In this study, the use of a continuous-wave (CW) supercontinuum (SC) seeded by an erbium-doped fiber’s amplified spontaneous emission (ASE) for optical-coherence tomography imaging is experimentally demonstrated. It was shown, by taking an in-depth image of a human tooth sample, that due to the smooth, flat spectrum and long-term stability of the proposed CW SC, it can be readily applied to the spectral-domain optical-coherence tomography system. The relative-intensity noise level and spectral bandwidth of the CW SC are also experimentally analyzed as a function of the ASE beam power.
I. INTRODUCTION
Optical-coherence tomography (OCT) is a highly pro-mising method for the high-resolution, noninvasive imaging of tissue morphology in vivo
[1]
. Conventional OCT systems are constructed based on low-coherence interfero-metry, and the axial-image resolution is determined by the spectral bandwidth of the light source employed. This means that ultrabroad-bandwidth light sources must be used so that systems can obtain higher in-depth-resolution tissue images. The commonly employed broadband light sources include semiconductor-based superluminescent diodes (SLDs)
[2]
, amplified spontaneous emission (ASE) from semicon-ductor optical amplifiers
[3]
, rare-earth-doped-fiber ASE
[4]
, and supercontinuum (SC) sources
[5]
.
Even if good-performance OCT imaging can be achieved with the use of the light sources mentioned above, there is still a need to develop new types of light sources to improve the OCT performance. One high potential candidate is the optical-fiber-based SC source. Conventional fiber-based SC sources have been realized by using the combination of a high-peak-power subpicosecond pulse laser and a highly nonlinear optical fiber
[6]
. When high-peak-power pulses propagate through a highly nonlinear optical fiber, their optical spectrum is broadened due to a variety of nonlinear effects, and the spectrum is finally converted into an SC. In generating an SC from ultrashort pulses, the use of normally dispersive nonlinear fibers is essential to suppre-ssing significant spectral modulation and amplitude fluctuations, which are caused by the nonlinear amplification of input pulse noise
[7]
. The pulse-mode SC has been widely investigated as a broadband source for high-resolution OCT imaging
[8
, 9]
.
On the other hand, SC was also found to be generated in the continuous-wave (CW) mode by using a partially-coherent CW pump beam
[10
-13]
. The physical mechanism for CW SC evolution in optical fiber is slightly different from pulse-mode SC evolution
[10
-13]
. Modulation insta-bility (MI) converts an initial, partially-coherent CW beam coupled into a nonlinear anomalous-dispersion fiber into large numbers of ultrashort soliton-like pulses. When the noisy pulses of random peak powers and durations propagate through the fiber, stimulated Raman scattering (SRS) trans-forms the time-averaged spectrum of the noisy pulses into a broad and flat spectral continuum
[13]
. Various types of partially-coherent light sources have been proposed for the generation of CW SC; for example, a high-power Raman fiber laser
[10
, 14
,
15]
, a rare-earth-doped-fiber amplifiedspontaneous- emission (ASE) source
[16
,
17]
, a low-coherencesemiconductor laser diode
[18]
, and a rare-earth-doped-fiber laser
[19
,
20]
. It is evident that recent technological advances in implementing high-quality nonlinear optical fibers as well as high-power fiber amplifiers enable the practical implementation of stable CW SC sources. The applicability of CW SCs to OCT imaging has been investigated by Hsiung et al.
[20]
. They performed an experimental demonstration, using a CW SC source that had been generated from a high-power Yb fiber laser.
A series of investigations of CW SCs have also been carried out by our group
[15
,
17
,
21
,
22
,
23]
. In particular, the research has focused on CW SCs seeded by erbiumdoped fiber (EDF)’s ASE in telecommunication bands because low-cost, all-fiberized optical components commonly employed for telecommunication systems can be readily used. Through our investigations, it was concluded that such applications as photonic microwave filters
[22]
and wavelength- division-multiplexed passive optical networks (WDMPONs)
[23]
, where spectrum-sliced incoherent beams are employed, could benefit from using the CW SC due to its ultrawide bandwidth and high spectral-power density.
