Abstract.
We give a continuum limit value of the lowest moment of a twist-2 operator in pion states from non-perturbative lattice calculations. We find that the non-perturbatively obtained renormalization group invariant matrix element is \(\langle x\rangle_{\mathrm{RGI}} = 0.179(11)\), which corresponds to \(\langle x \rangle^{\overline{\mathrm{MS}}}(2\mathrm{ GeV}) = 0.246(15)\). In obtaining the renormalization group invariant matrix element, we have controlled important systematic errors that appear in typical lattice simulations, such as non-perturbative renormalization, finite size effects and effects of a non-vanishing lattice spacing. The crucial limitation of our calculation is the use of the quenched approximation. Another question that remains not fully clarified is the chiral extrapolation of the numerical data.
Similar content being viewed by others
References
R. Devenish, A. Cooper-Sarkar, Deep inelastic scattering (Oxford Unversity Press, Oxford 2004)
S. Alekhin, Phys. Rev. D 63, 094022 (2001)
A.D. Martin, R.G. Roberts, W.J. Stirling, R.S. Thorne, hep-ph/0308087
J. Blümlein, H. Böttcher, Nucl. Phys. B 636, 225 (2002)
R. Petronzio, Nucl. Phys. B Proc. 73, 303 (1999); M. Göckeler, R. Horsley, D. Pleiter, P.E.L. Rakow, A. Schäfer, G. Schierholz, Nucl. Phys. B Proc. 119, 32 (2003); S. Capitani, Nucl. Phys. B Proc. 116, 115 (2003); K. Jansen, to be published in Nuclear Physics A, Proceedings of FB17, Durham, USA (2003); A. Shindler, to be published in the Proceedings of DIS04
A. Bucarelli, F. Palombi, R. Petronzio, A. Shindler, Nucl. Phys. B 552, 379 (1999)
M. Guagnelli, K. Jansen, R. Petronzio, Nucl. Phys. B 542, 395 (1999)
M. Guagnelli, K. Jansen, R. Petronzio, Phys. Lett. B 457, 153 (1999)
M. Guagnelli, K. Jansen, R. Petronzio, Phys. Lett. B 459, 594 (1999)
M. Guagnelli, K. Jansen, R. Petronzio, Phys. Lett. B 493, 77 (2000)
ZeRo Collaboration: M. Guagnelli, K. Jansen, F. Palombi, R. Petronzio, A. Shindler, I. Wetzorke, Nucl. Phys. B 664, 276 (2003)
Talk presented by K. Jansen at the XXXth International Conference on High Energy Physics (ICHEP (2000)), July 27-August 2 (2000), hep-lat/0010038
M. Guagnelli, K. Jansen, F. Palombi, R. Petronzio, A. Shindler, I. Wetzorke, plenary talk given by A. Shindler Electron-Nucleus Scattering VII, June 24-28 (2002), Elba; Eur. Phys. J. A 17, 365 (2003)
M. Guagnelli, K. Jansen, F. Palombi, R. Petronzio, A. Shindler, I. Wetzorke (World Scientific, Genoa 2002), Gerasimov-Drell-Hearn sum rule and the spin structure of the nucleon, 69-76
K. Jansen, Nucl. Phys. B Proc. 129-130, 3 (2004)
C. Bernard et al. , Nucl. Phys. B Proc. 106, 199 (2002)
M. L\” uscher, R. Narayanan, P. Weisz, U. Wolff, Nucl. Phys. B 384, 168 (1992); S. Sint, Nucl. Phys. B 421, 135 (1994); B 451, 416 (1995); K. Jansen, C. Liu, M. L\” uscher, H. Simma, S. Sint, R. Sommer, P. Weisz, U. Wolff, Phys. Lett. B 372, 275 (1996); M. L\” uscher, S. Sint, R. Sommer, P. Weisz, Nucl. Phys. B 478, 365 (1996)
