Fullrange spectral domain optical coherence tomography (SDOCT) with a 1μm band light source is shown here. The phase of the reference beam is continuously stepped while the probing beam scans the sample laterally (Bscan). The two dimensional spectral interferogram obtained is processed by a Fourier transform method to obtain a complex spectrum leading to a fullrange OCT image. A detailed mathematical explanation of the complex conjugate resolving method utilized is provided. The system’s measurement speed was 7.96 kHz, the measured axial resolution was 9.6 μm in air and the maximum sensitivity 99.4 dB. To demonstrate the effect of mirror image elimination,
In vivo
human
eye
pathology was measured.
I. INTRODUCTION
Optical coherence tomography (OCT) offers a very effective noninvasive method for the visualization of biological tissues with high resolution and measurement speed
[1]
. The development of Fourier domain OCT (FDOCT)
[2]
has great advantages in terms of acquisition time and sensitivity compared with timedomain OCT (TDOCT). These properties have made FDOCT applicable for 3D ophthalmic imaging
[3]
.
Conventional retinal OCT uses a probing wavelength of 830 nm, but 1μm retinal OCT systems have also been developed. What makes 1μm OCT a very interesting alternative for retinal ophthalmic imaging is that the water absorption has a local minimum at 1.06μm
[4]
. In addition, the longer wavelength scatters less than 830 nm wavelength and allows light to access even the choroid and sclera, providing the great imaging depth mandatory for retinal and choroidal imaging
[5]
. Another important feature of this wavelength is that the zero dispersion point for water exists in this wavelength range
[6]
. Most of the previously reported Fourier domain OCT (FDOCT) systems for the 1μm probing band are based on swept source OCT (SSOCT) technology [
5
,
7
,
8
]. It is still uncertain which is better for ophthalmic retinal imaging, SSOCT or SDOCT, and that is one reason why we want to evaluate our fullrange SDOCT system. Although 1μm SDOCT is a very promising imaging technique for ophthalmic imaging, implementing a practical system is a challenging task. SDOCT requires a highspeed spectrometer utilizing a highspeed line camera. Currently, only a few line detectors are available for the 1μm band, and most of them suffer from a low pixel number, typically less than 1024 pixels. The achievable imaging depth of SDOCT z
_{depth}
is determined by spectrometer’s resolution δλ and the central wavelength λ 0 according to z
_{depth}
= (2ln2/π n) (λ
_{0}
^{2}
/δλ ), where
n
is the refractive index of the sample. Because z
_{depth}
is inversely proportional to δλ , which depends on the pixel number of the line camera, the measurement range of 1 μm is limited. This makes 1μm SDOCT unsuitable for some ophthalmic investigations, such as imaging of the optic nerve head (ONH) of patients with deep cupping, or some pathologies with a large elevation, including agerelated macular degeneration (AMD) with retinal pigment epithelium detachment or a macular hole. Required imaging depth for retina and choroid imaging is even more than 3 mm, while, by using currently available
A severe problem with SDOCT, and not only in the 1μm band, is mirror images which significantly reduce the imaging depth and the signaltonoise ratio (SNR). As SDOCT images are calculated from a measured noncomplex spectral interferogram, they not only comprise a primary OCT image, but also an autocorrelation image and a spatially reversed complex conjugate image. Coherent mirror images reduce the measurement depth range of SDOCT to less than half the original range. In addition, they decrease the SNR of the measured signal.
To eliminate these artifacts, several techniques including phaseshifting methods [
9

23
], a polarization based demodulation method
[24]
, and a 3 × 3 fiber coupler based method
[25]
have been proposed. By obtaining the full complex interferogram, the complex ambiguity problems of SDOCT can be solved. However, for that purpose we have to measure at least two Ascans from the same sampling position with different phase.
When OCT is used for ophthalmic applications, high imaging speed and good tolerance for sample motion is needed. Methods that are based on simultaneous detection of the phase shifted signals [
12
,
17
,
24

25
] tolerate the sample movement, mechanical vibration or air fluctuation. Thus, they are quite useful for
in vivo
retinal imaging where there is quite large and rapid involuntary head movement. However, these techniques require complex system configuration [
24

25
] and even very high speed line detectors
[23]
or 2D detector arrays [
12
,
17
] to be suitable for retinal imaging.
