C. Kleffner’s research while affiliated with GSI Helmholtz Centre for Heavy Ion Research and other places

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Publications (40)


New Test of Modulated Electron Capture Decay of Hydrogen-Like 142^{142}Pm Ions: Precision Measurement of Purely Exponential Decay
  • Preprint

July 2019

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146 Reads

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B. Akkus

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[...]

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the TBWD Collaboration

An experiment addressing electron capture (EC) decay of hydrogen-like 142^{142}Pm60+^{60+} ions has been conducted at the experimental storage ring (ESR) at GSI. The decay appears to be purely exponential and no modulations were observed. Decay times for about 9000 individual EC decays have been measured by applying the single-ion decay spectroscopy method. Both visually and automatically analysed data can be described by a single exponential decay with decay constants of 0.0126(7) s1^{-1} for automatic analysis and 0.0141(7) s1^{-1} for manual analysis. If a modulation superimposed on the exponential decay curve is assumed, the best fit gives a modulation amplitude of merely 0.019(15), which is compatible with zero and by 4.9 standard deviations smaller than in the original observation which had an amplitude of 0.23(4).


Fig. 3. (Top) Number of EC-decays per 0.63 s as determined in the automatic analysis (8839 EC decays in total). The data points are fitted with a pure exponential function (solid line). (Bottom) Same as (Top) but for one of the manual analyses (9001 EC decays in total), see text.
Fig. 4. Disappearance of a stable 142 Nd 60+ ion which is due to non-radioactive losses of the ions from the ring. The entire measurement cycle is shown.
Fig. 5. Traces of 142 Nd 60+ daughter ions without a significant tail. If several daughter ions are present at the time of such decay, the identification of the latter in a manual analysis is complicated. The automatic analysis however finds decays independent of the occurrence of a cooling tail and thus should be less prone to overlooking such cases.
New Test of Modulated Electron Capture Decay of Hydrogen-Like 142Pm Ions: Precision Measurement of Purely Exponential Decay
  • Article
  • Full-text available

July 2019

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316 Reads

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26 Citations

Physics Letters B

An experiment addressing electron capture (EC) decay of hydrogen-like Pm60+142 ions has been conducted at the experimental storage ring (ESR) at GSI. The decay appears to be purely exponential and no modulations were observed. Decay times for about 9000 individual EC decays have been measured by applying the single-ion decay spectroscopy method. Both visually and automatically analysed data can be described by a single exponential decay with decay constants of 0.0126(7)s−1 for automatic analysis and 0.0141(7)s−1 for manual analysis. If a modulation superimposed on the exponential decay curve is assumed, the best fit gives a modulation amplitude of merely 0.019(15), which is compatible with zero and by 4.9 standard deviations smaller than in the original observation which had an amplitude of 0.23(4). Keywords: Two body weak decay, Orbital electron capture, Single particle decay spectroscopy, Heavy ion storage ring

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STATUS OF THE FAIR PROTON LINAC

October 2018

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348 Reads

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5 Citations

As part of the accelerator chain for antiproton production of the FAIR facility, a special high-intensity short pulsed 325 MHz Proton Linac is being developed [1], [2]. The Proton Linac is designed to deliver a beam current of 70 mA with an energy of 68 MeV. A 2.45 GHz ECR source designed for the generation of 100 mA beams with an energy of 95 keV is currently being tested at CEA/Saclay. The production of the structure of the IAP ladder RFQ is nearly completed. All parts of the RFQ vacuum chambers have been successfully copperplated at the GSI. Seven Thales Klystrons have been delivered to GSI at the beginning of 2018 and are nearly ready for use. The completion of the setup of the HV modulator is expected mid of the year 2019. The state of procurement Figure 2: Proton Linac Interface Wall with the construction area for the Proton Linac in front.


High intensity proton injector for the FAIR p-linac

September 2018

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66 Reads

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2 Citations

AIP Conference Proceedings

For the Facility for Antiproton and Ion Research (FAIR) a compact proton linac will produce proton beams with energy of 68 MeV that will be injected into upgraded Heavy Ion Synchrotron (SIS 18), accelerated to 4 GeV, and further accelerated to 30 GeV in SIS 100. The commissioning of the proton injector which would serve for the injection into the proton linac has already started at CEA/Saclay. The ion source operating with a microwave frequency of 2.45 GHz based on Electron Cyclotron Resonance (ECR) plasma production with two coils each with 87.5 mT magnetic field, will deliver a 100 mA proton beam at 95 keV of energy. The Low Energy Beam Transport (LEBT) including two short solenoids system and integrated steerers will transport the proton beam to the RFQ entrance with an expected emittance lower than 0.3π mm mrad (normalized, rms). After the LEBT an electrostatic chopper will be mounted in front of RFQ to shorten the beam pulse to 36 µs. This paper presents the status of the commissioning phases including first results of proton injector.


