{"id":2797,"date":"2023-06-29T14:55:45","date_gmt":"2023-06-29T14:55:45","guid":{"rendered":"https:\/\/beamq.com\/laser\/?p=2797"},"modified":"2023-06-29T15:18:38","modified_gmt":"2023-06-29T15:18:38","slug":"1600nm-fiber-coupled-aom-for-self-heterodyne-line-width-measurement","status":"publish","type":"post","link":"https:\/\/beamq.com\/laser\/1600nm-fiber-coupled-aom-for-self-heterodyne-line-width-measurement\/","title":{"rendered":"1600nm Fiber-coupled AOM for Self Heterodyne Line width Measurement"},"content":{"rendered":"\n

1600nm Fiber-coupled Acousto-optic Modulator Optical AOM with its driver for Self Heterodyne Line width Measurement. <\/a><\/p>\n\n\n\n

Features: <\/p>\n\n\n\n

Low insertion loss
Compact and stable performance
Custom configuration<\/p>\n\n\n\n

Application:<\/p>\n\n\n\n

Optical switch laser wavelength shifting<\/p>\n\n\n\n

Material:TeO2
Wavelength:1600
Insertion loss: 4200m\/s
Extinction Ratio: 4.5dB
Rising edge time:30ns
Frequency: 80MHz
Frequency shift:+\/-80MHz
RF power: 2.5W
Voltage Standing Wave Ratio:1.2:1
input resistance: 50
Device interface:SMA
Fiber type:PM\/SM
Fiber length: 1.5m
Fiber Interface:FC\/APC
Operating temperature:-20~+60
Storage temperature: -30~+70<\/p>\n\n\n\n

<\/p>\n\n\n\n

Check the datasheet <\/a>here. <\/p>\n\n\n\n

\"\"<\/figure>\n\n\n\n
\"\"<\/figure>\n\n\n\n

<\/p>\n\n\n\n

Self Heterodyne Line width Measurement for lasers<\/p>\n\n\n\n

The self-heterodyne method is a heterodyne technique which can be used to measure the linewidth (width of the optical spectrum) of a laser, particularly a single-frequency laser. The basic setup is shown in Figure 1. One portion of the laser beam is sent through a long optical fiber which provides some time delay.<\/p>\n\n\n\n

<\/p>\n\n\n\n

\"\"<\/figure>\n\n\n\n

<\/p>\n\n\n\n

Another portion is sent through an acousto-optic modulator (AOM), which is driven with a constant frequency (typically some tens of megahertz) and shifts all the optical frequency components by that frequency. Both beams are finally superimposed on a beam splitter, and the resulting beat note (centered at the AOM frequency) is recorded with a photodetector (typically a photodiode). From this signal, the laser linewidth can then be calculated.<\/p>\n\n\n\n

For sufficiently long delays, the superimposed beams are essentially uncorrelated, and the output spectrum becomes a simple self-convolution of the laser output spectrum, from which the laser linewidth is easily retrieved. However, what \u201csufficiently long\u201d means in a specific case, can be a difficult question. The criterion which is usually used is that the delay length must be larger than the coherence length, and the latter is derived from the (measured) linewidth itself. This is correct for white frequency noise, but not in situations with higher (e.g. ) low-frequency noise, as can occur e.g. for narrow-linewidth fiber lasers. If such issues are not completely understood, the measured linewidth values may be wrong (often too low).<\/p>\n\n\n\n

The delay time in the self-heterodyne setup can be interpreted as a finite measurement time, which implies that the impact of noise frequencies below that inverse measurement time is low. A consequence of that is that measurements with shorter delay time yield smaller linewidth values if the instantaneous frequency fluctuations exhibit substantial noise, as is the case for many laser diodes.<\/p>\n\n\n\n

For lasers with a very narrow line width (long coherence length), it may not be practical to have a long enough time delay to obtain uncorrelated beams. In that case, shorter delays can be used, but the data processing then has to be substantially more sophisticated. Another possibility is to use an extension of this method, based on recirculating fiber loops<\/p>\n","protected":false},"excerpt":{"rendered":"

1600nm Fiber-coupled Acousto-optic Modulator Optical AOM with its driver for Self Heterodyne Line width Measurement. Features: Low insertion lossCompact and stable performanceCustom configuration Application: Optical switch laser wavelength shifting Material:TeO2Wavelength:1600Insertion loss: 4200m\/sExtinction Ratio: 4.5dBRising edge time:30nsFrequency: 80MHzFrequency shift:+\/-80MHzRF power: 2.5WVoltage Standing Wave Ratio:1.2:1input resistance: 50Device interface:SMAFiber type:PM\/SMFiber length: 1.5mFiber Interface:FC\/APCOperating temperature:-20~+60Storage temperature: -30~+70 Check the […]<\/p>\n","protected":false},"author":1,"featured_media":2801,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":[],"categories":[23],"tags":[72,222],"_links":{"self":[{"href":"https:\/\/beamq.com\/laser\/wp-json\/wp\/v2\/posts\/2797"}],"collection":[{"href":"https:\/\/beamq.com\/laser\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/beamq.com\/laser\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/beamq.com\/laser\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/beamq.com\/laser\/wp-json\/wp\/v2\/comments?post=2797"}],"version-history":[{"count":6,"href":"https:\/\/beamq.com\/laser\/wp-json\/wp\/v2\/posts\/2797\/revisions"}],"predecessor-version":[{"id":2805,"href":"https:\/\/beamq.com\/laser\/wp-json\/wp\/v2\/posts\/2797\/revisions\/2805"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/beamq.com\/laser\/wp-json\/wp\/v2\/media\/2801"}],"wp:attachment":[{"href":"https:\/\/beamq.com\/laser\/wp-json\/wp\/v2\/media?parent=2797"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/beamq.com\/laser\/wp-json\/wp\/v2\/categories?post=2797"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/beamq.com\/laser\/wp-json\/wp\/v2\/tags?post=2797"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}