The phase of the spectral interferometric signal can also be measured time sequentially to obtain the full complex interferogram. The phase shifting interferometric method
[9]
requires more than three frames with different phase offset to construct a complex spectrum. Stable phase shift between these frames is required. On the other hand, the phase shifting error caused by sample motion can be corrected
[10]
, but it increases the needed signal processing gratuitously. One of the main problems in ophthalmic imaging is the sample motion and that is the reason why this method is not so suitable for in vivo imaging. The two frame method [
11
,
13
,
16
,
22
] reduces the number of required frames to resolve complex ambiguity making it faster than the phase shifted interferometric method. The drawback of that two frame method is that it requires exact 90 degree phase shift between adjacent frames. Yet another method for the phase measurement of the spectral interferometric signal is simultaneous B and Mmode scanning method (BM analysis method) [
14

15
,
19

21
,
27

29
]. This method modulates the phase of the probe or reference beam along transversal scanning, and extracts the phase of the spectral interference signal by a digital demodulation of the transversal carrier signal which has been generated by the phase modulation. It is know that the BM analysis method has good tolerance to sample motion, miscalibration of the phase shifting device and chromatic phase shifting error. Because of these advantages, we decided to use the BManalysis method in our SDOCT for human retinal and choroidal imaging. The phase modulation is typically performed by a piezoelectric device [
14

15
] which means that phase modulation is based on mechanical movement of a mirror. Thus the temporal response is quite poor in high speed SDOCT applications. Another approach to perform phase modulation is based on transverse scanning by a scanner [
19

21
]. The advantage of this method is that the phase modulation can be performed without any additional components. However, the phase modulation depends on the beam offset on the scanning mirror and the scanning angle. These properties restrict the scanning protocol. To bypass this problem, the electrooptical phase modulator (EOM) is utilized in our system
[26]
. A stepwise control waveform is used to drive the phase modulator to avoid fringe washout.
In this paper we present complex conjugate resolved 1μm spectral domain OCT for human retina imaging in vivo. To resolve complex conjugate ambiguity in SDOCT we modulate the phase of the reference signal using electrooptical phase modulator. The detailed description of our method and experimental setup is presented and experimental fullrange images of the healthy and the AMD patient eye are shown. It should be noted that this paper is organized to supplement our previous paper
[29]
which describes a highspeed fullrange ophthalmic OCT applications based on the method described in this paper but does not describe the mathematical details.
II. SETUP AND DATA PROCESSING
Figure 1
shows the optical setup of our SDOCT system based on the Michelson interferometer. As a light source, a 1μm ASE source (NP Photonics) with a bandwidth of 62.3 nm (FWHM) and a central wavelength of 1042 nm is employed. The light beam is split by a 10/90 coupler and 10 percent of the power is coupled to the sample arm and is connected to a semicustom retinal OCT scanning head based on the TOPCON 3DOCT 1000 (Topcon corporation, Japan) scanning module. After beam splitting, light passes through polarization controllers placed in the sample and reference arms. The optical probing power on the cornea was 840 μW, which is lower than the ANSI safety standard (ANSI Z136.82000). In the reference arm, the beam is collimated and linearly polarized before EOM (Thorlabs, EOPMNRC2). In the measurement arm, the backscattered light and reference signal are combined and guided to a transmission grating (Wasatch Photonics, 1450 lines/mm). A combination of two achromatic lenses (f = 300 mm and f = 150 mm, effective f = 160 mm) is used for spectrum imaging along the horizontal detector area of the line camera
Schematic of measurement system used. (ASE) is light source, (PC) polarization controller, (C) collimator, (LP) linear polarizer, (EOM) electrooptical phase modulator, (NDF) neutral density filter, (OL) objective lens, (M) mirror, (G) grating and (HVA) is high voltage amplifier.
(Sensors Unlimited Inc., SU1024LE, 1024 pixels, 7.69 kHz line rate, integration time 24.4 μs and duty cycle 18.8 %). The axial resolution of the measurement system is 9.6 μm in air.
For the proper operation of the SDOCT system, the data acquisition of the line camera, the scanning of the probing beam and the phase modulation of reference arm have to be synchronized. Control signals are generated by a standard PC running custom built LabVIEW software. EOM control is performed so that the phase step between each Ascan is π /2 rad. The phase of the reference arm is modulated simultaneously as the probing beam scans the sample laterally (Bscan). The spacing of each adjacent Aline is kept smaller than the lateral optical resolution (~20 μm) to be able to separate signal from its complex conjugate signal in the spatial frequency domain. The ratio (spacing/spot size) should be smaller than π /8 and thus the spacing between adjacent Ascans is 2.93 μm. The measurement time to obtain a 2D spectral interferogram is identical with that of a noncomplex FDOCT
[14]
.