Figure 1: The beam envelope for optics used for the most part of 2014 run. Only part up to the pion target is shown.
Figure 2: The beam envelope for the new, proposed optics.
UPGRADE OF GSI HADES BEAM LINE IN PREPARATION FOR HIGH INTENSITY RUNS

May 2017

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101 Reads

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4 Citations

HADES is a fixed target experiment using SIS18 heavy-ion beams. It investigates the microscopic properties of matter formed in heavy-ion, proton and pion-induced reactions in the 1-3.5 GeV/u energy regime. In 2014 HADES used a secondary pion beam produced by interaction between high-intensity nitrogen primary beam and a beryllium target. In these conditions beam losses, generated by slow extraction and beam transport to the experimental area, led to activation of the beam line elements and triggered radiation alarms. The primary beam intensity had to be reduced and the beam optics modified in order to keep radiation levels within the allowed limits. Similar beam conditions are requested by HADES experiment for upcoming run in 2018 and in the following years. Therefore, a number of measures have been proposed to improve beam transmission and quality. These measures are: additional shielding, additional beam instrumentation, modification of beam optics and increase of vacuum chambers' apertures in critical locations. The optics study and preliminary results of FLUKA simulations for optimization of location of loss detectors are presented.


Status and outlook of the CRYRING@ESR project

January 2017

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82 Reads

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13 Citations

Hyperfine Interactions

Once operational, CRYRING@ESR will store and decelerate ions delivered by the experimental storage ring ESR at energies well below those of ESR. In addition to that, CRYRING@ESR has an electron cooler operating with an ultracold electron beam, allowing to provide cooled ion beams for precision experiments. These ions will be delivered to a broad range of experiments presently in preparation; either in-ring or extracted to a dedicated beamline for experiments. An overview and status report of the installation and commissioning of the CRYRING-@ESR storage ring for highly charged ions at the GSI Helmholtzzentrum für Schwerionenforschung is presented. The installation of this storage ring started in 2014 and was completing end of 2016, when this publication was written.


Figure 1. The RCE spectra of 2s-2p 3/2 transition in the 190 MeV/u Li-like U 89+ beam from (a) SIS and (b) ESR .
Enhancing the energy resolution of resonant coherent excitation using the cooled U 89+ beam extracted from the ESR

September 2015

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32 Reads

Journal of Physics Conference Series

We report on the resonant coherent excitation (RCE) of the 2s-2p3/2 transition in Li-like U89+ with an enhanced energy resolution, which was achieved by reducing the projectiles momentum spread. The kinetic temperature of the beam was decreased by electron cooling in the ESR, and the collisional momentum broadening in the target was suppressed by the use of thin crystal (1.0 and 2.5 μm-thick). The resonance width was observed to be ~1.4 eV in FWHM, which is three-times narrower than that from the previous work.



Radioactive beam accumulation for a storage ring experiment with an internal target

January 2013

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16 Reads

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5 Citations

A radioactive 56Ni beam was successfully accumulated for an experiment with an internal hydrogen target at the storage ring ESR of GSI, Germany. The radioactive beam was produced and separated at the GSI fragment separator from a stable 58Ni beam. About 8 · 10456Ni28+ions were injected into the ESR on a high relative momentum orbit. The beam was subjected to stochastic precooling, bunched and transported to a low relative momentum orbit. Slightly below this deposition momentum, the beam was accumulated and continuously cooled by means of electron cooling. After accumulating about 60 shots, this beam was prepared to overlap with the ESR internal gas jet target for a nuclear physics experiment. Data acquisition was started with a stored beam of roughly 4.8 · 10 6 particles in the beginning.


Status of linac beam commissioning for the italian hadron therapy center CNAO

June 2010

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54 Reads

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1 Citation

The CNAO (Centro Nazionale di Adroterapia Oncologica), located in Pavia (Italy), is a dedicated clinical synchrotron facility for cancer therapy using high energy proton and Carbon beams. The 400 MeV/u synchrotron is injected by a 216.8 MHz 7 MeV/u linac composed by a low energy beam transport (fed by 2 ion sources), a 400 keV/u 4-rod type RFQ and a 20 MV IH-DTL. The commissioning of the two ECRIS ion sources and the low-energy line was successfully completed at the end of January 2009 reaching the proper beam conditions for injection into the RFQ. After installation and conditioning, the RFQ was commissioned with beam by the GSI-CNAO-INFN team in March 2009. The beam tests results are presented and compared to the design parameters.


