51 research outputs found
Analytical description of the time-over-threshold method based on the time properties of plastic scintillators equipped with silicon photomultipliers
A new high-granular compact time-of-flight neutron detector for the
identification and energy measurement of neutrons produced in nucleus-nucleus
interactions at the BM@N experiment, Dubna, Russia, at energies up to 4 AGeV is
under development. The detector consists of approximately 2000 fast plastic
scintillators, each with dimensions of 404025 mm, equiped
with SiPM (Silicon Photomultiplier) with an active area of 66 mm.
The signal readout from these scintillators will employ a single-threshold
multichannel Time-to-Digital Converter (TDC) to measure their response time and
amplitude using the time-over-threshold (ToT) method. This article focuses on
the analytical description of the signals from the plastic scintillator
detectors equipped with silicon photomultipliers. This description is crucial
for establishing the ToT-amplitude relationship and implementing slewing
correction techniques to improve the time resolution of the detector. The
methodology presented in this paper demonstrates that a time resolution at the
70 ps level can be achieved for the fast plastic scintillator coupled with
silicon photomultiplier with epitaxial quenching resistors
ON THE LOCAL SUM CONJECTURE IN TWO DIMENSIONS
In this paper we give an elementary proof of the local sum conjecture in two
dimensions. In a remarkable paper [CMN, arXiv:1810.11340], this conjecture has
been established in all dimensions using sophisticated, powerful techniques
from a research area blending algebraic geometry with ideas from logic. The
purpose of this paper is to give an elementary proof of this conjecture which
will be accessbile to a broad readership.Comment: 32 Page
Measurement of Time Resolution of Scintillation Detectors with EQR-15 Silicon Photodetectors for the Time-of-Flight Neutron Detector of the BM@N Experiment
To study the dependence of the equation of state of high density nuclear
matter on the term characterizing the isospin (proton-neutron) asymmetry of
nuclear matter, it is necessary to measure azimuthal flow of neutrons as well
as azimuthal flow of charged particles from a dense nuclear matter in the
nuclear-nuclear collisions. For this purpose INR RAS is developing a new
high-granular neutron detector which will be used in the BM@N experiment at the
extracted beam of the Nuclotron accelerator at JINR (Dubna). This detector will
identify neutrons and measure their energies in the heavy-ion collisions up to
4 GeV per nucleon.
This article presents the results of measurements of the time resolution and
light yields of samples of scintillation detectors with sizes
404025 mm that will be used in a neutron detector based on
the currently available fast plastic scintillator manufactured by JINR using an
EQR15 11-6060D-S photodetector for light readout. For comparison, the results
of measurements for a detector of the same size with a fast scintillator EJ-230
and with the same type of photodetector are given. The measurements were made
on cosmic muons as well as on the electron synchrotron "Pakhra" of the Lebedev
Physical Institute of the Russian Academy of Sciences located in Troitsk,
Moscow
The PSD CBM Supermodule Response Study for Hadrons in Momentum Range 2 – 6 GeV/c at CERN Test Beams
The Projectile Spectator Detector (PSD) will be used at the Compressed Baryonic Matter (CBM) experiment at FAIR to measure the centrality and orientation of the reaction plane in heavy-ion collisions. A study of PSD supermodule response at proton and pion momentum range 2 – 6 GeV has been done at the CERN T10 beam line. The PSD supermodule is 3x3 array of 9 modules. Each module has transverse dimensions of 20x20 cm2 and longitudinal dimension of 5.6 interaction lengths. The modules have sandwich structure of 60 lead/scintillator layers with the sampling ratio 4:1. Light from each scintillator plate is collected by a WLS fiber. Scintillator light from 6 consecutive scintillator plates (one longitudinal section) is detected by a 3x3 mm2 Hamamatsu MPPC placed at the end of the module. In total, 10 MPPCs are used to detect light from 10 longitudinal sections in each module. Preliminary results on the longitudinal profile of energy deposition, linearity of the response and energy resolution of the supermodule are discussed
Development of High Granular Neutron Time-of-Flight Detector for the BM@N experiment
The HGND (High Granular Neutron Detector) is developed for the BM@N (Baryonic
Matter at Nuclotron) experiment on the extracted beam of the Nuclotron at JINR,
Dubna. The HGND will be used to measure the azimuthal flow of neutrons produced
with energies ranging from 300 to 4000 MeV in heavy-ion collisions at beam
energies of 2--4 AGeV. The azimuthal flow of charged particles will be measured
using the BM@N magnet spectrometer. The data on the azimuthal flow of neutrons
will shed light on the study of the high-density Equation of State (EoS) of
isospin-symmetric nuclear matter, which is crucial for studying astrophysical