In this study, the potential of the depolarized, incoherent CW SC in another application area (OCT imaging) is explored. More specifically, the use of an EDF’s ASE-seeded CW SC for the high-performance OCT imaging of a human tooth sample is experimentally demonstrated. The implemented all-fiberized CW SC source exhibits a 3-dB spectral bandwidth of ~110 nm, covering the range from 1565~1675 nm, which corresponds to the telecommunication bands of the L-band (1565~1625 nm) and U-band (1625~1675 nm). It is known that the telecommunication band covering 1.4~1.7 ㎛ can also be attractive for OCT imaging due to both its reduced optical scattering and its increased penetration depth at longer wavelengths
[24
-
28]
. One benefit of using telecommunication band light sources is that low-cost, all-fiberized optical components designed for telecommunication systems can be easily used. In this work, it is experimentally demonstrated that imaging of ahuman tooth sample can be readily achieved using aspectral-domain (SD)-OCT system incorporating the CW SC.
II. MATERIALS AND METHOD
- 2.1 CW Supercontinuum Seeded by Erbium-doped Fiber’s ASE
The experimental setup of an SD-OCT system that incorporates the proposed ASE-based CW SC source is shown in
Fig. 1
. The broadband, incoherent, ASE-based CW SC was composed of a seed ASE generator based on a pumped EDF, a high-power Er/Yb amplifier, a cascade of a 1-km highly nonlinear dispersion-shifted fiber (HNL-DSF), a 10-km conventional DSF, and a 50-km standard SMF. A seed ASE beam generated from a pumped EDF was spectrum-sliced using a 3-nm bandpass filter at 1560 nm. The 3-nm ASE beam with ~-13 dBm power was amplified up to ~32 dBm using the high-power Er/Yb amplifier and was subsequently coupled into the 1-km HNL-DSF. The 10-km DSF was cascaded to the HNL-DSF. The 1-km HNL-DSF, the only available highly nonlinear optical fiber in our laboratory, is not long enough to generate sufficient nonlinear effects. The HNL-DSF and DSF, both of which had a zero dispersion wavelength (λ
0
) of 1550 nm exhibited nonlinearity parameters () of ~28 and ~2 W
-1
. km
-1
, respectively, and their narrowband ASE beam was converted into a depolarized spectral continuum due to the combined effects of MI and SRS
[13
,
14]
. MI leads to soliton-like structure formation that experiences subsequent self-Raman interaction. The Raman soliton formation is induced by the random phase and intensity fluctuations of the pump beam propagating through an anomalous-dispersion optical fiber. The large numbers of noisy solitonic structures randomly distributed in space and time give rise to a broad spectral continuum. The 50-km SMF was used as a broadband attenuator to reduce the SC power output to ~15 dBm as a broadband inline attenuator covering the L- and U-bands was not available in our laboratory. Further details on the CW SC source are provided in Ref.
[17]
.
Experimental schematic diagram of the proposed OCT imaging system incorporating a CW SC seeded by EDF’s ASE.Abbreviations: ND, neutral-density filter; GM, galvanometer mirror.
(a) Measured optical spectra of the CW SC for variouspower levels of the amplified 3-nm-bandwidth ASE beam.(b) A linear scaled view of the optical spectrum of the CW SCat an amplified 3-nm-bandwidth ASE beam power of 32 dBm.
Fig. 2
(a) shows the output spectra measured as a function of the amplified 3-nm-bandwidth ASE beam that was coupled into the HNL-DSF. The output spectrum from the 50-km SMF was observed to broaden and flatten as the amplified 3-nm-bandwidth ASE beam power was increased. A linear scaled view of the output SC spectrum at an amplified 3-nm-bandwidth ASE beam power of 32 dBm is shown in
Fig. 2
(b). As a matter of fact, the sharp spectral edge, which was observed at short wavelengths, is undesirable as it causes side lobes in the axial point spread function (PSF). At present, attempts are being made to improve the SC spectral shape without using external spectralshaping filters as external spectral shaping may result in the decrease of the spectral bandwidth. The full-width halfmaximum of the SC bandwidth was determined to be ~110 nm, centered at ~1595 nm, and the corresponding theoretical axial resolution (△z) of imaging was estimated to be 10.2 ㎛ using the following simple relation
[1]:
where λ and λ are the center wavelength and the spectral bandwidth of the broadband source, respectively.
