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Photoelectric Emission and Energy Structure of Cs<sub>3</sub>Sb
24
Citations
5
References
1953
Year
SemiconductorsPhotoelectric EmissionPhotoelectric SensorThermal RadiationEngineeringPhysicsElectron SpectroscopyOptical PropertiesCs 3Applied PhysicsCondensed Matter PhysicsQuantum MaterialsAtomic PhysicsPhotoelectric MeasurementEnergy DistributionsOptoelectronicsPhotoelectric Yield
Spectral distributions of the photoelectric yield and energy distributions of the photoelectrons were observed at room temperature, 195°K and 90°K for Cs 3 Sb. The facts obtained are as follows: (1) The quantum efficiency Y rises rapidly as h ν increases above 2ev, and reaches the maximum at h ν∼3.8ev, where the magnitude of Y exceeds 10 -1 . Further, there appears the second maximum at h ν∼5ev. (2) For \(h\nu{\gtrsim}3\)ev Y increases with the decrease in temperature in accordance with the relation \((\partial{Y}/\partial{T})/Y{\fallingdotseq}-10^{-3}\)/deg. (3) On the contrary, in the low energy tails at h ν∼-2ev Y decreases with decreasing temperature, or the photoelectric work function ϕ shifts with temperature in the form ∂ϕ/∂ T =-3∼5×10 -4 ev/deg. (4) At lower temperatures a minor hump in Ycan be seen at h ν∼2.2ev. (5) Energy distributions are comparatively temperature-insensitive, but for h ν∼5ev, corresponding to the second maximum in Y , there is a growing preponderance of low velocity electrons, which is quite unlike those for smaller h ν. These results are discussed in terms of a possible energy structure for Cs 3 Sb.
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