1,176 research outputs found
Possible Formation of QGP-droplets in Proton-Proton Collisions at the CERN Large Hadron Collider
Proton-proton (pp) collisions have been traditionally used as a baseline
measurement in the search for a deconfined state of matter in heavy-ion
collisions at ultrarelativistic energies. The unprecedented collision energies
that are available at the Large Hadron Collider (LHC) at the European
Laboratory for Nuclear Research (CERN) have illuminated new challenges in
understanding the possible formation of droplets of this deconfined matter of
partonic degrees of freedom in hadronic collisions, especially in
high-multiplicity events. Enhancement of multi-strange particles compared to
pions, degree of collectivity, comparable freeze-out temperature with heavy-ion
collisions, observation of a long-range ridge-like structure for
high-multiplicity events are some of the experimental observations in this
direction. In this article, we discuss some of the experimental observables and
outline new theoretical directions to understand the possibilities of exploring
the formation of QGP-droplets in pp collisions at the LHC.Comment: 6-pages, Featured invited article for beginners in the field,
appeared in AAPPS Bulleti
A new description of transverse momentum spectra of identified particles produced in proton-proton collisions at high energies
The transverse momentum spectra of identified particles produced in high
energy proton-proton () collisions are empirically described by a new
method with the framework of participant quark model or the multisource model
at the quark level, in which the source itself is exactly the participant
quark. Each participant (constituent) quark contributes to the transverse
momentum spectrum, which is described by the TP-like function, a revised
Tsallis--Pareto-type function. The transverse momentum spectrum of the hadron
is the convolution of two or more TP-like functions. For a lepton, the
transverse momentum spectrum is the convolution of two TP-like functions due to
two participant quarks, e.g. projectile and target quarks, taking part in the
collisions. A discussed theoretical approach seems to describe the
collisions data at center-of-mass energy GeV, 2.76 TeV, and 13
TeV very well.Comment: 19 pages, 7 figures. Advances in High Energy Physics, accepte
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