IP Library Granted Patent US 9,696,471
Granted Patent B2
US 9,696,471 · App. 13/847,616 · Granted Jul 4, 2017

Filtered ASE swept source for OCT medical imaging

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Quick Facts
Patent No.
US 9,696,471
App. No.
13/847,616
Granted
Jul 4, 2017
Kind
B2
Abstract

An integrated swept wavelength optical source uses a filtered ASE signal with an optical amplifier and tracking filter. This source comprises a micro optical bench, a source for generating broadband light, a first 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, and a second tunable Fabry Perot filter, installed on the bench, for spectrally filtering the amplified tunable signal from the amplifier. A self-tracking arrangement is also possible 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 (36)

1. A wavelength swept optical source, comprising:

a micro optical bench;

a source for generating broadband light;

a first tunable Fabry Perot filter, installed on the bench, for spectrally filtering the broadband light from the broadband source to generate a tunable signal, wherein a full width half maximum bandwidth of the first Fabry-Perot tunable filter is less than 20 GHz;

an amplifier, installed on the bench, for amplifying the tunable signal;

at least one filter-amplifier lens, installed on the bench, for coupling the tunable signal from the first tunable Fabry Perot filter into the amplifier;

a second tunable Fabry Perot filter, installed on the bench, for spectrally filtering the amplified tunable signal from the amplifier; and

at least one amplifier-filter lens, installed on the bench, for coupling the tunable signal from the amplifier into the second tunable Fabry Perot filter;

wherein the amplifier is located on the bench optically between the first tunable Fabry-Perot filter and the second tunable Fabry-Perot filter.

2. A wavelength swept optical source as claimed in claim 1 , further comprising a hermetic package, the micro optical bench being installed within the hermetic package.

3. A wavelength swept optical source as claimed in claim 2 , wherein the hermetic package is a butterfly package.

4. A wavelength swept optical source as claimed in claim 1 , further comprising thermoelectric cooler attached to a backside of the optical bench to control a temperature of the optical bench.

5. A wavelength swept optical source as claimed in claim 1 , wherein the source comprises a superluminescent light emitting diode, which is installed on the bench.

6. A wavelength swept optical source as claimed in claim 1 , wherein the source comprises a semiconductor optical amplifier, which is installed on the bench.

7. A wavelength swept optical source as claimed in claim 1 , wherein the first tunable Fabry Perot filter and the second tunable Fabry Perot filter are operated in a reflective mode.

8. A wavelength swept optical source as claimed in claim 1 , wherein a full width half maximum bandwidth of the second Fabry-Perot tunable filter is at least 2 times broader in frequency than the bandwidth of the first Fabry-Perot tunable filter.

9. A wavelength swept optical source as claimed in claim 1 , wherein a full width half maximum bandwidth of the first Fabry-Perot tunable filter is about 10 GHz or less.

10. A wavelength swept optical source as claimed in claim 1 , wherein the amplifier is a semiconductor optical amplifier.

11. A wavelength swept optical source as claimed in claim 1 , further comprising a second amplifier for amplifying the amplified tunable signal from the second tunable Fabry Perot filter.

12. A wavelength swept optical source as claimed in claim 1 , further comprising an isolator between the first tunable Fabry Perot filter and the amplifier.

13. A wavelength swept optical source as claimed in claim 1 , further comprising an isolator between the amplifier and second tunable Fabry Perot filter.

14. An optical tomography system comprising:

a wavelength swept optical source, including: 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 tunable signal, an amplifier, installed on the bench, for amplifying the tunable signal, and at least one filter-amplifier lens, installed on the bench, for coupling the tunable signal from the tunable Fabry Perot filter into the amplifier, wherein a full width half maximum bandwidth of the Fabry-Perot tunable filter is less than 20 GHz; and

an interferometer for transmitting the amplified tunable signals from the wavelength swept optical source to a sample and reference path and combining the optical signals from the sample and the reference path to generate an interference signal.

15. A system as claimed in claim 14 , wherein the wavelength swept optical source further includes a second amplifier, installed on the bench, for amplifying the amplified tunable signal from the amplifier.

16. A system as claimed in claim 14 , wherein the wavelength optical swept source further includes a second tunable Fabry Perot filter, installed on the bench, for spectrally filtering the amplified tunable signal from the amplifier.

17. A system as claimed in claim 14 , further comprising a hermetic package, the micro optical bench being installed within the hermetic package.

18. A system as claimed in claim 17 , wherein the hermetic package is a butterfly package.

19. A system as claimed in claim 14 , further comprising thermoelectric cooler attached to a backside of the optical bench to control a temperature of the optical bench.

20. A system as claimed in claim 14 , wherein the source comprises a superluminescent light emitting diode, which is installed on the bench.

21. A system as claimed in claim 14 , wherein the source comprises a semiconductor optical amplifier, which is installed on the bench.

22. A system as claimed in claim 14 , wherein the tunable Fabry Perot filter is a microelectromechanical filters.

23. A system as claimed in claim 16 , wherein a full width half maximum bandwidth of the second Fabry-Perot tunable filter is at least 2 times broader in frequency than the bandwidth of the first Fabry-Perot tunable filter.

24. A system as claimed in claim 14 , wherein a full width half maximum bandwidth of the first Fabry-Perot tunable filter is about 10 GHz or less.

25. A system as claimed in claim 14 , wherein the amplifier is a semiconductor optical amplifier.

26. A system as claimed in claim 14 , further comprising an isolator between the tunable Fabry Perot filter and the amplifier.

Assignments (7)
RELEASE OF FIRST LIEN SECURITY INTEREST IN INTELLECTUAL PROPERTY Recorded Aug 12, 2022
From: JPMORGAN CHASE BANK, N.A., AS COLLATERAL AGENT
To: AXSUN TECHNOLOGIES, INC.
Reel/Frame 061161/0854 →
RELEASE OF SECOND LIEN SECURITY INTEREST IN INTELLECTUAL PROPERTY Recorded Aug 12, 2022
From: ROYAL BANK OF CANADA, AS COLLATERAL AGENT
To: AXSUN TECHNOLOGIES, INC.
Reel/Frame 061161/0942 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Dec 11, 2020
From: AXSUN TECHNOLOGIES INC.
To: EXCELITAS TECHNOLOGIES CORP.
Reel/Frame 054698/0911 →
FIRST LIEN INTELLECTUAL PROPERTY SECURITY AGREEMENT Recorded Jan 2, 2019
From: AXSUN TECHNOLOGIES, INC.
To: JPMORGAN CHASE BANK, N.A.
Reel/Frame 048000/0692 →
SECOND LIEN INTELLECTUAL PROPERTY SECURITY AGREEMENT Recorded Jan 2, 2019
From: AXSUN TECHNOLOGIES, INC.
To: ROYAL BANK OF CANADA, AS COLLATERAL AGENT
Reel/Frame 048000/0711 →
CHANGE OF NAME Recorded Aug 31, 2017
From: AXSUN TECHNOLOGIES, LLC
To: AXSUN TECHNOLOGIES, INC.
Reel/Frame 043733/0195 →
CHANGE OF NAME Recorded Feb 24, 2016
From: AXSUN TECHNOLOGIES, INC.
To: AXSUN TECHNOLOGIES LLC
Reel/Frame 037901/0152 →