phenomena such as neutron stars and their mergers. The HGND has a highly
granular structure with approximately 2000 plastic scintillation detectors
(cells), each measuring 442.5 cm. These detectors are
arranged in 16 layers, with 121 detectors in each layer, and are subdivided by
copper absorber plates with a thickness of 3 cm. The light from each cell is
detected with SiPM (Silicon Photomultiplier) with an active area of 66
mm. Developed multi-channel TDC board based on the Kintex FPGA chip with a
bin width of 100 ps will be used to perform precise timestamp and amplitude
measurement using Time-over-Threshold (ToT) method. Good spatial resolution due
to the high granularity together with a cell's time resolution of 100-150 ps
ensures neutron reconstruction with good energy resolution. The design of the
detector as well as the results from test measurements and simulations have
been presented
Production of {\pi}+ and K+ mesons in argon-nucleus interactions at 3.2 AGeV
First physics results of the BM@N experiment at the Nuclotron/NICA complex
are presented on {\pi}+ and K+ meson production in interactions of an argon
beam with fixed targets of C, Al, Cu, Sn and Pb at 3.2 AGeV. Transverse
momentum distributions, rapidity spectra and multiplicities of {\pi}+ and K+
mesons are measured. The results are compared with predictions of theoretical
models and with other measurements at lower energies.Comment: 29 pages, 20 figure
meson production in inelastic p+p interactions at 40 and 80 beam momenta measured by NA61/SHINE at the CERN SPS
Measurements of K∗(892)0 resonance production via its K+π− decay mode in inelastic p+p collisions at beam momenta 40 and 80 GeV /c (sNN−−−−√=8.8 and 12.3 GeV ) are presented. The data were recorded by the NA61/SHINE hadron spectrometer at the CERN Super Proton Synchrotron. The template method was used to extract the K∗(892)0 signal. Transverse momentum and rapidity spectra were obtained. The mean multiplicities of K∗(892)0 mesons were found to be (35.1±1.3(stat)±3.6(sys))⋅10−3 at 40 GeV /c and (58.3±1.9(stat)±4.9(sys))⋅10−3 at 80 GeV /c. The NA61/SHINE results are compared with the Epos1.99 and Hadron Resonance Gas models as well as with world data. The transverse mass spectra of K∗(892)0 mesons and other particles previously reported by NA61/SHINE were fitted within the Blast-Wave model. The transverse flow velocities are close to 0.1–0.2 of the speed of light and are significantly smaller than the ones determined in heavy nucleus-nucleus interactions at the same beam momenta
Measurements of K, Λ , and production in 120 GeV / c p + C interactions
This paper presents multiplicity measurements of K0S, Λ, and ¯Λ produced in 120 GeV/c proton-carbon interactions. The measurements were made using data collected at the NA61/SHINE experiment during two different periods. Decays of these neutral hadrons impact the measured π+, π−, p and ¯p multiplicities in the 120 GeV/c proton-carbon reaction, which are crucial inputs for long-baseline neutrino experiment predictions of neutrino beam flux. The double-differential multiplicities presented here will be used to more precisely measure charged-hadron multiplicities in this reaction, and to reweight neutral hadron production in neutrino beam Monte Carlo simulations
Measurements of , , and spectra in Ar+Sc collisions at 13 to 150 GeV/
The NA61/SHINE experiment at the CERN Super Proton Synchrotron studies the
onset of deconfinement in strongly interacting matter through a beam energy
scan of particle production in collisions of nuclei of varied sizes. This paper
presents results on inclusive double-differential spectra, transverse momentum
and rapidity distributions and mean multiplicities of , ,
and produced in Ar+Sc collisions at beam momenta of
13, 19, 30, 40, 75 and 150 GeV/. The analysis uses the 10%
most central collisions, where the observed forward energy defines centrality.
The energy dependence of the / ratios as well as of inverse
slope parameters of the transverse mass distributions are placed in
between those found in inelastic + and central Pb+Pb collisions. The
results obtained here establish a system-size dependence of hadron production
properties that so far cannot be explained either within statistical (SMES,
HRG) or dynamical (EPOS, UrQMD, PHSD, SMASH) models
Measurements of , , , , and production in 120 GeV/ p + C interactions
This paper presents multiplicity measurements of charged hadrons produced in
120 GeV/ proton-carbon interactions. The measurements were made using data
collected at the NA61/SHINE experiment during two different data-taking
periods, with increased phase space coverage in the second configuration due to
the addition of new subdetectors. Particle identification via was
employed to obtain double-differential production multiplicities of ,
, , , and . These measurements are presented as a
function of laboratory momentum in intervals of laboratory polar angle covering
the range from 0 to 450 mrad. They provide crucial inputs for current and
future long-baseline neutrino experiments, where they are used to estimate the
initial neutrino flux
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