M. G. Munhoz
- High-Energy Particle Collisions Research
- Particle physics theoretical and experimental studies
- Quantum Chromodynamics and Particle Interactions
- Nuclear physics research studies
- Nuclear reactor physics and engineering
- Particle Detector Development and Performance
- Nuclear Physics and Applications
- Atomic and Molecular Physics
- Astronomical and nuclear sciences
- Pulsars and Gravitational Waves Research
- Cosmology and Gravitation Theories
- Stochastic processes and statistical mechanics
- Dark Matter and Cosmic Phenomena
- X-ray Spectroscopy and Fluorescence Analysis
- Statistical Methods and Bayesian Inference
- Particle Accelerators and Free-Electron Lasers
- Cold Fusion and Nuclear Reactions
- Education and Digital Technologies
- Radiation Detection and Scintillator Technologies
- Radiopharmaceutical Chemistry and Applications
- Education Pedagogy and Practices
- Cold Atom Physics and Bose-Einstein Condensates
- Medical Imaging Techniques and Applications
- Computational Physics and Python Applications
- Particle accelerators and beam dynamics
Hospital Universitário da Universidade de São Paulo
2016-2025
A. Alikhanyan National Laboratory
2015-2024
Universidade de São Paulo
2013-2024
University of Illinois Urbana-Champaign
2019-2024
Universidade Cidade de São Paulo
2022
Aligarh Muslim University
2020
Center for Research and Advanced Studies of the National Polytechnic Institute
2020
Centro de Aplicaciones Tecnológicas y Desarrollo Nuclear
2020
California Polytechnic State University
2020
Istituto Nazionale di Fisica Nucleare, Sezione di Bologna
2020
Open and hidden heavy-flavor physics in high-energy nuclear collisions are entering a new exciting stage towards reaching clearer understanding of the experimental results with possibility to link them directly advancement lattice Quantum Chromo-Dynamics (QCD). Recent from experiments theoretical developments regarding open dynamics have been debated at Lorentz Workshop Tomography Quark-Gluon Plasma Heavy Quarks, which was held October 2016 Leiden, The Netherlands. In this contribution, we...
Excitation functions for sub- and near-barrier total (complete + incomplete) fusion cross sections are presented the 6,7Li+59Co reactions. Evaporation residues were identified by their characteristic γ rays corresponding yields measured with both IReS Garel array at Vivitron facility São Paulo Ge 8UD Pelletron tandem using standard γ-ray techniques. The data extend to medium-mass systems previous works exploring coupling effects (hindrance versus enhancement) in reactions of lighter heavier...
The $^{10}\mathrm{B}(p,{\ensuremath{\alpha}}_{0})^{7}\mathrm{Be}$ bare nucleus astrophysical $S(E)$ factor has been measured for the first time at energies from about 100 keV down to 5 by means of Trojan Horse method (THM). In this energy region, is strongly dominated 8.699 MeV $^{11}\mathrm{C}$ level (${J}^{\ensuremath{\pi}}={\frac{5}{2}}^{+}$), producing an $s$-wave resonance centered 10 in entrance channel. Up now, only high--energy tail measured, while low-energy trend extrapolated...
Complete fusion of light radioactive nuclei is predicted to be hindered at near-barrier energies. This feature investigated in the case least bound stable nuclei. Evaporation residues resulting from ${}^{6,7}\mathrm{Li}{+}^{9}\mathrm{Be}$ and ${}^{6,7}\mathrm{Li}{+}^{12}\mathrm{C}$ reactions have been measured order study common features involving weakly The experimental excitation functions revealed that cross section significantly smaller than total reaction also expected available...
A new measurement of the 11B(p,?0)8Be has been performed applying Trojan horse method (THM) to 2H(11B,?80Be)n quasi-free reaction induced at a laboratory energy 27 MeV. The astrophysical S(E) factor extracted from ?600 keV down zero by means an improved data analysis technique and it compared with direct available in literature. range investigated here overlaps region light element LiBeB stellar burning that future aneutronic fusion power plants using 11B+p fuel cycle. investigation...
This paper presents the test results of second prototype SAMPA, ASIC designed for upgrade read-out front end electronics ALICE Time Projection Chamber (TPC) and Muon (MCH). SAMPA is made in a 130 nm CMOS technology with 1.25 V nominal voltage supply provides 32 channels, selectable input polarity, three possible combinations shaping time sensitivity. Each channel consists Charge Sensitive Amplifier, semi-Gaussian shaper 10-bit ADC; Digital Signal Processor digital filtering compression...
For the first time astrophysical factor of $^{10}\mathrm{B}(p,{\ensuremath{\alpha}}_{0})^{7}\mathrm{Be}$ reaction has been measured over a wide energy range, from 5 keV to 1.5 MeV, via Trojan horse method (THM) applied quasifree $^{2}\mathrm{H}(^{10}\mathrm{B},\ensuremath{\alpha}^{7}\mathrm{Be})n$ reaction. Therefore, $S(E)$ recast into absolute units by scaling in range 200 keV--1.2 MeV recent measurement using activation method, leading normalization uncertainty $4%$. An $R$-matrix fit THM...
