J. Gerber

ORCID: 0000-0001-6470-6553
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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
  • Nuclear physics research studies
  • Atomic and Molecular Physics
  • X-ray Spectroscopy and Fluorescence Analysis
  • Nuclear Physics and Applications
  • Advanced Chemical Physics Studies
  • Ion-surface interactions and analysis
  • Atomic and Subatomic Physics Research
  • Quantum, superfluid, helium dynamics
  • Advanced NMR Techniques and Applications
  • Dark Matter and Cosmic Phenomena
  • Particle accelerators and beam dynamics
  • Electron and X-Ray Spectroscopy Techniques
  • Mass Spectrometry Techniques and Applications
  • Diamond and Carbon-based Materials Research
  • Computational Physics and Python Applications
  • Astrophysical Phenomena and Observations
  • Superconducting Materials and Applications
  • Particle Detector Development and Performance
  • Neutrino Physics Research
  • Pulsars and Gravitational Waves Research
  • Particle Accelerators and Free-Electron Lasers
  • Laser-Plasma Interactions and Diagnostics

Columbia University
2023-2024

Macquarie University
2014

Institut de Recherche Dupuy de Lôme
2003

University of Bonn
1999

Centre de Gestion Scientifique
1993-1996

Institut National de Physique Nucléaire et de Physique des Particules
1969-1995

Centre National de la Recherche Scientifique
1990-1995

Université de Strasbourg
1975-1993

Karlsruhe Institute of Technology
1992

Aptiv (United States)
1989-1992

Nostalgia is a frequently experienced complex emotion, understood by laypersons in the United Kingdom and States of America to (a) refer prototypically fond, self-relevant, social memories (b) be more pleasant (e.g., happy, warm) than unpleasant sad, regretful). This research examined whether people across cultures conceive nostalgia same way. Students 18 countries 5 continents (N = 1,704) rated prototypicality 35 features nostalgia. The samples showed high levels agreement on rank-order...

10.1037/a0036790 article EN Emotion 2014-01-01

The g factors of the first ${2}^{+}$ states and $B(E2)$ values ${(2}_{1}^{+}\ensuremath{\rightarrow}{0}_{1}^{+})$ transitions have been determined with high precision for all stable doubly even Zn isotopes employing combined technique projectile Coulomb excitation in inverse kinematics transient magnetic fields. In addition, this systematic study was supplemented by a measurement radioactive ${}^{62}\mathrm{Zn}$ ${(T}_{1/2}=9.2 h)$ formed an $\ensuremath{\alpha}$-transfer reaction...

10.1103/physrevc.65.034308 article EN Physical Review C 2002-02-14

$g$ factors have been measured for the first ${2}^{+}$ states of ${}^{58,60,62,64}\mathrm{Ni}$ isotopes employing combined technique projectile Coulomb excitation and transient magnetic fields. Lifetimes low-lying were redetermined using Doppler shift attenuation method technique. The same target has used in all measurements provided by ion source accelerator. These conditions guarantee high reliability precision as demonstrated earlier experiments. g deduced $B(E2)$ values are well...

10.1103/physrevc.63.064306 article EN Physical Review C 2001-05-02

Measurements of magnetic moments and lifetimes 2(+)(1) 4(+)(1) states (46,48)Ti (50,52)Cr were performed with high accuracy via projectile Coulomb excitation the technique transient fields. The quality data allows for first time to establish stringent constraints on large scale shell model calculations. Whereas global behavior is well explained by full fp calculations, distinct deviations in g factors B(E2) values from theoretical predictions can be attributed excitations 40Ca core. This...

10.1103/physrevlett.84.416 article EN Physical Review Letters 2000-01-17

HEX-P is a probe-class mission concept that will combine high spatial resolution X-ray imaging ($<10"$ FWHM) and broad spectral coverage (0.2-80 keV) with an effective area far superior to current facilities' (including XMM-Newton NuSTAR). These capabilities enable revolutionary new insights into variety of important astrophysical problems. We present scientific objectives simulations observations the Galactic Center (GC) Bulge. demonstrate unique powerful observatory for studying both point...

