Spectrally shaped tunable short-cavity laser

Patent metadata

Field	Value
Publication number	US-2018254608-A1
Application number	US-201815967019-A
Country	US
Kind code	A1
Filing date	Apr 30, 2018
Priority date	Jul 27, 2012
Publication date	Sep 6, 2018
Grant date	—

Abstract

A tunable source includes a short-cavity laser optimized for performance and reliability in SSOCT imaging systems, spectroscopic detection systems, and other types of detection and sensing systems. The short cavity laser has a large free spectral range cavity, fast tuning response and single transverse, longitudinal and polarization mode operation, and includes embodiments for fast and wide tuning, and optimized spectral shaping. Disclosed are both electrical and optical pumping in a MEMS-VCSEL geometry with mirror and gain regions optimized for wide tuning, high output power, and a variety of preferred wavelength ranges; and a semiconductor optical amplifier, combined with the short-cavity laser to produce high-power, spectrally shaped operation. Several preferred imaging and detection systems make use of this tunable source for optimized operation are also disclosed.

First claim

What is claimed is:

1 . A tunable laser operative to emit tunable radiation over an emission wavelength range having a center wavelength, with an output power spectrum over said wavelength range and an average emission power, said tunable laser comprising:
an optical cavity including a first and second mirror; a gain region interposed between said first and second mirrors; a source of pump energy, a tuning region; and means for adjusting an optical path length of said tuning region to create wavelength tuning of said tunable laser;
wherein:
a free spectral range (FSR) of said optical cavity exceeds 5% of said center wavelength;
said tunable laser operates substantially in a single longitudinal and transverse mode over said wavelength range; and
said pump energy is dynamically controlled during said wavelength tuning.

2 . The tunable laser of claim 1 , wherein said output power spectrum has a target spectral shape, and said dynamically controlled pump energy is controlled to achieve said target spectral shape.

3 . The tunable laser of claim 1 , wherein said dynamically controlled pump energy turns off said tunable radiation over a portion of said wavelength tuning.

4 . The tunable laser of claim 1 , wherein said tunable laser is optically pumped and said pump energy is an optical pump.

5 . The tunable laser of claim 1 , wherein said tunable laser is electrically pumped and said pump energy is an electrical drive current.

6 . The tunable laser of claim 2 , wherein said spectral shape is substantially Gaussian.

7 . The tunable laser of claim 1 , further comprising an optical amplifier.

8 . The tunable laser of claim 7 , wherein said pump energy pumps said optical amplifier.

9 . The tunable laser of claim 1 , wherein said pump energy pumps said gain region between said first and second mirrors.

10 . A tunable laser operative to emit tunable radiation over an emission wavelength range having a center wavelength, with an output power spectrum having a target spectral shape over said wavelength range and an average emission power, said tunable laser comprising:
an optical cavity including a first and second mirror; a gain region interposed between said first and second mirrors; a tuning region; means for adjusting an optical path length of said tuning region to create wavelength tuning of said tunable laser; and an optical amplifier having an amplified spontaneous emission (ASE) spectrum; wherein: a free spectral range (FSR) of said optical cavity exceeds 5% of said center wavelength; said tunable laser operates substantially in a single longitudinal and transverse mode over said wavelength range; and an alignment of said ASE spectrum relative to said emission wavelength range is controlled to achieve said target spectral shape.

11 . The tunable laser of claim 10 , wherein said ASE spectrum is blue-shifted relative to said emission wavelength range.

12 . A system for swept source optical coherence tomography, the system comprising a swept laser source generating wavelength swept radiation, said swept laser source comprising:
the tunable laser of claim 1 ; means for directing said wavelength-swept radiation to a reference path and a sample; an optical detector for detecting an interference signal between light back-reflected from said sample and light traversing said reference path; and means for signal processing of said interference signal to infer structural information about said sample.

13 . A system for swept source optical coherence tomography, the system comprising a swept laser source generating wavelength swept radiation, said swept laser source comprising:
the tunable laser of claim 8 ; means for directing said wavelength-swept radiation to a reference path and a sample; an optical detector for detecting an interference signal between light back-reflected from said sample and light traversing said reference path; and means for signal processing of said interference signal to infer structural information about said sample.

14 . A system for swept source optical coherence tomography, the system comprising a swept laser source generating wavelength swept radiation, said swept laser source comprising:
the tunable laser of claim 10 ; means for directing said wavelength-swept radiation to a reference path and a sample; an optical detector for detecting an interference signal between light back-reflected from said sample and light traversing said reference path; and means for signal processing of said interference signal to infer structural information about said sample.

15 . A method for generating an output power variation versus wavelength over a wavelength range from a tunable laser operative to emit tunable radiation over an emission wavelength range having a center wavelength, with an output power spectrum over said wavelength range and an average emission power, said tunable laser comprising: an optical cavity including a first and second mirror; a gain region interposed between said first and second mirrors; a tuning region; and means for adjusting an optical path length of said tuning region; wherein: a free spectral range (FSR) of said optical cavity exceeds 5% of said center wavelength; and said tunable laser operates substantially in a single longitudinal and transverse mode over said wavelength range; the method comprising dynamically controlling a pump energy entering into the gain region versus wavelength during wavelength tuning.

16 . The method of claim 15 , wherein said output power spectrum has a target spectral shape, and said pump energy is dynamically controlled during said wavelength tuning to achieve said target spectral shape.

17 . A method for generating a desired output power variation versus wavelength over a wavelength range from a tunable laser operative to emit tunable radiation over an emission wavelength range having a center wavelength, with an output power spectrum over said wavelength range and an average emission power, said tunable laser comprising: an optical cavity including a first and second mirror; a gain region interposed between said first and second mirrors; a tuning region; and means for adjusting an optical path length of said tuning region; wherein: a free spectral range (FSR) of said optical cavity exceeds 5% of said center wavelength; and said tunable laser operates substantially in a single longitudinal and transverse mode over said wavelength range; the method comprising defining a target power variation over the wavelength range, and adjusting a reflectivity spectrum of one of said first and second mirrors until said output power variation matches said target power variation over the wavelength range.

Assignees

• Thorlabs Inc
• Praevium Res Inc

Inventors

• Cable Alex Ezra
• Jayaraman Vijaysekhar
• Potsaid Benjamin Michael

Classifications

• H01S5/041

  Optical pumping · CPC title

• H01S5/18311

  using selective oxidation · CPC title

• H01S5/18372

  by native oxidation · CPC title

• H01S3/10061

  Polarization control · CPC title

• H01S3/1396

  by using two modes present, e.g. Zeeman splitting (H01S3/1398 takes precedence) · CPC title