Poling Quality Enhancement of PPLN Devices Using Negative Multiple Pulse Poling Method
Poling Quality Enhancement of PPLN Devices Using Negative Multiple Pulse Poling Method
Journal of the Optical Society of Korea. 2011. Jun, 15(2): 182-186
Copyright ©2011, Optical Society of Korea
  • Received : January 01, 2011
  • Accepted : April 04, 2011
  • Published : June 25, 2011
Export by style
Cited by
About the Authors
Ju Won Choi
Graduate Program of Photonics and Applied Physics, Gwangju Institute of Science and Technology, Gwangju 500-712, Korea
Jung Hoon Ro
Department of Biomedical Engineering School of Medicine, Pusan National University, Busan 602-739, Korea
Do-Kyeong Ko
Advanced Photonics Research Institute, Gwangju Institute of Science and Technology, Gwangju 500-712, Korea
Nan Ei Yu
Advanced Photonics Research Institute, Gwangju Institute of Science and Technology, Gwangju 500-712, Korea
A poling method using multiple negative voltage was introduced to fabricate periodically poled lithium niobate (PPLN) devices with quasi-phase matching (QPM) period of 12.9 ㎛ by utilizing an real-time visualization system. We also performed variation of the electric field during the poling. Two different conventionally used poling method, negative and positive single pulses, were used and the poling quality compared through microscopic images and far-field diffraction pattern analysis. Etched images on the +z and ?z surfaces of PPLN showed that negative multiple pulse poling presented the highest periodicity in domain structures among the three methods. Duty ratio and its standard deviation were measured by analyzing far-field diffraction patterns. The newly introduced method of negative multiple pulse poling had duty ratio of 0.42 which was close to the ideal value of 0.50 and standard deviation of 0.020 that was about 3 times smaller than that of the other conventional methods.
Quasi-phase matching (QPM) devices are widely used because phase matching is always possible between interaction waves by reversing the sign of nonlinear coefficients at every coherence length . QPM has the advantage that the largest nonlinear coefficient can be utilized for obtaining high conversion efficiency. Moreover, phase matching within the transparent region of a nonlinear crystal is achieved easily and spatial walk-off can be eliminated by propagating light along the optic axis of a birefringent medium [1] .Possessing spontaneous polarizations which can be reversed by an external electric field, ferroelectric crystals have been widely used for fabricating QPM devices. There are many kinds of ferroelectric crystals such as LiTaO 3 , LiNbO 3 , KTiOPO 4 (KTP) and so on. Above all, LiNbO 3 is the most attractive ferroelectric crystal due to its large nonlinear coefficient (d 33 = 27 pm/V) [2] .
Fabrication of periodically poled LiNbO 3 (PPLN) has been developed since the 1980s [ 3 , 4 ]. In particular, a high electric field poling method at room temperature made it possible to fabricate periodically poled bulk devices [ 5 , 6 ]. Additional techniques such as corona discharging [7] , temperature elevation [8] , UV lightening [9] and back-switched voltage waveform [10] were demonstrated to manufacture high-quality PPLN with short-pitch QPM periods. Real-time monitoring of polarization reversal during electric field poling also assists to produce the high-quality PPLN because it is possible to observe domain structures nondestructively. Therefore,real-time domain visualization has been broadly used in many research groups [ 11 , 12 ].
In this work, we introduced a new poling method which was the negative multiple pulses poling (NMP) method combined with our real-time visualization system to fabricate uniform PPLNs in periodicity. We applied negative incubation voltage (-4.5 kV) before the poling voltage, then the pulse was repeated until the end of the poling process during the real-time monitoring of polarization reversal. The poling quality between NMP and other two conventional pulse poling methods was compared by showing microscope images on +z and ?z surfaces of PPLN samples and analyzing the duty ratios by utilizing far-field diffraction patterns.
We used a z-cut congruent LiNbO 3 (cLN) wafer 0.5-mmthick and 3-inch diameter (Crystal Technology Inc). Liquid electrodes using photoresist patterns (Clariant, AZ5214E)were formed on the +z surface of the cLN wafer. The pattern thickness was 1.2 ㎛ and the QPM period was 12.9 ㎛. For polarization reversals, high DC voltage was applied to the cLN crystal with the waveform as shown in Fig. 1 . The voltage waveform consisted of 3 parts: incubation(a), polarization reversal (poling) (b), and stabilization (c).The conventional incubation voltage of cLN was about 9 kV [13] , which had the role of preventing crystal damage from a sudden increase in the poling voltage. However,our incubation voltage in Fig. 1 (a) was -4.5 kV which was not only half of the conventional value but also a negative pulse. The reason is that it was observed that the polarization reversals occurred even in the photoresist part when a long pulse was applied for poling. It means that the domain merging which can obstruct the formation of periodic domain structures can occur due to the long poling time. Therefore, we ensured that photoresist was not a perfect insulator any more during the long poling time. If photoresist is considered as a capacitor, the negative incubation voltage (-4.5 kV) can support longer time than the conventional incubation voltage (9 kV) for charging up the photoresist.Accordingly, if the waveform with the negative incubation voltage shown as in Fig. 1 is repeated during the whole process, domain merging can be reduced.
