Analog differential-phase detection in optical coherence reflectometer

doi:10.1364/OE.16.012847

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Analog differential-phase detection in optical coherence reflectometer

Huan-Jang Huang, Tsung-Yu Hsieh, Li-Dek Chou, Wen-Chuan Kuo, and Chien Chou »View Author Affiliations

Optics Express, Vol. 16, Issue 17, pp. 12847-12858 (2008)
http://dx.doi.org/10.1364/OE.16.012847

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▸ Article Outline
– Abstract
1. Introduction
2. Principle of Differential-phase optical coherence reflectometer
3. Experimental setup and results
4. Conclusions and discussion
– References and links

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Abstract

A novel differential-phase optical coherence reflectometer (DP-OCR) was proposed using a low-coherence source, integrating it with an analog differential-phase decoding method. In the experiment, the DP-OCR performed a localized surface profile measurement of an optical grating (1200 lp/mm) and demonstrated its ability to measure the translation speed of a tilted mirror. Experimentally, the resolution of the axial displacement of proposed DP-OCR at 185 pm was demonstrated.

1. Introduction

Interferometer-based surface profile measurements have been developed for many years [1

T. Kubota, M. Nara, and T. Yoshino, “Interferometer for measuring displacement and distance,” Opt. Lett. 12, 310–312 (1987). [CrossRef] [PubMed]

, 2

G. Lai and T. Yatagai, “Generalized phase-shifting interferometry,” J. Opt. Soc. Am. A 8, 822–827 (1991). [CrossRef]

]. Most interferometers use monochromatic light sources and measure displacement by obtaining the phase information through decoding phase difference utilizing various analog methods such as a lock-in amplifier [3

C. Chou, J.C. Shyu, Y. C. Huang, and C. K. Yuan, “Common-path optical heterodyne profilometer: a configuration,” Appl. Opt. 37, 4137–4142 (1998). [CrossRef]

]. However, this method results in a slower response of the phase decoding. Moreover, decoding phase differences via numerical method through Hilbert transformation [4

C. K. Hitzenberger and A. F. Fercher, “Differential phase contrast in optical coherence tomography,” Opt. Lett. 24, 622–624 (1999). [CrossRef]

] or autocorrelation algorithm [5

S. Yazdanfar and J. A. Izatt, “Self-referenced Doppler optical coherence tomography,” Opt. Lett. 27, 2085–2087 (2002). [CrossRef]

] was proposed. The analog method is therefore preferred when attempting to obtain a precise measurement of localized surface profiles because it possesses the advantage of higher sensitivity from its high time-bandwidth product [3

C. Chou, J.C. Shyu, Y. C. Huang, and C. K. Yuan, “Common-path optical heterodyne profilometer: a configuration,” Appl. Opt. 37, 4137–4142 (1998). [CrossRef]

,6–8

C. Chou, C. W. Lyu, and L. C. Peng, “Polarized differential-phase laser scanning microscope,” Appl. Opt. 40, 96–99 (2001). [CrossRef]

]. Recently, low coherence surface profilometers have been developed based on low coherence interferometers [9–11

D. P. Dave and T. E. Milner, “Optical low-coherence reflectometer for differential phase measurement,” Opt. Lett. 25, 227–229 (2000). [CrossRef]

]. This includes the scanning white-light interferometer (SWLI) [12

L. Deck and P. de Groot, “High-speed noncontact profiler based on scanning white-light interferometry,” Appl. Opt. 33, 7334–7338 (1994). [CrossRef] [PubMed]

] and the optical coherence tomography (OCT) [13–15

D. Huang, E. A. Swanson, C. P. Lin, J. S. Shuman, W. G. Stinson, W. Chang, M. R. Hee, T. Flottee, K. Gregory, C. A. Puliafito, and J. G. Fujimoto, “Optical coherence tomography,” Science 254, 1178–1181 (1991). [CrossRef] [PubMed]

], both of which are used for various applications. These interferometers have short temporal coherence lengths represented by 2(ln 2)λ ² ₀/(πΔλ) for localized surface measurements, where λ ₀ is the central wavelength and Δλ is the spectral bandwidth. Thus, they can acquire tomographic images based on a low coherence length of the laser source. For a superluminescent diode (SLD) with the spectral bandwidth equal to 155 nm, almost 2 µm axial resolution of OCT was obtained [16

T. H. Ko, D. C. Adler, and J. G. Fujimoto, “Ultrahigh resolution optical coherence tomography imaging with a broadband superluminescent diode light source,” Opt. Express 12, 2112–2119 (2004). [CrossRef] [PubMed]

]. However, this system cannot measure a structure smaller than 2 µm in thickness variation through intensity response. Hence, various phase-sensitive detection methods, such as differential phase-contrast optical coherence tomography (DPC-OCT) [4