Measured relative-intensity noise levels of the EDF’sASE-seeded CW SC for various power levels of the amplified3-nm-bandwidth ASE beam together with that of C-bandEDF’s ASE.
One concern in investigating the applicability of CW SC to OCT imaging is its relative-intensity-noise (RIN) level because RIN can affect the sensitivity and dynamic range
[29]
. First, RIN measurement of the SC output was performed as a function of the amplified 3-nm-bandwidth ASE beam power by launching the SC output onto a low-noise photodetector with a bandwidth of 10 MHz, which was AC-coupled into an electrical spectrum analyzer. The measured RIN spectra are shown in Fig. 3 together with that of the full C-band EDF’s ASE. As we were interested in RIN within the typical demodulation range of OCT systems, the RIN measurement was carried out within the range of 0.01~10 MHz. The RIN level of the CW SC was found to be much higher than that of EDF’s ASE even if the CW SC was seeded by EDF’s ASE. Specifically, the CW SC RIN level at an amplified 3-nm-bandwidth ASE beam power of 32 dBm was found to be ~20 dB larger than that of the full C-band ASE. Furthermore, contrary to the well-known fact that the RIN of an incoherent broadbandwidth light source is inversely proportional to its spectral bandwidth
[30]
, the RIN of the CW SC was found to increase with the spectral bandwidth, as shown in
Fig. 4
. Such a high RIN level is believed to be due to stimulated- Raman-process-induced, amplified pump-to-stokes RIN transfer
[31]
. Note that the CW SC is generated mainly by the combination of the MI and SRS processes. The high RIN level of the CW SC might degrade the OCT imaging performance. The impact of RIN on the imaging quality can be indirectly inferred from the estimation of signal-tonoise ratio (SNR) of the light source. Note that the SNR estimation is commonly used for the evaluation of signal quality in telecommunication systems. The SNR limitation caused by RIN can be expressed as
[32]
RIN level and spectral bandwidth of the EDF’sASE-seeded CW SC as a function of the amplified3-nm-bandwidth ASE beam power.
where
f
0
and
f
1
are the electrical frequencies. Assuming that the typical demodulation frequency range of OCT systems is 0 ~ 10 MHz,
f
0
and
f
1
become 0 and 10 MHz, respectively. Using eq. (2) the SNR for the CW SC was estimated to be ~32 dB, which is ~ 12 dB lower than that of the full C-band EDF’s ASE (~ 44 dB). Even if the CW SC source exhibits a relatively low SNR compared to the full C-band EDF’s ASE, the SNR value of ~32 dB is believed to cause no significant degradation of imaging quality. This fact needs to be confirmed by a further investigation. Note that in fiber optic communication systems a transmitted, incoherent signal with a SNR more than 18 dB can be detected at the receiver end without bit errors (Bit Error Rate < 10-
14
)
[30]
.
- 2.2 Experimental OCT Setup Incorporating the CW Supercontinuum
Bearing in mind that the high RIN level of the CW SC may significantly affect the OCT imaging performance, we executed an exemplary demonstration of the use of the developed CW SC. As shown in
Fig. 1
, the OCT imaging setup was based on a Mach-Zehnder interferometer. A crosssectional image was produced by transversely scanning the beam across a sample using a galvanometer (GM), and by collecting a reflected profile at each point. The reflected intensities were recorded on a grayscale image as a function of the transverse and axial distances. An optical spectrum analyzer (OSA: AQ6317B, produced by ANDO Electronic Co.) was used in place of a spectrometer to obtain most of the OCT experimental data in this experiment, because an InGaAs-type CCD spectrometer for a 1550-nm region was not available in our laboratory
[2]
. The acquired data from the OSA was transferred to a computer through a shielded general-purpose interface bus cable (GPIB, produced by National Instruments)
[33]
. The maximum GPIB transfer rate was more than 7.2 Mb/s. The acquired data was processed and visualized using the customized software written with LabView
®
.
