2021
DOI: 10.1021/acs.jpcc.1c01609
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Unexpected Negative-Ion Conversion in Grazing Scattering of Negative Ions on HOPG

Abstract: An experimental study of 8.5–22.5 keV-energy C–, O–, and F– ion scattering from an HOPG surface has been performed at a grazing scattering angle. For a given incident angle or impact velocity, the F– fraction is the highest and the C– fraction is the smallest among these three projectiles, which is explained with the order of the electron affinity level of the projectile. Moreover, the unexpected observations are that the F– ion fraction increases monotonically with impact velocity and that the negative-ion fr… Show more

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Cited by 9 publications
(6 citation statements)
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“…By comparing the steady state absorption and TA spectra (Figure S7, Supporting Information), the PIB at ≈700 nm was attributed to the state‐filling effect under excitation. [ 20,60–62 ] PIA1 and PIA2 was assigned to the photoinduced free carrier absorption in the conduction band corresponding to the 3d state of Co 2+ and Co 3+ , respectively. [ 26,63–66 ] As shown in Figure 4c, PIB signal was appeared later than the signal of PIA1 and PIA2.…”
Section: Resultsmentioning
confidence: 99%
“…By comparing the steady state absorption and TA spectra (Figure S7, Supporting Information), the PIB at ≈700 nm was attributed to the state‐filling effect under excitation. [ 20,60–62 ] PIA1 and PIA2 was assigned to the photoinduced free carrier absorption in the conduction band corresponding to the 3d state of Co 2+ and Co 3+ , respectively. [ 26,63–66 ] As shown in Figure 4c, PIB signal was appeared later than the signal of PIA1 and PIA2.…”
Section: Resultsmentioning
confidence: 99%
“…Loading Ni‐based cocatalysts decreased the PL signals of HRP and RP. The stronger quenching effect in Ni‐HRP compared to that in Ni−RP indicated the role of the Ni single‐atom sites in suppressing the radiative electron‐hole recombination (Figure 6a) [26] . The increased surface photovoltage (SPV) intensity of Ni‐HRP confirmed the efficient separation of photogenerated electron‐hole pairs (Figure 6b), [27] which was further supported by the electrochemical impedance spectroscopy (EIS) analysis (Figure 6c and Table S3).…”
Section: Resultsmentioning
confidence: 99%
“…Kubelka‐Munk method was applied to determine the accurate band gaps of studied catalysts and Tauc plots of ( F ⋅ hν ) 2 versus hν are shown in Figure 7b. F was calculated according to the Kubelka‐Munk formula ( F =(1− R ) 2 /2 R ), where R is the relative diffuse reflectance determined by the formula of R =1/10 α ; α is the absorption coefficient [5c,25b] . The estimated values of direct band‐gaps for ZnO, ZnO/ZnS, ZnO/ZnS/CdS‐1, ZnO/ZnS/CdS‐2, ZnO/ZnS/CdS‐3 and ZnO/CdS were 3.14, 3.13, 2.62, 2.58, 2.55, and 2.29 eV, respectively, suggesting that the band‐gaps of heterostructures were successfully adjusted by varying the components and synthesis strategy.…”
Section: Resultsmentioning
confidence: 99%