C. K. Hitzenberger and A. F. Fercher, “Differential phase contrast in optical coherence tomography,” Opt. Lett. 24, 622–624 (1999). [CrossRef]

] and microscopy (DPC-OCM) [17

C. G. Rylander, D. P. Dave, T. Akkin, T. E. Milner, K. R. Diller, and A. J. Welch, “Quantitative phase-contrast imaging of cells with phase-sensitive optical coherence microscopy,” Opt. Lett. 29, 1509–1511 (2004). [CrossRef] [PubMed]

,18

M. Sticker, M. Pircher, E. Gotzinger, H. Sattmann, A. F. Fercher, and C. K. Hitzenberger, “En Face imaging of single cell layers by differential phase-contrast optical coherence microscopy,” Opt. Lett. 27, 1126–1128 (2002). [CrossRef]

], spectral-domain phase microscopy (SDPM) [19

M. A. Choma, A. K. Ellerbee, and C. Yang, “Spectral-domain phase microscopy,” Opt. Lett. 30, 1162–1164 (2005). [CrossRef] [PubMed]

], spectral-domain optical coherence phase microscopy(SD-OCPM) [20

C. Joo, T. Akkin, B. Cense, B. H. Park, and J. F. de Boer, “Spectral-domain optical coherence phase microscopy for quantitative phase-contrast imaging,” Opt. Lett. 30, 2131–2133 (2005). [CrossRef] [PubMed]

,21

C. Joo, K. H. Kim, and J. F. de Boer, “Spectral-domain optical coherence phase and multiphoton microscopy,” Opt. Lett. 32, 623–625 (2007). [CrossRef] [PubMed]

], and phase-sensitive OCT using Fourier domain mode-locked laser (FDML-PSOCT) [22

D. C. Adler, R. Huber, and J. G. Fujimoto, “Phase-sensitive optical coherence tomography at up to 370,000 lines per second using buffered Fourier domain mode-locked lasers,” Opt. Lett. 32, 626–628 (2007). [CrossRef] [PubMed]

], are proposed. All of these detection methods are in time or frequency domain. Among them, the SD-OCPM and FDML-PSOCT, which utilize a wider spectral range of low coherence sources, have the capability to acquire axial displacement and localize the surface profile with higher sensitivity compared to other methods using a narrower spectral range SLD in a conventional OCT. The stability and sensitivity of SD-OCPM and FDML-PSOCT on axial displacement are therefore enhanced to the sub-nanometer level [21

C. Joo, K. H. Kim, and J. F. de Boer, “Spectral-domain optical coherence phase and multiphoton microscopy,” Opt. Lett. 32, 623–625 (2007). [CrossRef] [PubMed]

, 22

]. Both methods, however, decode the phase variation numerically. Thus, the phase decoding speed is determined by the data sampling rate. Additionally, a low numerical aperture (NA) objective is adopted in their systems, thereby resulting in less lateral resolution as well. In this experiment, the proposed differential-phase optical coherence reflectometer (DP-OCR) is set up, wherein an SLD is employed as the light source. An analog differential-phase decoding method [6

C. Chou, C. W. Lyu, and L. C. Peng, “Polarized differential-phase laser scanning microscope,” Appl. Opt. 40, 96–99 (2001). [CrossRef]

] is integrated in the DP-OCR for localized surface profile measurement. Similar to SD-OCPM and FDML-PSOCT, the DP-OCR stability on axial displacement was measured and shown with sub-nanometer sensitivity in this experiment. The surface profile of an optical grating at 1200 lp/mm was also scanned. In addition, the translation speed of a tilted mirror was demonstrated as well by measuring the Doppler frequency shift successfully. The comparison between the DP-OCR and the atomic force microscope (AFM) on the surface profile measurement of an optical grating was then discussed. Finally, a novel DP-OCR simultaneously presenting high resolution on axial displacement and high lateral resolution based on a high NA objective and SLD on a localized surface profile measurement was experimentally verified.

2. Principle of Differential-phase optical coherence reflectometer

The experimental setup of DP-OCR is shown in Fig. 1. A SLD is employed as a low coherence light source emitting an elliptically polarized beam. The beam goes through three components composed of a half wave plate (HWP), a polarization beam splitter (PBS1), and a quarter wave plate (QWP) to establish an optical isolator resulting in a circularly polarized output beam. The beam can then be described by Jones vector as

E = E_{0} (\begin{matrix} 1 \\ \pm i \end{matrix}),

(1)

where E ₀=A ₀(k)exp[i(ωt)] and A ₀(k) denotes the electric field amplitude which is a function of the wave number k=2π/λ.

Fig. 1. Schematic diagram of DP-OCR: HWP, half wave plate; QWP, quarter wave plate; BS, beam splitter; PBS1, PBS2, PBS3, polarization beam splitters; D1, D2, photo detectors; DA, differential amplifier; ADC, analog-to-digital converter; S, sample; M, mirror; PZT, piezoelectric-supported mirror.

