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Because of the limited spatial resolution, the PEEM signal from p1 and p2 are superpositions of the emission from the emitter apexes (the low-energy shoulder) and the immediate vicinity (the peak at 0 eV).
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Because of the limited spatial resolution, the PEEM signal from p1 and p2 are superpositions of the emission from the emitter apexes (the low-energy shoulder) and the immediate vicinity (the peak at 0 eV).
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We calculated Β (calc) by the finite-element method with an adaptive meshing. We approximated our pyramidal shaped emitter by a cone-shaped emitter having same height and base size terminated by spherical surface with a radius of ρ at the apex.
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We calculated Β (calc) by the finite-element method with an adaptive meshing. We approximated our pyramidal shaped emitter by a cone-shaped emitter having same height and base size terminated by spherical surface with a radius of ρ at the apex.
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