A. F. Zeller

ORCID: 0000-0003-0211-2308
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About
Contact & Profiles
Research Areas
  • Nuclear physics research studies
  • Nuclear Physics and Applications
  • Particle accelerators and beam dynamics
  • Superconducting Materials and Applications
  • X-ray Spectroscopy and Fluorescence Analysis
  • Atomic and Molecular Physics
  • Ion-surface interactions and analysis
  • Quantum Chromodynamics and Particle Interactions
  • Spacecraft and Cryogenic Technologies
  • Mass Spectrometry Techniques and Applications
  • Astronomical and nuclear sciences
  • Chemical Reactions and Isotopes
  • Particle Accelerators and Free-Electron Lasers
  • Magnetic confinement fusion research
  • Particle Detector Development and Performance
  • Electron and X-Ray Spectroscopy Techniques
  • Astro and Planetary Science
  • Rare-earth and actinide compounds
  • Carbon Nanotubes in Composites
  • Inorganic and Organometallic Chemistry
  • Nuclear Materials and Properties
  • Advanced Thermodynamic Systems and Engines
  • Semiconductor materials and devices
  • Muon and positron interactions and applications
  • Chemical Synthesis and Analysis

Particle Beam Lasers (United States)
2022

Michigan State University
2005-2018

National Superconducting Cyclotron Laboratory
2001-2017

Facility for Rare Isotope Beams
1996-2012

Australian National University
1976-2008

Oak Ridge National Laboratory
2002

Brookhaven National Laboratory
2002

Argonne National Laboratory
2002

University Children’s Hospital Basel
1993

V. G. Khlopin Radium Institute
1985

Palladium nanoparticles (PdNp) were revealed as an efficient hydrogen isotope exchange catalyst for the deuterium and tritium labeling of benzylic positions complex molecules. A practical way to obtain small palladium apply them a (HIE) is presented. Several model compounds popular bioactive molecules submitted HIE reactions catalyzed by PdNp. Benzylic situated far away from heteroatoms labeled with high isotopic enrichments. The observed non-directed gave rise regioselectivities...

10.1002/anie.202109043 article EN Angewandte Chemie International Edition 2021-08-23

Momentum spectra have been measured for the reaction $^{11}\mathrm{B}$${(}^{7}$Li${,}^{8}$B${)}^{10}$Li at 130 MeV and laboratory angles of 5\ifmmode^\circ\else\textdegree\fi{} 3.5\ifmmode^\circ\else\textdegree\fi{}. There is strong evidence existence a broad state in unstable nucleus $^{10}\mathrm{Li}$, corresponding to single p-wave neutron resonance unbound decay by 538\ifmmode\pm\else\textpm\fi{}62 keV with wdith...

10.1103/physrevc.49.279 article EN Physical Review C 1994-01-01

We report initial results of exposing low-Z solid and high-Z liquid targets to 150-ns, 4/spl times/10/sup 12/ proton pulses with spot sizes on the order 1 2 mm. The energy deposition density approached 100 J/g. Diagnostics included fiberoptic strain sensors target high-speed photography targets. This work is part R&D program Neutrino Factory Muon Collider Collaboration.

10.1109/pac.2001.986739 article EN PACS2001. Proceedings of the 2001 Particle Accelerator Conference (Cat. No.01CH37268) 2002-11-14

Fast neutron imaging has a great potential as nondestructive technique for testing large objects. The main factor limiting applications of this is detection technology, offering relatively poor spatial resolution images and low efficiency, which results in very long exposure times. Therefore, research on development scintillators fast high importance. A comparison the light output, gamma radiation sensitivity commercially available scintillator screens composed PP/ZnS:Cu PP/ZnS:Ag different...

10.3390/jimaging3040060 article EN cc-by Journal of Imaging 2017-12-10

In an attempt to clarify the situation regarding low-lying structure of ${}^{10}\mathrm{Li}$, a spectroscopic measurement ${}^{10}\mathrm{Li}$ with ${}^{9}\mathrm{Be}{(}^{9}\mathrm{Be}{,}^{8}\mathrm{B}{)}^{10}\mathrm{Li}$ reaction at ${E(}^{9}\mathrm{Be})=40.1(1)$ MeV/nucleon was performed using S800 spectrograph Michigan State University. The data are fit best single p-wave resonance $\ensuremath{-}{S}_{n}=0.500(60) \mathrm{MeV}$ width $\ensuremath{\Gamma}=400(60) \mathrm{keV}$. No higher...