In Eq. (1), the electric field can be decomposed into one horizontal (E _P=E ₀[1, 0]^T) and one vertical (E _S=E ₀[0,±i] ^T ) polarization component, where the superscript T denotes the transpose. If the laser beam is right-hand circularly polarized, after being split by a 50:50 beam splitter (BS) into two equal-amplitude laser beams, then the reference beam and signal beam are

E_{1} = \frac{1}{\sqrt{2}} E_{0} (\begin{matrix} 1 \\ i \end{matrix}),

(2)

E_{2} = \frac{1}{\sqrt{2}} E_{0} (\begin{matrix} 1 \\ i \end{matrix}),

(3)

respectively. In the reference arm, PZT is modulated at a certain frequency to generate Doppler frequency shift, and the reference beam reflected by PZT is decomposed into P1 wave and S1 wave by PBS3. The signal beam is split by PBS2 into two orthogonal linearly polarized waves, denoted as the P2 wave and the S2 wave, which are expressed by

E_{P 2} = \sqrt{\frac{R_{S}}{2}} E_{0} (\begin{matrix} 1 \\ 0 \end{matrix}) \exp (- i 2 k l_{P 2}),

(4)

E_{S 2} = \sqrt{\frac{R_{M}}{2}} E_{0} (\begin{matrix} 0 \\ i \end{matrix}) \exp (- i 2 k l_{S 2}),

(5)

where R _S and R _M are the reflectivity of S and M, respectively. The l _P2 and l _S2 are the optical path lengths of P2 and S2 waves in the interferometer, respectively. The P2 wave is then focused by an objective (60X, NA=0.85, Olympus) onto the surface of the specimen (S) as the signal beam, and the S2 wave is reflected by M as the reference beam. Thus, two P waves (P1+P2) and two S waves (S1+S2) are recombined and then separated by PBS3, resulting in P- and S-polarized optical heterodyned signals at photo detectors D1 and D2, respectively. The electric fields of P1, P2, S1, and S2 are

E_{P 1} = \sqrt{\frac{R_{1}}{2}} E_{0} (\begin{matrix} 1 \\ 0 \end{matrix}) \exp (- i 2 k l_{P 1}),

(6)

E_{P 2} = \sqrt{\frac{R_{S}}{2}} E_{0} (\begin{matrix} 1 \\ 0 \end{matrix}) \exp (- i 2 k l_{P 2}),

(7)

E_{S 1} = \sqrt{\frac{R_{1}}{2}} E_{0} (\begin{matrix} 0 \\ i \end{matrix}) \exp (- i 2 k l_{S 1}),

(8)

E_{S 2} = \sqrt{\frac{R_{M}}{2}} E_{0} (\begin{matrix} 0 \\ i \end{matrix}) \exp (- i 2 k l_{S 2}),

(9)

where R ₁ is the reflectivity of the mirror mounted on PZT, and l _P1 and l _S1 are the optical path lengths of P1 and S1 waves in the interferometer, respectively. Thus,

E_{P} = \frac{1}{2} E_{0} [\sqrt{R_{1}} \exp (- i 2 k l_{P 1}) + \sqrt{R_{S}} \exp (- i 2 k l_{P 2})],

(10)

E_{S} = \frac{i}{2} E_{0} [\sqrt{R_{1}} \exp (- i 2 k l_{S 1}) + \sqrt{R_{M}} \exp (- i 2 k l_{S 2})],

(11)

i_{p} = γ 〈 E_{P}^{2} 〉

= \frac{γ A_{0}^{2} (k)}{4} [R_{1} + R_{S} + 2 \sqrt{R_{1} R_{S}} \cos (2 k Δ l_{P})],

(12)

i_{S} = γ 〈 E_{S}^{2} 〉

= \frac{γ A_{0}^{2} (k)}{4} [R_{1} + R_{M} + 2 \sqrt{R_{1} R_{M}} \cos (2 k Δ l_{S})],

(13)

where γ is the quantum efficiency of photo detectors, and Δl _P=l _P1-l _P2, Δl _S=l _S1-l _S2. Assume that the power spectrum of SLD, A ² ₀(k), satisfies the condition

A_{0}^{2} (k) = P_{0} S (k),

(14)

where P ₀ is the power of the laser source and S(k) is the Gaussian spectral density

S (k) = \frac{2 \sqrt{\ln 2}}{Δ k \sqrt{π}} \exp {- {[\frac{(k - k_{0}) 2 \sqrt{\ln 2}}{Δ k}]}^{2}},

(15)

k ₀ is the wave number on the central wavelength, and Δk is the spectral bandwidth (FWHM) of the source. The interference signal by integrating the whole spectrum is therefore