10.3389/fspas.2023.1292130 article EN cc-by Frontiers in Astronomy and Space Sciences 2024-01-08

Precession measurements have been performed on nuclear-excited nitrogen ions recoiling in magnetized iron employing the implantation perturbed-angular-correlation technique. The transient magnetic field, calibrated with $^{16}\mathrm{N}$(${1}^{\ensuremath{-}}$) state, was found to be enhanced by a factor of 2.1(5) over empirically adjusted Lindhard-Winther prediction. A negative sign determined for this $g$ and value $g=+0.9(3)$ that $^{15}\mathrm{N}({\frac{5}{2}}^{+})$ state.NUCLEAR...

10.1103/physrevc.11.1976 article EN Physical Review C 1975-06-01

Abstract We report timing and broadband spectral analysis of a Galactic X-ray source, CXOGBS J174517.0−321356 (J1745), with 614 s periodicity. Chandra discovered the source in direction Bulge. Gong proposed that J1745 was either an intermediate polar (IP) mass ∼1 M ⊙ , or ultracompact binary (UCXB). To confirm J1745's nature, we jointly fit XMM-Newton NuSTAR spectra, ruling out UCXB origin. have developed physically realistic model considers finite magnetosphere radius, absorption from...

10.3847/1538-4357/ace90c article EN cc-by The Astrophysical Journal 2023-08-31

$g$ factors and lifetimes have been measured for the first ${2}^{+}$ ${4}^{+}$ states of ${}^{46,48}\mathrm{Ti}$ ${}^{50,52}\mathrm{Cr}$ employing combined technique projectile Coulomb excitation transient magnetic fields. The same target was used in all measurements. individual isotopes were provided by ion source accelerator. These conditions guarantee high reliability precision as demonstrated earlier experiments. While global behavior data is well explained full $\mathrm{fp}$ shell model...

10.1103/physrevc.62.024305 article EN Physical Review C 2000-07-10

High precision g factors and $B(E2)$ values were obtained in measurements of the first ${2}^{+}$ states ${}^{58\ensuremath{-}64}\mathrm{Ni}$ using technique projectile Coulomb excitation combination with transient magnetic fields. The new results are well explained by large-scale shell model calculations which, for ${}^{58\ensuremath{-}62}\mathrm{Ni},$ up to $t=5$ nucleons excited from ${f}_{7/2}$ into remaining $\mathrm{fp}$ orbits. A complete calculation was carried out...

10.1103/physrevc.63.021302 article EN Physical Review C 2000-12-28

Measurements of g factors and lifetimes the 21+ states in 36,38Ar have been performed via α-transfer reactions using 32S 34S ions inverse kinematics combined with techniques transient magnetic fields Doppler-shift-attenuation. The variations, neutron number, measured B(E2) values 36,38,40Ar explained by large-scale shell model calculations. good agreement achieved between experiment theory demonstrates impact effective nucleon–nucleon interactions magic N=20 closure. present new results are...

10.1016/j.physletb.2005.10.052 article EN cc-by Physics Letters B 2005-10-27

The g factors of the short-lived ${2}_{1}^{+},{4}_{1}^{+}$, and ${3}_{1}^{\ensuremath{-}}$ states in $^{64}\mathrm{Zn}$ ${2}_{1}^{+},{4}_{1}^{+},{2}_{2}^{+}$, $^{68}\mathrm{Zn}$ have been measured using combined technique projectile Coulomb excitation inverse kinematics transient magnetic fields. In addition, $B(E2)$'s deduced from remeasured lifetimes several excited employing Doppler-shift-attenuation method. Whereas present data for ${2}_{1}^{+}$ agree very well with our previous results,...

10.1103/physrevc.71.034303 article EN Physical Review C 2005-03-08

From a bubble-chamber experiment, we studied the $\overline{p}d\ensuremath{\rightarrow}{p}_{s}\overline{p}p{\ensuremath{\pi}}^{\ensuremath{-}}, {p}_{s}\overline{p}p{\ensuremath{\pi}}^{\ensuremath{-}}{\ensuremath{\pi}}^{0}, {p}_{s}\overline{n}p{\ensuremath{\pi}}^{\ensuremath{-}}{\ensuremath{\pi}}^{\ensuremath{-}}$ reactions at 5.55 GeV/c in order to see whether $\ensuremath{\Delta}\ensuremath{-}\ensuremath{\Delta}$ component of deuteron wave function can be observed our data. This was...

10.1103/physrevlett.33.312 article EN Physical Review Letters 1974-07-29
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