INTERMITTENCY PATTERNS IN PROTON-NUCLEUS INTERACTIONS AT HIGH ENERGY

1993 ◽  
Vol 08 (40) ◽  
pp. 3853-3859 ◽  
Author(s):  
D. K. MAITY ◽  
P. K. BANERJEE ◽  
B. B. DAS ◽  
D. RAVINDRAN ◽  
D. K. BHATTACHARJEE
Keyword(s):  
Power Law ◽  
Quark Gluon Plasma ◽  
Center Of Mass ◽  
Gluon Plasma ◽  
High Energy ◽  
Mass Energy ◽  
Factorial Moments ◽  
Center Of Mass Energy

A study of intermittency in hadron-nucleus and the comparison with nucleus-nucleus interactions is presented. The power law behavior of the factorial moments and the variation of intermittency index with the center-of-mass energy are shown. Results favor the formation of quark-gluon plasma in preference to a cascade mechanism.

High(est) energy lepton colliders

2021 ◽  
pp. 2142016
Author(s):  
Roberto Franceschini
Keyword(s):  
Standard Model ◽  
Center Of Mass ◽  
High Energy ◽  
New Physics ◽  
Mass Energy ◽  
Center Of Mass Energy ◽  
Lepton Colliders ◽  
The Standard Model

We discuss the physics opportunities and challenges presented by high energy lepton colliders in the range of center-of-mass energy between few and several tens of TeV. The focus is on the progress attainable on the study of weak and Higgs interactions in connection with new physics scenarios motivated by the shortcomings of the Standard Model.

scholarly journals High-energy resummation in heavy-quark pair hadroproduction

2019 ◽  
Vol 79 (11) ◽  
Author(s):  
A. D. Bolognino ◽  
Francesco Giovanni Celiberto ◽  
M. Fucilla ◽  
D. Yu. Ivanov ◽  
A. Papa
Keyword(s):  
Heavy Quark ◽  
Cross Section ◽  
Center Of Mass ◽  
High Energy ◽  
Heavy Quarks ◽  
Mass Energy ◽  
Center Of Mass Energy ◽  
Large Separation ◽  
Bfkl Approach ◽  
Heavy Quark Pair

AbstractThe inclusive hadroproduction of two heavy quarks, featuring a large separation in rapidity, is proposed as a novel probe channel of the Balitsky–Fadin–Kuraev–Lipatov (BFKL) approach. In a theoretical setup which includes full resummation of leading logarithms in the center-of-mass energy and partial resummation of the next-to-leading ones, predictions for the cross section and azimuthal coefficients are presented for kinematic configurations typical of current and possible future experimental analyses at the LHC.

Single production of vector-like top partner in the Wb channel at eγ collision in the LHT model

2019 ◽  
Vol 34 (18) ◽  
pp. 1950093
Author(s):  
Guang Yang ◽  
Bingfang Yang ◽  
Biaofeng Hou ◽  
Hengheng Bi
Keyword(s):  
Search Strategy ◽  
Center Of Mass ◽  
High Energy ◽  
Mass Energy ◽  
Center Of Mass Energy ◽  
Energy Formula ◽  
Single Production ◽  
Detector Simulation ◽  
Higgs Data ◽  
Integrated Luminosity

In the framework of the littlest Higgs Model with T-parity (LHT), we investigate the single production of vector-like top partner [Formula: see text] decaying to [Formula: see text] in the leptonic channel at the high energy [Formula: see text] collision. We utilize the polarized electron beam and photon beam to enhance the signal and propose a search strategy by performing a detector simulation. On the basis of the current limits from the precision electroweak data and Higgs data, we find that the top partner mass can be excluded up to 1350 (1380) GeV with integrated luminosity of 1000 fb[Formula: see text] and 1400 (1470) GeV with integrated luminosity of 3000 fb[Formula: see text] for the [Formula: see text] TeV (2.4 TeV) at the [Formula: see text] level. If the center-of-mass energy can be improved to 3.0 TeV, the limits on the top partner mass will reach 1450 (1550) GeV with integrated luminosities of 1000 (3000) fb[Formula: see text].

scholarly journals Anisotropic flow of identified particles in Pb–Pb collisions at √SNN = 5.02 TeV

2018 ◽  
Vol 171 ◽  
pp. 17002
Author(s):  
Redmer Alexander Bertens
Keyword(s):  
Initial Conditions ◽  
Center Of Mass ◽  
Heavy Ion ◽  
Gluon Plasma ◽  
Mass Energy ◽  
Initial State ◽  
Anisotropic Flow ◽  
Center Of Mass Energy ◽  
Ion Collisions ◽  
Hydrodynamic Calculations