I_{P} = \int_{- \infty}^{\infty} i_{P} d k

= \frac{γ P_{0}}{4} \int_{- \infty}^{\infty} S (k) [R_{1} + R_{S} + 2 \sqrt{R_{1} R_{S}} \cos (2 k Δ l_{P})] d k

= \frac{γ P_{0}}{4} \exp [- {(\frac{2 Δ l_{P} \sqrt{\ln 2}}{l_{ω}})}^{2}] [R_{1} + R_{S} + 2 \sqrt{R_{1} R_{S}} \cos (2 k_{0} Δ l_{P})],

(16)

I_{S} = \int_{- \infty}^{\infty} i_{S} d k

= \frac{γ P_{0}}{4} \int_{- \infty}^{\infty} S (k) [R_{1} + R_{M} + 2 \sqrt{R_{1} R_{M}} \cos (2 k Δ l_{S})] d k

= \frac{γ P_{0}}{4} \exp [- {(\frac{2 Δ l_{S} \sqrt{\ln 2}}{l_{ω}})}^{2}] [R_{1} + R_{M} + 2 \sqrt{R_{1} R_{M}} \cos (2 k_{0} Δ l_{S})],

(17)

where the coherence length of the light source is

l_{ω} = \frac{4 \ln 2}{Δ k} = \frac{2 (\ln 2) λ_{0}^{2}}{π Δ λ},

(18)

and λ ₀ is the central wavelength of the low coherence light source. From Eqs. (16) and (17), the Gaussian profile of the interference signals is subsequently obtained. For simplicity, the condition Δl _P≅Δl _S=Δl is assumed in this setup when the surface profile being measured is an optical surface. Thus, Δl≪l_ω is satisfied. The differential signal by using a differential amplifier (DA) becomes

I_{diff} = ∣ I_{P} - I_{S} ∣

≅ ∣ \frac{γ P_{0}}{4} \exp [- {(\frac{2 Δ l \sqrt{\ln 2}}{l_{ω}})}^{2}] {(R_{S} - R_{M}) + 2 \sqrt{R_{1}} [\sqrt{R_{S}} \cos (2 k_{0} Δ l_{P}) - \sqrt{R_{M}} \cos (2 k_{0} Δ l_{S})]} ∣ .

(19)

By considering only the AC part of the signal,

I_{diff} ≅ \frac{γ P_{0} \sqrt{R_{1}}}{2} \exp [- {(\frac{2 Δ l \sqrt{\ln 2}}{l_{ω}})}^{2}] ∣ \sqrt{R_{S}} \cos (2 k_{0} Δ l_{P}) - \sqrt{R_{M}} \cos (2 k_{0} Δ l_{S}) ∣,

(20)

where 2k ₀Δl _P=ω_Dt+ϕ _P and 2k ₀Δl _S=ω_Dt +ϕ _S are defined, ω_D is the Doppler frequency shift from the modulation of PZT, and ϕ _P and ϕ _S are the phase terms corresponding to the path length from PBS2 to S and M, respectively. Therefore,

I_{diff} ≅ \frac{γ P_{0} \sqrt{R_{1}}}{2} \exp [- {(\frac{2 Δ l \sqrt{\ln 2}}{l_{ω}})}^{2}] ∣ \sqrt{R_{S}} \cos (ω_{D} t + ϕ_{P}) - \sqrt{R_{M}} \cos (ω_{D} t + ϕ_{S}) ∣

= \frac{γ P_{0} \sqrt{R_{1}}}{2} \exp [- {(\frac{2 Δ l \sqrt{\ln 2}}{l_{ω}})}^{2}] ∣ \sqrt{R_{S}} \cos (ω_{D} t + ϕ_{P} - ϕ_{S}) - \sqrt{R_{M}} \cos (ω_{D} t) ∣

= \frac{γ P_{0} \sqrt{R_{1}}}{2} \exp [- {(\frac{2 Δ l \sqrt{\ln 2}}{l_{ω}})}^{2}] ∣ \cos (ω_{D} t) [\sqrt{R_{S}} \cos (Δ ϕ) - \sqrt{R_{M}}] + \sin (ω_{D} t) [- \sqrt{R_{S}} \sin (Δ ϕ)] ∣

= \frac{γ P_{0} \sqrt{R_{1}}}{2} \exp [- {(\frac{2 Δ l \sqrt{\ln 2}}{l_{ω}})}^{2}] \sqrt{R_{S} + R_{M} - 2 \sqrt{R_{S} R_{M}} \cos (Δ ϕ)} \cos (ω_{D} t - θ),

(21)

where Δϕ=ϕ _P-ϕ _S is the differential-phase. During the derivation, a common phase ϕ_S was shifted in both cosine terms in Eq. (21) because the differential output signal from the differential amplifier (DA) in Fig. 1 is independent of the initial reference point of both heterodyne signals [6

C. Chou, C. W. Lyu, and L. C. Peng, “Polarized differential-phase laser scanning microscope,” Appl. Opt. 40, 96–99 (2001). [CrossRef]

]. Then

\cos θ = \frac{\sqrt{R_{S}} \cos (Δ ϕ) - \sqrt{R_{M}}}{\sqrt{R_{S} + R_{M} - 2 \sqrt{R_{S} R_{M}} \cos (Δ ϕ)}},

(22)

\sin θ = \frac{- \sqrt{R_{S}} \sin (Δ ϕ)}{\sqrt{R_{S} + R_{M} - 2 \sqrt{R_{S} R_{M}} \cos (Δ ϕ)}} .

