Ffecthigh kinetic energies. bandwidth of 4bottle was operated at retardation of
Ffecthigh kinetic energies. bandwidth of 4bottle was operated at retardation of magnetic bottle spectrometer 1/40 resolution [25], we arrive at a function width with the only five eV; taking the measured at these comparatively higher kinetic energies. The about 4 eV at E was operated valence characteristics only 5 eV; a slope of measured 1/40 magnetic bottlekin = 150 eV. The at retardation ofdisperse withtaking the one particular in h per eV in Ekin all through the entire measurement range, confirming the usage of The valence resolution [25], we arrive at a function width of about four eV at Ekin = 150 eV. fundamental undulator radiation. capabilities disperse using a slope of a single in h per eV in Ekin throughout the entire A second dispersive feature, starting basic undulator radiation. measurement range, confirming the use ofat Ekin = 47.9 eV, includes a binding energy of 108 eV (see A second dispersiveslope, equal towards the slope 47.9 eV, has a binding power of 108 eV also Figure two). The function, beginning at Ekin = of your valence lines, indicates its origin from photoemission using the basic slope from the valence lines, that this its stems (see also Figure 2). The slope, equal to theof the undulator. We suggestindicates lineorigin from the Al tip on the oven, sitting at a distance of undulator. We the interaction area from photoemission together with the fundamental from the several mm from recommend that this line but nonetheless being Al tip in the oven, sitting at a distance of some Al is nominally expected stems from thehit by some halo on the X-ray beam. The 2s line ofmm from the interactionMolecules 2021, 26, x FOR PEER Evaluation Molecules 2021, 26,five of 12 5 ofregion but still being hit by some halo of the X-ray beam. The 2s line of Al is nominally to become aroundbe about 120 eV, but resulting from patch charges at the oxidized tip, this line may possibly anticipated to 120 eV, but as a consequence of patch charges at the oxidized tip, this line might be shifted by a handful of eV towards itstowards its apparent binding108 eV. of 108 eV. be shifted by several eV apparent binding power of energyFigure three. Photoelectron spectra for photon energies above (175.25 eV) and below (157.25 eV) the Figure three. Photoelectron spectra for photon energies above (175.25 eV) and under (157.25 eV) the sulfur 2p binding energy. A dispersive behavior of your valence band is visible, moving from 140 to sulfur 2p binding power. A dispersive behavior from the valence band is visible, moving from 140 to 160 eV with growing photon power. Our valence spectrum at h = 155.75 eV is compared with 160 eV with increasing photon power. Our valence spectrum at h = 155.75 eV is compared having a a He-lamp-induced valence photoelectron spectrum (purple) from Ref. [24] in the inset, that is He-lamp-induced valence photoelectron spectrum (purple) from Ref. [24] within the inset, which is scaled scaled in kinetic power according to the distinction of photon energies made use of within the experiments. in kinetic power Auger Icosabutate site eitner feature is only ML-SA1 Autophagy present for the higherthe experiments. The AugerConversely, the as outlined by the difference of photon energies utilized in photon power. Conversely, the Auger eitner feature iswith the sulfur Auger eitner spectrum of OCS (green) from Ref. [26]. Meitner information are compared only present for the greater photon energy. The Auger eitner information are compared together with the sulfur Auger eitner spectrum of OCS (green) from Ref. [26].We now concentrate on the non-dispersive characteristics. At the limit on the highest photon We now concentrate on the non-dispersi.