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Band Structure of Gallium Phosphide from Optical Experiments at High Pressure
187
Citations
51
References
1964
Year
Short Wavelength OpticOptical MaterialsEngineeringEnergy Band StructureOptical GlassAbsorption SpectroscopySpectroscopic PropertySemiconductorsGallium PhosphideHydrostatic PressureOptical PropertiesQuantum MaterialsHigh PressureMaterials SciencePhotonicsPhysicsRadiative AbsorptionGallium OxideBrillouin ScatteringRoom TemperatureBand StructureApplied PhysicsCondensed Matter PhysicsLight Absorption
The effect of hydrostatic pressure on the following optical properties of GaP has been measured at room temperature: the fundamental absorption edge region from 2.2 to 2.7 eV, an infrared absorption band appearing in $n$-type material at 0.3-0.5 eV, peaks in the reflectivity spectrum at 2.8 and 3.7 eV, and recombination radiation in forward-biased $p\ensuremath{-}n$ junctions at 1.7-2.3 eV. The results have been interpreted by means of a proposed energy band structure in which the conduction band states ${{X}_{1}}^{c}$, ${{X}_{3}}^{c}$, ${{\ensuremath{\Gamma}}_{1}}^{c}$, ${{\ensuremath{\Gamma}}_{15}}^{c}$ are located at energies of 2.2, 2.5, 2.8, 3.7 eV, respectively, above the valence band maximum at ${{\ensuremath{\Gamma}}_{15}}^{v}$. The following pressure coefficients have been measured (the transition involved is given in parenthesis), where energy is expressed in eV and pressure in ${10}^{6}$ bars: ${E}_{G}({{\ensuremath{\Gamma}}_{15}}^{v}\ensuremath{\rightarrow}{{X}_{1}}^{c})=2.22\ensuremath{-}1.1P$; ${E}_{0}({{\ensuremath{\Gamma}}_{15}}^{v}\ensuremath{\rightarrow}{{\ensuremath{\Gamma}}_{1}}^{c})=2.78+10.7P$; ${{E}_{0}}^{\ensuremath{'}}({{\ensuremath{\Gamma}}_{15}}^{v}\ensuremath{\rightarrow}{{\ensuremath{\Gamma}}_{15}}^{c})=3.71+5.8P$; $\ensuremath{\Delta}{E}_{2}({{X}_{1}}^{c}\ensuremath{\rightarrow}{{X}_{3}}^{c})=0.3+1P$. The coefficients of ${E}_{G}$ and ${{E}_{0}}^{\ensuremath{'}}$ are close to those for the corresponding transitions in Si; that of ${E}_{0}$ is close to the corresponding coefficient in Ge. The weak reflectivity peak at 2.8 eV, the direct gap, shifts with temperature at a rate of about -4.6\ifmmode\times\else\texttimes\fi{}${10}^{\ensuremath{-}4}$ eV/\ifmmode^\circ\else\textdegree\fi{}K, compared to a value of about -5.2\ifmmode\times\else\texttimes\fi{}${10}^{\ensuremath{-}4}$ eV/\ifmmode^\circ\else\textdegree\fi{}K for the 2.2 eV indirect gap.
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