- 2.3 Human Tooth Sample
A human tooth sample was carefully prepared for the experimental demonstration. As enamel and dentin possess ~2 and ~18% water concentrations, which are substantially lower than that of the skin, their dominant light loss factor is scattering rather than water absorption. Furthermore, the fact that smaller scattering exists at the 1500~1700 nm bands than at the 800 or 1300 nm band allows for low-noise imaging. Note that scattering decreases at longer wavelengths in proportion to (1/λ), indicating that the magnitude at the 1500~1700 nm wavelengths is over 30 times lower than that at the visible wavelengths
[28]
.
III. RESULTS AND DISCUSSION
The shorter the coherence length of the source, the more closely the sample and reference arm group delays must be matched for constructive interference to occur. The OCT system performance was characterized by measuring the PSF using a mirror as a sample. At the 1.2-mm imaging axial distance measured in air, the experimentally determined axial resolution was ~12.2 ㎛ whereas the theoretical resolution with the Gaussian spectrum was ~10.2 ㎛ for the output CW SC spectrum at an amplified 3-nm-bandwidth ASE beam power of 32 dBm. The degradation of the axial resolution can be attributed to various factors, such as the non-Gaussian spectral shape of the light source, the use of a Hamming spectral window before discrete Fourier transform (DFT), and the wavelength dependence of the fiber-optic components employed. To analyze the changes in the dynamic range from the SC source, the point spread functions (PSFs) for variable lengths of the reference arm were measured as presented in
Fig. 5
(a). Since the proposed OCT system using an OSA showed a larger optical-saturation power limit, it was not easy to define the overall sensitivity value of this SD-OCT system. The maximum dynamic range of the logarithm-scaled PSFs at the optical length of 110 ㎛ was found to be ~40 dB, which was determined by detecting the minimum visible intensity of a mirror reflection at the position of the sample with the incident source power of 30 mW.
Fig. 5
(b) shows the obtained OCT image of the sample human tooth sample. The image had 256 transverse pixels and 512 axial pixels. Due to the data acquisition mechanism that was used, the quality of the OCT image acquired using an OSA could not be as high as that acquired using a conventional CCD spectrometer, as explained in Ref.
[2]
. It is expected that a higher-quality OCT image can be obtained with the proposed light source only if an InGaAstype CCD spectrometer for a 1550-nm region is employed in the proposed OCT imaging system. The required time for acquiring the interference signal of an A-line using the OSA over a 130 nm bandwidth in a high-sensitivity-mode resolution bandwidth of 0.05 nm is more than 1.3 s. One of the critical factors contributing to the production of
(a) Measured axial point spread functions at variousoptical-length differences. (b) OCT image of a human toothsample. The brighter regions correspond to the areas with alarger backscattered intensity (unit: dB). A picture of thesample surface is shown in the inset. The double-headedarrow indicates the sample’s scan range for the OCT image.Abbreviations: E, enamel; D, dentin; DEJ, dentoepithelialjunction.
significant signal distortion in the SD-OCT system is the fringe washout phenomenon, which is caused by a very slow readout process. This means that an OCT system using an OSA cannot produce an image with quality as high as that of the images acquired using a conventional CCD spectrometer. Variability in enamel morphology was still evident, however, with a sharp drop in the coherent backscattered intensity clearly delineating the junction between the enamel and dentin layers, as shown in
Fig. 5
(b). The inset shows a surface picture of the human tooth sample. The double-headed arrow in the inset indicates the scan range of the light source which traverses the direction for the OCT image.
