Abstract
Now, are hard collisions really all that easy? To be sure, calculation (not to mention measurement) of hard-collision processes is far from simple, and I mean no disrespect by the title. It is meant in the physicists’ sense that “what is possible to do is easy; the impossible is merely hard.”
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References
J. Bjorken and S. Drell, “Relativistic Quantum Fields”, McGraw-Hill (New York, 1965 ).
See J. Bjorken, Proceedings of the 1979 SLAC Summer Institute on Particle Physics, ed. A. Mosher, SLAG Report SLAC-224(1980), p.219.
T. Sloan, CERN preprint CERN-EP/87–188(October, 1987 ).
J. Bjorken, Phys. Rev. 148, 1467 (1966).
J. Ellis and R. Jaffe, Phys. Rev. D9, 1444 (1974).
F. Close, these proceedings.
S. Brodsky, J. Ellis, and M. Karliner, SLAC-PUB-4519(Jan. 1988), present an interesting new interpretation of these data.
See G. Bodwin, Phys. Rev. D31, 2616(1985) and references therein.
See for example S. Brodsky, Acta Physica Polonica B15, 1059(1984) and references therein.
I believe that in modern language this inconsistency has to do with the presence of vacuum-to-vacuum bubbles in the evolution matrix U(t), but I am not sure on this point. Infinite renormalization constants also complicate the issue.
Actually, a better estimate is E/Am2, where Am2 = m2 - m2 is the mass (squared) splitting between the pion and tfie next important massive state x. I thank M. Strikman for this comment.
See for example the contributions of G. Marchesini, of T. Gottschalk, of F. Paige and S. Protopopescu, and of H. Bengtsson, Proceedings of the UCLA Workshop “Observable Standard Model Physics at the SSC: Monte Carlo Simulation and Detector Capabilities,” ed. H. V. Bengtsson, C. Buchanan, T. Gottschalk, and A. Soni, World Scientific(Singapore ), 1986.
W. Hofmann, Proceedings of the XXIII International Conference on High Energy Physics, Berkeley, CA, July, 1986, ed. S. Loken, World Scientific(Singapore), 1987, Vol. II, p. 1093.
Y. Azimov, Y. Dokshitzer, V. Khose, and S. Troyan, Phys. Lett. 165B, 147(1985); Yad. Fiz. 43, 149(1986) and references 1177.6in.
S. Parke and T. Taylor, Phys. Lett. 157B, 81 (1985).
N. Nikolaev and V. Zakharov, Phys. Lett. 55B, 197 (1975).
J. Bjorken, in Particles and Detectors: Festschrift for Jack Steinberger, ed. K. Kleinknecht and T.D. Lee, Springer Tracts II, 108 ( Springer-Verlag, Berlin, 1986 ), p. 17.
For a nice discussion, see A. Bialas and I. Chinaj, Phys. Lett. 133B, 241 (1983).
S. Brodsky and G. Farrar, Phys. Rev. D11, 1309 (1975).
A. Mueller, Proceedings of the 27th Rencontre de Moriond on Perturbative QCD, ed. J. Tran Thaa. Van, Editions Frontieres, Gif-sur-Yvette(1987).
A. Carroll et. al., Penn State preprint PSU HEP/88–02.
G. Farrar, Phys. Rev. Letters 56, 1643(1986).The theoretical argument for banning polarization measurements is expressed in this paper: the full amplitude is A = C + D where C, the clean amplitude, is computable and D, the dirty amplitude, is not. D in magnitude is 30% of C so it only affects unpolarized data at the 10% level. Polarization data dependent on the interference term is dirty even though asymmetries up to 60% are possible.
See for example S. Brodsky and G. DeTeramond, SLAC preprint SLACPUB-4504, Dec, 1987.
Internal-target data from Fermilab show backward protons (xF - 0.8±0.1) about 7% polarized at pi, = 500 MeV; this polarization disappears at pT = 1 GeV. But what about higher pT? And what about pp -( n + x? See M. Corcoran et. al., Phys. Rev. D22, 2624(1980).
G. Ingelman and P. Schlein, Phys. Lett. 152B, 256 (1985).
An excellent analysis of the situation is presented by E. Berger, J. Collins, D. Soper, and G. Sterman, Nucl. Phys. B286, 704 (1987).
It can be done. See J. Bjorken, Forward Spectrometers at the SSC, FERMILAB-CONF-86/22.
For color singlet initial-state partons, the existence of a rapidity gap is very credible; an example is W+W -( H° as discussed by Y. Dokshitzer, V. Khose, and S. Troyan, Proceedings of the 6th International Conference on Physics in Collision, ed. M. Derrick, World Scientific(Singapore), 1987, p. 417.
K. Ellis and C. Quigg, Fermilab Report, FN-445, Jan. 1987, and these proceedings.E. Berger, Proceedings of the 22nd Rencontre de Moriond, March 1987, and these proceedings.
P. Coteus et. al., Phys. Rev. Letters 59, 1530 (1987).
J. Bjorken, L. Frankfurt, and M. Strikman, “Hadronization of Heavy Quarks,” in preparation.
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Bjorken, J.D. (1988). QCD: Hard Collisions are Easy and Soft Collisions are Hard. In: Cox, B. (eds) QCD Hard Hadronic Processes. NATO ASI Series, vol 197. Springer, Boston, MA. https://doi.org/10.1007/978-1-4684-8842-5_1
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