1993
DOI: 10.1007/bf01466043
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Investigations concerning the work function of doped graphite

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Cited by 9 publications
(8 citation statements)
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“…It is evident that, as the number of conjugated carbon atoms increases, the electronegativity becomes constant. For graphite, two experimental values (3.93 and 4.8 eV) for the mean electron work function were previously reported. , Two approximations were also employed in order to theoretically deduce the electron work function. In the first, it is equal to the HOMO energy (defined for semiconducting carbon tubes); as the HOMO energy is equal to the ionization energy (within the ionizations theorems of Perdew et al; see ref ), the ionization energy for large systems can be considered to be equivalent to the electron work function.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…It is evident that, as the number of conjugated carbon atoms increases, the electronegativity becomes constant. For graphite, two experimental values (3.93 and 4.8 eV) for the mean electron work function were previously reported. , Two approximations were also employed in order to theoretically deduce the electron work function. In the first, it is equal to the HOMO energy (defined for semiconducting carbon tubes); as the HOMO energy is equal to the ionization energy (within the ionizations theorems of Perdew et al; see ref ), the ionization energy for large systems can be considered to be equivalent to the electron work function.…”
Section: Resultsmentioning
confidence: 99%
“…On the other hand, it was reported previously that many properties pertaining to large polynuclear aromatics must approach those of graphite at its largest size limit. Among these properties are included the ionization energy and electron affinity, both of which are expected to approach the work function of graphite. However, in the case of linear polyene-conjugated systems, no previous reports exist that are focused on clarifying how various properties observed in graphite differ from those of smaller molecules.…”
Section: Introductionmentioning
confidence: 99%
“…As supported by previous UPS work, , the Mg−Alq 3 complex is likely to have an energy level in the gap between the LUMO of the bulk Alq 3 film and the Mg Fermi level. Graphitic carbon could also possess energy states in this gap region because its work function is known to be lower than that of Mg and subject to mediation by the presence of metallic impurities . These gap states could serve as intermediate states for electron injection from the metal Fermi level to the Alq 3 LUMO, thereby lowering the energy required for this process. , The presence of both reaction products and decomposition products is also likely to create disorder within the interface that would further broaden interfacial state energies and lower the energy required for electron injection.…”
Section: Discussionmentioning
confidence: 99%
“…Combining the effects both from carbon core and surface functional groups, the equations may be written as and For graphite, the effective masses of electron and hole are 0.09 and 0.11 m 0 , respectively . As the work function of graphite is −3.93 ± 0.19 eV and that of graphene is −4.30 ± 0.05 eV, we adopted −4.11 eV (mean value of them) as the value of E WF in our calculation. The values of D / A for surface functional groups C–COOH, C–OH, and C–H are calculated to be 0.159, −0.115, and −0.037 eV, respectively.…”
Section: Resultsmentioning
confidence: 99%
“…For graphite, the effective masses of electron and hole are 0.09 and 0.11 m 0 , respectively. 25 As the work function of graphite is −3.93 ± 0.19 eV 26 and that of graphene is −4.30 ± 0.05 eV, 27 we adopted…”
mentioning
confidence: 99%