(23)

In the experiment, peak values of Eqs. (16), (17), and (21) are simultaneously measured using an analog–to-digital converter:

I_{P}^{M} = Max {\frac{γ P_{0} \sqrt{R_{1} R_{S}}}{2} \exp [- {(\frac{2 Δ l \sqrt{\ln 2}}{l_{ω}})}^{2}] \cos (2 k_{0} Δ l_{P})},

(24)

I_{S}^{M} = Max {\frac{γ P_{0} \sqrt{R_{1} R_{M}}}{2} \exp [- {(\frac{2 Δ l \sqrt{\ln 2}}{l_{ω}})}^{2}] \cos (2 k_{0} Δ l_{S})},

(25)

I_{diff}^{M} = Max {\frac{γ P_{0} \sqrt{R_{1}}}{2} \exp [- {(\frac{2 Δ l \sqrt{\ln 2}}{l_{ω}})}^{2}] \sqrt{R_{S} + R_{M} - 2 \sqrt{R_{S} R_{M}} \cos (Δ ϕ)} \cos (ω t - θ)} .

(26)

In Eq. (26), the differential amplifier’s output signal is related to the differential-phase Δϕ, which varies with the optical path difference of P2 and S2 waves. Finally, the surface height Δh of sample S relative to the reference on M can be calculated by

Δ h = \frac{1}{2} \cdot \frac{λ_{0}}{2 π} \cdot Δ ϕ

= \frac{λ_{0}}{4 π} \cos^{- 1} [\frac{{(I_{S}^{M})}^{2} + {(I_{P}^{M})}^{2} - {(I_{diff}^{M})}^{2}}{{2 I}_{S}^{M} I_{P}^{M}}] .

(27)

However, there might be a residual phase bias generated by optical components or a fixed optical path difference between the two beams from PBS2 to M and S in Fig. 1. This results in a constant surface height Δh ₀ in the measurement. In order to avoid the occurrence of Δh ₀, a calibration procedure is necessary before proceeding with the measurement, wherein the specimen S is replaced by a perfect mirror. The Δh ₀ is then obtained, such that the result from Eq. (27) is modified to be

Δ h = \frac{λ_{0}}{4 π} \cos^{- 1} [\frac{{(I_{S}^{M})}^{2} + {(I_{P}^{M})}^{2} - {(I_{diff}^{M})}^{2}}{{2 I}_{S}^{M} I_{P}^{M}}] - Δ h_{0} .

(28)

3. Experimental setup and results

3.1 DP-OCR configuration and system performance evaluation

In this setup, PZT is modulated at 1Hz frequency and 2 µm longitudinal displacement, resulting in a 4 µm/s average velocity that introduces a ω_D =60.32 rad/s of Doppler frequency shift. The output power of the elliptically polarized SLD (BWC-SLD11, Superlum) is 2 mW and its spectral bandwidth (FWHM) is 25 nm centered at λ ₀=827 nm. To prevent the back-reflected laser beam incident into the laser cavity and attain better source stability, an optical isolator composed of a half wave plate (HWP), a polarization beam splitter (PBS), and a quarter wave plate (QWP) was set up as shown in Fig. 1. The bandwidth of the differential amplifier (LeCroy DA 1855A) is capable of 100 MHz in full bandwidth. To test the temporal stability of the DP-OCR, a plane mirror was used as a tested sample and the fluctuation of axial displacement is measured for a specified period of time. The result is shown in Fig. 2, with the standard deviation calculated at 370 pm within 100 seconds of the measurement. The resolution of axial displacement of 185 pm was then achieved because the displacement is twice as large as the surface profile being measured in this experiment. However, it becomes 3 nm when the measurement lasts 10 minutes due to a long term drift of the system brought by environmental disturbance in the interferometer. A quasi-sinusoidal drift of the mirror was apparently produced in the measurement as shown in Fig. 2. The sampling rate of data acquisition in this experiment was 200K sample/s (single channel). According to the equation of ΔΦ=(4π/λo)Δz, the differential phase sensitivity becomes δ(ΔΦ)=(4π/λo)δ(Δz). Thus, δ(ΔΦ)=0.16° is calculated of this DP-OCR in measurement. The SNR=Δz/δ(Δz)=23 dB was obtained as well in the experiment as shown in Fig. 2. To compare the differential phase sensitivity at 1.8° via Hilbert transformation [23