10.1103/physrevc.60.064322 article EN Physical Review C 1999-11-22

The heavy-ion charge exchange reaction $^{12}$C${(}^{12}$C,$^{12}$N${)}^{12}$ B has been studied at E${(}^{12}$C)=35 MeV/nucleon. Angular distributions in the range 3.7--12.1\ifmmode^\circ\else\textdegree\fi{} (c.m.) have measured for ${1}^{+}$ (0.0 MeV), ${2}^{+}$ (0.95 ${2}^{\mathrm{\ensuremath{-}}}$ (1.67 and ${4}^{\mathrm{\ensuremath{-}}}$,${2}^{\mathrm{\ensuremath{-}}}$ (4.5 MeV) states $^{12}$B. A broad peak 7.8 MeV excitation was also observed. Microscopic one-step distorted-wave Born...

10.1103/physrevc.33.1333 article EN Physical Review C 1986-04-01

Red emitting CaTiO3:Pr phosphors with a nominal composition of Ca0.998+xPr0.002TiO3+δ (0.02≤x≤0.04) were prepared by solid state reactions different thermal post treatments and characterized X-ray diffraction, transmission electron microscopy photoluminescence. The Ca excess exhibited complete solubility up to 4% in the samples treated at 1400 °C but segregation form Ruddlesden-Popper phases (Ca3Ti2O7 - Ca4Ti3O10) was observed 1500 °C. increase temperature for stoichiometric showed monotonic...

10.1364/ome.2.000405 article EN cc-by Optical Materials Express 2012-03-07

Counter-telescope and recoil-coincidence techniques were used to observe the reaction $^{18}\mathrm{O}$($^{18}\mathrm{O}$, $^{14}\mathrm{O}$)$^{22}\mathrm{O}$ at 100 MeV. These data indicate a mass excess for $^{22}\mathrm{O}$ of 9.48\ifmmode\pm\else\textpm\fi{}0.10 MeV, which differs by \ensuremath{\sim}2.0 MeV from previous value, but is in excellent agreement with several theoretical predictions.

10.1103/physrevlett.37.130 article EN Physical Review Letters 1976-07-19

The two Cyclotron gas stopper superconducting solenoid coils will be kept cold at 4.25 to 4.6 K using three pulse tube coolers per coil. These are designed produce from 1.35 1.6 W cooler when the first stage is about 45 K. cyclotron so that they can separated while cold, but unpowered. This design decision means maintenance performed on cyclotron. MSU decided would cooled down 300 4 connected a thermal-siphon cooling loop. was in part influenced by have axis perpendicular direction of...

10.1063/1.4860890 article EN AIP conference proceedings 2014-01-01

Cold diodes and resistors in parallel with the coils are keys components passive quench protection system of low-current (high inductance) superconducting magnets. The prevent current from flowing circuits that sections coil when magnet is being charged or discharged. use reduce peak voltages to ground and, some cases, hot-spot temperature during a quench. This paper presents measurements onset (low current) forward voltage several power as function magnetic field.

10.1109/tasc.2014.2362574 article EN IEEE Transactions on Applied Superconductivity 2015-01-20

Abstract Palladium nanoparticles (PdNp) were revealed as an efficient hydrogen isotope exchange catalyst for the deuterium and tritium labeling of benzylic positions complex molecules. A practical way to obtain small palladium apply them a (HIE) is presented. Several model compounds popular bioactive molecules submitted HIE reactions catalyzed by PdNp. Benzylic situated far away from heteroatoms labeled with high isotopic enrichments. The observed non‐directed gave rise regioselectivities...

10.1002/ange.202109043 article EN Angewandte Chemie 2021-08-23

Neutrino beams from the decay of muons in a storage ring offer prospect very high flux, well-understood spectra, and equal numbers electron muon neutrinos, as desirable for detailed exploration neutrino oscillations via long baseline detectors. Such require large muons, hence performance target station at which 1-4 MW proton beam 16-24 GeV impinges on compact target, all inside field solenoid channel to capture much phase volume soft pions possible. A first concept was based carbon reported...

10.1109/pac.2001.986755 article EN PACS2001. Proceedings of the 2001 Particle Accelerator Conference (Cat. No.01CH37268) 2002-11-14

The $^{28}\mathrm{Si}$($^{4}\mathrm{He}$,$^{8}\mathrm{He}$)$^{24}\mathrm{Si}$ reaction has been used to determine the mass of $^{24}\mathrm{Si}$. $Q$ value and excess were found be -61.433\ifmmode\pm\else\textpm\fi{}0.021 10.782\ifmmode\pm\else\textpm\fi{}0.022 MeV, respectively. $^{24}\mathrm{Si}$ completes fifth member $A=24$ isobaric quintet. quintet members are in good agreement with quadratic multiplet equation.NUCLEAR REACTIONS $^{28}\mathrm{Si}$($^{4}\mathrm{He}$,...

10.1103/physrevc.22.17 article EN Physical Review C 1980-07-01
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