5.6 Drawings 5.7 Fiber Coupling onto Small Detector Area 5.8 Safety 5.9 Manufacturer Address 5.10 Return of Devices 5.11 Certifications and Compliances 5.12 Warranty 5.13 Copyright and Exclusion of Liability 5.14 List of Acronyms 5.15 Thorlabs Worldwide Contacts and WEEE policy...
The detector housing can be integrated in optical setups using convenient 8-32 and M4 combi- thread mounting holes that are compatible with both imperial and metric threading. The housing accommodates Thorlabs' SM05 (0.535"-40) and SM1 (1.035"-40) threaded adap- ters and accessories. This allows convenient mounting of external optics, light filters, and aper- tures.
3 Operating Instruction 3 Operating Instruction 3.1 Operating Elements APD440A and APD440A2 have identical operating elements. Here shown is the APD440A, representing both APD440A and APD440A2. 3.2 Mounting Housing The APD440x is housed in a rugged, shielded, 74.5 mm x 56.1 mm x 27.4 mm aluminum en- closure.
Thorlabs’ SM05 (0.535"-40) threads and SM1 (1.035"-40) threads that are com- patible with any number of Thorlabs 1” and ½” threaded accessories. This also allows conveni- ent mounting of lens tubes or cage systems. For accessories, please visit our website or con-...
Electrostatic coupling of electrical noise associated with ground loops can be critical. In most cases an electrically isolated post (see Thorlabs parts TRE or TRE/M) will suppress electrical noise coupling. Electrical noise sources should always be identified and the distance to the Avalanche Photodetector should be increased.
M-factor that is equivalent to a gain variation. 3.5.1 Optical Input The APD440A uses a Silicon Avalanche Photodiode with a detector active area diameter of 1.0 mm, operating from 400 to 1000 nm and the APD440A2 uses an UV-enhanced Silicon Avalanche Photodiode with a detector active area diameter of 1.0 mm, operating from...
(l) for a given wavelength can be read from the typical spectral responsivity curves (see · Appendix · The M-factor (gain) adjustment range is 5 - 50 (APD440A2) and 10 - 100 (APD440A) at 23°C ambient temperature. · The amplifier’s transimpedance gain G is 50 MV/A (High-Z termination) and 25 MV/A (50 W).
Conversion Gain at the Peak Responsivity Wavelength. The Conversion Gain is a product of the Transimpedance Gain and the Responsivity for a given M factor and wavelength. At Maximum Gain Setting. For more information on how NEP is calculated, please see Thorlabs' Noise Equivalent Power White Paper.
Below is a possible arrangement, shown on the example of the APD430A2/M. The arrangement is identical for all Thorlabs Avalance Photodiodes. The assembly in front of the detector comprises of a fiber collimator (dependent on fiber), a lens tube collimator adapter (AD11F or AD12F, dependent on collimator), a SM1L1 lens tube with aspheric lens inside (not visible above) and a LM1XY X-Y translation mount.
If necessary, ask for replacement packaging. Refer servicing to qualified personnel! Only with written consent from Thorlabs may changes to single components be made or com- ponents not supplied by Thorlabs be used. All modules must only be operated with duly shielded connection cables.
Thorlabs warrants material and production of the APD440x for a period of 24 months starting with the date of shipment. During this warranty period Thorlabs will see to defaults by repair or by exchange if these are entitled to warranty.
Contact Thorlabs for more information. Waste treat- ment is your own responsibility. “End of life” units must be returned to Thorlabs or handed to a company specializing in waste recovery. Do not dispose of the unit in a litter bin or at a public waste disposal site.
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