2013
DOI: 10.1088/1742-6596/425/3/032011
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Developments in Polarization and Energy Control of APPLE-II Undulators at Diamond Light Source

Abstract: Abstract.A pair of 2m long APPLE-II type undulators have been built for the I10 BLADE beamline at Diamond Light Source. These 48mm period devices have gap as well as four moveable phase axes which provide the possibility to produce the full range of elliptical polarizations as well as linear polarization tilted through a full 180deg. The mechanical layout chosen has a 'master and slave' arrangement of the phase axes on the top and bottom. This arrangement allows the use of symmetries to provide operational eas… Show more

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Cited by 5 publications
(4 citation statements)
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“…2. The spectra are measured across both the L 3 edge and the L 2 edge first for right circular polarization, and then for left circular polarization provided by versatile I10's APPLE-II insertion devices [32]. According to the standard convention, "right" circular polarization is defined with the…”
Section: Soft-x-ray Magnetic Circular Dichroism Resultsmentioning
confidence: 99%
“…2. The spectra are measured across both the L 3 edge and the L 2 edge first for right circular polarization, and then for left circular polarization provided by versatile I10's APPLE-II insertion devices [32]. According to the standard convention, "right" circular polarization is defined with the…”
Section: Soft-x-ray Magnetic Circular Dichroism Resultsmentioning
confidence: 99%
“…A periodic magnetic structure forces the electrons to oscillate and emit radiation. However, to generate circularly polarized x-ray radiation for probing the spatial structure of complex molecules and the magnetic properties of materials, the magnetic field of inserts (wiggler or undulator) would be of a complicated design and hard to control [2]. In contrast, laser plasma wakefield accelerators can generate one thousand times larger acceleration gradients [3][4][5][6], thus reducing a hundred meter synchrotron facility to a few centimeters [7,8].…”
Section: Introductionmentioning
confidence: 99%
“…quadrants Q2 and Q4 as indicated in Fig. 2 (Longhi et al, 2013). Therefore, to set linear polarization with arbitrary angle we have a two-valued two-dimensional function F representing the beam state which must be invertible (for energy/angle readback) (Young et al, 2002),…”
Section: Introductionmentioning
confidence: 99%