Abstract
We present the first next-to-leading-order QCD analysis of neutrino charm production, using a sample of 6090ν μ − and\(\bar \nu _\mu \)-induced opposite-sign dimuon events observed in the CCFR detector at the Fermilab Tevatron. We find that the nucleon strange quark content is suppressed with respect to the non-strange sea quarks by a factor κ=0.477 +0.063−0.053 , where the error includes statistical, systematic and QCD scale uncertainties. In contrast to previous leading order analyses, we find that the strange seax-dependence is similar to that of the non-strange sea, and that the measured charm quark mass,m c =1.70±0.19 GeV/c2, is larger and consistent with that determined in other processes. Further analysis finds that the difference inx-distributions betweenxs(x) and\(x\bar s{\text{(}}x{\text{)}}\) is small. A measurement of the Cabibbo-Kobayashi-Maskawa matrix element |V cd |=0.232 +0.018−0.020 is also presented.
Similar content being viewed by others
References
J.C. Collins, D.E. Soper and G. Sterman, in: Perturbative Quantum Chromodynamics, ed. A.H. Mueller (World Scientific, Singapore, 1989)
J. Botts et al. (CTEQ Collab.), Phys. Lett. B 304 (1993) 159
A.D. Martin, R.G. Roberts and W.J. Stirling, Phys. Lett. B 306 (1993) 145
W.K. Sakumoto et al. (CCFR Collab.), Nucl. Instrum. Methods Phys. Res. A 294 (1990) 179
B.J. King et al. (CCFR Collab.), Nucl. Instrum. Methods Phys. Res. A 302 (1991) 254
S.A. Rabinowitz et al. (CCFR Collab.), Phys. Rev. Lett. 70 (1993) 134
R. Barbieri, J. Ellis, M.K. Gaillard and G.G. Ross, Nucl. Phys. B 117 (1976) 50
M.A.G. Aivazis, F.I. Olness and W.-K. Tung, Phys. Rev. D 50 (1994) 3085
R.M. Barnett, Phys. Rev. Lett. 36 (1976) 1163; H. Georgi and H.D. Politzer, Phys. Rev. D 14 (1976) 1829
V.N. Gribov and L.N. Lipatov, Sov. J. Nucl. Phys. 15 (1972) 438; G. Altarelli and G. Parisi, Nucl. Phys. B 126 (1977) 298
S. Dasu et al., Phys. Rev. Lett. 61 (1988) 1061
M.A.G. Aivazis, F.I. Olness and W.-K. Tung, Phys. Rev. Lett. 65 (1990) 2339
M.A.G. Aivazis, J.C. Collins, F.I. Olness and W.-K. Tung, Phys. Rev. D 50 (1994) 3102
G. Kramer and B. Lampe, Z. Phys. C 54 (1992) 139
J.J. van der Bij and G.J. van Oldenborgh, Z. Phys. C 51 (1991) 477
N. Ushida et al. (E531 Collab.), Phys. Lett. B 206 (1988) 375; B 206 (1988) 380
P. Collins and T. Spiller, J. Phys. G 11 (1985) 1289
T. Sjostrand et al., Comput. Phys. Commun. 27 (1982) 243
P.H. Sandler et al. (CCFR Collab.), Z. Phys. C 57 (1993) 1
D. Bardin and N. Shumeiko, Sov. J. Nucl. Phys. 29 (1979) 499
P.Z. Quintas et al. (CCFR Collab.), Phys. Rev. Lett. 71 (1993) 1307
W.C. Leung et al. (CCFR Collab.), Phys. Lett. B 317 (1993) 655
The parton distributions are parameterized at a reference scaleμ 20 byxq NS (x,μ 20 )=A NS x η 1(1-x)η 2+B NS x η 3,xq SI (x,μ 20 )=xq NS (x,μ 20 )+A sea(1-x)η sea and\(xg(x,\mu _{\text{0}}^{\text{2}} ) = A_g (1 - x{\text{)}}^{\eta _g } \) and evolved to all other values ofμ 2 using the GLAP [10] evolution equations.A NS is constrained by the fermion conservation sum rule\(\int {\tfrac{{dx}}{x}xq_{NS} (x{\text{) = 3}}} \), andA g is constrained by the momentum sum rule\(\int {dx {\text{[}}xq} _{SI} (x{\text{)}} + xg{\text{(}}x{\text{)] = 1}}\). The final fit parameter is the strong coupling constant, given by\(\Lambda _{\overline {MS} } \), for a total of eight fit parameters. Atμ 20 =1 GeV2/c2, the parameters are\(\Lambda _{\overline {MS} } \)=0.210±0.021 GeV/c,η 1=0.947±0.027,η 2=3.81±0.059,η 3=0.0519±0.0064,B NS =0.0210±0.0039,A sea=1.404±0.047,η sea=6.49±0.22,η g =3.18±0.70, where the errors are statistical only
W.G. Seligman et al. (CCFR Collab.), in: Proc. XXVIIIth Rencontre de Moriond: QCD and High Energy Hadronic Interactions (Les Arcs, March 1993), ed. J. Tran Thanh Van (Editions Frontieres, Gif-sur-Yvette, 1993) p. 39
D. Duke and J. Owens, Phys. Rev. D 30 (1984) 49
P. Amaudruz et al. (NMC Collab.), Nucl. Phys. B 371 (1992) 3
K. Hikasa et al. (Particle Data Group), Phys. Rev. D 45 (1992)
C. Peterson et al., Phys. Rev. D 27 (1983) 105
J.C. Anjos et al. (E691 Collab.), Phys. Rev. Lett. 65 (1990) 2503
J.C. Collins, in: Proc. XXVth Rencontre de Moriond: High Energy Hadronic Interactions (Les Arcs, March 1990), ed. J. Tran Thanh Van (Editions Frontieres, Gif-sur-Yvette, 1990), p. 123
M. Virchaux and A. Milsztajn, Phys. Lett. B 274 (1992) 221
M. Arneodo et al. (NMC Collab.), Phys. Lett. B 309 (1993) 222
S.J. Brodsky, C. Peterson and N. Sakai, Phys. Rev. D 23 (1981) 2745
M. Burkardt and B.J. Warr, Phys. Rev. D 45 (1992) 958; J.D. Bjorken, private communication
T. Bolton, Nevis R#501
D. Bortoletto et al. (CLEO Collab.), Phys. Rev. D 37 (1988) 1719
A. Bodek et al., Phys. Rev. Lett. 50 (1983) 1431; 51 (1983) 534
P. Amaudruz et al. (NMC Collab.), Phys. Lett. B 295 (1992) 159
A.C. Benvenuti et al. (BCDMS Collab.), Phys. Lett. B 223 (1989) 485; B 237 (1990) 592
A. Donnachie and P.V. Landshoff, Z. Phys. C 61 (1994) 139
Author information
Authors and Affiliations
Consortia
Rights and permissions
About this article
Cite this article
CCFR Collaboration., Bazarko, A.O., Arroyo, C.G. et al. Determination of the strange quark content of the nucleon from a next-to-leading-order QCD analysis of neutrino charm production. Z. Phys. C - Particles and Fields 65, 189–198 (1995). https://doi.org/10.1007/BF01571875
Received:
Issue Date:
DOI: https://doi.org/10.1007/BF01571875