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IR Detectors from Vigo System - Boston Electronics Corporation

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3TE cooled optically immersed detectorsModel λ op, μm Type D*, cmHz 1/2 /W τ, nsPVI-3TE-3 3 PV 7×10 11 15PVI-3TE-3.4 3.4 PV 5×10 11 15PVI-3TE-4 4 PV 4×10 11 20PVI-3TE-5 5 PV 8×10 10 20PVI-3TE-6 6 PV 3×10 10 10PVI-3TE-8 8 PV 3×10 9 7PVMI-3TE-8 8 PV 3×10 9 7PCI-3TE-9 9 PC 6×10 9 8PCI-3TE-10.6 10.6 PC 2.5×10 9 5PVI-3TE-10.6 10.6 PV 1.5×10 9 3PVMI-3TE-10.6 10.6 PV 2.5×10 9 7PCI-3TE-12 12 PC 9×10 8 5PCI-3TE-13 13 PC 4.5×10 8 4λ op , μm – Optimal wavelength - The wavelength for which adevice was optimized for. For near <strong>IR</strong> detectors λ op is close topeak value. In contrast, for uncooled (300K) long wavelengthdetectors λ op is larger is than λ co .Device type:PC – Photoconductive,PV- Photovoltaic,PEM – PhotoelectromagneticD*, cmHz ½ /W – minimum detectivity. The higher the D*value, the better the detector.τ, ns - maximum time constant (“1/e” time)Time constants have been measured using Alpes Lasers SAquantum cascade lasers (QCL) (www.alpeslasers.ch).3TE cooled detectors without optical immersionModel λ op, μm Type D*, cmHz 1/2 /W τ, nsPV-3TE-3 3 PV 1×10 11 15PV-3TE-3.4 3.4 PV 7×10 10 15PV-3TE-4 4 PV 4×10 10 20PV-3TE-5 5 PV 1×10 10 20PV-3TE-6 6 PV 4×10 9 10PV-3TE-8 8 PV 3×10 8 7PV-3TE-10.6 10.6 PV 1.5×10 8 3PC-3TE-9 9 PC 1.5×10 9 8PC-3TE-10.6 10.6 PC 2.5×10 8 5PC-3TE-12 12 PC 9×10 7 5PC-3TE-13 13 PC 6×10 7 44TE cooled detectorsModel λ op, μm Type D*, cmHz 1/2 /W τ, nsPV-4TE-3 3 PV 1.5×10 11 15PV-4TE-3.4 3.4 PV 1×10 11 15PV-4TE-4 4 PV 6×10 10 20PV-4TE-5 5 PV 1.5×10 10 20PV-4TE-6 6 PV 5×10 9 10PV-4TE-8 8 PV 4×10 8 7PV-4TE-10.6 10.6 PV 2×10 8 3PVI-4TE-3 3 PV 8×10 11 15PVI-4TE-3.4 3.4 PV 7×10 11 15PVI-4TE-4 4 PV 4×10 11 20PVI-4TE-5 5 PV 1×10 11 20PVI-4TE-6 6 PV 4×10 10 10PVI-4TE-8 8 PV 4×10 9 7PVI-4TE-10.6 10.6 PV 2×10 9 3A.P. 25.09.2010Infrared <strong>Detectors</strong> <strong>from</strong> VIGO <strong>System</strong> S.A.

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