurpose antineutrino detector currently under construction in Jiangmen, China. The central detector, containing 20 kton of a liquid scintillator, will be equipped with ∼18 000 20 inch and 25 600 3 inch photomultiplier tubes. Measuring the reactor antineutrinos of two powerplants at a baseline of 53 km with an unprecedented energy resolution of 3%/√︀E(MeV), the main physics goal is to determine the neutrino mass hierarchy within six years of run time with a significance of 3–4q. Additional physics goals are the measurement of solar neutrinos, geoneutrinos, supernova burst neutrinos, the diffuse supernova neutrino background, and the oscillation parameters sin2 O12, Δm212, and |Δm2ee| with a precision <1%, as well as the search for proton decays. The construction is expected to be completed in 2021.


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