C. Hitzenberger, E. Goetzinger, M. Sticker, M. Pircher, and A. Fercher, “Measurement and imaging of birefringence and optic axis orientation by phase resolved polarization sensitive optical coherence tomography,” Opt. Express 9, 780–790 (2001). [CrossRef] [PubMed]

] and 5.16° by autocorrelation algorithm [5

S. Yazdanfar and J. A. Izatt, “Self-referenced Doppler optical coherence tomography,” Opt. Lett. 27, 2085–2087 (2002). [CrossRef]

], it is obviously that DP-OCR performs better differential-phase stability

Fig. 2. Stability test of DP-OCR on axial displacement.

In order to verify the DP-OCR principle experimentally, R ₁≅R _S≅R _M=R is arranged by using a plane mirror as testing surface. Equations (21), (22), and (23) are then simplified to be

I_{diff} = ∣ γ P_{0} R \cdot \exp [- {(\frac{2 Δ l \sqrt{\ln 2}}{l_{ω}})}^{2}] \cos (\frac{Δ ϕ}{2}) \cos (ω_{D} t - θ) ∣,

(29)

\cos θ = \cos (\frac{Δ ϕ}{2}),

(30)

\sin θ = - \sin (\frac{Δ ϕ}{2}) .

(31)

To verify Eq. (29) of the output signal from DA, the differential signal variation with respect to the optical path difference produced by displacing the mirror longitudinally at 28 nm on each step was measured using a PZT-controlled precision stage. The experimental results (dots) and theoretical calculation (solid line) in accordance with Eq. (27) are largely consistent with each other as shown in Fig. 3, in which the normalized intensity (V) is defined by

V = \frac{{(I_{diff}^{M})}^{2} - {(I_{V}^{M})}^{2} - {(I_{H}^{M})}^{2}}{2 I_{V}^{M} I_{H}^{M}} = \cos (Δ ϕ)

(32)

Fig. 3. The measured data (dots) and computer simulation (solid line) of a plane mirror axially displaced at 28 nm in each step by use of DP-OCR. The error bar of the measurement is smaller than the size of dots.

3.2 Surface profile measurement of an optical grating

To demonstrate the performance of the DP-OCR, a one-dimensional surface profile of an optical grating (1200 lp/mm) was measured by laterally scanning it in the experiment. Because of the slow speed of the PZT (1 Hz) in this experiment, it limits the measured speed at one data point per second in this experiment. In Fig. 4, the surface profiles scanned by DP-OCR (dots) and by AFM (solid line) are shown and compared.

Fig. 4. Surface profile of an optical grating (1200 lp/mm) measured by DP-OCR (dots) and by AFM (solid line). The error bar of the measured data by DP-OCR is less than the size of the dots.

As seen in Fig. 4, the depth of each groove of optical grating is 55 nm in both methods. However, there is a bias on the surface height (h ₀≅8 nm) between the two measurements. This is due to a residual phase bias attributed by optical components in the DP-OCR. This introduces an optical path difference between P and S polarized heterodyne signals in this measurement. From Fig. 4, it indicates that the principle of DP-OCR is implemental for surface profile measurement.

3.3 Translational velocity measurement of a tilted mirror

To apply DP-OCR in the translational velocity measurement, a tilted mirror was displaced laterally in this experiment to introduce the Doppler frequency shift for velocity measurement in real time. Theoretically, the Doppler shift f_D can be calculated by

f_{D} = \frac{Δ ϕ}{2 π T}

= \frac{1}{2 π T} \cos^{- 1} [\frac{{(I_{S}^{M})}^{2} + {(I_{P}^{M})}^{2} - {(I_{diff}^{M})}^{2}}{2 I_{S}^{M} I_{P}^{M}}],

(33)

where Δϕ and T are the phase difference and the time interval between successive differential-phase measurement, respectively. Thus the translational velocity is calculated [24

C. J. Pedersen, D. Huang, M. A Shure, and A. M Rollins, “Measurement of absolute flow velocity vector using dual-angle, delay-encoded Doppler optical coherence tomography,” Opt. Lett. 32, 506–508, (2007). [CrossRef] [PubMed]