Figure 2
presents a time chart used to control the galvanoscanner, the linecamera and the EOM.
Our previously published paper summarized the principle of the complex conjugate resolving method in general
[29]
. However, a more comprehensive explanation of mathematical details is provided here to clarify the method which is employed. As the phase of the reference arm is modulated synchronously with the lateral scanning of the sample, the obtained 2D spectral interferogram Ĩ (
x
, ω) can be expressed as
where
x
is the transversal position of the B scan,
and
are the temporal Fourier transforms of the complex profiles of the probing and the reference beams,respectively, φ is the phase offset and * denotes the complex conjugate of the concerned term. The abbreviation
Time chart of SDOCT control signals used. Signal(a) controls the angle of galvano mirror (b) triggers the linecamera to start data acquisition (c) is the Ascan trigger and(d) is used to control EOM. Each step in signal (d) cause π /2 rad phase shift for reference signal.
c.c. refers to the complex conjugate of the third term on the righthand side of this equation. The first two terms are the autocorrelation of the probe beam and the reference beam, respectively. The third term corresponds to the OCT signal, and it is modulated by the exponential term of exp[
iφ
(
x
)]. The forth term corresponds to a mirror image and is modulated by an exponential term of exp [
iφ
(
x
)]. In our method,
φ
(
x
) is configured as shown in
Fig. 2
(d),which is a linear phase function of x with a slope denoted by
β
. Hence Eq. (2) proves that, due to the phase modulation of the reference signal, the components of the autocorrelation signals, complex conjugate signal and OCT signal possess different carrier spatial frequencies. Namely,the autocorrelation terms have no carrier frequency, the OCT signal has positive carrier frequency in proportion to
β
, while the mirror image has negative carrier frequency in proportion to 
β
. Because of this difference in carrier frequency, these signals can be distinguished after a Fourier transform along
x
as
where
u
is the Fourier conjugate of
x
, Γu and * are a correlation operator and a convolution operator along
u
, respectively, and F
_{x}
[ ] denotes the Fourier transform operator along x.
Information on the OCT signal is extracted by using a suitable frequency filter, which clips only the third term of Eq. (2), followed by an inverse Fourier transformation.
As expressed in this equation, the complex 2D spectrum btained is identical to the complex spectra obtained by phaseshifting FDOCT
[9]
. Using that 2D complex spectrum allows us to obtain fullrange imaging depth.
In order to remove fixedpattern noise, the measured raw data was filtered. For each image, the spectra with different phase shift (0, π /2, π , 3π /2) were assorted to their own groups. The averaged spectrum for each phase shift is calculated and subtracted from the original spectra with corresponding phase shift
[30
,
31]
. Using that procedure the great fixedpattern noise rejection in the final OCT image is obtained.
III. RESULTS AND DISCUSSION
The efficiency of the method used in removing the complex conjugate signal was evaluated quantitatively using a mirror as a sample.
Figure 3
shows the obtained results. Both of the red and blue curves were obtained by the same full range measurement but different configuration of numerical dispersion compensation. Since the interferometer used in this study has unbalance dispersion between the sample and reference arms, numerical compensation of dispersion,by which a numerical phase pattern is added to the OCT spectrum, is required. In addition, the numerical phase patterns which compensate the dispersions of the OCT image and mirror image are conjugate to each other. Namely, the numerical phase which cancels the dispersion of the OCT image blurs the mirror image, and vice versa. To fairly evaluate the ability of our full range method, the elimination ratio of the mirror signal is defined by the ratio between the peak intensity of an OCT signal which is numerically dispersioncompensated for itself (red sharp peak in
Fig. 3
)and that of mirror signal which is again numerically dispersioncompensated for itself (blue sharp peak in
Fig.3
).
Figure 3
shows that our method suppresses the mirror signal by about 27.8 dB at the depth of 0.5 mm and suppresses the autocorrelation signal to the noise level.
Measured OCT signals when mirror is used as a sample. Blue is the fullrange OCT signal with counter dispersion compensation; red the OCT signal with dispersion compensation.
Due to the dispersion of the used EOM, the signal peak obtained from the mirror is distorted. However, by employing a numerical dispersion compensation method, the peak of the OCT signal is sharpened and the conjugate signal peak is further degraded. This property of dispersion further enhances the mirror image extinction ratio. The complex conjugate rejection ratio (CCRR) as a function of imaging depth is shown in
Fig. 4.
