M. J. Tannenbaum
A5040533490- High-Energy Particle Collisions Research
- Particle physics theoretical and experimental studies
- Quantum Chromodynamics and Particle Interactions
- Nuclear reactor physics and engineering
- Nuclear physics research studies
- Superconducting Materials and Applications
- Particle Detector Development and Performance
- Particle Accelerators and Free-Electron Lasers
- Particle accelerators and beam dynamics
- X-ray Spectroscopy and Fluorescence Analysis
- Dark Matter and Cosmic Phenomena
- Statistical Methods and Bayesian Inference
- Muon and positron interactions and applications
- Radiation Detection and Scintillator Technologies
- Metal and Thin Film Mechanics
- Nuclear Physics and Applications
- Ion-surface interactions and analysis
- Computational Physics and Python Applications
- High-Temperature Coating Behaviors
- Medical Imaging Techniques and Applications
- Atomic and Subatomic Physics Research
- Neutrino Physics Research
- Financial Risk and Volatility Modeling
- Astrophysics and Cosmic Phenomena
- Pediatric Urology and Nephrology Studies
Brookhaven National Laboratory
2016-2025
Banaras Hindu University
2003-2024
Bhabha Atomic Research Centre
2017-2024
Augustana University
2014-2024
PHENIX laboratory
2005-2023
Kurchatov Institute
2023
Abilene Christian University
2003-2023
Charles University
2016-2023
Los Alamos National Laboratory
2019
University of Bergen
2019
Semi-inclusive spectra of ${\ensuremath{\pi}}^{\ifmmode\pm\else\textpm\fi{}}$, ${K}^{\ifmmode\pm\else\textpm\fi{}}$, and p have been measured near midrapidity for central collisions 14.6A-GeV/c $^{28}\mathrm{Si}$ with $^{197}\mathrm{Au}$ nuclei. The invariant cross sections are all well fit by exponential distributions in transverse mass, within the ranges. \ensuremath{\pi} K can also be Boltzmann distributions. From integrated yields, at midrapidity, kaon/pion yield ratios...
Semi-inclusive proton and pion distributions from central Au+Au reactions at 11.6A GeV/c have been measured. The rapidity distribution shows significantly increased stopping compared to lighter systems, providing strong evidence for the formation of a state matter with baryon density substantially greater than normal nuclear matter. Unlike this energy induced by heavy ions, low mt−m0 invariant spectra deviate single exponential shape become flatter, while π− are found rise faster π+...
Experimental physics with relativistic heavy ions dates from 1992 when a beam of 197Au energy greater than 10 A GeV/c first became available at the Alternating Gradient Synchrotron Brookhaven National Laboratory (BNL) soon followed in 1994 by 208Pb 158A Super Proton CERN (European Center for Nuclear Research). Previous pioneering measurements Berkeley Bevalac (Gutbrod et al 1989 Rep. Prog. Phys. 52 1267–132) late 1970s and early 1980s were much lower bombarding energies (≲1A GeV/c) where...
In this document the PHENIX collaboration proposes a major upgrade to detector at Relativistic Heavy Ion Collider. This upgrade, sPHENIX, enables an extremely rich jet and beauty quarkonia physics program addressing fundamental questions about nature of strongly coupled quark-gluon plasma (QGP), discovered experimentally RHIC be perfect fluid. The startling dynamics QGP on fluid-like length scales is emergent property quantum chromodynamics (QCD), seemingly implicit in Lagrangian but...
Proton and deuteron distributions from $11.6A \mathrm{GeV}/c$ Au + collisions measured by the E802 Collaboration in experiment E-866 are presented. The invariant yield of protons deuterons is studied as a function transverse mass for different cuts rapidity centrality. At low ${m}_{t}\ensuremath{-}{m}_{0}$ proton spectra deviate single exponential shape. average ${m}_{t}$ centrality used to explore effect collective flow reaction. ratio squared momentum, rapidity, probe coalescence model...
Particle production in proton-induced reactions at 14.6 GeV/c on Be, Al, Cu, and Au targets has been systematically studied using the E-802 spectrometer BNL-Alternating Gradient Synchrotron. Particles are measured angular range from 5\ifmmode^\circ\else\textdegree\fi{} to 58\ifmmode^\circ\else\textdegree\fi{} identified up momenta of 5, 3.5, 8 for pions, kaons, protons, respectively. Mechanisms particle discussed comparison with heavy-ion-induced same incident energy per nucleon.
A systematic study of the spectra and yields ${K}^{+}$ ${K}^{\ensuremath{-}}$ is reported by experiment E866 as a function centrality in Au+Au collisions at $11.6A \mathrm{GeV}/c.$ The invariant transverse for both kaon species are well described exponentials ${m}_{t},$ with inverse slope parameters that largest midrapidity which increase centrality. slopes slightly larger than spectra. rapidity density peaks distribution wider ${K}^{\ensuremath{-}}.$ integrated total nonlinearly steadily...
Charged kaon production has been measured in Si+Al and Si+Au collisions at 14.6 A GeV/c, Au+Au 11.1 GeV/c by Experiments 859 866 (the E--802 Collaboration) the BNL AGS. Invariant transverse mass spectra rapidity distributions for both K+ K- are presented. The centrality dependence of rapidity-integrated yields is studied. Strangeness enhancement observed as an increase slope yield with total number participants well per participant. starts peripheral (relative to N+N) appears saturate a...
The AGS spectrometer experiment E-802 has measured transverse mass spectra for charged hadrons over a wide rapidity interval in Si+Au, Si+Cu, and Si+Al reactions at 14.6A Gev/c. These results are compared two different trigger conditions: central collisions corresponding to 7% of the inelastic cross section selected on multiplicity particles peripheral roughly 50% high kinetic energy zero degrees. invariant well described by exponentials allowing extraction distributions inverse slope...
The production of ${\mathrm{\ensuremath{\pi}}}^{\ifmmode\pm\else\textpm\fi{}}$,${\mathit{K}}^{\ifmmode\pm\else\textpm\fi{}}$,p has been measured in p+Be and p+Au collisions for comparison with central Si+Au collisions. inverse slope parameters ${\mathit{T}}_{0}$ obtained by an exponential fit to the invariant cross sections transverse mass are found be, ${\mathit{T}}_{0}^{\mathit{p},}$${\mathit{K}}^{+}$,${\mathrm{\ensuremath{\pi}}}^{\mathrm{\ensuremath{\pi}}}$\ensuremath{\sim}140--160 MeV...