] by

V = \frac{f_{D} λ_{0}}{2 \cos θ},

(34)

where θ is the Doppler angle between the probing beam and the translation direction of the tilted mirror. Figure 5 shows the linear relationship between the translational speed of the electronically driven tilted mirror and the measured Doppler shift. The solid line (red) represents a least squares linear fit to the measured data (blue). In this experiment, the mirror was tilted to set the Doppler angle at 89.75° and the modulation frequency of PZT was 40 Hz. The surface height variation contributing to the differential-phase can be ignored in this phase decoding process in order to ensure the Doppler frequency shift’s accuracy because DP-OCR is localized on the tested mirror’s surface during the measurement. As a result, the uncertainty in Fig. 5 is minimized if a high quality optical mirror is tested in the experiment. However, it was observed that the higher the speed of the mirror being translated, the larger the uncertainty of the Doppler frequency shifted by the DP-OCR due to the instability of the translation stage, as shown in Fig. 5. The DP-OCR is not only able to provide high sensitivity on speed measurement based on the high time-bandwidth product of differential-phase measurement by way of analog amplitude-sensitive phase decoding method using envelope detection technique [25

R. E. Ziemer and W. H. Tranter, Principle of communications: Systems, modulation, and noise , (Houghton Mifflin Co., Boston, MA, 1976).

], it also enables us to reduce excess noise from the laser intensity fluctuation, which implies the possibility of shot-noise-limited detection [6

C. Chou, C. W. Lyu, and L. C. Peng, “Polarized differential-phase laser scanning microscope,” Appl. Opt. 40, 96–99 (2001). [CrossRef]

,26

C. Chou, H. K. Teng, C. C. Tsai, and L. P. Yu, “Balanced detector interferometric ellipsometer,” J. Opt. Soc. Am. A , 23, 2871–2879 (2006). [CrossRef]

]. This experiment is focused on localized surface displacement rather than conventional optical Doppler tomography of the volume medium consideration [27

Z. Chen, T. E. Milner, S. Srinivas, X. Wang, A. Malekafzali, M. J. C. van Gemert, and J. S. Nelson, “Noninvasive imaging of in vivo blood flow velocity using optical Doppler tomography,” Opt. Lett. 22, 1119–1121 (1997). [CrossRef] [PubMed]

], of which the environmental disturbed phase noise in the tested medium induces the fluctuation on velocity measurement.

Fig. 5. Linear relationship between the translational speed of tilted mirror and Doppler shift by DP-OCR.

4. Conclusions and discussion

A novel DP-OCR coupled with an analog differential-phase decoding method using a differential amplifier with a low coherence light source and a high NA objective was set up and demonstrated in the experiment. The advantage of DP-OCR is the combination of high NA objective and narrower band width of SLD that result in better surface localization for surface profile measurement under the non-common configuration in Fig. 1. This is equivalent to the case of SD-OCPM and FDML-PSOCT using lower NA objective and broadband laser source to give better depth resolve performance with a common-path configuration and a cover glass. There is a trade-off on Rayleigh region and lateral resolution in DP-OCR and SD-OCPM or FDML-PSOCT. The DP-OCR benefits from the developed analog differential-phase decoding method which can convert phase modulation into amplitude modulation via conventional envelope detection technique. This results in high SNR and phase detection sensitivity via modified balanced detector scheme and synchronized heterodyne detection [6

C. Chou, C. W. Lyu, and L. C. Peng, “Polarized differential-phase laser scanning microscope,” Appl. Opt. 40, 96–99 (2001). [CrossRef]

]. Moreover, the developed analog decoding method can achieve large time-bandwidth product, wherein the differential amplifier in the DP-OCR is capable of attaining 100MHz in full bandwidth. This obviously results in higher sensitivity on the surface profile measurement.

Three channels’ amplitude modulated heterodyne signals (P wave, S wave, and their difference) are measured simultaneously in DP-OCR. It is not only to decode the difference phase in terms of the demodulated amplitudes of three heterodyne signals simultaneously but also the common phase noise rejection mode as well by use of a differential amplifier. This is critical to the phase decoding sensitivity because high SNR of the detected signal is obtained experimentally. With Hilbert transformation, the correlation between P and S heterodyne signals is degraded numerically. This results in the lower common phase noise rejection ability of phase difference by Hilbert transformation compared with that in DP-OCR. To adopt differential amplifier in DP-OCR mainly the differential-phase is conducted analogically and highly correlated as shown in balanced detector scheme. Besides, the excess noise from the laser intensity fluctuation is reduced too. These are all critical to the improvement on the detection sensitivity of phase decoding in DP-OCR. In the mean time, the sensitivity on envelop detection technique and its fast temporal response are beneficial too. Potentially, DP-OCR is capable of presenting high temporal response when a high speed phase modulator in reference beam is available. This analytical solution of the differential-phase decoding method in DP-OCR is able to recover the localized surface profile’s fine structure at high sensitivity. This is in contrast to the conventional method of using a numerical method with a limited sampling rate to make it difficult to reconstruct surface roughness. As previously discussed, the detection sensitivity and stability on the surface profile are enhanced in DP-OCR because of the analog differential-phase decoding method, which conducts an amplitude sensitive detection in real time. In this experiment, 185 pm on the resolution of axial displacement was achieved by monitoring the stability within 100 seconds. Because the DP-OCR is integrated a conventional SLD of narrow spectral bandwidth (25nm) with a high NA objective, thus, a localized surface profile or translation speed measurement is suitable for DP-OCR. However, DP-OCR is an order of magnitude off from the performance on surface roughness measurement of SD-OCPM [21

C. Joo, K. H. Kim, and J. F. de Boer, “Spectral-domain optical coherence phase and multiphoton microscopy,” Opt. Lett. 32, 623–625 (2007). [CrossRef] [PubMed]

] and FDML-PSOCT [22

] in experiment.

