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note
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l, it is straightforward to extract perpendicular components of momentum widths and velocities [shown in Fig. 3 and Fig. 4(a)].
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note
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F)| (particle-hole mixing), and our velocities become approximations, representing mean values over the measured energy interval. This is valid within the "quasiparticle" picture. However, if the injected hole decays into more fundamental excitations. the photoemission spectrum loses the "quasiparticle pole" and both the EDCs and MDCs represent a broad many-particle continuum.
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Yusof, Z.1
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