Publications (4)0 Total impact
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ABSTRACT: We calculate P(k_\perp), the probability distribution for an energetic parton
that propagates for a distance L through a medium without radiating to pick up
transverse momentum k_\perp, for a medium consisting of weakly coupled
quark-gluon plasma. We use full or HTL self-energies in appropriate regimes,
resumming each in order to find the leading large-L behavior. The jet quenching
parameter \hat q is the second moment of P(k_\perp), and we compare our results
to other determinations of this quantity in the literature, although we
emphasize the importance of looking at P(k_\perp) in its entirety. We compare
our results for P(k_\perp) in weakly coupled quark-gluon plasma to expectations
from holographic calculations that assume a plasma that is strongly coupled at
all length scales. We find that the shape of P(k_\perp) at modest k_\perp may
not be very different in weakly coupled and strongly coupled plasmas, but we
find that P(k_\perp) must be parametrically larger in a weakly coupled plasma
than in a strongly coupled plasma at large enough k_\perp. This means that by
looking for rare (but not exponentially rare) large-angle deflections of the
jet resulting from a parton produced initially back-to-back with a hard photon,
experimentalists can find the weakly coupled short-distance quark and gluon
quasiparticles within the strongly coupled liquid quark-gluon plasma produced
in heavy ion collisions, much as Rutherford found nuclei within atoms or
Friedman, Kendall and Taylor found quarks within nucleons.
11/2012;
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ABSTRACT: We calculate the probability distribution P(k_\perp) for the momentum
perpendicular to its original direction of motion that an energetic quark or
gluon picks up as it propagates through weakly coupled quark-gluon plasma in
thermal equilibrium.
10/2011;
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ABSTRACT: We analyze the transverse momentum broadening in the absence of radiation of
an energetic parton propagating through quark-gluon plasma via Soft Collinear
Effective Theory (SCET). We show that the probability for picking up transverse
momentum k_\perp is given by the Fourier transform of the expectation value of
two transversely separated light-like path-ordered Wilson lines. The subtleties
about the ordering of operators do not change the \hat q value for the strongly
coupled plasma of N=4 SYM theory.
10/2010;
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ABSTRACT: We use Soft Collinear Effective Theory (SCET) to analyze the transverse
momentum broadening, or diffusion in transverse momentum space, of an energetic
parton propagating through quark-gluon plasma. Since we neglect the radiation
of gluons from the energetic parton, we can only discuss momentum broadening,
not parton energy loss. The interaction responsible for momentum broadening in
the absence of radiation is that between the energetic (collinear) parton and
the Glauber modes of the gluon fields in the medium. We derive the effective
Lagrangian for this interaction, and we show that the probability for picking
up transverse momentum k_\perp is given by the Fourier transform of the
expectation value of two transversely separated light-like path-ordered Wilson
lines. This yields a field theoretical definition of the jet quenching
parameter \hat q, and shows that this can be interpreted as a diffusion
constant. We close by revisiting the calculation of \hat q for the strongly
coupled plasma of N=4 SYM theory, showing that previous calculations need some
modifications that make them more straightforward and do not change the result.
06/2010;
Institutions
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2010
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Massachusetts Institute of Technology
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Center for Theoretical Physics
Cambridge,
MA,
USA