The measured CCRR is almost depth independent.
The acceptable axial motion is calculated to be  0.11< vz < 0.29 mm/s. This acceptable axial motion is defined as the maximum allowable Doppler frequency at which, in the spatial frequency domain of the transversal scanning, the 3 dB point of the OCT signal overlaps the 3 dB point of the frequency filter which is employed for the BM analysis. If the axial motion exceeds this velocity, the OCT signal shifts out from the spatial frequency filter, and is degraded significantly.
The sensitivity of the SDOCT device was measured as a function of imaging depth with and without phase modulation in the reference arm. A reflector and a neutral density filter were attached to the sample arm. The single pass sample beam attenuation was measured to be 18.1 dB. The signal of sample mirror is located at delay of 550 μm and 512 Ascans were measured and averaged in intensity to determine the signal strength, while the noise level is determined from the standard deviation of the noise floor. The sensitivity is defined as an attenuationcorrected SNR. The obtained results are shown in
Fig. 5
. The sensitivity gain achieved exceeded 3 dB and was found to depend on the frequency filter bandwidth. The measurement results are fitted by theoretical sensitivity decay curves
[32]
. Since this method is based on bandwidth limitation, sensitivity is increased due to a reduction in noise power. In our experiments, average sensitivity increased by 5.12 dB if our phase modulation method is used. The detailed theory of this sensitivity gain is described in Ref. 29.
Complex conjugate rejection ratio as a function ofdepth. Measured sensitivity of SDOCT as a function of measurement depth. Blue without phase modulation red with modulation. The measurement results are fitted by theoretical sensitivity decay curves [31].
Measured sensitivity of SDOCT as a function of measurement depth. Blue without phase modulation red with modulation. The measurement results are fitted by theoretical sensitivity decay curves [31].
Full range imaging also enables the sample measurement at zero delay position where the SNR reaches its maximum. This is because the effect of depthdependent signal degradation is minimized. Assuming that the 2.0mm effective imaging depth is needed, the measured OCT signal will be decreased about 11 dB if halfrange imaging is performed. The corresponding signal degradation of fullrange imaging will be less than 4 dB. Taking into account the effect of average sensitivity increment of our method and lower depth dependent signal degradation, more than 12dB sensitivity improvement can be achieved over 2mm imaging range compared with halfrange imaging.
To demonstrate the effect of eliminating the mirror image of this SDOCT, a normal eye of an Asian male was measured in the normal and mirrorimage elimination modes.
Figure 6
displays the measurement results. Both crosssectional images comprise 1024 Ascans, and the width of the measured line was 3 mm. Moreover, with a dynamic range of 45 dB and a minimum value of 5 dB subtracted from the noise floor, the images are fully comparable. Although
Fig. 6
shows only the regionofinterest (ROI) of 3.6 mm, the maximum imaging depth was 5.4 mm. In the normal mode (A), the ROI is close to the zero delay and thus the autocorrelation images and complex conjugate image disturb the image quality. This means that if half range imaging is performed, the ROI has to be located sufficiently far from the zero delay. Thus, the effective imaging depth is less than half of the original (2.7 mm) which is not always sufficient for the study of pathologic eyes. However, mirror image elimination mode (B) solves the problem, enabling a clear visualization of the retina and choroid with sufficient imaging range.
As we already mentioned, the requirements for OCT system are typically much higher for investigation of pathologic eyes. Thus the macula of an Asian male with AMD was
Bscan images of optic nerve head (A) normal mode (B) mirrorimageelimination mode.
measured in the normal and mirrorimage elimination modes to demonstrate the applicability of our system to real patient imaging.
Figure 7
shows the measurement results. The imaging was performed with similar settings to the normal eye measurement except that the ROI in normal imaging mode is shifted away from zero delay. This is done to minimize the effect of complex conjugate and autocorrelation artifacts on the ROI. Comparing the images obtained using normal mode (A) and mirror image elimination mode (B), it can be seen that the contrast is decreased in normal mode imaging because the sensitivity of SDOCT is imaging depth dependent.
The development of the highspeed and 3D version of this system is now in progress. We believe that this highspeed property reduces the problems of the fringe washout and improves the modulation phase stability among Bscans. Because of these advantages, the measurement stability of our system will be improved. In addition, we expect that almost no missing frames exist in the 3D OCT volume making that system very effective for retinal imaging
in vivo
.