Citations (26)


... At first, a modulation of about 20% amplitude and 7 s period of the expected exponential decay curve was observed for both of the nuclei [71]. Subsequently, a new measurement of the 142 Pm lifetime was compatible with a purely exponential decay, with a possible modulation of, at most, about 2% amplitude [72]. With our new 40 K setup we will be able to test the above-mentioned parameter space region, in a different EC nuclear decay process, with about 4 orders of magnitude better sensitivity. ...

Reference:

Weak nuclear decays deep-underground as a probe of axion dark matter
New Test of Modulated Electron Capture Decay of Hydrogen-Like 142Pm Ions: Precision Measurement of Purely Exponential Decay

Physics Letters B

... HADES [2] is one of the largest experiments and it is placed at the end of an about 160 meter long beamline starting at the magnetic septum of SIS18. The beamline contains 21 individually powered quadrupoles and two active dipoles tilted by 21.7 • to bring the beam to the elevated position of the experimental area [3,4]. HADES is designed to work in two main modes, using either primary or secondary particles. ...

UPGRADE OF GSI HADES BEAM LINE IN PREPARATION FOR HIGH INTENSITY RUNS

... Optimization with multi-objective particle swarm (MOPSA) shown similar result with fast convergence. A 3D Pareto front has been generated for proton injector is also shown in Fig. 8. 18 The outcome of this optimization study and heuristic analysis of the MTI demonstrate that a low-loss injection for several emittance over many turns for various proton currents could be achieved. Three case with brilliance of 4, 5 and 6 mA/(mm mrad) has been marked in Fig. 8. ...

STATUS OF THE FAIR PROTON LINAC

... Experimental access to the binding energies of few-electron heavy ions is usually provided by the X-ray spectroscopy of characteristic transitions, in particular the K α (n = 2 → n = 1) transitions, which occur between the most strongly bound states [5]. For such studies, storage rings equipped with electron cooler devices are the facilities of choice, e.g., the Experimental Storage Ring (ESR) [6] or the CRYRING@ESR [7,8], both located at GSI, Darmstadt. Electron cooling exploits the Coulomb interaction between stored ions and a cold electron beam to reduce the emittance as well as the kinetic energy dispersion [9] of the ion beam, thus reducing the Doppler broadening of the spectral lines emitted by the ions. ...

Status and outlook of the CRYRING@ESR project

Hyperfine Interactions

... They are made of a moveable screen (chromox in our case), and a camera which registers the image of the beam-provoked scintillation. The system of scintillating screens installed in HEST is being upgraded from analog cameras, giving only an image of the beam spot on CRT screens, to a fully digital CUPID system [3]. Waiting for a full transition some of the cameras were digitized using frame grabbers [4] and it became possible to analyse the transverse beam profiles. ...

CUPID: New System for Scintillating Screen based Diagnostics

... After an additional stripper stage, fragments of 118 Te with a charge state of q ¼ 52 þ were filtered out and injected into the ESR at 400 MeV= nucleon. In the ring, stochastic cooling [25] and beam accumulation [26] of several injections was applied in order to increase the stored intensity to about 7 × 10 6 ions. Subsequently, the ions were decelerated to low energies and subjected to permanent electron cooling [27] in order to provide a beam of small momentum spread Δp=p ∼ 10 −5 and also to compensate for energy loss in the H 2 target [28]. ...

Radioactive beam accumulation for a storage ring experiment with an internal target
  • Citing Article
  • January 2013

... horizontal and vertical) or installing rotating beam lines, the so-called gantries. Nowadays, gantries for protons are present in most facilities; on the contrary, a gantry for carbon ions must have a higher weight and size, and up to now only the Heidelberg facility is equipped with a carbon ion gantry (weighing 600 ton, with a diameter of 13 m compared with the standard dimensions for protons of 100 ton and 10 m) that is being commissioned [32]. ...

COMMISSIONING OF THE CARBON BEAM GANTRY AT THE HEIDELBERG ION THERAPY (HIT) ACCELERATOR

... This IH-DTL accelerates the Hbeam from 3 MeV to 7 MeV in 1.1 m. The comparison of the effective shunt impedance between the cavity at THU and other IH-DTLs [4][5][6][7][8] is shown in Fig. 1. The effective shunt impedance decreases with the increase of the beam velocity and the RF frequency. ...

STATUS OF THE LINAC COMPONENTS FOR THE ITALIAN HADRONTHERAPY CENTRE CNAO
  • Citing Article