N. Atanov
Joint Institute for Nuclear Research
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Featured researches published by N. Atanov.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2016
N. Atanov; V. Baranov; J. Budagov; R. Carosi; F. Cervelli; F. Colao; M. Cordelli; G. Corradi; E. Danè; Yu. I. Davydov; S. Di Falco; S. Donati; R. Donghia; B. Echenard; K. T. Flood; S. Giovannella; V. Glagolev; F. Grancagnolo; F. Happacher; D. G. Hitlin; M. Martini; S. Miscetti; T. Miyashita; L. Morescalchi; P. Murat; D. Pasciuto; G. Pezzullo; F. C. Porter; A. Saputi; I. Sarra
The Mu2e experiment at Fermilab aims at measuring the neutrinoless conversion of a negative muon into an electron and reach a single event sensitivity of 2.5×10^(-17) after three years of data taking. The monoenergetic electron produced in the final state, is detected by a high precision tracker and a crystal calorimeter, all embedded in a large superconducting solenoid (SD) surrounded by a cosmic ray veto system. The calorimeter is complementary to the tracker, allowing an independent trigger and powerful particle identification, while seeding the track reconstruction and contributing to remove background tracks mimicking the signal. In order to match these requirements, the calorimeter should have an energy resolution of O(5)% and a time resolution better than 500 ps at 100 MeV. The baseline solution is a calorimeter composed of two disks of BaF_2 crystals read by UV extended, solar blind, Avalanche Photodiode (APDs), which are under development from a JPL, Caltech, RMD consortium. In this paper, the calorimeter design, the R&D studies carried out so far and the status of engineering are described. A backup alternative setup consisting of a pure CsI crystal matrix read by UV extended Hamamatsu MPPC׳s is also presented.
Journal of Instrumentation | 2017
N. Atanov; V. Baranov; J. Budagov; F. Cervelli; F. Colao; M. Cordelli; G. Corradi; E. Danè; Yu. I. Davydov; S. Di Falco; E. Diociaiuti; S. Donati; R. Donghia; B. Echenard; K. T. Flood; S. Giovannella; V. Glagolev; F. Grancagnolo; F. Happacher; D. G. Hitlin; M. Martini; S. Miscetti; T. Miyashita; L. Morescalchi; P. Murat; G. Pezzullo; F. C. Porter; F. Raffaelli; T. Radicioni; M. Ricci
The Mu2e experiment at Fermilab looks for Charged Lepton Flavor Violation (CLFV) improving by 4 orders of magnitude the current experimental sensitivity for the muon to electron conversion in a muonic atom. A positive signal could not be explained in the framework of the current Standard Model of particle interactions and therefore would be a clear indication of new physics. In 3 years of data taking, Mu2e is expected to observe less than one background event mimicking the electron coming from muon conversion. Achieving such a level of background suppression requires a deep knowledge of the experimental apparatus: a straw tube tracker, measuring the electron momentum and time, a cosmic ray veto system rejecting most of cosmic ray background and a pure CsI crystal calorimeter, that will measure time of flight, energy and impact position of the converted electron. The calorimeter has to operate in a harsh radiation environment, in a 10^(−4) Torr vacuum and inside a 1 T magnetic field. The results of the first qualification tests of the calorimeter components are reported together with the energy and time performances expected from the simulation and measured in beam tests of a small scale prototype.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2016
N. Atanov; V. Baranov; F. Colao; M. Cordelli; G. Corradi; E. Danè; Yu. I. Davydov; K. T. Flood; S. Giovannella; V. Glagolev; F. Happacher; D. G. Hitlin; M. Martini; S. Miscetti; T. Miyashita; L. Morescalchi; G. Pezzullo; A. Saputi; I. Sarra; S. R. Soleti; G. Tassielli; V. Tereshchenko
In this paper we present the time resolution measurements of the Lutetium–Yttrium Oxyorthosilicate (LYSO) calorimeter prototype for the Mu2e experiment. The measurements have been performed using the e− beam of the Beam Test Facility (BTF) in Frascati, Italy in the energy range from 100 to 400 MeV. The calorimeter prototype consisted of twenty five 30 x 30 x 130 mm^3, LYSO crystals read out by 10 × 10 mm^2 Hamamatsu Avalanche Photodiodes (APDs). The energy dependence of the measured time resolution can be parametrized as σ_t(E)=a/√E/GeV⊕b, with the stochastic and constant terms a=(51 ± 1)ps and b=(10 ± 4)ps, respectively. This corresponds to the time resolution of (162 ±4 )ps at 100 MeV.