DP-OCR belongs to analog approach rather than in digital domain because the differential amplifier outputs analog signal in real time whereas, the DAQ card samples the output heterodyne signal from differential amplifier in digital domain. This arrangement doesn’t lose the feature of the analog approach with high time-bandwidth product on differential-phase decoding in DP-OCR. It is similar to a digital amplifier integrated with an analog preamplifier for high quality signal detection. In other words, three demodulated amplitudes of I_p and I_S and their difference can be obtained simultaneously by using three independent digital voltmeters with envelope detection in DP-OCR as well. The differential-phase is then able to be decoded precisely in real time [29

C. Tsai, H. Wei, S. Huang, C. Lin, C. Yu, and C. Chou, “High speed interferometric ellipsometer,” Opt. Express 16, 7778–7788 (2008). [CrossRef] [PubMed]

]. Comparison DP-OCR with conventional dual-channel low coherence reflectometers [4

C. K. Hitzenberger and A. F. Fercher, “Differential phase contrast in optical coherence tomography,” Opt. Lett. 24, 622–624 (1999). [CrossRef]

S. Yazdanfar and J. A. Izatt, “Self-referenced Doppler optical coherence tomography,” Opt. Lett. 27, 2085–2087 (2002). [CrossRef]

,30

D. P. Davé and T. E. Milner, “Optical low-coherence reflectometer for differential phase measurement,” Opt. Lett. 25, 227–229 (2000). [CrossRef]

,31

C. Yang, A. Wax, I. Georgakoudi, E. B. Hanlon, K. Badizadegan, R. R. Dasari, and M. S. Feld, “Interferometric phase-dispersion microscopy,” Opt. Lett. 25, 1526–1528 (2000). [CrossRef]

], the sensitivity on differential-phase detection is in the range from 0.7° to 5.16°. It is in contrast to DP-OCR whereas 0.16° of the differential-phase stability was obtained in this experiment. Theoretically, the DP-OCR is capable of simultaneously providing high time-bandwidth and space-bandwidth products on a localized surface profile measurement. In comparison with a white light phase-shifting interferometer (PSI) for surface profile measurement, the DP-OCR exhibited the same sensitivity on the resolution of axial displacement [11

T. Dresel, G. Hausler, and H. Venzke, “Three-dimensional sensing of rough surfaces by coherence radar,” Appl. Opt. 31, 919–925 (1992). [CrossRef] [PubMed]

,12

L. Deck and P. de Groot, “High-speed noncontact profiler based on scanning white-light interferometry,” Appl. Opt. 33, 7334–7338 (1994). [CrossRef] [PubMed]

]. However, a better lateral resolution than a PSI-based profilometer is anticipated.

Fundamentally, the DP-OCR is able to be extended into differential-phase polarization sensitive optical coherence tomography (DP-PSOCT) for birefringent phase measurement. DP-OCR can also utilize a swept source in the Fourier domain [27

] to become SS-DP-PSOCT, which can further enhance the speed on tomographic phase retardation imaging for biomedical applications.

Acknowledgment

This research was partially supported by National Science Council of Taiwan through Grant # NSC95-2221-E-010-015-MY3. The support by “Aim for top university plan” is also appreciated.

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OCIS Codes
(110.4500) Imaging systems : Optical coherence tomography
(120.3180) Instrumentation, measurement, and metrology : Interferometry
(120.5050) Instrumentation, measurement, and metrology : Phase measurement
(120.6660) Instrumentation, measurement, and metrology : Surface measurements, roughness
(110.3175) Imaging systems : Interferometric imaging

ToC Category:
Instrumentation, Measurement, and Metrology

History
Original Manuscript: May 30, 2008
Revised Manuscript: July 12, 2008
Manuscript Accepted: July 28, 2008
Published: August 8, 2008

Virtual Issues
Vol. 3, Iss. 10 Virtual Journal for Biomedical Optics

Citation
Huan-Jang Huang, Tsung-Yu Hsieh, Li-Dek Chou, Wen-Chuan Kuo, and Chien Chou, "Analog differential-phase detection in optical coherence reflectometer," Opt. Express 16, 12847-12858 (2008)
http://www.opticsinfobase.org/oe/abstract.cfm?URI=oe-16-17-12847

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