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Strained Superlattice GaAs
Be doping (cm ) -3 GaAs P 1-x x , 0<x<0.36 (2.5 μm) p-type GaAs substrate GaAs (5 nm) GaAs (4 nm) GaAsP (3 nm) GaAs P 0.64 0.36 (2.5 μm) 14 pairs 5.10 19 17 18 SVT associates, per SLAC specs.
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Higher Quantum Efficiency
QE (%) QE ~ 1% versus 0.2% from “traditional” strained layer material we operate here Wavelength (nm)
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Higher Beam polarization
Measurements at Test Cave as high as 85% Recent injector measurement 82% Typical polarization from traditional material ~75% Polarization (%) Wavelength for Good QE and Polarization Wavelength (nm)
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Analyzing power (ie: QE anisotropy)
Analyzing power smaller by factor of 3 compared with strained-layer material; 4% versus 12%. This means; Smaller inherent intensity and position asymmetries on beam. Analyzing power (%) Wavlength for good QE and polarization Wavelength (nm)
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QE vs hydrogen cleaning
Typical H-dose to clean anodized samples Drawback; Delicate material Can’t clean with atomic hydrogen Makes it tough to anodize edge of cathode Try arsenic capped samples (on order) QE (%) Hydrogen exposure time (min)
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Superlattice vs strained layer
Polarization higher than strained layer P ~ 80% QE is 5 times higher QE ~ 1% Analyzing power smaller A.P. ~ 3% Material difficult to clean once it gets “dirty”. Makes it tough to anodize edge of sample. Suffer shorter operating lifetime. ? Pros: Cons:
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