Anisotropic flow is sensitive to the shear (η/s) and bulk (ζ/s) viscosity of the quark-gluon plasma created in heavy-ion collisions, as well as the initial state of such collisions and hadronization mechanisms. In these proceedings, elliptic (υ2) and higher harmonic (υ3, υ4) flow coefficients of π±, K±, p(p) and the ϕ-meson, are presented for Pb—Pb collisions at the highest-ever center-of-mass energy of [see formula in PDF] = 5.02 TeV. Comparisons to hydrodynamic calculations (IP-Glasma, MUSIC, UrQMD) are shown to constrain the initial conditions and viscosity of the medium.

scholarly journals EXCITED HADRONS AS A SIGNAL FOR QUARK–GLUON PLASMA FORMATION

2006 ◽  
Vol 21 (16) ◽  
pp. 3421-3440 ◽  
Author(s):  
BISWANATH LAYEK ◽  
AJIT M. SRIVASTAVA ◽  
SOMA SANYAL
Keyword(s):  
Transition Temperature ◽  
Excited States ◽  
Quark Gluon Plasma ◽  
Center Of Mass ◽  
Heavy Ion ◽  
Gluon Plasma ◽  
Large Error ◽  
Relativistic Heavy Ion Collisions ◽  
Excitation Energies ◽  
Center Of Mass Energy

At the quark–hadron transition, when quarks get confined to hadrons, certain orbitally excited states, namely those which have excitation energies above the respective L = 0 states of the same order as the transition temperature Tc, may form easily because of thermal velocities of quarks at the transition temperature. We propose that the ratio of multiplicities of such excited states to the respective L = 0 states can serve as an almost model independent signal for the quark–gluon plasma (QGP) formation in relativistic heavy-ion collisions. For example, the ratio R* of multiplicities of [Formula: see text] and [Formula: see text] when plotted with respect to the center-of-mass energy of the collision [Formula: see text] (or vs. centrality/number of participants), should show a jump at the value of [Formula: see text] beyond which the QGP formation occurs. This should happen irrespective of the shape of the overall plot of R* vs. [Formula: see text]. Recent data from RHIC on Λ*/Λ vs. N part for large values of N part may be indicative of such a behavior, though there are large error bars. We give a list of several other such candidate hadronic states.

scholarly journals Bottomonium spectroscopy in the quark–gluon plasma

2020 ◽  
Vol 35 (29) ◽  
pp. 2030016
Author(s):  
Georg Wolschin
Keyword(s):  
Quark Gluon Plasma ◽  
Center Of Mass ◽  
Decisive Role ◽  
Spectroscopic Properties ◽  
Heavy Ion ◽  
Gluon Plasma ◽  
Parton Density ◽  
Relativistic Heavy Ion Collisions ◽  
Center Of Mass Energy ◽  
Collisional Damping

The spectroscopic properties of heavy quarkonia are substantially different in the quark–gluon plasma (QGP) that is created in relativistic heavy-ion collisions as compared to the vacuum situation that can be tested in [Formula: see text] collisions at the same center-of-mass energy. In this paper, a series of recent works about the dissociation of the [Formula: see text] and [Formula: see text] states in the hot QGP are summarized. Quarkonia dissociation occurs due to (1) screening of the real quark-antiquark potential, (2) collisional damping through the imaginary part of the potential, and (3) gluon-induced dissociation. In addition, reduced feed-down plays a decisive role for the spin-triplet ground state. Transverse-momentum and centrality-dependent data are well reproduced in Pb–Pb collisions at LHC energies. In the asymmetric [Formula: see text]-Pb system, alterations of the parton density functions in the lead nucleus account for the leading fraction of the modifications in cold nuclear matter (CNM), but the hot-medium effects turn out to be relevant in spite of the small initial spatial extent of the fireball, providing additional evidence for the generation of a quark–gluon droplet.

scholarly journals THE SCALAR UNPARTICLE PRODUCTION FROM THE COLLISION PROCESS IN UNPARICLE PHYSCIS

2020 ◽  
Vol 36 (1) ◽  
Author(s):  
Lê Như Thục
Keyword(s):  
Differential Cross Section ◽  
Cross Section ◽  
Center Of Mass ◽  
High Energy ◽  
Mass Energy ◽  
Collision Process ◽  
Missing Energy ◽  
Energy Distributions ◽  
Center Of Mass Energy ◽  
High Energy Collider

The production of scalar unparticle (spin - 0) in the photon - electron  collider are calculated in all s-, t-, and u-channels in detail as well as interference between channels together. By searching for missing energy distributions as well as evaluating dependence of  differential cross section (DCS) on the scattering angle  and cross section (CS) on the center of mass energy , we hope that the unparticles production in high energy collider might be detected in future.

