scholarly journals Predictions for boson-jet observables and fragmentation function ratios from a hybrid strong/weak coupling model for jet quenching

2016 ◽  
Vol 2016 (3) ◽  
Author(s):  
Jorge Casalderrey-Solana ◽  
Doga Can Gulhan ◽  
José Guilherme Milhano ◽  
Daniel Pablos ◽  
Krishna Rajagopal
Keyword(s):  
Fragmentation Function ◽  
Weak Coupling ◽  
Coupling Model ◽  
Jet Quenching ◽  
Jet Observables

scholarly journals A Comprehensive Analysis of Jet Quenching via a Hybrid Strong/Weak Coupling Model for Jet-Medium Interactions

2016 ◽  
Vol 956 ◽  
pp. 613-616
Author(s):  
Jorge Casalderrey-Solana ◽  
Doga Can Gulhan ◽  
José Guilherme Milhano ◽  
Daniel Pablos ◽  
Krishna Rajagopal
Keyword(s):  
Weak Coupling ◽  
Coupling Model ◽  
Comprehensive Analysis ◽  
Jet Quenching

scholarly journals The angular structure of jet quenching within a hybrid strong/weak coupling model

2017 ◽  
Vol 289-290 ◽  
pp. 359-362
Author(s):  
Jorge Casalderrey-Solana ◽  
Doga Can Gulhan ◽  
José Guilherme Milhano ◽  
Daniel Pablos ◽  
Krishna Rajagopal
Keyword(s):  
Weak Coupling ◽  
Coupling Model ◽  
Jet Quenching ◽  
Angular Structure

scholarly journals Angular structure of jet quenching within a hybrid strong/weak coupling model

2017 ◽  
Vol 2017 (3) ◽  
Author(s):  
Jorge Casalderrey-Solana ◽  
Doga Can Gulhan ◽  
José Guilherme Milhano ◽  
Daniel Pablos ◽  
Krishna Rajagopal
Keyword(s):  
Weak Coupling ◽  
Coupling Model ◽  
Jet Quenching ◽  
Angular Structure

scholarly journals Boson-Jet Correlations in a Hybrid Strong/Weak Coupling Model for Jet Quenching in Heavy Ion Collisions

2016 ◽  
Vol 276-278 ◽  
pp. 285-288
Author(s):  
Jorge Casalderrey-Solana ◽  
Doga Can Gulhan ◽  
José Guilherme Milhano ◽  
Daniel Pablos ◽  
Krishna Rajagopal
Keyword(s):  
Weak Coupling ◽  
Heavy Ion Collisions ◽  
Coupling Model ◽  
Heavy Ion ◽  
Jet Quenching ◽  
Ion Collisions

Low-lying Negative-parity Levels of 17N and 18N

1984 ◽  
Vol 37 (1) ◽  
pp. 17 ◽  
Author(s):  
FC Barker
Keyword(s):  
Shell Model ◽  
Weak Coupling ◽  
Coupling Model ◽  
Negative Parity ◽  
Positive Parity ◽  
Model Calculations

On the basis of a weak-coupling model, adjustments are made to the interactions used in the full shell model calculations of Millener in order to fit the experimental energies of the low-lying negativeparity levels of 16N and of the low-lying positive-parity levels of 180 and 190 . The predicted energies of the low-lying negative-parity levels of 17N then agree better with experiment, while those for 18N lead to suggested spin assignments for the observed levels.

Carrier tunneling in nanocrystalline silicon–silicon dioxide superlattices: A weak coupling model

2004 ◽  
Vol 69 (23) ◽  
Author(s):  
B. V. Kamenev ◽  
G. F. Grom ◽  
D. J. Lockwood ◽  
J. P. McCafrey ◽  
B. Laikhtman ◽  
...  
Keyword(s):  
Silicon Dioxide ◽  
Weak Coupling ◽  
Coupling Model ◽  
Nanocrystalline Silicon ◽  
Carrier Tunneling ◽  
Silicon Silicon

Application of the unified weak-coupling model to neutron scattering byC12

1977 ◽  
Vol 16 (1) ◽  
pp. 76-79 ◽  
Author(s):  
J. E. Purcell ◽  
M. R. Meder
Keyword(s):  
Neutron Scattering ◽  
Weak Coupling ◽  
Coupling Model

Weak-Coupling Model forPb212andPb204

1973 ◽  
Vol 8 (6) ◽  
pp. 2379-2389 ◽  
Author(s):  
C. M. Ko ◽  
T. T. S. Kuo ◽  
J. B. McGrory
Keyword(s):  
Weak Coupling ◽  
Coupling Model

scholarly journals Jet tomography in high-energy nuclear collisions

2019 ◽  
Vol 206 ◽  
pp. 04004 ◽  
Author(s):  
Ben-Wei Zhang ◽  
Guo-Yang Ma ◽  
Wei Dai ◽  
Sa Wang ◽  
Shan-Liang Zhang
Keyword(s):  
Energy Loss ◽  
Heavy Ion ◽  
High Energy ◽  
Jet Quenching ◽  
Parton Energy Loss ◽  
Matrix Elements ◽  
Leading Order ◽  
Nuclear Collisions ◽  
Ion Collisions ◽  
Jet Observables

When an energetic parton traversing the QCD medium, it may suffer multiple scatterings and lose energy. This jet quenching phenomenon may lead to the suppression of leading hadron productions as well as medium modifications of full jet observables in heavy-ion collisions. In this talk we discuss the nuclear modificationfactors and yield ratios of identified meson such as η, ρ0, φ, ω, and $ K_{\rm{S}}^0 $ as well as π meson at large pT in A+A collisions at the next to-leading order (NLO) with high-twist approach of parton energy loss. Then we discuss a newly developed formalism of combing NLO matrix elements and parton shower (PS) for initial hard production with parton energy loss in the QGP, and its application in investigating massivegauge boson(Z0/W±)tagged jet productions and b $ \bar {b} $ dijet correlations in Pb+Pb at the LHC.

Sign in / Sign up

Export Citation Format

Share Document