SPIE Digital Library Get updates from SPIE Newsroom
  • Newsroom Home
  • Astronomy
  • Biomedical Optics & Medical Imaging
  • Defense & Security
  • Electronic Imaging & Signal Processing
  • Illumination & Displays
  • Lasers & Sources
  • Micro/Nano Lithography
  • Nanotechnology
  • Optical Design & Engineering
  • Optoelectronics & Communications
  • Remote Sensing
  • Sensing & Measurement
  • Solar & Alternative Energy
  • Sign up for Newsroom E-Alerts
  • Information for:
SPIE Defense + Commercial Sensing 2017 | Register Today

OPIE 2017

OPIC 2017




Print PageEmail PageView PDF

Biomedical Optics & Medical Imaging

1065nm and 1310nm MEMS tunable VCSEL light source technology for OCT imaging

A novel vertical-cavity surface-emitting laser with a microelectromechanical tuning element enables high-speed, centimeter-range optical coherence tomography.
20 August 2012, SPIE Newsroom. DOI: 10.1117/2.1201207.004347

Optical coherence tomography (OCT) is a noninvasive optical imaging technique that can generate micron-resolution 2D and 3D images of tissue and other scattering materials.1 First demonstrated for imaging the human eye and coronary arteries in 1991,1 OCT has become a clinical standard for diagnosing and monitoring treatment of eye disease, with approximately 16 million ophthalmic OCT procedures performed in the US in 2010.2 OCT can also be used for intravascular imaging of plaque to assess heart disease, cancer biopsy imaging, developmental biology research, art preservation, and industrial inspection.

Newer Fourier-domain OCT detection methods3–6 enable orders of magnitude faster imaging speeds compared to the original time-domain methods. Fourier-domain detection can be implemented in two ways. The first, called spectral-domain OCT (SD-OCT), uses a broadband light source along with an interferometer, a spectrometer, and a line-scan camera. The second method, called swept-source OCT (SS-OCT),7 uses a wavelength-swept laser light source, that is, one whose emission sweeps back and forth across a range of wavelengths. An interferometer and a detector with a high speed analog-to-digital (A/D) converter complete the SS-OCT imaging system. State-of-the-art, commercial retinal OCT instruments currently use SD-OCT technology and take images at speeds of 20,000 to 50,000 axial scans per second. However, SS-OCT has several fundamental advantages over SD-OCT, and the research community has shown great interest in SS-OCT for demonstrating ultrahigh imaging speeds, deep tissue penetration, Doppler OCT flow analysis, and long imaging range. Indeed, record OCT imaging speeds with axial scan rates in the megahertz range have recently been shown using SS-OCT with a Fourier-domain mode-locking laser as the source of wavelength-swept light.8

Figure 1. (A) Wafer of vertical-cavity surface-emitting lasers (VCSELs) and microscopy image of one of the microelectromechanical system (MEMS) actuators. (B) Schematic of 1310nm MEMS-tunable VCSEL structure. GaAs: Gallium arsenide. AlxOy: Aluminum oxide. InP: Indium phosphide. MQW: Multiple quantum well.

Historically, SS-OCT has been available to only a few select research groups and commercial entities because of a lack of a compact, high-performance, low-cost swept source. To fulfill this need, we developed a new light-source technology for OCT, consisting of a vertical-cavity surface-emitting laser (VCSEL) with a microelectromechanical system (MEMS) actuator to tune the emission wavelength. Our technology achieves a combination of ultrahigh sweep speeds, wide spectral tuning range, adjustability in sweep trajectory, and extremely long coherence length that has not been simultaneously achieved with any other previously demonstrated OCT light-source technology. The technical advantages of the VCSELs suggest that they are a near-ideal light source for OCT applications.

Figure 2. (A) Optical coherence tomography (OCT) cross sectional image of the anterior of a human eye obtained with a 1310nm VCSEL at 100kHz axial scan rate. (B) 3D rendering of a 400×400 axial scan volume of the anterior eye, also obtained at 1310nm and 100kHz axial scan rate. (C) OCT cross sectional image of a human retina obtained at 1065nm and 350kHz axial scan rate (four images averaged).

The integrated design of the VCSEL enables high volume, wafer-based production (see Figure 1). The VCSEL is optically pumped, and a low-mass, electrostatically actuated mirror enables high-speed wavelength tuning.9 Prototype 1065nm and 1310nm devices achieve 100—115nm of tuning range. The micron-scale cavity length of the VCSEL enables single-mode operation without mode hopping. Consequently, the laser's coherence length can be extremely long, which translates to a greatly extended OCT imaging range. A semiconductor booster optical amplifier increases the output power up to 35mW while maintaining the intrinsic tuning bandwidth. A single device can operate over a range of sweep lengths and at axial scan rates of 50kHz—1.2MHz by adjusting the actuator's drive waveform.10

Figure 3. 1310nm OCT cross sectional images of a human finger obtained at axial scan rates of (A) 60kHz and (B) 1MHz.

