Broadband Fourier domain mode-locked laser for optical coherence tomography at 1060 nm
Publication: Research - peer-review › Conference article – Annual report year: 2012
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Broadband Fourier domain mode-locked laser for optical coherence tomography at 1060 nm. / Marschall, Sebastian; Klein, Thomas; Wieser, Wolfgang; Torzicky, Teresa; Pircher, Michael; Biedermann, Benjamin R.; Pedersen, Christian; Hitzenberger, Christoph K.; Huber, Robert; Andersen, Peter E.
In: Proceedings of SPIE, the International Society for Optical Engineering, Vol. 8213, 2012, p. 82130R.Publication: Research - peer-review › Conference article – Annual report year: 2012
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TY - CONF
T1 - Broadband Fourier domain mode-locked laser for optical coherence tomography at 1060 nm
A1 - Marschall,Sebastian
A1 - Klein,Thomas
A1 - Wieser,Wolfgang
A1 - Torzicky,Teresa
A1 - Pircher,Michael
A1 - Biedermann,Benjamin R.
A1 - Pedersen,Christian
A1 - Hitzenberger,Christoph K.
A1 - Huber,Robert
A1 - Andersen,Peter E.
AU - Marschall,Sebastian
AU - Klein,Thomas
AU - Wieser,Wolfgang
AU - Torzicky,Teresa
AU - Pircher,Michael
AU - Biedermann,Benjamin R.
AU - Pedersen,Christian
AU - Hitzenberger,Christoph K.
AU - Huber,Robert
AU - Andersen,Peter E.
PB - S P I E - International Society for Optical Engineering
PY - 2012
Y1 - 2012
N2 - Optical coherence tomography (OCT) in the 1060nm range is interesting for in vivo imaging of the human posterior eye segment (retina, choroid, sclera) due to low absorption in water and deep penetration into the tissue. Rapidly tunable light sources, such as Fourier domain mode-locked (FDML) lasers, enable acquisition of densely sampled three-dimensional datasets covering a wide field of view. However, semiconductor optical amplifiers (SOAs)-the typical laser gain media for swept sources-for the 1060nm band could until recently only provide relatively low output power and bandwidth. We have implemented an FDML laser using a new SOA featuring broad gain bandwidth and high output power. The output spectrum coincides with the wavelength range of minimal water absorption, making the light source ideal for OCT imaging of the posterior eye segment. With a moderate SOA current (270 mA) we achieve up to 100nm total sweep range and 12 μm depth resolution in air. By modulating the current, we can optimize the output spectrum and thereby improve the resolution to 9 μm in air (~6.5 μm in tissue). The average output power is higher than 20mW. Both sweep directions show similar performance; hence, both can be used for OCT imaging. This enables an A-scan rate of 350 kHz without buffering the light source output.
AB - Optical coherence tomography (OCT) in the 1060nm range is interesting for in vivo imaging of the human posterior eye segment (retina, choroid, sclera) due to low absorption in water and deep penetration into the tissue. Rapidly tunable light sources, such as Fourier domain mode-locked (FDML) lasers, enable acquisition of densely sampled three-dimensional datasets covering a wide field of view. However, semiconductor optical amplifiers (SOAs)-the typical laser gain media for swept sources-for the 1060nm band could until recently only provide relatively low output power and bandwidth. We have implemented an FDML laser using a new SOA featuring broad gain bandwidth and high output power. The output spectrum coincides with the wavelength range of minimal water absorption, making the light source ideal for OCT imaging of the posterior eye segment. With a moderate SOA current (270 mA) we achieve up to 100nm total sweep range and 12 μm depth resolution in air. By modulating the current, we can optimize the output spectrum and thereby improve the resolution to 9 μm in air (~6.5 μm in tissue). The average output power is higher than 20mW. Both sweep directions show similar performance; hence, both can be used for OCT imaging. This enables an A-scan rate of 350 kHz without buffering the light source output.
U2 - 10.1117/12.906148
DO - 10.1117/12.906148
JO - Proceedings of SPIE, the International Society for Optical Engineering
JF - Proceedings of SPIE, the International Society for Optical Engineering
SN - 1605-7422
VL - 8213
SP - 82130R
ER -