CEPC booster design study

2017 ◽  
Vol 32 (34) ◽  
pp. 1746009
Author(s):  
Tianjian Bian ◽  
Jie Gao ◽  
Chuang Zhang ◽  
Xiao-Hao Cui ◽  
Yi-Wei Wang ◽  
...  
Keyword(s):  
Beam Energy ◽  
Center Of Mass ◽  
High Energy ◽  
Low Energy ◽  
Mass Energy ◽  
Dipole Magnet ◽  
Center Of Mass Energy ◽  
The Earth ◽  
Electron Positron ◽  
Normal Ring

In September 2012, Chinese scientists proposed a Circular Electron Positron Collider (CEPC) in China at 240 GeV center-of-mass energy for Higgs studies. The booster provides 120 GeV electron and positron beams to the CEPC collider for top-up injection at 0.1 Hz. The design of the full energy booster ring of the CEPC is a challenge. The ejected beam energy is 120 GeV and the injected beam energy is 6 GeV. In this paper we describe two alternative schemes, the wiggler bend scheme and the normal bend scheme. For the wiggler bend scheme, we propose to operate the booster ring as a large wiggler at low energy and as a normal ring at high energy to avoid the problem of very low dipole magnet fields. For the normal bend scheme, we implement the orbit correction to correct the earth field.

scholarly journals BLACK HOLE AND BRANE PRODUCTION IN TEV GRAVITY: A REVIEW

2003 ◽  
Vol 18 (11) ◽  
pp. 1843-1882 ◽  
Author(s):  
MARCO CAVAGLIÀ
Keyword(s):  
Black Holes ◽  
Black Hole ◽  
Extra Dimensions ◽  
Large Extra Dimensions ◽  
Center Of Mass ◽  
Cosmic Ray ◽  
High Energy ◽  
Mass Energy ◽  
Particle Collisions ◽  
Center Of Mass Energy

In models with large extra dimensions, particle collisions with center-of-mass energy larger than the fundamental gravitational scale can generate nonperturbative gravitational objects such as black holes and branes. The formation and the subsequent decay of these super-Planckian objects would be detectable in particle colliders and high energy cosmic ray detectors, and have interesting implications in cosmology and astrophysics. In this paper we present a review of black hole and brane production in TeV-scale gravity.

scholarly journals Search for Anomalous Quartic ZZγγ Couplings in Photon-Photon Collisions

2016 ◽  
Vol 2016 ◽  
pp. 1-8 ◽  
Author(s):  
M. Köksal ◽  
V. Arı ◽  
A. Senol
Keyword(s):  
Linear Collider ◽  
Center Of Mass ◽  
High Energy ◽  
New Physics ◽  
Energy Scale ◽  
Mass Energy ◽  
Abelian Gauge ◽  
Center Of Mass Energy ◽  
High Energy Scale ◽  
Integrated Luminosity

The self-couplings of the electroweak gauge bosons are completely specified by the non-Abelian gauge nature of the Standard Model (SM). The direct study of these couplings provides a significant opportunity to test the validity of the SM and the existence of new physics beyond the SM up to the high energy scale. For this reason, we investigate the potential of the processes γγ→ZZ, e-γ→e-γ⁎γ→e-ZZ,  and e+e-→e+γ⁎γ⁎e-→e+ZZe- to examine the anomalous quartic couplings of ZZγγ vertex at the Compact Linear Collider (CLIC) with center-of-mass energy 3 TeV. We calculate 95% confidence level sensitivities on the dimension-8 parameters with various values of the integrated luminosity. We show that the best bounds on the anomalous fM2/Λ4, fM3/Λ4, fT0/Λ4, and fT9/Λ4 couplings arising from γγ→ZZ process among those three processes at center-of-mass energy of 3 TeV and integrated luminosity of Lint=2000 fb−1 are found to be [-3.30;3.30]×10-3 TeV−4, [-1.20;1.20]×10-2 TeV−4, [-3.40;3.40]×10-3 TeV−4, and [-1.80;1.80]×10-3 TeV−4, respectively.

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