  Some of the most important probes of the quark-gluon plasma (QGP) produced in
heavy ion collisions come from the analysis of how the shape and energy of jets
are modified by passage through QGP. We model an ensemble of back-to-back
dijets to gain a qualitative understanding of how the shapes of the individual
jets and the asymmetry in the energy of the pairs of jets are modified by
passage through an expanding droplet of strongly coupled plasma, as modeled in
a holographic gauge theory. We do so by constructing an ensemble of strings in
the gravitational description of the gauge theory. We model QCD jets in vacuum
using strings whose endpoints move "downward" into the gravitational bulk
spacetime with some fixed small angle that represents the opening angle (ratio
of jet mass to jet energy) that the QCD jet would have in vacuum. Such strings
must be moving through the gravitational bulk at (close to) the speed of light;
they must be (close to) null. This condition does not specify the energy
distribution along the string, meaning that it does not specify the shape of
the jet being modeled. We study the dynamics of strings that are initially not
null and show that strings with a wide range of initial conditions rapidly
accelerate and become null and, as they do, develop a similar distribution of
their energy density. We use this distribution of the energy density along the
string, choose an ensemble of strings whose opening angles and energies are
distributed as in perturbative QCD, and show that we can then fix one model
parameter such that the mean jet shape in our ensemble matches that measured in
p-p collisions reasonably well. We send our strings through the plasma,
choosing the second model parameter to get a reasonable suppression in the
number of jets, and study how the mean jet shape and the dijet asymmetry are
modified, comparing both to data from LHC heavy ion collisions.