R. Sommer, Lectures at Schladming 1997, hep-lat/9711243
M. Lüscher, Lectures given at the Les Houches Summer School, Probing the Standard Model of Particle Interactions, July 28-September 5, 1997, hep-lat/9802029
R. Sommer, Nucl. Phys. B Proc. 119, 185 (2003)
ZeRo Collaboration: M. Guagnelli, K. Jansen, F. Palombi, R. Petronzio, A. Shindler, I. Wetzorke, Phys. Lett. B 597, 216 (2004)
JLQCD Collaboration, S. Aoki et al. , Phys. Rev. D 68, 054502 (2003)
A.W. Thomas, W. Melnitchouk, F.M. Steffens, Phys. Rev. Lett. 85, 2892 (2000)
W. Detmold et al. , Phys. Rev. Lett. 87, 172001 (2001)
D. Arndt, M.J. Savage, Nucl. Phys. A 697, 429 (2002)
J.W. Chen, M.J. Savage, Nucl. Phys. A 707, 452 (2002)
S.R. Beane, M.J. Savage, Phys. Rev. D 68, 114502 (2003)
J.W. Chen, X. Ji Phys. Rev. Lett. 88, 052003 (2002)
P.J. Sutton, A.D. Martin, R.G. Roberts, W.J. Stirling, Phys. Rev. D 45, 2349 (1992); M. Glück, E. Reya, I. Schienbein, Eur. Phys. J. C 10, 313 (1999)
M. Baake, B. Gemünden, R. Oedingen, J. Math. Phys. 23, 944 (1982); J.E. Mandula, G. Zweig, J. Govaerts, Nucl. Phys. B 228, 91 (1983)
ALPHA Collaboration: M. Guagnelli et al. , Nucl. Phys. B 560, 465 (1999)
ALPHA Collaboration: M. Lüscher et al. , Nucl. Phys. B 491, 323 (1997)
B. Sheikholeslami, R. Wohlert, Nucl. Phys. B 259, 572 (1985)
S. Capitani et al. , Nucl. Phys. B Proc. 63, 153 (1998); S. Capitani et al. , Nucl. Phys. B 544, 669 (1999)
R. Sommer, private comunication
S. Necco, R. Sommer, Nucl. Phys. B 622, 328 (2002)
O.V. Tarasov, A.A. Vladimirov, A.Yu. Zharkov, Phys. Lett. B 93, 429 (1980)
E.G. Floratos, D.A. Ross, C.T. Sachrajda, Nucl. Phys. B 129, 66 (1977); Erratum B 139, 545 (1978); A. Gonzalez-Arroyo, C. Lopez, F.J. Yndurain, Nucl. Phys. B 153, 161 (1979); G. Curci, W. Furmanski, R. Petronzio, Nucl. Phys. B 175, 27 (1980)
R. Sommer, Nucl. Phys. B 411, 839 (1994); M. Guagnelli, R. Sommer, H. Wittig, Nucl. Phys. B 535, 389 (1998)
C. Best et al. , Phys. Rev. D 56, 2743 (1997)
ZeRo Collaboration: A. Shindler, M. Guagnelli, K. Jansen, F. Palombi, R. Petronzio, I. Wetzorke, Nucl. Phys. B Proc. 129-130, 278 (2004)
G. Schierholz, private communication
LHPC Collaboration: D. Dolgov et al. , Phys. Rev. D 66, 034506 (2002)
Author information
Consortia
Additional information
Received: 28 October 2004, Published online: 4 February 2005
PACS:
11.15.Ha, 12.38.Gc
Rights and permissions
About this article
Cite this article
The Zeuthen-Rome (Zero) Collaboration. Non-perturbative pion matrix element of a twist-2 operator from the lattice. Eur. Phys. J. C 40, 69–80 (2005). https://doi.org/10.1140/epjc/s2005-02121-5
Issue Date:
DOI: https://doi.org/10.1140/epjc/s2005-02121-5