In summary, a fullrange 1μm SDOCT device was demonstrated. A complex conjugate resolved OCT signal was
Bscan images of macula with AMD (A) normal mode (B) mirrorimageelimination mode.
obtained by modulating the phase of the reference signal using an electrooptical modulator. A comprehensive mathematical explanation of the complex conjugate resolving method that was used was provided. The measurements performed on a normal and AMD eye proved that this method is applicable to practical ophthalmic studies.
Acknowledgements
This study is partially supported by the Japan Science and Technology Agency through the contract of the development program of advanced measurement systems. This study was presented in part at a conference of Coherence Domain Optical Methods and Optical Coherence Tomography in Biomedicine XII, BiOS, Photonics West in 2008.
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
Fercher A. F
,
Hitzenberger C. K
,
Kamp G
,
ElZaiat S. Y
1995
Measurement of intraocular distances by back scattering spectral interferometry
Opt. Comm.
117
43 
48
DOI : 10.1016/00304018(95)00119S
Nassif N
,
Cense B
,
Park B
,
Pierce M
,
Yun S
,
Bouma B
,
Tearney G
,
Chen T
,
de Boer J
2004
In vivo highresolution videorate spectraldomain optical coherence tomography of the human retina and optic nerve
Opt.Express
12
367 
376
DOI : 10.1364/OPEX.12.000367
Hale G. M
,
Querry M. R
1973
Optical constants of water in the 200nm to 200$m wavelength region
Optical constants of waterin the 200nm to 200$m wavelength region
12
555 
563
Yasuno Y
,
Hong Y
,
Makita S
,
Yamanari M
,
Akiba M
,
Miura M
,
Yatagai T
2007
In vivo highcontrast imaging of deep posterior eye by 1um swept source opticalcoherence tomography and scattering optical coherenceangiography
Opt. Express
15
6121 
6139
DOI : 10.1364/OE.15.006121
Wang Y
,
Nelson J
,
Chen Z
,
Reiser B
,
Chuck R
,
Windeler R
2003
Optimal wavelength for ultrahighresolutionoptical coherence tomography
Opt. Express
11
1411 
1417
DOI : 10.1364/OE.11.001411
Zhang J
,
Wang Q
,
Rao B
,
Chen Z
,
Hsu K
2006
Sweptlaser source at 1 μm for Fourier domain optical coherencetomography
Appl. Phys. Lett.
89
073901 
DOI : 10.1063/1.2335405
Lee E. C
,
de Boer J. F
,
Mujat M
,
Lim H
,
Yun S. H
2006
In vivo optical frequency domain imaging of humanretina and choroid
Opt. Express
14
4403 
4411
DOI : 10.1364/OE.14.004403
Wojtkowski M
,
Kowalczyk A
,
Leitgeb R
,
Fercher A. F
2002
Full range complex spectral optical coherence tomography technique in eye imaging
Opt. Lett.
27
1415 
1417
DOI : 10.1364/OL.27.001415
Targowski P
,
Wojtkowski M
,
Kowalczyk A
,
Bajraszewski T
,
Szkulmowski M
,
Gorczynska I
2004
Complex spectral OCT in human eye imaging in vivo
Opt. Comm.
229
79 
84
DOI : 10.1016/j.optcom.2003.10.041
Leitgeb R. A
,
Hitzenberger C. K
,
Fercher A. F
,
Bajraszewski T
2003
Phaseshifting algorithm to achieve highspeedlongdepthrange probing by frequencydomain opticalcoherence tomography
Opt. Lett.
28
2201 
2203
DOI : 10.1364/OL.28.002201
Yasuno Y
,
Makita S
,
Endo T
,
Aoki G
,
Sumimura H
,
Itoh M
,
Yatagai T
2004
Oneshotphaseshifting Fourierdomain optical coherence tomography by reference wavefronttilting
Opt. Express
12
6184 
6191
DOI : 10.1364/OPEX.12.006184
Gotzinger E
,
Pircher M
,
Leitgeb R
,
Hitzenberger C
2005
High speed full range complex spectral domain opticalcoherence tomography
Opt. Express
13
583 
594
DOI : 10.1364/OPEX.13.000583
Yasuno Y
,
Makita S
,
Endo T
,
Aoki G
,
Itoh M
,
Yatagai T
2006
Simultaneous BMmode scanning method for realtime fullrange Fourier domain optical coherence tomography
Appl. Opt.