In general the incubation voltage was determined by not only the back-poling field but also the difference between
PPT Slide
Lager Image
Voltage waveform with negative incubation. Itconsists of three parts; incubation (a), poling (b) andstabilization region (c). This pulse form repeated 10 times forchanging poling time to 10, 5 (5 times) and 3ms (4 times) insequence.
the incubation voltage and the poling voltage. Because the incubation voltage should not create polarization reversals,so it is higher than the back-poling voltage which can invert polarization switch back to the original polarization state. The reported back-poling field of cLN is about -16 kV/mm [14] . Furthermore, a large difference between the incubation and poling voltage can cause crystal damage.Therefore, we applied the incubation voltage of -4.5 kV for 5 seconds. In the case of cLN, coercive field for inverting polarizations is about 21 kV/mm [14] . The poling voltage as shown in Fig. 1 (b) reversing the spontaneous polarization of cLN should be higher than coercive field because nucleation density depends on electric field strength. The applied poling voltage was 11.4 kV and the poling charge(Q) was estimated by the hysteresis loop of cLN (Q ~ P s A, P s = spontaneous polarization of cLN (~ 78 μC/cm 2 ), A = poled area) [15] . The calculated poling charge was 73.1 μC and the poling current was set to 2.1 mA, so the estimated poling time was 34.8 ms.
After polarization reversal, the reversed domain is not stable for some moments thus a sudden voltage drop can be induced by back-switching. To protect against back-switching a stabilization voltage should exist after the poling as shown in Fig. 1 (c). It was known that the stabilization time needed to be longer than ~50 ms for maintaining the inverted polarizations after polarization reversal [15] .Therefore, we applied 9 kV of stabilization voltage for a long enough time such as 100 ms. The designed waveform as presented in Fig. 1 was applied to the cLN crystal repeatedly by changing the poling time ( Fig. 1 (b) part)using measured voltages in oscilloscope and real-time visualization images.
Fig. 2 shows the expansion of the poled area in the +z surface of cLN during electric field poling by the real-time visualization system. Because of the electro-optic effect on the domain boundary one can see the contrast of the domain images [16] . The grey color of the images represented the patterned area on the +z side and the black color was the non-patterned area. The color difference between the patterned and non-patterned surfaces was due to its reflectivity. Most of the domain nucleation had occurred at the edges of the patterned area and the domains created had propagated along patterned areas as presented in Fig. 2 . When all patterned areas had been poled by checking the real-time images, the poling process was terminated.
The measured voltage is also one of the key parameters for manufacturing high quality PPLN. Figure 3 (a) shows the oscilloscope data during the first poling time of 10 ms.Measured current was 2.1 mA. The high-voltage amplifier(Trek 30/20) had a current limit thus the trend of the control voltage was not the same as that of the measured voltage during the poling. Figure 3 (b) showed the variation of the poling voltages measured by each pulse during the electric poling. After the nucleation voltage (10.77 kV)was applied, the voltage was dropped to 10.71 kV then kept constant for 10 ms. The constant voltage, which was
PPT Slide
Lager Image
Images on patterned sides using real-time domainvisualization for negative multiple pulse poling. The order ofdomain propagation is (a), (b), (c), (d), (e), (f), (g), (h), (i) and(j) with accumulated poling time, 8.4, 11.8, 15.2, 18.6, 22,25.4, 26.8, 28.2, 29.6 and 31 ms, respectively. Each mage wassaved during incubation voltage (-4.5 kV).
lower than the nucleation voltage, means that the polarization reversal was carried out without domain merging. After 18.6 ms of the whole poling process, the poling voltage began to increase due to the creation of the inverted polarization under photoresist. The open ratio of the photoresistpatterned on cLN was 0.2 (electrode width of 2.6 ㎛), so some voltage increase was needed for making the PPLN with duty ratio of ideal value of 0.5. Viewing the realtime visualization images and comparing with the calculated poling time, we determined we have to stop the poling process at 10.95 kV. The measured total poling time was
PPT Slide
Lager Image
Oscilloscope data for first 10 ms poling time (a) andvariation of measured voltage for electrical field poling (b).
31 ms which was a little bit smaller than the estimated poling time of 34.8 ms.
For comparing the poling quality between NMP method and other conventional pulse poling methods, we performed the electric field poling with two different pulse poling methods. One is the positive single pulse poling (PSP) by conventional pulse form with the incubation voltage of 9 kV. The other is the negative single pulse poling (NSP)with the incubation pulse of -4.5 kV. After finishing the poling with three different methods, the poling quality with three samples was checked by observing the etched microscopic images and analyzing by far-field diffraction patterns. First of all, we etched the three samples in a HF:HNO 3 (1:2) solution and observed the domain structures on +z and ?z surfaces. Fig. 4 (a) with NMP method showed the uniform periodic domain structures on both +z and -z side. However, Fig. 4 (b) and (c) obtained by NSP and PSP, respectively, showed the domain merging and non-periodic poled domains.