IV. CONCLUSION
The possibility of using a depolarized, incoherent CW SC seeded by EDF’s ASE as a broadband source for SD-OCT imaging was investigated. Such a CW SC showed a smooth and flat spectrum as well as long-term stability. It was experimentally shown that the CW SC could be readily applied to the OCT imaging of a human tooth sample. As a matter of fact, several high-quality works on the OCT imaging of human teeth have already been carried out with ~800- and ~1300-nm light sources
[34-
37]
. Even if the image quality obtained with the CW SC in this work is not superior to that obtained in the previous demonstrations using conventional light sources, it can be concluded from our feasibility demonstration that higher-quality OCT images can be achieved through the further optimization and improvement of the OCT setup using a CCD spectrometer, or through the Gaussian spectral shaping of the output CW SC beam.
Acknowledgements
This research was supported by Basic Science Research Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Education, Science and Technology (R01-2007-000-20553-0).
Huang D
,
Swanson E.A
,
Lin C.P
,
Schuman J.S
,
Stinson W.G
,
Chang W
,
Hee M.R
,
Flotte T
,
Gregory K
,
Puliafito C.A
,
Fujimoto J.G
1991
Optical coherence tomography
Science
254
1178 -
1181
DOI : 10.1126/science.1957169
Jung E.J
,
Park J.S
,
Jeong M.Y
,
Kim C.S
,
Eom T.J
,
Yu B.A
,
Gee S
,
Lee J
,
Kim M.K
2008
Spectrallysampled OCT for sensitivity improvement from limited optical power
Opt Exp
16
17457 -
17467
DOI : 10.1364/OE.16.017457
Brezinski E
,
Fujimoto J.G
1998
Optical coherence tomographic imaging of human tissue at 155 μm and 181 μ using Er and Tm-doped fiber sources
J Biomed Opt
3
76 -
79
DOI : 10.1117/1.429898
Nishizawa N
,
Chen Y
,
Hsiung P
,
Ippen E.P
,
Fujimoto J.G
2004
Real-time ultrahigh-resolution optical coherence tomography with an all-fiber femtosecond fiber laser continuum at 15 μ
Opt Lett
29
2846 -
2848
DOI : 10.1364/OL.292846
Westbrook P.S
,
Nicholson J.W
,
Feder K.S
,
Yablon A.D
2005
Improved supercontinuum generation through UV processing of highly nonlinear fibers
IEEE J Lightwave Technol
23
13 -
18
DOI : 10.1109/JLT.2004.840361
Corwin K.L
,
Newbury N.R
,
Dudley J.M
,
Coen S
,
Diddams S.A
,
Weber K
,
Windeler R.S
2003
Fundamental noise limitations to supercontinuum generation in microstructure fiber
Phys Rev Lett
90
113904 -
DOI : 10.1103/PhysRevLett.90.113904
Bourquin S
,
Aguirre A.D
,
Hartl I
,
Hsiung P
,
Ko T.H
,
Fujimoto J.G
,
Birks T.A
,
Wadsworth W
,
Bunting U
,
Kopf D
2003
Ultrahigh resolution real time OCT imaging using a compat femtosecond Nd:Glass laser and nonlinear fiber
Opt Exp
11
3290 -
3297
Wang Y
,
Tomov I
,
Nelson J.S
,
Chen Z
,
Lim H
,
Wise F
2005
Low-noise broadband light generation from optical fibers for use in high-resolution optical coherence tomography
J Opt Soc Am A
22
1492 -
1499
DOI : 10.1364/JOSAA.221492
Martin-Lopez S
,
Gonzalez-Herraez M
,
Carrasco-Sanz A
,
Vanholsbeeck F
,
Coen S
,