Figure 2(A) shows preliminary results imaging the anterior segment of a human eye with a 1310nm VCSEL.10 The long coherence length of the VCSEL enables a long imaging range extending from the cornea to the posterior lens surface. Through linearization of the VCSEL sweep trajectory and by using both the forward and backward sweeps, the peak A/D sampling rate for the image of a human eye is only 380 Msamples/s: see Figure 2(A). Consequently, commonly available and relatively low-cost 400—500 Msample/s A/D converters with 12—14 bits of resolution can be used to obtain a long OCT imaging range with the VCSEL source. Obtained at a 350kHz axial scan rate (approximately 10× faster than commercial systems), the retinal images show deep penetration and imaging into the choroid vasculature behind the retina: see Figure 2(B,C).

An OCT cross sectional image of a human finger demonstrates the deep penetration of 1310nm light and long coherence length of the laser, which enables the visualization of blood vessels below the skin's surface: see Figure 3(A). In an OCT image of a finger obtained at an axial scan rate of 1MHz, fingerprint ridges, sweat glands, and dermal layers can be seen with high detail and contrast, indicating the capability of OCT imaging with this new light source: see Figure 3(B).

In summary, we demonstrated a novel MEMS-tunable VCSEL light-source technology for OCT imaging. The VCSEL technology offers a novel combination of high speed, record coherence length, and flexibility in wavelength sweep trajectory. As we continue to refine and demonstrate the VCSEL in research applications, Thorlabs is commercializing the technology to be offered in either a complete OCT imaging system or as a stand-alone swept source for system integration by original equipment manufacturers.

This research was supported in part by NIH grants 2R44CA10167-05, R01-EY011289-25, R01-EY013516-09, R01-EY013178-11, R01-CA075289-15, R01-NS057476-05, R01-HL0957170-03, and R01- EY018184-05; AFOSR grants FA9550-10-1-0063 and FA9550-10-1-0551; and at Praevium Research by Thorlabs matching funds. IG acknowledges support from the Foundation for Polish Science (KOLUMB Programme; KOL/3/2010-I).

Benjamin Potsaid
Thorlabs, Inc.
Newton, NJ
Massachusetts Institute of Technology (MIT)
Cambridge, MA

Benjamin Potsaid is a research scientist at Thorlabs and a visiting scientist at MIT.

Vijaysekhar Jayaraman
Praevium Research, Inc.
Santa Barbara, CA

Vijaysekhar Jayaraman is the founder and principal investigator.

James Y. Jiang and Alex E. Cable
Thorlabs, Inc.
Newton, NJ

James Jiang is head of optical coherence tomography research.

Alex Cable is the founder and president.

Peter J. S. Heim
Thorlabs Quantum Electronics
Jessup, MD

Peter Heim is the chief technology officer.

Ireneusz Grulkowski, James G. Fujimoto
Cambridge, MA

Ireneusz Grulkowski is a postdoctoral researcher.

James G. Fujimoto is a professor and principal investigator.

1. D. Huang, E. Swanson, C. Lin, J. Schuman, W. Stinson, W. Chang, M. Hee, Optical coherence tomography, Science 254(5035), p. 1178-1181, 1991.
2. E. A. Swanson, D. Huang, Ophthalmic OCT reaches $1 billion per year, Retinal Physician 8(4), p. 45, 2011.
3. R. I. MacDonald, Frequency domain optical reflectometer, Appl. Opt. 20(10), p. 1840-1844, 1981.
4. R. Leitgeb, C. Hitzenberger, A. Fercher, Performance of Fourier domain vs. time domain optical coherence tomography, Opt. Express 11(8), p. 889-894, 2003.
5. M. Choma, M. Sarunic, C. Yang, J. Izatt, Sensitivity advantage of swept source and Fourier domain optical coherence tomography, Opt. Express 11(18), p. 2183-2189, 2003.
6. J. F. de Boer, B. Cense, B. H. Park, M. C. Pierce, G. J. Tearney, B. E. Bouma, Improved signal-to-noise ratio in spectral-domain compared with time-domain optical coherence tomography, Opt. Lett. 28(21), p. 2067-2069, 2003.
7. S. R. Chinn, E. A. Swanson, J. G. Fujimoto, Optical coherence tomography using a frequency-tunable optical source, Opt. Lett. 22(5), p. 340-342, 1997.
8. W. Wieser, B. R. Biedermann, T. Klein, C. M. Eigenwillig, R. Huber, Multi-megahertz OCT: High quality 3D imaging at 20 million A-scans and 4.5 Gvoxels per second, Opt. Express 18(14), p. 14685-14704, 2010.
9. V. Jayaraman, J. Jiang, H. Li, P. Heim, G. Cole, B. Potsaid, J. G. Fujimoto, A. Cable, OCT imaging up to 760kHz axial scan rate using single-mode 1310nm MEMS-tunable VCSELs with >100nm tuning range, CLEO:2011—Laser Appl. to Photonic Appl., p. PDPB2, 2011.
10. B. Potsaid, V. Jayaraman, J. G. Fujimoto, J. Jiang, P. J. S. Heim, A. E. Cable, MEMS tunable VCSEL light source for ultrahigh speed 60kHz–1MHz axial scan rate and long range centimeter class OCT imaging, Proc. SPIE 8213, p. 82130M, 2012. doi:10.1117/12.911098