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Robert Harlander:
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Top quark pair production near threshold
Lippmann-Schwinger equation
Because the lifetime of a top quark is shorter than the typical time
scale for a bound toponium state, the top--anti-top system turns out to
be a unique testing ground for QCD. The production cross section near
threshold can be computed by solving a Lippmann-Schwinger-like
equation which involves the QCD potential.
Lippmann-Schwinger equation
in diagrammatical form. The shaded blob denotes the tt-bar vertex in
the threshold region.
Polarization of top quarks
Our contribution in this field was to investigate the polarization
of the top quarks in the threshold region. One of the main
results ([1], [2]) was that the
maximal component of the polarization vector which is parallel to the
electron beam is hardly affected by threshold effects. It is therefore
well suited for experimental studies of the top--anti-top system at a
future linear collider.
Rescattering corrections
Rescattering corrections between the top quark and
its decay
products near threshold are formally of the same order of magnitude as
the non-maximal components of the polarization vector. Therefore it was
necessary to calculate these contributions which was done in
[3],
[4],
[5]. It turned
out that indeed they can give rise to effects of comparable
size. However, it was shown that the normal component of the
polarization vector is insensitive to rescattering effects and provides
a direct measure of the strong coupling constant.
Higgs potential
Since the top quark is an exceptionally heavy particle, it may play a
crucial role in the generation of masses. In particular, the top quark
system may be optimally suited for investigations of the Higgs sector
of the Standard Model. Therefore, we calculated the influence of a
scalar and pseudo-scalar Higgs boson on the top quark production
cross section near threshold
[6]. It turned out
that this cross section is significantly modified by the presence of a
Higgs potential, especially for a low Higgs mass as it is favored by
recent data compilations.
Review
A comprehensive presentation of the main results obtained
during the
workshops on physics at a next linear collider (see [5])
can be found in [7].
New developments
The calculations mentioned above are valid mostly to
next-to-leading order in the top quark velocity. Meanwhile there
has been considerable theoretical progress, so that now the NNLO
corrections to top quark pair production in the threshold
region are available. The corresponding results showed a
surprisingly strong
dependence on the renormalization scale and have lead to
interesting new
ideas. For a review and a list of references see
the paper on
"Top-Anittop
Pair Production close to Threshold: Synopsis of recent NNLO Results"
[ref].
Literature:
[1] |
R. Harlander,
M. Jezabek, J.H. Kühn, T. Teubner, | |
Polarization in Top
Quark Pair Production near Threshold, | |
Phys. Lett. B346 (1995) 137-142. | | | |
| [2] |
R. Harlander M. Jezabek, J.H. Kühn, T. Teubner, | |
Polarization in Top Pair Production and Decay near Threshold, | |
Proceedings of the Workshop "Spin 94", Bloomington, IN, Sept. 1994,
pp. 675-680. | | | |
| [3] |
R. Harlander, M. Jezabek, J.H. Kuehn, M. Peter, | |
Top Quark Polarization in Polarized e^+e^-
Annihilation near Threshold, | |
Z. Phys. C73 (1997) 477-494. | | | |
| [4] |
M. Jezabek, R. Harlander, J.H. Kühn, M. Peter, | |
Polarized Top Quarks, | |
Proceedings of the workshop on Physics and Experiments with Linear Colliders, Morioka-Appi, 1995, pp. 436-446. | | | |
| [5] |
R. Harlander, M. Jezabek, J.H. Kühn, M. Peter, | |
Top quarks at a polarized linear collider, | |
Proceedings of the workshop on e^+e^-
collisions at TeV energies: the physics
potential, part D, Annecy, Gran Sasso, Hamburg, 1995, pp. 5-20,
ed. P. Zerwas. | | | |
| [6] | R. Harlander, M. Jezabek, J.H. Kühn, | |
Higgs effects in top quark pair production, | |
Acta Phys.Polon. B27 (1996) 1781-1788. | | | |
| [7] | ECFA/DESY LC Physics Working Group:
E. Accomando, et al., | |
Physics with e^+e^-Linear Colliders, | |
Phys. Rept. 299 (1998) 1-78. | | | |
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Robert Harlander:
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