Impulse-resolving photo-electron spectrometer and method for impulse-resolving photo-electron spectroscopy
A technology of optoelectronics and energy spectrometer, applied in the field of physics
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example 1
[0104] can be vacuumed up to 10 -10 In the hPa vacuum chamber, starting from the electron emission sample, the electron emission sample and the focusing system are arranged successively along the optical axis.
[0105] Electron emission samples made of TaSe 2 composition and have the following dimensions: surface diameter 1mm and height 0.2mm.
[0106] The focusing system consists of electronic lenses and detectors.
[0107] The electron lens consists of a cylindrical container with a length of 108 mm and a diameter of 140 mm and a cylindrical inlet with a diameter of 30 mm and a length of 15 mm.
[0108] Two cylinders were successively arranged in the container at intervals of 5 mm along the optical axis direction, each having a radius of 49 mm, and the length of the first cylinder was 35 mm, and the length of the second cylinder was 42 mm. The cylindrical element adjacent to the inlet of the vessel was spaced 11 mm from the inner edge of the cylindrical inlet.
[0109] T...
example 2
[0120] To map the momentum distribution of electrons with energies below the Fermi energy (e.g. 16.98eV), all negative voltages are scaled down (V G = 0V, V 1 = -16.78V, V 2 = -16.63V, V D = -16.98V).
[0121] In this case, all electrons with energies of 16.98 eV and above up to the Fermi energy reach the detector. To determine the momentum distribution at 16.98 eV, the momentum distribution at the Fermi energy of the electrons of the same sample is subtracted to obtain the desired momentum distribution for an electron with a kinetic energy of 16.8 eV.
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