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TO-can

Gain-chips (GC)

Gain-chip is the irreplaceable component as a gain medium for the building of the tunable diode laser or high stable external cavity diode laser. Gain-chip is similar to laser diode chip except the fact that it has deep antireflecting coating on one or both facets which significantly increases threshold of self lasing or eliminate it.

Typical external cavity diode laser configurations are Littrow- and Littman/Metcalf cavities. For the Littrow configuration, a diffraction grating is mounted in a way that light of the desired wavelength is diffracted back along the incident beam. Wavelength is scanned by rotating the grating. Generally an intracavity achromatic lens is used to collimate expanded beam on a relatively large area of the grating. The zero order diffracted beam can be used as the output laser beam.

Littrow configuration
Littrow configuration

Littman configuration
Littman/Metcalf configuration

Part number indentification:

GC-1030-150-TO-200-B

  • 1030 - central wavelength of tuning range (nm)

  • 150 - tuning range width (nm)

  • TO - heatsink type (TO-header)

  • 200 - optical power out of external cavity (mW)

  • B - type of gain-chip


Available on heatsinks:

  • TO-header (can)

  • C-mount

  • AlN submount


TO-header
TO-header

C-mount
C-mount


Typical parameters* of gain-chips (type A, B) mounted on TO-headers

Part numberCentral
wavelength
of tuning
range
tuning
range
Wavelength
of maximum
power
Power out
of external
cavity
Fast axis
beam
divergence
Slow axis
beam
divergence
ASE
power w/o
feedback
Stripe
length
Operating
current


nmnmnmmWdegdegmWmmmA

GC-780-40-TO-30-B780407803020851.5150

GC-780-40-TO-100-B78040780110208202250

GC-800-40-TO-100-B7954580011022852250

GC-800-40-TO-130-B80040800130325252250

GC-920-90-TO-200-B9059092020033871.5400

GC-950-110-TO-200-B950110980240326351.5400

GC-1030-150-TO-200-B10301501060200381031.5400

GC-1030-160-TO-200-B10301601080220178501.5400

GC-1060-150-TO-200-B10601501090210169501.5400

GC-1105-130-TO-200-B110513011302004091.51.4400

GC-1110-70-TO-300-A111070112035035483600

GC-1160-90-TO-200-A115090116023040523600

GC-1180-80-TO-200-A116080117022042433600

GC-1180-100-TO-200-B115010011702104071103600

GC-1220-110-TO-200-B12201101240230376153800

GC-1260-60-TO-200-B12601101270210387203800

GC-1270-60-TO-200-A127060127020033533800

GC-1270-130-TO-200-B12701301230, 13202003864.53800

GC-1270-140-TO-200-A12701301230, 13102203851.53800

GC-1300-60-TO-200-B13006013202003864.53800

GC-1310-60-TO-200-A13106013102203851.53800

GC-1330-60-TO-200-A133060133020040453800

GC-1330-70-TO-200-B1330701340200377173800

* - @ CW, 25C heatsink temperature, external cavity in Littman configuration with ≈10% feedback

Any customized wavelength from the 780-1330 nm range is possible. Please, contact us for the details.


Gain-chip types

Gain-chip types

Gain-chip types
Gain-chip types

Innolume Gain-chip product line subdividing in two main categories:

  • One side optical access (Types A and B)

  • Two sides optical access (Types C and D)


One side optical access Gain-chip is ideal component for operation in the scheme where the output power is outcoupled from the external cavity. Typically they are supplied in TO-can package.

Two sides optical access Gain-chip can be used in scheme allowing power outcoupling directly from the Gain-chip Facet to reduce the optical losses or in optical scheme for the amplification.

Type A Gain-chip has straight stripe normal to the facets with high reflecting (HR) and deep antireflecting (AR) coatings. This is the most cost effective solution for the building of the external cavity diode laser. Type A GC has symmetrical beam far field providing efficient coupling to the external cavity and back using high NA aspheric lens. This type of the Gain-chips has relatively low gain spectra ripples suppression compare to the other types. It results from the fact that the reflection of the AR coated facet is on the level of 0.1% and can be further reduced by using curved stripe-to-facer design only.

Type B GC has curved stripe with HR- on normal side and deep AR-coating on the tilted one. The curved stripe together with deep AR-coating provides extremely low reflection (< 10E-5) allowing suppression of self lasing and minimizing of gain ripples. The drawback of the curved stripe is the distortion of the output beam which embarrasses collimation and reduces efficiency of back coupling. High NA optics must be used.

Type C GC has curved stripe and deep AR-coating at the tilted side and a few percent reflection at the normal side. The wavelength selecting feedback has to be placed at the tilted side (with the same advantages and drawbacks as for the Type B), whereas the output power goes out from the normal side. This design allows high output power and relatively good output beam. The reflection of the facet with normal stripe has to be designed individually depending on the configuration of the system and required output power.

Type D GC has a tilted stripe with a deep AR on both sides, typically it used for the advanced optical schemes were the build-in amplifying unit is needed. Innovative facet coating technology which includes facet passivation meets high reliability requirements. The ISO9001:2008 conform production is based on careful design, manufacturing and extensive testing. Each device is individually tested and shipped with a specified set of test data.



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