2014
DOI: 10.1109/tasc.2013.2295921
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Test of Short Mockups for Optimization of Superconducting Undulator Coils

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Cited by 12 publications
(11 citation statements)
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“…The copper to non-copper ratio of the wire is 0.6. The operation current in the NbTi coils must be below the critical current which depends on the maximum magnetic field and the temperature (4.2 K) in the coil packs (Casalbuoni et al, 2014;Karasev et al, 2013). Through simulation, we obtained the operation current and the critical current in the NbTi coils versus the maximum magnetic field in the superconductors, and the dependence of the operation current with respect to the magnetic field on-axis, as shown in Fig.…”
Section: Simulationmentioning
confidence: 99%
“…The copper to non-copper ratio of the wire is 0.6. The operation current in the NbTi coils must be below the critical current which depends on the maximum magnetic field and the temperature (4.2 K) in the coil packs (Casalbuoni et al, 2014;Karasev et al, 2013). Through simulation, we obtained the operation current and the critical current in the NbTi coils versus the maximum magnetic field in the superconductors, and the dependence of the operation current with respect to the magnetic field on-axis, as shown in Fig.…”
Section: Simulationmentioning
confidence: 99%
“…Above this limit of the engineering current density, the ohmic losses become untreatable. For the same period length and vacuum gap, especially for long period lengths, superconducting undulators can produce higher magnetic peak fields on axis than the permanent magnet ones 27 . Superconducting undulators can also be used to obtain the same magnetic peak field using a larger vacuum gap, which allows to reduce the frequency cut off of the vacuum chamber, and to transmit most of the THz radiation of interest, starting from the first harmonic up to higher frequencies.…”
Section: Feasibility Of the Thz Superconducting Undulatormentioning
confidence: 99%
“…The measured flux through a pinhole with 50 μm diameter at 14.9 m from the source, using a Si 111 channel cut monochromator and an ionization chamber (Oken Ltd, Japan) [4], is shown in Fig. 2a (thick dark blue line) as a function of the photon energy.…”
Section: Scu15mentioning
confidence: 99%
“…(a) Flux through a slit of 1 mm x 1 mm at 10 m from the source calculated using the ANKA beam parameters and a beam current of 100 mA, a beam stay clear of 7 mm and the measured magnetic field of the SCU20 mockup (blue line) at the nominal current of 380 A. This is compared to the flux calculated using the ideal magnetic field of 0.74 T [3] of a CPMU with 20 mm period length made of the best material available PrFeB (redline) [4]. (b) First and second field integrals measured at different values of the current in the entrance and exit correction coils [6].…”
Section: Scu20mentioning
confidence: 99%