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1 October 2008 Improved fast scanning delay line in optical coherence tomography applications utilizing fiber stretcher
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We demonstrate an improved fiber-stretcher-based scanning delay line in terms of both the scanning speed and the delay range. Such a module is essential to optical coherence tomography (OCT) applications. An 18-mm delay range at 2-kHz scanning frequency is achieved and verified in a dental OCT setup. Repeatability and reliability of the new design are further evaluated through multiple trials within days. The results confirm its feasibility into practical applications.



Optical coherence tomography (OCT) has been one of the hot research topics in the last few years and has become one of the promising biomedical solutions as related techniques being improved.1, 2, 3, 4, 5, 6, 7, 8 Compared to conventional methods, OCT is capable of cross-sectional imaging of biological tissues or even organs at micrometer-scale resolution. In general, the OCT technique can be achieved in either time-domain (TD-OCT), utilizing scanning time delay lines, or frequency-domain (FD-OCT), scanning the spectrum of the light source itself. As one of the key components of TD-OCT systems, scanning delay lines should have several desired features, especially the high scanning speed and large generated delay range.

Although various schemes of scanning delay lines have been demonstrated in research labs,9, 10, 11 unfortunately, it is difficult in practice to generate a large delay change while keeping the delay variation speed sufficiently high and without sacrificing the reliability.

In this paper, we demonstrate an improved scanning delay line using fiber-stretching technology. Through special and optimized design of the mechanical body and the stretching mechanism, both the scanning speed and the generated delay range are significantly increased. An 18-mm delay at 2kHz is achieved with superior reliability (for practical purposes). This improved design with large scanning range and high speed is further verified in a dental OCT setup.


Improved Fiber Stretcher Design

Several problems existed in previous and available fiber-stretcher designs: (i) unsatisfied reliability, especially the repeatability, and (ii) generating limited delay range, typically several millimeters (e.g., 23mm ). To solve these problems, we specially design a new fiber stretcher as shown in Fig. 1, with several highlighted features: (i) two piezo-electric actuators (PZTs) are used to provide longitudinal stretch on the mechanical frame (used to hold optical fibers); (ii) the mechanical frame is optimized to match the resonance behavior of the PZTs, hence, capable of providing high-speed stretching; and (iii) special procedures are used to secure the optical fibers winding on the frame, such as fiber gluing, to improve the reliability and repeatability. The intrinsic loss of such a module can be as low as 0.1dB if the optical connector losses are neglected ( 0.5dB with connectors).

Fig. 1

Illustration of the improved fiber stretcher design, showing the two PZTs and the main frame.



Results and Discussion

On the basis of this new design, we test the generated delay versus driving frequency using the Mach–Zehnder interferometer configuration (not shown here, as can be found in various fundamental literature). The delay is calculated by counting the interference fringes through a frequency counter. Each interference fringe corresponds to a delay variation of a center wavelength λSource ( 1550-nm light source is used). Assuming that the frequencies of the interference signal and the reference signal are fInterference and fReference , respectively, the delay range can be calculated as (λSourcefInterference)(2fReference) . Figure 2 shows measurement results with a driving voltage of only 55V . At the resonant frequency of the new fiber stretcher (i.e., 1890Hz , which though, can also be tuned to slightly above 2kHz ), the generated delay can be as high as 18mm (corresponding to a scan speed of 34ms ). There are also some peaks with less generated delay at other frequencies (e.g., 13 and 19kHz ), where the delay is typically <1mm limited by the electronic driving circuits.

Fig. 2

Measurement results of generated delay vs driving frequency (the amplitude of the driving signal is 55V ).


Furthermore, we evaluate the reliability (repeatability) of this new module driven at the resonant frequency (i.e., 2kHz ). The results are shown in Fig. 3. Ten independent trails are taken in several days under the same measurement environment (e.g., the driving voltage and frequency), and the almost overlapping traces in Fig. 3 indicate a promising repeatability in terms of delay versus frequency: the delay variation around the resonant frequency is very small and the window of the resonant frequency is not a narrow one (100Hz) . The superior repeatability can guarantee reliable OCT scanning results, while the 100-Hz frequency window can release the requirements for the accuracy and stability of the driving frequency. Both advantages are desired features for practical applications.

Fig. 3

Repeatability (reliability) evaluation results with ten independent trails around the resonant frequency 2kHz .


As such a fast scanning delay line is ideal for OCT applications (e.g., dental or eye diagnosis), where a large delay scanned at high frequencies is generally required, we build a simple dental OCT setup (1-D only) to verify the improved design (Fig. 4). Again, the fiber stretcher is driven at 2kHz . A tooth sample is scanned in one direction using a probe, and the interference output is detected through a fast photodetector [InGaAs PIN type]. The detection circuit includes a transimpedence amplifier and a demodulation circuit. A data acquisition (DAQ) card is used to capture instantaneous voltages (converted from intensities of optical signals) to construct images. The typical result is shown in Fig. 5. Two different positions [Fig. 5a and 5b] of a tooth sample are measured and processed as the probe scanning the sample along the horizontal direction. We can clearly see the profile of the tooth, even at the sharp edge. Note that the picture is symmetric because of the scanning itself, which is not eliminated in our software.

Fig. 4

Evaluation setup for the 1-D dental OCT application. SLD: Super luminescent diode; PD: photodetector; FRM: Faraday rotation mirror.


Fig. 5

(a, b) Photos taken at two different positions as the probe crossing the tooth sample in the horizontal direction.


Here although we optimize the design to have such characteristics, it is still possible to further increase the delay range, as well as the resonant frequency, through more rigorous, and also more time- and cost-consuming engineering designs.



We improved the current fiber-stretcher design to significantly increase both the scanning speed and the delay range and further verified the module in a dental OCT setup. Such a module can be used as an essential part for TD-OCT applications, as well as other possible ones (e.g., microwave photonics networks12).


The authors thank Karen Li and Peter Betts at General Photonics Corp. for help with the design and measurements.



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©(2008) Society of Photo-Optical Instrumentation Engineers (SPIE)
Lianshan Yan, X. Steve Yao, Lynn S. Lin, and Xiaojun Chen "Improved fast scanning delay line in optical coherence tomography applications utilizing fiber stretcher," Optical Engineering 47(10), 100501 (1 October 2008).
Published: 1 October 2008

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