arXiv: Instrumentation and Detectors | 2017
N. Atanov; V. Baranov; J. Budagov; R. Carosi; F. Cervelli; F. Colao; M. Cordelli; G. Corradi; E. Danè; Yu. I. Davydov; S. Di Falco; S. Donati; R. Donghia; B. Echenard; K. T. Flood; S. Giovannella; V. Glagolev; F. Grancagnolo; F. Happacher; D. G. Hitlin; M. Martini; S. Miscetti; T. Miyashita; L. Morescalchi; P. Murat; G.M. Piacentino; G. Pezzullo; F. Raffaelli; A. Saputi; I. Sarra
The Mu2e experiment at Fermilab searches for the charged-lepton flavor violating neutrino-less conversion of a negative muon into an electron in the field of a aluminum nucleus. The dynamic of such a process is well modeled by a two-body decay, resulting in a monoenergetic electron with an energy slightly below the muon rest mass (104.967 MeV). The calorimeter of this experiment plays an important role to provide excellent particle identification capabilities and an online trigger filter while aiding the track reconstruction capabilities. The baseline calorimeter configuration consists of two disks each made with about 700 undoped CsI crystals read out by two large area UV-extended Silicon Photomultipliers. These crystals match the requirements for stability of response, high resolution and radiation hardness. In this paper we present the final calorimeter design.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2016
N. Atanov; V. Baranov; F. Colao; M. Cordelli; G. Corradi; E. Danè; Yu. I. Davydov; K. T. Flood; S. Giovannella; V. Glagolev; F. Happacher; D. G. Hitlin; M. Martini; S. Miscetti; T. Miyashita; L. Morescalchi; P. Ott; G. Pezzullo; A. Saputi; I. Sarra; S. R. Soleti; G. Tassielli; V. Tereshchenko; A. W. Thomas
We have measured the performances of a LYSO crystal matrix prototype tested with electron and photon beams in the energy range 60–450 MeV. This study has been carried out to determine the achievable energy and time resolutions for the calorimeter of the Mu2e experiment.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2018
N. Atanov; V. Baranov; J. Budagov; D. Caiulo; F. Cervelli; F. Colao; M. Cordelli; G. Corradi; Yu.I. Davydov; S. Di Falco; E. Diociaiuti; S. Donati; R. Donghia; B. Echenard; S. Giovannella; V. Glagolev; F. Grancagnolo; F. Happacher; D. G. Hitlin; M. Martini; S. Miscetti; T. Miyashita; L. Morescalchi; P. Murat; E. Pedreschi; G. Pezzullo; F. C. Porter; F. Raffaelli; M. Ricci; A. Saputi
The Mu2e calorimeter is composed of two disks each containing 1348 pure CsI crystals, each crystal read out by two arrays of 6x6 mm^2 monolithic SiPMs. The experimental requirements have been translated in a series of technical specifications for both crystals and SiPMs. Quality assurance tests, on first crystal and then SiPM production batches, confirm the performances of preproduction samples previously assembled in a calorimeter prototype and tested with an electron beam. The production yield is sufficient to allow the construction of a calorimeter of the required quality in the expected times.
IEEE Transactions on Nuclear Science | 2018
N. Atanov; V. Baranov; J. Budagov; Yu. I. Davydov; V. Glagolev; V. Tereshchenko; Z. Usubov; F. Cervelli; S. Di Falco; S. Donati; L. Morescalchi; E. Pedreschi; G. Pezzullo; F. Raffaelli; F. Spinella; F. Colao; M. Cordelli; G. Corradi; E. Diociaiuti; R. Donghia; S. Giovannella; F. Happacher; M. Martini; S. Miscetti; M. Ricci; A. Saputi; I. Sarra; B. Echenard; D. G. Hitlin; Chen Hu
The Mu2e experiment is constructing a calorimeter consisting of 1348 undoped cesium iodide (CsI) crystals in two disks. Each crystal has a dimension of
arXiv: Instrumentation and Detectors | 2017
G. Pezzullo; N. Atanov; V. Baranov; J. Budagov; F. Cervelli; F. Colao; E. Diociaiuti; M. Cordelli; G. Corradi; E. Danè; Yu. I. Davydov; S. Donati; R. Donghia; S. Di Falco; B. Echenard; L. Morescalchi; S. Giovannella; V. Glagolev; F. Grancagnolo; F. Happacher; D. G. Hitlin; M. Martini; S. Miscetti; T. Miyashita; P Murat; E. Pedreschi; F. C. Porter; F. Raffaelli; M. Ricci; A. Saputi
34\times 34\times200
IEEE Transactions on Nuclear Science | 2016
N. Atanov; V. Baranov; F. Colao; M. Cordelli; G. Corradi; E. Danè; Yu. I. Davydov; K. T. Flood; S. Giovannella; V. Glagolev; F. Happacher; D. G. Hitlin; M. Martini; S. Miscettti; T. Miyashita; L. Morescalchi; P. Ott; G. Pezzullo; A. Saputi; I. Sarra; S. R. Soleti; G. Tassielli; V. Tereshchenko; A. W. Thomas
mm3 and is readout by a large-area silicon photomultipliers array. A series of technical specifications on mechanical and optical parameters was defined according to the calorimeter physics requirements. Preproduction CsI crystals were procured from three firms: Amcrys, Saint-Gobain, and Shanghai Institute of Ceramics. We report the quality assurance on crystal’s scintillation properties and their radiation hardness against ionization dose and neutrons. With a fast decay time of about 30 ns and a light output of more than 100 p.e./MeV measured by a bialkali photomultiplier tube, undoped CsI crystals provide a cost-effective solution for Mu2e.
arXiv: Instrumentation and Detectors | 2018
N. Atanov; V. Baranov; J. Budagov; S. Ceravolo; F. Cervelli; F. Colao; M. Cordelli; G. Corradi; E. Danè; Yu. I. Davydov; S. Di Falco; S. Donati; E. Diociaiuti; R. Donghia; B. Echenard; K. T. Flood; S. Giovannella; V. Glagolev; F. Grancagnolo; F. Happacher; D. G. Hitlin; M. Martini; S. Miscetti; T. Miyashita; L. Morescalchi; P. Murat; D. Pasciuto; G. Pezzullo; F. C. Porter; T. Radicioni
The Mu2e experiment at Fermilab will search for the charged lepton flavor violating process of neutrino-less