scholarly journals Hadroproduction of Massive Lepton Pairs and QCD

Author(s):  
Edmond L. Berger
Keyword(s):  
1980 ◽  
Vol 21 (7) ◽  
pp. 2034-2035 ◽  
Author(s):  
Enrico C. Poggio ◽  
Howard J. Schnitzer

2012 ◽  
Vol 716 (1) ◽  
pp. 82-102 ◽  
Author(s):  
S. Chatrchyan ◽  
V. Khachatryan ◽  
A.M. Sirunyan ◽  
A. Tumasyan ◽  
W. Adam ◽  
...  
Keyword(s):  

2011 ◽  
Vol 2011 (10) ◽  
Author(s):  
Alan J. Barr ◽  
Sky T. French ◽  
James A. Frost ◽  
Christopher G. Lester
Keyword(s):  

2018 ◽  
Vol 177 ◽  
pp. 04010 ◽  
Author(s):  
V. Shalaev ◽  
I. Gorbunov ◽  
S. Shmatov

In this paper we review the results of a measurement of the forward-backward asymmetry of oppositely charged lepton pairs produced via Z/γ* boson in pp collisions during the LHC Run 1 at √s = 8 TeV with integrated luminosity 19.1 fb-1 (2012). We also present our preliminary results obtained with Monte Carlo samples at √s = 13 TeV


2014 ◽  
Vol 32 (4) ◽  
pp. 537-548 ◽  
Author(s):  
Frans Olofson ◽  
Leif Holmlid

AbstractLaser-induced fusion in ultra-dense deuterium D(-1) is reported in several studies from our group, using ns- and ps-pulsed lasers. The ejection of ultra-dense hydrogen particles with thermal distributions and energy up to 20 MeV u−1 was studied previously by time-of-flight measurements. The investigations of the new processes continue now by studying the interaction of these particles with metal surfaces. In the present experiments, such particles penetrate in two steps through 1 mm of metal and reach three levels of collectors at distances up to 1 m. Only the fastest particles penetrate and move to the next level. The thermal time-of-flight distributions together with tests with strong magnetic fields exclude electrons as the particles observed. The sign of the signals to the metal collectors depends on the bias (negative bias gives positive signal and conversely) while the time variations of the signals for positive and negative bias are similar. The rapid variation of the signals indicates electrons and positrons ejected from the collectors, thus lepton-pair production. An increase in bias up to ± 400 V increases the peak signal up to 1 A with no observed limiting. A thick metal plate removes slow particles and most gamma photons. The number of lepton-pairs produced is > 4 × 1012 sr−1 in the forward direction per laser shot.


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