45
1861 
1965
DOI : 10.1364/OPEX.12.006184
Wang R
2007
In vivo full range complex Fourier domainoptical coherence tomography
Appl. Phys. Lett.
90
054103 
DOI : 10.1063/1.2437682
Bachmann A
,
Leitgeb R
,
Lasser T
2006
Heterodyne Fourier domain optical coherence tomography for full range probing with high axial resolution
Opt. Express
14
1487 
1496
DOI : 10.1364/OE.14.001487
Tao Y. K
,
Zhao M
,
Izatt J. A
2007
Highspeed complexconjugate resolved retinal spectral domain optical coherencetomography using sinusoidal phase modulation
Opt. Lett.
32
2918 
2920
DOI : 10.1364/OL.32.002918
Baumann B
,
Pircher M
,
Gotzinger E
,
Hitzenberger C. K
2007
Full range complex spectral domain optical coherence tomographywithout additional phase shifters
Opt. Express
15
13375 
13387
DOI : 10.1364/OE.15.013375
Leitgeb R. A
,
Michaely R
,
Lasser T
,
Sekhar S. C
2007
Complex ambiguityfree Fourier domain optical coherencetomography through transverse scanning
Opt. Lett.
32
3453 
3455
DOI : 10.1364/OL.32.003453
An L
,
Wang R. K
2007
Use of a scanner to modulatespatial interferograms for in vivo fullrange Fourierdomainoptical coherence tomography
Opt. Lett.
32
3423 
3455
DOI : 10.1364/OL.32.003423
Bachmann A
,
Michaely R
,
Lasser T
,
Leitgeb R
2007
Dual beam heterodyne Fourier domain optical coherencetomography
Opt. Express
15
9254 
9266
DOI : 10.1364/OE.15.009254
Vakhtin A
,
Peterson K
,
Kane D
2007
Demonstration ofcomplexconjugateresolved harmonic Fourierdomain opticalcoherence tomography imaging of biological samples
Appl. Opt.
46
3870 
3877
DOI : 10.1364/AO.46.003870
Vakoc B
,
Yun S
,
Tearney G
,
Bouma B
2006
Eliminationof depth degeneracy in optical frequencydomain imagingthrough polarizationbased optical demodulation
Opt. Lett.
31
362 
364
DOI : 10.1364/OL.31.000362
Sarunic M
,
Choma M. A
,
Yang C
,
Izatt J. A
2005
Instantaneous complex conjugate resolved spectral domainand sweptsource OCT using 3×3 fiber couplers
Opt. Express
13
957 
967
DOI : 10.1364/OPEX.13.000957
Zhang J
,
Nelson J. S
,
Chen Z
2005
Removal of a mirrorimage and enhancement of the signaltonoise ratio inFourierdomain optical coherence tomography using anelectrooptic phase modulator
Opt. Lett.
30
147 
149
DOI : 10.1364/OL.30.000147
Fabritius T
,
Makita S
,
Yamanari M
,
Myllyla R
,
Yatagai T
,
Yasuno Y
2008
Full range 1μm spectral domainoptical coherence tomography by using electroopticalphase modulator
Proc. SPIE
6847
68471S110 
Vergnole S
,
Lamouche G
,
Dufour M. L
2008
Artifactremoval in Fourierdomain optical coherence tomographywith a piezoelectric fiber stretcher
Opt. Lett.
33
732 
764
DOI : 10.1364/OL.33.000732
Makita S
,
Fabritius T
,
Yasuno Y
2008
Fullrange highspeedhighresolution 1μm spectraldomain optical coherencetomography using BMscan for volumetric imaging of thehuman posterior eye
Opt. Express
16
8406 
8420
DOI : 10.1364/OE.16.008406
Gotzinger E
,
Pircher M
,
Hitzenberger C. K
2005
Highspeed spectral domain polarization sensitive optical coherencetomography of the human retina
Opt. Express
13
10217 
10229
DOI : 10.1364/OPEX.13.010217
Wang R. K
,
Ma Z
2006
A practical approach to eliminateautocorrelation artefacts for volumerate spectral domainoptical coherence tomography
Phys. Med. Biol.
51
3231 
3239
DOI : 10.1088/00319155/51/12/015
Yun S
,
Tearney G
,
Bouma B
,
Park B
,
de Boer J
2003
Highspeed spectraldomain optical coherence tomographyat 1.3 μm wavelength
Opt. Express
11
3598 
3604
DOI : 10.1364/OE.11.003598