We present measurements from BNL AGS Experiment 864 of the $_{\ensuremath{\Lambda}}^{3}\mathrm{H}$ yield and an upper limit on $_{\ensuremath{\Lambda}}^{4}\mathrm{H}$ in central $11.5A\phantom{\rule{0.3em}{0ex}}\text{GeV}∕c\phantom{\rule{0.3em}{0ex}}\text{Au}+\text{Pt}$ collisions. The span a rapidity range center mass, ${y}_{\mathrm{c.m.}}$, to ${y}_{\mathrm{c.m.}}+1$ transverse momentum $0<{p}_{t}\ensuremath{\leqslant}1.5\phantom{\rule{0.3em}{0ex}}\text{GeV}∕c$. compare these results with...
The elastic scattering for the $^{6,7}\mathrm{Li}+^{59}\mathrm{Co}$ systems was investigated in bombarding energy range $12\phantom{\rule{0.3em}{0ex}}\text{MeV}\ensuremath{\leqslant}{E}_{\mathrm{lab}}\ensuremath{\leqslant}30\phantom{\rule{0.3em}{0ex}}\text{MeV}$ by means of an analysis using S\~ao Paulo potential, through which behavior real and imaginary parts as function established. experimental results suggest that overall there is evidence usual threshold anomaly both systems, although...
We report on measurements by the E864 experiment at BNL-AGS of yields light nuclei in collisions 197Au with beam momentum 11.5AGeV/c targets 208Pb and 197Pt. The are reported for baryon number A=1 up to A=7, typically cover a rapidity range from yc.m. yc.m.+1 transverse approximately 0.1<~pT/A<~0.5GeV/c. calculate coalescence scale factors BA which we extract model-dependent source dimensions collective flow velocities. also examine dependences number, spin, isospin produced nuclei.Received...
This paper presents the SAMPA, an ASIC designed for upgrade of read-out front end electronics ALICE Time Projection Chamber (TPC) and Muon Chambers (MCH). SAMPA is made in a 130 nm CMOS technology with 1.25 V nominal voltage supply includes 32 channels, selectable input polarity, five possible combinations shaping time sensitivity. Each channel comprises Charge Sensitive Amplifier, semi-Gaussian shaper 10-bit ADC, followed by Digital Signal Processor. A prototype multi project run was...
We present Experiment 864's measurement of invariant antideuteron yields in 11.5A GeV/c Au+Pt collisions. The analysis includes 250×106 triggers representing 14×109 10% central interactions sampled for events with high mass candidates. find (1/2πpt)d2N/dydpt=3.5±1.5(stat)−0.5+0.9(syst)×10−8GeV−2c2 1.8<y<2.2, 〈pt〉=0.35GeV/c ( yc.m.=1.6) and 3.7±2.7(stat)−1.5+1.4(syst)×10−8 GeV−2c2 1.4<y<1.8, 〈pt〉=0.26GeV/c, a coalescence parameter B2¯ 4.1±2.9(stat)−2.4+2.3(syst)×10−3GeV2c−3. Implications...
We present results of a search for strange quark matter (strangelets) in 11.5AGeV/cAu+Pb collisions from the 1994 and 1995 runs experiment E864 at Brookhaven's Alternating Gradient Synchrotron. observe no strangelet candidates set 90% confidence level upper limit approximately 3×10−8 per 10% central interaction production |Z|=1 |Z|=2 strangelets over large mass range with metastable lifetimes about 50 ns or more. These place constraints primarily on quark-gluon plasma based models...
Light nuclei can be produced in the central reaction zone via coalescence relativistic heavy-ion collisions. Experiment 864 at BNL has measured production of ten light with nuclear number $A\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}1$ to $A\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}7$ rapidity $y\ensuremath{\simeq}1.9$ and ${p}_{T}/A\ensuremath{\le}300\mathrm{MeV}/c$. Data were taken a Au beam momentum $11.5A\mathrm{GeV}/c$ on Pb or Pt target different experimental settings....
A large hadronic lead scintillating fiber calorimeter has been built and integrated into the AGS experiment E864 [C. Pruneau et al., Collaboration, Proc. 6th Internal. Conf. on Calorimetry in High Energy Physics, 1996, Frascati, Italy; F. Rotondo Quark Matter'96, Heidelberg, Germany, 20 May 1996] spectrometer to provide an independent measurement of mass particles produced heavy ion collisions. The "spaghetti-type" design construction techniques are described detail. Results from a prototype...
Combining event-by-event hydrodynamics with heavy quark energy loss we compute correlations between the and soft sectors for elliptic triangular flow harmonics v2 v3 of D0 mesons in PbPb collisions at 2.76 TeV 5.02 TeV. Our results indicate that is strongly influenced by fragmentation temperature it builds up later than during evolution system.
We present results from Experiment 864 for antiproton production and antideuteron limits in Au + Pb collisions at 11.5 GeV/c per nucleon. have measured invariant multiplicities antiprotons rapidities 1.4<y<2.4 low transverse momentum as a function of collision geometry. When compared with the 878 our measurements suggest significant contribution to yield decay strange antibaryons. also searched antideuterons see no statistically signal. Thus, we set upper on approximately 3×10−7 10% highest...