Fernandez H
,
Solis J
,
Corredera P
,
Hernanz M.L
2006
Broadband spectrally flat and high power density light source for fiber sensing purposes
Meas Sci Technol
17
1014 -
1019
DOI : 10.1088/0957-0233/17/5/S13
Prabhu M
,
Kim N.S
,
Ueda K
2000
Ultra-broadband CW supercontinuum generation centered at 14834 nm from Brillouin/Raman fiber laser”
Jpn J Appl Phys
39
L291 -
L293
DOI : 10.1143/JJAP.39.L291
Avdokhin A.V
,
Popov S.V
,
Taylor J.R
2003
Continuouswave high-power Raman continuum generation in holey fibers
Opt Lett
28
1353 -
1355
DOI : 10.1364/OL.281353
Kobtsev S.M
,
Smirnov S.V
2005
Modelling of high-power supercontinuum generation in highly nonlinear dispersion shifted fibers at CW pump
Opt Exp
13
6912 -
6918
DOI : 10.1364/OPEX.136912
Abeeluck A.K
,
Headley C
,
Jorgensen C.G
2004
Highpower supercontinuum generation in highly nonlinear dispersion- shifted fibers by use of a continuous-wave Raman fiber laser
Opt Lett
29
2163 -
2165
DOI : 10.1364/OL.292163
Lee J.H
,
Takushima Y
,
Kikuchi K
2005
Continuouswave supercontinuum laser based on an erbium-doped fiber ring cavity incorporating a highly nonlinear fiber
Opt Lett
30
2599 -
2602
DOI : 10.1364/OL.302599
de Matos C.J.S
,
Popov S.V
,
Taylor J.R
2004
Temporal and noise characteristics of continuous-wave pumped continumm generation in holey fibers around 1300 nm
Appl Phys Lett
85
2706 -
2708
DOI : 10.1063/1.1801175
Lee J.H
,
Han Y.G
,
Lee S.B
2006
Experimental study on seed light source coherence dependence of continuouswave supercontinuum performance
Opt Exp
14
3443 -
3452
DOI : 10.1364/OE.143443
Abeeluck A.K
,
Headley C
2004
Supercontiuum growth in a highly nonlinear fiber with a low-coherence semiconductor laser diode
Appl Phys Lett
85
4863 -
4865
DOI : 10.1063/1.1818332
Champert P.A
,
Couderc V
,
Barthelemy A
2004
15-20 μ multiwatt continuum generation in dispersion-shifted fiber by use of high-power continuous-wave fiber source
IEEE Photon Technol Lett
16
2445 -
2447
DOI : 10.1109/LPT.2004.834924
Hsiung P.L
,
Chen Y
,
Ko T.H
,
Fujimoto J.G
,
de Matos C.J.S
,
Popov S.V
,
Taylor J.R
,
Gapontsev V.P
2004
Optical coherence tomography using a continuous-wave high-power Raman continuum light source
Opt Exp
12
5287 -
5295
DOI : 10.1364/OPEX.125287
Kim C.S
,
Kang J.U
2004
Multi-wavelength switching of Raman fiber ring laser incorporating composite PMF Lyot-Sagnac filter
Appl Opt
43
3151 -
3157
DOI : 10.1364/AO.433151
Lee J.H
,
Chang Y.M
,
Han Y.G
,
Lee S.B
,
Chung H
2007
Fully reconfigurable photonic microwave transversal filter based on digital micromirror device and continuous wave incoherent supercontinuum source
Appl Opt
46
5158 -
5167
DOI : 10.1364/AO.465158
Lee J.H
,
Lee K
,
Han Y.G
,
Lee S.B
,
Kim C.H
2007
Single depolarized CW supercontinuum-based wavelength division multiplexed passive optical network architecture with C-band OLT L-band ONU and U-band monitoring
IEEE J Lightwave Technol
26
2891 -
2897
Nishizawa N
,
Chen Y
,
Hsiung P
,
Ippen E.P
,
Fujimoto J.G
2004
