IES990865A2 - Method and apparatus for determining the drive currents of a laser - Google Patents

Method and apparatus for determining the drive currents of a laser

Info

Publication number
IES990865A2
IES990865A2 IES990865A IES990865A2 IE S990865 A2 IES990865 A2 IE S990865A2 IE S990865 A IES990865 A IE S990865A IE S990865 A2 IES990865 A2 IE S990865A2
Authority
IE
Ireland
Prior art keywords
wavelength
filter
laser
output
drive currents
Prior art date
Application number
Inventor
Ronan O'dowd
Original Assignee
Ronan O Dowd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Ronan O Dowd filed Critical Ronan O Dowd
Priority to IES990865 priority Critical patent/IES990865A2/en
Priority to EP00968155A priority patent/EP1221186A1/en
Priority to KR1020027004845A priority patent/KR20020070266A/en
Priority to CN008142696A priority patent/CN1218450C/en
Priority to JP2001530164A priority patent/JP2003511866A/en
Priority to AU78107/00A priority patent/AU777908B2/en
Priority to US10/110,415 priority patent/US6807204B1/en
Priority to PCT/IB2000/001476 priority patent/WO2001028052A2/en
Publication of IES990865A2 publication Critical patent/IES990865A2/en

Links

Abstract

A novel method to characterise a multi-section semiconductor laser for use as a wavelength tunable transmitter. The invention exploits to full advantage a filter whose optical throughput or transmission varies in a know way with wavelength so that the output power is measured and this is used to compute wavelength in the described manner. Furthermore, a data input/output unit is used to increment currents, as required, to the laser and also to read back current from a photo-detector which is in turn a measure of the wavelength as modified by the filter in a known fashion. This means that a single data acquisition unit, or DAQ, which multiple input and output channels can be used to replace the host of electronic current sources and a wavelength meter or analyser, while avoiding the associated time-consuming delays. A microprocessor may be used to replace the DAQ.

Description

A novel method to characterise a multi-section semiconductor laser for use as a wavelength tunable transmitter.
Multi-section semiconductor lasers are used in telecommunications, sensors, spectroscopy and elsewhere to provide a light output that can be tuned in wavelength by the variation of the input electrical currents to the sections.
The conventional method is to input electric currents to the sections of the multi-section laser in a controlled manner and measure the resultant output wavelength with a wavemeter or optical spectrum analyser. This involves expensive apparatus and takes considerable time, even when fully automated under computer control due to instrument communication delays. As many as 1000,000 or more data points need to be measured. For example, to increment in 0.1 mA steps from 0 to 100 mA for just two sections alone requires 1000x1000 measurement points.
The invention exploits to full advantage a filter whose optical throughput or transmission varies in a known way with wavelength so that the output power is measured and this is used to compute wavelength in the described manner.
Furthermore, a data input/output unit is used to increment currents, as required, to the laser and also to read back current from a photo-detector which is in tum a measure of the wavelength as modified by the filter in a known fashion. This means that a single data acquisition unit, or DAQ, with multiple input and output channels can be used to replace the host of electric current sources and a wavelength meter or analyser, while avoiding the associated time-consuming delays. A microprocessor may be used to replace the DAQ. We have reduced a week long session to one hour in this way. A further benefit is that environmental changes that de-stabilise optical equipment have minimal time to act.
The filter can be of many types. For example a fibre optic coupler designed to separate two wavelength bands at 1480 nanometers and above was found to be very suitable in that it has an almost linear transmission power characteristic, decreasing with increasing wavelength. This can be calibrated against a wave-meter and then used repeatedly without further access to the optical instrument.
Another filter is a fibre optic with embedded diffraction Bragg grating. Another is a coloured glass filter, for example a type used with NdYAG lasers.
INT CL -^//o/S 3/co - . Gtoi ΣΓ 9/00 OPEN TO PUBLIC INSPECTION UNDER SECTION 28 AND RULE 23 JNL No. .flM-.....OF SNSDOCID: IE990865 The laser characterisation set-up is illustrated in figure 1. It comprises a suitable optical filter (transmission linear or otherwise with wavelength), with an optical splitter to divide the beam. One portion passes through the filter and the photo-detector current is a measure of transmitted power. The other portion is directly measured by the same or a second photo-detector and acts as a reference. The three or four currents to the laser sections are automatically stepped in increments as required and the wavelength is calculated at each setting. A single data acquisition unit, DAQ, with D/A outputs to the laser current driver circuits and A/D input channels) from the photo-detector(s) can perform all of these functions under PC or microprocessor control. The control currents needed for each chosen wavelength channel are thereby established for use in a look-up table to tune the laser.
Figure 1.
The wavelength is calculated from the two photodetector currents, one being proportional to or representational of wavelength as transmitted by the filter, and the other being a reference measure of optical power input to the filter.
WAVELENGTH = (Power through filter / power into filter) x (Cl) + C2.
The correction factors Cl and C2 are derived from the initial filter throughput spectrum. If the filter is not linear then this calculation is modified accordingly to match the calibrated function.

