A5029594549- Particle physics theoretical and experimental studies
- High-Energy Particle Collisions Research
- Quantum Chromodynamics and Particle Interactions
- Particle Detector Development and Performance
- Dark Matter and Cosmic Phenomena
- Computational Physics and Python Applications
- Neutrino Physics Research
- Superconducting Materials and Applications
- Cosmology and Gravitation Theories
- Particle Accelerators and Free-Electron Lasers
- Radiation Detection and Scintillator Technologies
- Particle accelerators and beam dynamics
- Distributed and Parallel Computing Systems
- Atomic and Subatomic Physics Research
- Black Holes and Theoretical Physics
- CCD and CMOS Imaging Sensors
- Astrophysics and Cosmic Phenomena
- Noncommutative and Quantum Gravity Theories
- Muon and positron interactions and applications
- advanced mathematical theories
- Nuclear Physics and Applications
- Radiation Therapy and Dosimetry
- Stochastic processes and financial applications
- International Science and Diplomacy
- Radiomics and Machine Learning in Medical Imaging
European Organization for Nuclear Research
2011-2025
University of Antwerp
2009-2024
Institute of High Energy Physics
2022-2024
A. Alikhanyan National Laboratory
2022-2024
National Central University
2022-2023
Paul Scherrer Institute
2023
Cukurova University
2022
Ludwig-Maximilians-Universität München
2000-2020
Campbell Collaboration
2005-2011
Yale University
2001-2009
The anomalous magnetic moment of the negative muon has been measured to a precision 0.7 ppm (ppm) at Brookhaven Alternating Gradient Synchrotron. This result is based on data collected in 2001, and over an order magnitude more precise than previous measurement for muon. a(mu(-))=11 659 214(8)(3) x 10(-10) (0.7 ppm), where first uncertainty statistical second systematic, consistent with measurements anomaly positive average a(mu)(exp)=11 208(6) (0.5 ppm).
Three independent searches for an electric dipole moment (EDM) of the positive and negative muons have been performed, using spin precession data from muon g-2 storage ring at Brookhaven National Laboratory. Details on experimental apparatus three analyses are presented. Since individual results muon, as well combined result, d=-0.1(0.9)E-19 e-cm, all consistent with zero, we set a new EDM limit, |d| < 1.9E-19 e-cm (95% C.L.). This represents factor 5 improvement over previous best limit EDM.
A higher precision measurement of the anomalous g value, a(mu)=(g-2)/2, for positive muon has been made at Brookhaven Alternating Gradient Synchrotron, based on data collected in year 2000. The result a(mu(+))=11 659 204(7)(5)x10(-10) (0.7 ppm) is good agreement with previous measurements and an error about one-half that combined data. present world average experimental value a(mu)(expt)=11 203(8)x10(-10) ppm).
The TOTEM Experiment will measure the total pp cross-section with luminosity-independent method and study elastic diffractive scattering at LHC. To achieve optimum forward coverage for charged particles emitted by collisions in interaction point IP5, two tracking telescopes, T1 T2, be installed on each side pseudorapidity region 3.1 ⩽ |η| 6.5, Roman Pot stations placed distances of ±147 m ±220 from IP5. Being an independent experiment but technically integrated into CMS, first operate...
Received 22 August 2002DOI:https://doi.org/10.1103/PhysRevLett.89.129903©2002 American Physical Society
The TOTEM collaboration has measured the proton-proton total cross section at $\sqrt{s}=13$ TeV with a luminosity-independent method. Using dedicated $β^{*}=90$ m beam optics, Roman Pots were inserted very close to beam. inelastic scattering rate been by T1 and T2 telescopes during same LHC fill. After applying optical theorem is $σ_{\rm tot}=(110.6 \pm 3.4$) mb, well in agreement extrapolation from lower energies. This method also allows one derive elastic sections: el} = (31.0 1.7)$ mb...
The TOTEM experiment at the LHC has performed first measurement $\sqrt{s} = 13$ TeV of $ρ$ parameter, real to imaginary ratio nuclear elastic scattering amplitude $t=0$, obtaining following results: $ρ= 0.09 \pm 0.01$ and 0.10 0.01$, depending on different physics assumptions mathematical modelling. unprecedented precision measurement, combined with total cross-section measurements in an energy range larger than 10 (from 2.76 13 TeV), implied exclusion all models classified published by...
The spin precession frequency of muons stored in the $(g-2)$ storage ring has been analyzed for evidence Lorentz and CPT violation. Two violation signatures were searched for: a nonzero $\Delta\omega_{a}$ (=$\omega_{a}^{\mu^{+}}-\omega_{a}^{\mu^{-}}$); sidereal variation $\omega_{a}^{\mu^{\pm}}$. No significant effect is found, following limits on standard-model extension parameters are obtained: $b_{Z} =-(1.0 \pm 1.1)\times 10^{-23}$ GeV; $(m_{\mu}d_{Z0}+H_{XY}) = (1.8 6.0 \times 10^{-23})$...
2nd workshop on the implications of HERA for LHC physics. Working groups: Parton Density Functions Multi-jet final states and energy flows Heavy quarks (charm beauty) Diffraction Cosmic Rays Monte Carlos Tools
Silicon detectors for the Roman Pots of large hadron collider TOTEM experiment aim full sensitivity at edge where a terminating structure is required electrical stability. This work provides an innovative approach reducing conventional width to less than 100 microns, still using standard planar fabrication technology. The objective this new development decouple electric behaviour surface from sensitive volume within tens microns. explanation basic principle together with experimental...
Proton-proton elastic scattering has been measured by the TOTEM experiment at CERN Large Hadron Collider √s = 7 TeV in special runs with Roman Pot detectors placed as close to outgoing beam seven times transverse size. The differential cross-section measurements are reported |t|-range of 0.36 2.5 GeV2. Extending range data low t values from 0.02 0.33 GeV2, and utilizing luminosity CMS, total proton-proton cross section is be (98.3 ±0.2stat ±2.8syst) mb.
Beam collimation in high-energy colliders is customarily carried out by means of massive amorphous absorbers surrounding the circulating beam. Several studies were performed last decades to establish an innovative technique that relies on particle deflection channeling between crystalline planes a bent crystal. We report operational use crystal Large Hadron Collider was achieved during special high-${\ensuremath{\beta}}^{\ensuremath{\ast}}$ physics run with low-intensity beams, representing...