1
However far we roam, the gluon attraction pulls us home.
2
Limits are set on scalar resonances produced through gluon-gluon fusion, and on Randall-Sundrum gravitons.
3
This result shows that the gluon distributions in the proton and neutron are very similar.
4
Models incorporating initial-state gluon saturation or partonic energy loss in dense matter are largely consistent with observations.
5
These observations are qualitatively consistent with a saturation picture of the low-x gluon structure of heavy nuclei.
6
Among the possible particles is a heavy cousin to the massless gluon, the particle that binds quarks together.
7
It constitutes a new well-controlled reference for testing theoretical models of the parton passage through the quark-gluon plasma.
8
Another boson is called the gluon.
9
A jet is a spray of particles produced by a quark or a gluon in a high-energy collision.
10
We find the higher twist matrix element d˜2, which arises strictly from quark-gluon interactions, to be unambiguously nonzero.
11
The gluon string is capable of absorbing more and more energy as the quarks separate and the string stretches.
12
When a colored gluon escapes from its source, then that hue is transferred to the Quark that catches it.
13
Furthermore, quark and gluon jet fractions are used to extract the average charged-particle multiplicity for quark and gluon jets separately.
14
Anomalously large sizes or emission durations, which have been suggested as signals of quark-gluon plasma formation and rehadronization, are not observed.
15
Relativistic hydrodynamics simulations of quark-gluon plasma play a pivotal role in our understanding of heavy ion collisions at RHIC and LHC.
16
It is believed that this force is carried by a particle, called the gluon, which interacts only with itself and with the quarks.