1999 European School of High-Energy Physics: Časta-Papiernička, Slovak Republic, 22 August-4 September 1999 : ProceedingsA. Olchevski |
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Results 1-3 of 45
Page 312
... gluon emission diagrams . For the real gluon contributions , it is convenient to write the three - body phase space integration as dP3 ~ da dß dy d1d2 , ( 17 ) where a , ẞ , y are Euler angles , and x1 = 2Eq / √s and x2 = 2Eq / √s are ...
... gluon emission diagrams . For the real gluon contributions , it is convenient to write the three - body phase space integration as dP3 ~ da dß dy d1d2 , ( 17 ) where a , ẞ , y are Euler angles , and x1 = 2Eq / √s and x2 = 2Eq / √s are ...
Page 333
... gluon . To obtain information on the gluon distribution at large x , input from other processes is needed . For example , in prompt photon production in hadron - hadron ( pN ) collisions the gluon enters at leading order via the QCD ...
... gluon . To obtain information on the gluon distribution at large x , input from other processes is needed . For example , in prompt photon production in hadron - hadron ( pN ) collisions the gluon enters at leading order via the QCD ...
Page 382
... gluons between the ūd pair and between all constituents of the B and D mesons are included . Recall the factorization idea in Eq . ( 65 ) . Gluon corrections across the exchange can be parametrized by a contribution F1ɛ1 ( μ ) . The ...
... gluons between the ūd pair and between all constituents of the B and D mesons are included . Recall the factorization idea in Eq . ( 65 ) . Gluon corrections across the exchange can be parametrized by a contribution F1ɛ1 ( μ ) . The ...
Contents
Field Theory and the Standard Model | 1 |
Astrophysics and cosmology | 109 |
Determination of cosmological parameters | 126 |
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