R. Mountain

ORCID: 0000-0003-1908-4219
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About
Contact & Profiles
Research Areas
  • Particle physics theoretical and experimental studies
  • Quantum Chromodynamics and Particle Interactions
  • High-Energy Particle Collisions Research
  • Neutrino Physics Research
  • Particle Detector Development and Performance
  • Radiation Detection and Scintillator Technologies
  • Dark Matter and Cosmic Phenomena
  • Black Holes and Theoretical Physics
  • Medical Imaging Techniques and Applications
  • Atomic and Subatomic Physics Research
  • Particle Accelerators and Free-Electron Lasers
  • Superconducting Materials and Applications
  • Computational Physics and Python Applications
  • Diamond and Carbon-based Materials Research
  • Nuclear physics research studies
  • Stochastic processes and statistical mechanics
  • Radiation Effects in Electronics
  • Advanced NMR Techniques and Applications
  • Cosmology and Gravitation Theories
  • Distributed and Parallel Computing Systems
  • International Science and Diplomacy
  • Radioactive Decay and Measurement Techniques
  • Astrophysics and Cosmic Phenomena
  • Advanced Data Storage Technologies
  • Nuclear Physics and Applications

Syracuse University
2016-2025

Universitat Ramon Llull
2023-2024

Universitat de Barcelona
2023

Monash University
2023

European Organization for Nuclear Research
2011-2021

Jožef Stefan Institute
2016-2018

Centro Brasileiro de Pesquisas Físicas
2013-2017

Istituto Nazionale di Fisica Nucleare, Sezione di Ferrara
2014-2017

University of Maryland, College Park
2017

University of Zurich
2013-2016

The LHCb experiment has been taking data at the Large Hadron Collider (LHC) CERN since end of 2009. One its key detector components is Ring-Imaging Cherenkov (RICH) system. This provides charged particle identification over a wide momentum range, from 2–100 GeV/c. operation and control, software, online monitoring RICH system are described. performance presented, as measured using LHC. Excellent separation hadronic types (π, K, p) achieved.

10.1140/epjc/s10052-013-2431-9 article EN cc-by The European Physical Journal C 2013-05-01

The Vertex Locator (VELO) is a silicon microstrip detector that surrounds the proton-proton interaction region in LHCb experiment. performance of during first years its physics operation reviewed. system operated vacuum, uses bi-phase CO2 cooling system, and sensors are moved to 7 mm from LHC beam for data taking. stability these characteristic features described, details material budget given. calibration timing processing algorithms implemented FPGAs described. fully characterised. have...

10.1088/1748-0221/9/09/p09007 article EN cc-by Journal of Instrumentation 2014-09-09

We present the first measurement of D*(+) width using 9/fb e(+)e(-) data collected near Upsilon(4S) resonance by CLEO II.V detector. Our method uses advanced tracking techniques and a reconstruction that takes advantage small vertical size Cornell Electron-positron Storage Ring beam spot to measure energy release distribution from D*(+)-->D(0)pi(+) decay. find gamma(D*(+)) = 96+/-4 (stat)+/-22 (syst) keV. also in decay compute Delta m identical with m(D*(+))-m(D(0)) 145.412+/-0.002...

10.1103/physrevlett.87.251801 article EN Physical Review Letters 2001-11-01

Beam test results of the radiation tolerance study chemical vapour deposition (CVD) diamond against different particle species and energies is presented. We also present beam on independence signal size incident rate in charged detectors based un-irradiated irradiated poly-crystalline CVD over a range fluxes from 2 kHz/cm2 to 10 MHz/cm2. The pulse height sensors was measured with readout electronics peaking time 6 ns. In addition functionality 3D devices demonstrated tests are shown be...

10.1088/1748-0221/13/01/c01029 article EN Journal of Instrumentation 2018-01-23

Using the CLEO-II detector, we have obtained evidence for a new meson decaying to $D^0 K^+$. Its mass is $2573.2^{+1.7}_{-1.6}\pm 0.8\pm 0.5$ {}~MeV/$c^2$ and its width $16^{+5}_{-4}\pm 3$~MeV/$c^2$. Although do not establish spin parity, consistent with predictions an $L=1$, $S=1$, $J_P=2^+$ charmed strange state.

10.1103/physrevlett.72.1972 article EN Physical Review Letters 1994-03-28

10.1016/0168-9002(94)91244-0 article EN Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment 1994-11-01

We have studied the performance of scintillating glass fiber-optic plates using 10 GeV/c particles at SLAC test beam. The were composed of: (1) Terbium activated cladded-glass cores in a matrix 15 #x003BC;m spacing; and (2) Cerium variable spacing 6-10 #x003BC;m. target viewed with three-stage, gatable image intensifier. Particle tracks nuclear interactions recorded on film for both materials. observe 5 detected hits/mm minimum ionizing Tb glass, 1-2 Ce glass. results indicate that can be...

10.1109/tns.1984.4333212 article EN IEEE Transactions on Nuclear Science 1984-02-01

A fiber-optic plate imaging system has been developed for active target and tracking applications, in which the element is Ce(3+) a silicate glass. Particle tracks interactions have recorded with hit density of ≳ 4/mm minimum ionizing particles spatial resolution σ ~ 28μ m.

10.1109/tns.1986.4337068 article EN IEEE Transactions on Nuclear Science 1986-02-01

Abstract We have measured the radiation tolerance of poly-crystalline and single-crystalline diamonds grown by chemical vapor deposition (CVD) process measuring charge collected before after irradiation in a 50 m pitch strip detector fabricated on each diamond sample. irradiated one group sensors with 800 MeV protons, second 24 GeV steps, to protons cm −2 respectively. observe sum mean drift paths for electrons holes both CVD decreases fluence from its initial value according simple damage...

10.1088/1361-6463/ab37c6 article EN cc-by Journal of Physics D Applied Physics 2019-08-01

Diamond devices have now become ubiquitous in the LHC experiments, finding applications beam background monitoring and luminosity measuring systems. This sensor material is maturing to point that large pads existing diamond detectors are being replaced by highly granular tracking devices, both pixel strip configurations, for detector systems will be used Run II at beyond. The RD42 collaboration has continued seek out additional manufacturers quantify limits of radiation tolerance this...

10.1016/j.nuclphysbps.2015.09.160 article EN cc-by Nuclear and Particle Physics Proceedings 2016-04-01

A measurement of the cross section for combined two-photon production charged pion and kaon pairs is performed using 1.2~$\rm fb^{-1}$ data collected by CLEO~II detector at Cornell Electron Storage Ring. The measured invariant masses system between 1.5 5.0 GeV/$c^2$, scattering angles more than $53^\circ$ away from $\gamma\gamma$ collision axis in center-of-mass frame. large background leptonic events suppressed utilizing CsI calorimeter conjunction with muon chamber system. reported...

10.1103/physrevd.50.3027 article EN Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields 1994-09-01

10.1016/j.nima.2018.06.009 article EN publisher-specific-oa Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment 2018-06-07

10.1016/j.nima.2024.169202 article EN Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment 2024-02-23

SALT, a new dedicated readout Application Specific Integrated Circuit (ASIC) for the Upstream Tracker, silicon detector in Large Hadron Collider beauty (LHCb) experiment, has been designed and developed. It is 128-channel chip using an innovative architecture comprising low-power analogue front-end with fast pulse shaping 40 MSps 6-bit Analog-to-Digital Converter (ADC) each channel, followed by Digital Signal Processing (DSP) block performing pedestal Mean Common Mode (MCM) subtraction zero...

10.3390/s22010107 article EN cc-by Sensors 2021-12-24
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