Claims (1)

1. A novel characterization method to find the set of control currents required to tune a multisection semiconductor laser with respect to wavelength. Changes in output wavelength are converted to optical power information by a suitable optical filter in a known way. The filter is characterised once with a wavemeter for transmission spectrum which may but need not be linear. The relative power is then sufficient to calculate the laser wavelength for the selected set of input drive currents without recourse to an optical wavelength meter. Dependent claims. The filter can be of many embodiments. A fibre optic coupler for seperating wavelength bands near the tuning range of interest has been found to work very well. A fibre Bragg grating filter also suffices as does a suitably selected glass filter or diffraction grating.. For the controller the electrical input drive currents and the photodetector output current can be embodied in a data acquisition card with multiple input/output channels. A microprocessor with memory also suffices. An application specific circuit (ASIC) with embedded or connected memory is another embodiment.
IES990865 1999-10-15 1999-10-15 Method and apparatus for determining the drive currents of a laser IES990865A2 (en)

Priority Applications (8)

Application Number Priority Date Filing Date Title
IES990865 IES990865A2 (en) 1999-10-15 1999-10-15 Method and apparatus for determining the drive currents of a laser
EP00968155A EP1221186A1 (en) 1999-10-15 2000-10-16 Optoelectronic device incorporating a tunable laser and method of characterisation thereof
KR1020027004845A KR20020070266A (en) 1999-10-15 2000-10-16 Optoelectronic device incorporating a tunable laser and method of characterisation thereof
CN008142696A CN1218450C (en) 1999-10-15 2000-10-16 Optoelectronic device incorporating tunable laser and method of characterisation thereof
JP2001530164A JP2003511866A (en) 1999-10-15 2000-10-16 Optoelectronic devices incorporating tunable lasers and methods for adjusting their characteristics.
AU78107/00A AU777908B2 (en) 1999-10-15 2000-10-16 Optoelectronic device incorporating a tunable laser and method of characterisation thereof
US10/110,415 US6807204B1 (en) 1999-10-15 2000-10-16 Optoelectronic device incorporating a tunable laser and method of characterization thereof
PCT/IB2000/001476 WO2001028052A2 (en) 1999-10-15 2000-10-16 Optoelectronic device incorporating a tunable laser and method of characterisation thereof

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
IES990865 IES990865A2 (en) 1999-10-15 1999-10-15 Method and apparatus for determining the drive currents of a laser

Publications (1)

Publication Number Publication Date
IES990865A2 true IES990865A2 (en) 2001-11-14

Family

ID=27637673

Family Applications (1)

Application Number Title Priority Date Filing Date
IES990865 IES990865A2 (en) 1999-10-15 1999-10-15 Method and apparatus for determining the drive currents of a laser

Country Status (1)

Country Link
IE (1) IES990865A2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US9915611B2 (en) 2013-10-10 2018-03-13 Halliburton Energy Services, Inc. Optical computing device and method for compensating light fluctuations

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US9915611B2 (en) 2013-10-10 2018-03-13 Halliburton Energy Services, Inc. Optical computing device and method for compensating light fluctuations

Similar Documents

Publication Publication Date Title
US6233262B1 (en) Device and method for monitoring and controlling laser wavelength
US4927266A (en) Optical signal generating apparatus and optical power meter calibrating system using the same
WO1999040654A1 (en) Method of optimizing the operation points of lasers and means for carrying out the method
WO2004056018A1 (en) Osnr monitoring method and apparatus using tunable optical bandpass filter and polarization nulling method
US4433238A (en) Optical measurement system for spectral analysis
DE19712768A1 (en) Polarisation mode dispersion measuring unit with variable light source wavelength
US7426348B2 (en) Calibrating an optical transceiver via adaptive testing
US20020030868A1 (en) Monitoring of signal wavelengths in optical fiber
CN1300123A (en) Method and apparatus for stabilizing wave lenth of laser
CA2111963A1 (en) Method and apparatus for multivariate characterization of optical instrument response
US20040190566A1 (en) Method of characterising a tuneable laser
JPH10300629A (en) Optical transmission characteristic measuring equipment and calibration method using the same
CA2275823A1 (en) Method for measuring interference effects on glass fiber transmission links as well as a transmission system
EP0855586A1 (en) Wavelength dependence correction method in optical variable attenuator
US20100225914A1 (en) Method for monitoring and measuring optical properties of device in polarization maintaining fibers by using reference fiber bragg grating and fiber components manufactured thereby
Niemi et al. Tunable silicon etalon for simultaneous spectral filtering and wavelength monitoring of a DWDM transmitter
US6560255B1 (en) Method and apparatus for characterizing laser modules
IES990865A2 (en) Method and apparatus for determining the drive currents of a laser
US7068944B2 (en) Multi-function optical performance monitor
CN107655506B (en) Fiber grating sensing demodulation device based on microwave frequency mixing technology
JP2942654B2 (en) Optical spectrum analyzer
EP1442509B1 (en) Stability factors for tuneable multi-section semiconductor lasers
Simova et al. Characterization of chromatic dispersion and polarization sensitivity in fiber gratings
IES991022A2 (en) Novel Embodiment of a Multisection Semiconductor laser for use as a wavelength tunable transmitter with channel location and locking.
CN116865854B (en) Wavelength detection device capable of being integrated on photon integrated chip

Legal Events

Date Code Title Description
FJ9A Application deemed to be withdrawn section 31(3)