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Figure 1
ARPES schematic. Incident photons excite a distribution of photoelectrons at the sample. The photoelectrons in a plane are dispersed in energy and angle by a combination of an electron lens coupled to a hemispherical capacitor. Electrons with a range of energy and angles are directly imaged onto a two-dimensional multi-channel detector. A sample goniometer allows for the XYZ and angular positioning of the sample with respect to the detector and incident photon beam. [Reproduced from Rotenberg (2010BB33).]

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 21| Part 5| August 2014| Pages 1048-1056
doi:10.1107/S1600577514015409
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