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On the other hand, there is certainly nevertheless no NLO calculation for J/ production in deep inelastic scattering available, as, for instance, measured most not too long ago by H1 [1171]. f. Additional production observables The LHCb experiment with its especially wealthy quarkonium program has also measured absolutely new observables which nonetheless must be exploited totally in theory tests: For the very first time in pp collisions the double J/ production cross section was measured [1172], as well because the production of J/ in association with charmed mesons [1173]. Like double charmonium production, J/ + cc was previously only measured at the B factories, latest inside the Belle analysis [1174], which was vital for testing J/ production mechanisms in e+ e- production. J/ production in association with W bosons has for the first time been measured by the ATLAS collaboration [1175]. Exclusive charmonium hadroproduction has been observed recently by CDF [1176] and LHCb [1177,1178]. Exclusive production had previously been a domain of ep experiments; see [1179] for any current update by the H1 collaboration. Yet another observable for which theory predictions exist would be the J/ production price in  scattering. This observable has previously been measured at LEP by DELPHI [1180] with extremely substantial uncertainties and could possibly be remeasured at an ILC. 4.five.2 NLO tests of NRQCD LDME universality The phenomenological relevance from the NRQCD factorization conjecture is closely tied to the question of irrespective of whether or not the LDMEs may be shown to be universal. Within this section recent operates is going to be reviewed which aim at examining this universality at Next-to-Leading Order (NLO) in s . Within the case of c J , these tests include things like just the leading [1] order of the NRQCD v expansion, formed by the n = three PJ and n = three S 1 states. In [https://dx.doi.org/10.1089/jir.2014.0026 title= jir.2014.0026] the case of three S1 quarkonia, these tests [https://dx.doi.org/10.1038/srep39151 title= srep39151] consist of the terms as much as relative order O(v 4 ) inside the [1] v expansion, namely the n = 3 S1 color singlet state, as [8] [8] [8] properly as the n = 1 S0 , three S1 , and 3 PJ Color Octet (CO) states; see Table 5. The relativistic corrections involving the [1] [1] P H (3 S1 ) and Q H (3 S1 ) LDMEs are, however, not aspect of these analyses, despite the fact that they are of order O(v two ) and O(v 4 ) in the v expansion. You'll find two reasons for that: 1st, the corresponding NLO calculations are far beyond the reach of existing tactics, and secondly, they're expected to provide substantial contributions to hadroproduction only at m c and for photoproduction only at z 1. This behavpT ior is inferred from the [https://www.medchemexpress.com/Dacomitinib.html MedChemExpress PF-00299804] behavior at LO in s [1187,1188][8]and might be understood by noting that new topologies of Feynman diagrams open up when carrying out the transition from [1] the 3 S1 state towards the CO states, but not when calculating relativistic corrections: For example, at major order in s the slope in the transverse momentum distribution in [1] -8 hadroproduction is d/dpT  pT for the three S1 state, com[8] [8] -6 pared to d/dpT  pT for the 1 S0 and 3 PJ states and [8] -4 d/dpT  pT for the 3 S1 state.
 
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Версия 05:11, 20 декабря 2017

On the other hand, there is certainly nevertheless no NLO calculation for J/ production in deep inelastic scattering available, as, for instance, measured most not too long ago by H1 [1171]. f. Additional production observables The LHCb experiment with its especially wealthy quarkonium program has also measured absolutely new observables which nonetheless must be exploited totally in theory tests: For the very first time in pp collisions the double J/ production cross section was measured [1172], as well because the production of J/ in association with charmed mesons [1173]. Like double charmonium production, J/ + cc was previously only measured at the B factories, latest inside the Belle analysis [1174], which was vital for testing J/ production mechanisms in e+ e- production. J/ production in association with W bosons has for the first time been measured by the ATLAS collaboration [1175]. Exclusive charmonium hadroproduction has been observed recently by CDF [1176] and LHCb [1177,1178]. Exclusive production had previously been a domain of ep experiments; see [1179] for any current update by the H1 collaboration. Yet another observable for which theory predictions exist would be the J/ production price in scattering. This observable has previously been measured at LEP by DELPHI [1180] with extremely substantial uncertainties and could possibly be remeasured at an ILC. 4.five.2 NLO tests of NRQCD LDME universality The phenomenological relevance from the NRQCD factorization conjecture is closely tied to the question of irrespective of whether or not the LDMEs may be shown to be universal. Within this section recent operates is going to be reviewed which aim at examining this universality at Next-to-Leading Order (NLO) in s . Within the case of c J , these tests include things like just the leading [1] order of the NRQCD v expansion, formed by the n = three PJ and n = three S 1 states. In title= jir.2014.0026 the case of three S1 quarkonia, these tests title= srep39151 consist of the terms as much as relative order O(v 4 ) inside the [1] v expansion, namely the n = 3 S1 color singlet state, as [8] [8] [8] properly as the n = 1 S0 , three S1 , and 3 PJ Color Octet (CO) states; see Table 5. The relativistic corrections involving the [1] [1] P H (3 S1 ) and Q H (3 S1 ) LDMEs are, however, not aspect of these analyses, despite the fact that they are of order O(v two ) and O(v 4 ) in the v expansion. You'll find two reasons for that: 1st, the corresponding NLO calculations are far beyond the reach of existing tactics, and secondly, they're expected to provide substantial contributions to hadroproduction only at m c and for photoproduction only at z 1. This behavpT ior is inferred from the MedChemExpress PF-00299804 behavior at LO in s [1187,1188][8]and might be understood by noting that new topologies of Feynman diagrams open up when carrying out the transition from [1] the 3 S1 state towards the CO states, but not when calculating relativistic corrections: For example, at major order in s the slope in the transverse momentum distribution in [1] -8 hadroproduction is d/dpT pT for the three S1 state, com[8] [8] -6 pared to d/dpT pT for the 1 S0 and 3 PJ states and [8] -4 d/dpT pT for the 3 S1 state.