ASE swept source with self-tracking filter for OCT medical imaging

• US 8,526,472 B2
• Filed: 05/08/2010
• Issued: 09/03/2013
• Est. Priority Date: 09/03/2009
• Status: Expired due to Fees

• Current Assignee: Excelitas Technologies Corporation (Excelitas Technologies Holdings LLC)
• Original Assignee: Axsun Technologies Incorporated
• Inventors: Flanders, Dale C., Atia, Walid A., Kuznetsov, Mark E.
• Primary Examiner(s): Rodriguez, Armando
• Assistant Examiner(s): HAGAN, SEAN P
• Application Number:
  US12/776,373
• Publication Number:
  US 20110051143A1
• Time in Patent Office: 1,214 Days
• Field of Search: None
• US Class Current: 372/20
• CPC Class Codes: F21V 9/20 Dichroic filters, i.e. devices operating on the principle of wave interference to pass specific ranges of wavelengths while cancelling others
• CPC Class Codes: G01B 9/02004 using frequency scans
• CPC Class Codes: G01B 9/02091 Tomographic interferometers, e.g. based on optical coherence
• CPC Class Codes: H01S 2301/02 ASE (amplified spontaneous emission), noise; Reduction thereof
• CPC Class Codes: H01S 5/005 Optical components external to the laser cavity, specially adapted therefor, e.g. for homogenisation or merging of the beams or for manipulating laser pulses, e.g. pulse shaping H01S5/026, H01S5/18388 take precedence
• CPC Class Codes: H01S 5/0064 Anti-reflection components, e.g. optical isolators
• CPC Class Codes: H01S 5/0078 for frequency filtering
• CPC Class Codes: H01S 5/02216 Butterfly-type, i.e. with electrode pins extending horizontally from the housings
• CPC Class Codes: H01S 5/02251 using optical fibres
• CPC Class Codes: H01S 5/02325 Mechanically integrated components on mount members or optical micro-benches
• CPC Class Codes: H01S 5/5018 using two or more amplifiers or multiple passes through the same amplifier
• CPC Class Codes: H01S 5/5036 the arrangement being polarisation-selective
• CPC Class Codes: H01S 5/5063 operating above threshold

Abstract

An integrated swept wavelength tunable optical source uses a narrowband filtered broadband signal with an optical amplifier and self-tracking filter. This source comprises a micro optical bench, a source for generating broadband light, a tunable Fabry Perot filter, installed on the bench, for spectrally filtering the broadband light from the broadband source to generate a narrowband tunable signal, an amplifier, installed on the bench, for amplifying the tunable signal. The self-tracking arrangement is used where a single tunable filter both generates the narrowband signal and spectrally filters the amplified signal. In some examples, two-stage amplification is provided. The use of a single bench implementation yields a low cost high performance system. For example, polarization control between components is no longer necessary.

Claims

1. A swept optical source, comprising:

a tunable filter for spectrally filtering light from a broadband source to generate a tunable optical signal that is spectrally tuned over a scanband;

a semiconductor optical amplifier for amplifying the tunable optical signal with the amplified tunable optical signal being again filtered by the tunable filter before exiting the swept optical source without again being amplified by the semiconductor optical amplifier to prevent lasing and formation of a resonator; and

a tuning controller that drives the tunable filter to tune over the scanband at speeds greater than 10 kiloHertz.

2. A swept source as claimed in claim 1, wherein the broadband source generates light over the scanband.

3. A swept source as claimed in claim 1, wherein the broadband source comprises an amplified spontaneous emission source that generates light over the scanband.

4. A swept source as claimed in claim 1, wherein the tunable filter is a Fabry Perot tunable filter.

5. A swept source as claimed in claim 1, wherein the tunable filter is a micro electro mechanical system Fabry Perot tunable filter.

6. A swept source as claimed in claim 1, wherein in a passband of the tunable optical filter is less than 20 GigaHertz (FWHM).

7. A swept source as claimed in claim 1, wherein in a passband of the tunable optical filter is less than 5 GigaHertz (FWHM).

8. A swept source as claimed in claim 1, further comprising a tuning controller that drives the tunable filter to tune over the scanband at speeds greater than 100 kiloHertz.

9. A swept source as claimed in claim 1, further comprising a reflector for reflecting the tunable optical signal to pass through the optical amplifier a second time and back to the tunable filter.

10. A swept source as claimed in claim 1, further comprising a loop including the optical amplifier for directing the tunable optical signal back to the tunable filter.

11. A swept source as claimed in claim 1, further comprising a polarization rotation system for rotating a polarization of the tunable optical signal between being filtered by the tunable filter.

12. A swept source as claimed in claim 11, wherein the polarization rotation system includes a non-reciprocal polarization rotation element.

13. A swept source as claimed in claim 11, wherein the polarization rotation system includes a halfwave plate.

14. A swept source as claimed in claim 1, wherein the filtering by the tunable filter of the tunable optical signal is co-directional with the filtering of the amplified tunable optical signal by the tunable filter.

15. A swept source as claimed in claim 1, wherein the filtering by the tunable filter of the tunable optical signal is contra-directional with the filtering of the amplified tunable optical signal by the tunable filter.

16. A method for generating a tunable optical signal, comprising:

spectrally filtering light to generate a tunable optical signal with a tunable filter that is spectrally tuned over a scanband;

amplifying the tunable optical signal to generate an amplified tunable optical signal;

spectrally filtering the amplified tunable optical signal with the same tunable filter;

transmitting the amplified tunable optical signal as an output and preventing further amplification to prevent lasing and formation of a resonator; and

tuning the tunable filter over the scanband at a speeds greater than 10 kiloHertz.

17. A method as claimed in claim 16, further comprising generating the light with a broadband source that generates light over the scanband.

18. A method as claimed in claim 16, wherein the tunable filter is a Fabry Perot tunable filter.

19. A method as claimed in claim 16, further comprising tuning the tunable filter over the scanband at a speeds greater than 100 kiloHertz.

20. A method as claimed in claim 16, further comprising directing the tunable optical signal back to the tunable filter using a loop.

21. A method as claimed in claim 16, further comprising directing the tunable optical signal back to the tunable filter using a reflector.

22. A tunable amplifier, comprising:

a tunable filter for spectrally filtering light to generate a tunable optical signal that is spectrally tunable over a spectral band;

a semiconductor optical amplifier for amplifying the tunable optical signal with the amplified tunable optical signal being filtered by the tunable filter with no more than two passes through the optical amplifier to prevent lasing and formation of a resonator; and

a tuning controller that drives the tunable filter to tune over the scanband at speeds greater than 10 kiloHertz.

23. A swept optical source, comprising:

a tunable filter for spectrally filtering light from a broadband source to generate a tunable optical signal that is spectrally tuned over a scanband;

a semiconductor optical amplifier for amplifying the tunable optical signal in a first pass;

a reflector for reflecting the tunable optical signal to pass through the optical amplifier in a only second pass to prevent lasing and formation of a resonator; and

a tuning controller that drives the tunable filter to tune over the scanband at speeds greater than 10 kiloHertz.