1976
DOI: 10.1088/0022-3719/9/17/027
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Optical properties, phonons and electronic structure of iron pyrite (FeS2)

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1986
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Cited by 131 publications
(70 citation statements)
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“…However, in our calculation, the momentum matrices related these transitions are almost zero, due to the very small overlap between the Fe t 2g and S ppσ * orbitals. Schlegel et al 11 related the structure at ~2 eV ("B" CP) to 3d intraband transitions from t 2g states to antibonding e g * states, and the high-energy structures ("F" CP) to interband transitions from states of largely S 3p character into Fe e g * states. These assignments appear to be arbitrary and do not agree with our results in Fig.…”
Section: (B)mentioning
confidence: 99%
See 1 more Smart Citation
“…However, in our calculation, the momentum matrices related these transitions are almost zero, due to the very small overlap between the Fe t 2g and S ppσ * orbitals. Schlegel et al 11 related the structure at ~2 eV ("B" CP) to 3d intraband transitions from t 2g states to antibonding e g * states, and the high-energy structures ("F" CP) to interband transitions from states of largely S 3p character into Fe e g * states. These assignments appear to be arbitrary and do not agree with our results in Fig.…”
Section: (B)mentioning
confidence: 99%
“…5 However, only a limited number of ε and N spectra are available for pyrite from electronic structure calculations [6][7][8][9] or optical reflectance measurements. [10][11][12][13] Moreover, significant discrepancies exist among the reported spectra and no trustworthy theoretical explanation has been made available so far.…”
Section: Introductionmentioning
confidence: 99%
“…1,2 Iron pyrite (FeS 2 ) is a promising photovoltaic material because of its suitable band gap (E g = 0.95 eV), strong light absorption (α > 10 5 cm -1 for hν > 1.4 eV), long minority carrier diffusion length (100-1000 nm), and essentially infinite elemental abundance. 3,4,5,6,7,8 Pyrite photoelectrochemical and solid-state Schottky solar cells have shown large short-circuit current densities (30-42 mA cm -2 ) and quantum efficiencies as high as 90%. 9,10 The main obstacle for the development of pyrite is its low open-circuit photovoltage (V OC ), which is typically only < 200 mV.8 Since 1984, a few dozen studies have explored possible causes of the low V OC , such as bulk nonstoichiometry (mostly S or Fe vacancies), 8,11,12,13 surface states that cause Fermi pinning and thermionic-field emission, and large dark currents, 14,15,16 metallic FeS-like surface layers, 17,18 and small-band gap phase impurities in the pyrite bulk (including marcasite, pyrrhotite, and amorphous iron sulfide phases).…”
Section: Introductionmentioning
confidence: 99%
“…Bither, Bouchard, Cloud, Donohue & Siemons, 1968;Goodenough, 1971;Vaughan & Craig, 1978). FeS2 is a diamagnetic semiconductor with a band gap of -0.95 eV (Schlegel & Wachter, 1976) between the tzg states and the empty e* band. CoS2 is ferromagnetic and has metallic conductivity.…”
Section: Introductionmentioning
confidence: 99%