2011
DOI: 10.1088/1742-6596/298/1/012002
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Status and recent developments at the polarized-electron injector of the superconducting Darmstadt electron linear accelerator S-DALINAC

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Cited by 11 publications
(7 citation statements)
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“…Similarly, we observe normalized transverse rms emittances of x = 0.108 mm mrad and y = 0.194 mm mrad. This is a good match compared to the values measured at operating photo-electron guns [9,10]. An rms energy spread of ∆E rms = 48.4 eV is observed at the chamber exit for a field strength of 2.99 MV m −1 on the photocathode surface at −300 kV bias voltage, compared to 84 eV with 2.5 MV m −1 at −200 kV, as reported in [55].…”
Section: B Particle Tracking Resultssupporting
confidence: 86%
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“…Similarly, we observe normalized transverse rms emittances of x = 0.108 mm mrad and y = 0.194 mm mrad. This is a good match compared to the values measured at operating photo-electron guns [9,10]. An rms energy spread of ∆E rms = 48.4 eV is observed at the chamber exit for a field strength of 2.99 MV m −1 on the photocathode surface at −300 kV bias voltage, compared to 84 eV with 2.5 MV m −1 at −200 kV, as reported in [55].…”
Section: B Particle Tracking Resultssupporting
confidence: 86%
“…However, a high bias voltage is desired to provide sufficient initial acceleration for the beam and to minimize emittance in spite of space-charge effects. Since common negative bias voltages of state-of-the-art DC photo-electron guns are in the range of −100 kV to −500 kV [8][9][10][11], the combination of * peter.foerster@cem.temf.de such high voltages with a suitable electrode geometry and material poses a great challenge for the design of compact guns. The decisive limiting factor is the field emission threshold of the electrode material, imposing a maximum electric field strength on the geometric design.…”
Section: Introductionmentioning
confidence: 99%
“…Email address: g.weber@gsi.de (G. Weber) During the last two years, such polarimeters were applied in a series of polarization-resolved bremsstrahlung measurements that have been carried out at the teststand of the polarized electron source SPIN [13,14] at the Technical University of Darmstadt. In these experiments the polarization transfer was studied in collisions of polarized electrons with gold foils of about 100 µg/cm 2 thickness and at an impact energy of 100 keV [15,16].…”
Section: Introductionmentioning
confidence: 99%
“…Comparably, albeit at a smaller scale, a dedicated test stand for DC photo-gun research and development, Photo-CATCH, with a 60 kV photo-gun and 60 keV beamline has been constructed at the Institut für Kernphysik of the Technische Universität Darmstadt. It provides an environment for research and development to optimize the existing DC photo-gun, which is located at the Spin-Polarized Injector SPIn of the in-house electron accelerator S-DALINAC [11][12][13]. A collaboration between the two institutes has been established in order to effectively capitalize on our joint area of research.…”
Section: Introductionmentioning
confidence: 99%