Real-time ultrahigh-resolution optical coherence tomography with an all-fiber femtosecond fiber laser continuum at 15 μm
Opt Lett
29
2846 -
2848
DOI : 10.1364/OL.292846
Choi D
,
Amano T
,
Hiro-Oka H
,
Furukawa H
,
Miyazawa T
,
Yoshimura R
,
Nakanishi M
,
Shimizu K
,
Ohbayashi K
2005
Tissue imaging by OFDR-OCT using an SSG-DBR laser
Proc SPIE
5690
101 -
103
DOI : 10.1117/12.592544
Unterhuber A
,
Povazay B
,
Bizheva K
,
Hermann B
,
Sattmann H
,
Stingl A
,
Le T
,
Seefeld M
,
Menzel R
,
Preusser M
,
Budka H
,
Schubert C
,
Reitsamer H
,
Ahnelt P.K
,
Morgan J.E
,
Cowey A
,
Drexler W
2004
Advances in broad bandwidth light sources for ultrahigh resolution optical coherence tomography
Phys Med Biol
49
1235 -
DOI : 10.1088/0031-9155/49/7/011
Sharma U
,
Chang E.W
,
Yun S.H
2008
Long wavelength optical coherence tomography at 17 μ for enhanced imaging depth
Opt Exp
16
19712 -
19723
DOI : 10.1364/OE.16.019712
Fried D
,
Glena R.E
,
Featherstone J.D.B
,
Seka W
1995
Nature of light scattering in dental enamel and dentin at visible and near-infrared wavelengths
Appl Opt
34
1278 -
1285
DOI : 10.1364/AO.341278
Moon S
,
Kim D.Y
2007
Normalization detection scheme for high-speed optical frequency-domain imaging and reflectometry
Opt Exp
15
15129 -
15146
DOI : 10.1364/OE.15.015129
Lee J.S
,
Chung C.H
,
Digiovanni D.J
1998
Spectrumsliced fiber amplifier light source for multi-channel WDM application
IEEE Photon Technol Lett
5
1458 -
1461
Fludger C.R.S
,
Handerek V
,
Mears R.J
2001
Pump to signal RIN transfer in Raman fiber amplifiers
IEEE J Lightwave Technol
19
1140 -
1148
DOI : 10.1109/50.939794
Sato K
,
Toba H
2001
Reduction of mode partition noise by using semiconductor optical amplifiers
IEEE J Select Topics Quantum Electron
7
328 -
333
DOI : 10.1109/2944.954146
Lee H.S
,
Jung E.J
,
Jeong M.Y
,
Kim C.S
2009
Broadband wavelength-swept Raman laser for Fourier-domain mode locked swept-source OCT
J Opt Soc Korea
13
316 -
320
DOI : 10.3807/JOSK.2009.13.3.316
Fonseca D.D.D
,
Kyoyoku B.B.C
,
Maia A.M.A
,
Gomes A.S.L
2009
In vitro imaging of remaining dentin and pulp chamber by optical coherence tomography: comparison between 850 and 1280 nm
J Biomed Opt
14
024009 -
1~024009
DOI : 10.1117/1.3103584
Madjarova V.D
,
Yasuno Y
,
Makita S
,
Hori Y
,
Yamanari M
,
Itoh M
,
Yatagai T
,
Tamura M
,
Nanbu T
2006
In-vivo three dimensional Fourier-domain optical coherence tomography for soft and hard oral tissue measurements
Proc Biomedical Optics Topical Meeting (BIOMED)
FortLauderdale FL USA
Mar 2006
WE3 -
Feldchtein F.I
,
Gelikonov G.V
,
Gelikonov V.M
,
Iksanov R.R
,
Kuranov R.V
,
Sergeev A.M
,
Gladkova N.D
,
Ourutina M.N
,
Warren J.A
,
Reitze D.H
1998
In vivo OCT imaging of hard and soft tissue of the oral cavity
Opt Exp
3
239 -
250
DOI : 10.1364/OE.30239
Manesh S.S
,
Darling C.L
,
Fried D
2009
Polarizationsensitive optical coherence tomography for the nondestructive assessment of the remineralization of dentin
J Biomed Opt
14
044002 -
1~044002
DOI : 10.1117/1.3158995