Although we knew just from observing just microscopic etched images that the sample fabricated by NMP method had better poling quality that was not sufficient to perform quantitative analysis of the device quality. Therefore, we applied far-field diffraction pattern analysis which was introduced by Cha and co-authors [17] to evaluate the poling quality, especially duty ratio which is the ratio of the poled (un-poled) domain width divided by the grating
PPT Slide
Lager Image
Microscopic images after HF:HNO3 solution etchingon +z and ?z surfaces: (a) NMP, (b) NSP, (c) PSP.
PPT Slide
Lager Image
Set-up for far-field diffraction experiment (a) anddiffraction image about negative multiple pulse poling (b).
period. SHG spectrum presents overall nonlinear performance of QPM device, but it is mathematically equivalent to the far-field diffraction pattern and experimentally proved by Refs. 18-19. As shown in Fig. 5 (a), He-Ne laser at the wavelength of 633 nm passed through the poled sample along the z-direction of the crystal and then the light was diffracted by the internal field variation of PPLN shown by Fig. 5 (b). It was known that the intensity ratio between the first and second diffraction orders presented as [ 18 - 19 ]
PPT Slide
Lager Image
where I 1 and I 2 are the intensity of first and second
PPT Slide
Lager Image
Far-field diffraction pattern from 0th to 2nd order for NMP (a), NSP (b), PSP (c).
diffraction order, respectively, and R is the duty ratio. The diffraction intensities about three samples were measured as shown in Fig. 6 . The duty ratio was averaged in the poled area within the beam diameter. The focusing diameter was 75 ㎛ of full width half maximum and QPM period was 12.9 ㎛, so 5 or 6 grating periods were participated in one focusing area of the sample.
We measured the intensities of first and second orders 20 times while changing the poled areas and evaluated the duty ratio using Eq. (1) and obtained the standard deviations for each sample. The results were summarized in Table 1 .The cLN sample with NMP had the highest R among
Duty ratios (R) and standard deviations (SD)among the three samples (NMP, NSP and PSP)
PPT Slide
Lager Image
Duty ratios (R) and standard deviations (SD)among the three samples (NMP, NSP and PSP)
three samples. Moreover, the SD was 2~3 times smaller than that of the NSP and PSP. The R of the sample obtained by NMP was still smaller than ideal duty ratio 0.5 for acquiring the highest conversion efficiency. One reason to be considered was that the poling charge was not enough. However, NMP indicated relatively low SD as distinct from NSP and PSP.
In summary, we fabricated 0.5-mm-thick PPLN with QPM period of 12.9 ㎛. For fabricating high-quality PPLN,a new NMP method was demonstrated combined with the real-time visualization system, and the variation of the measured voltages was monitored during electric field poling.Through comparing poling quality for three different ways(NMP, NSP and PSP), it was determined that the proposed NMP method gave the highest duty ratio of 0.42 and the smallest standard deviation of 0.020 by far-field diffraction pattern analysis. We expect that NMP method can be used for fabricating short-pitch QPM device with the real-time visualization system. The fabricated QPM device can be utilized for various optical applications such as optical parametric oscillator, second harmonic generation, THz generation and so on. Recently, we applied the NMP method using a metal electrode to fabricate short-pitch QPM device of 6.5㎛ for green light generation.
This research was partially supported by the Basic Science Research Program through the National Research Foundation of Korea funded by the Ministry of Education, Science and Technology (R15-2008-006-02001-0), (No. 2010-0009146)and also by the Asian Laser Center Program provided by the Gwangju Institute of Science and Technology.An author (J.H. Ro) was supported by Medical Research Institute Grant (2004-34) by Pusan National University Hospital.
Hum D. S , Fejer M. M 2007 Quasi-phasematching Comptes Rendus Physique 8 180 - 198
Boyd R. W 2008 Nonlinear Optics 3rd ed. Academic Press Inc. San Diego USA
Lim E. J , Fejer M. M , Byer R. L 1989 Second-harmonic generation of green light in periodically poled planar lithium niobate waveguide Electron. Lett. 25 174 - 175
Matsumoto S , Lim E. J , Hertz H. M , Fejer M. M 1991 Quaiphase-matched second harmonic generation of blue light in electrically periodically-poled lithium tantalate waveguides Electron. Lett. 27 2040 - 2042
Myers L. E , Eckardt R. C , Fejer M. M , Byer R. L , Bosenberg W. R , Pierce J. W 1995 Quasi-phase-matched optical parametric oscillators in bulk periodically poled LiNbO3 J. Opt. Soc. Am. B 12 2102 - 2116
Kuroda A , Kurimura S , Uesu Y 1996 Domain inversion in ferroelectric MgO:LiNbO3 by applying electric fields Appl. Phys. Lett. 69 1565 - 1567
Harada A , Nihei Y 1996 Bulk periodically poled MgOLiNbO3 by corona discharge method Appl. Phys. Lett. 69 2629 - 2631
Ishizuki H , Shoji I , Taira T 2003 Periodical poling characteristics of congruent MgO:LiNbO3 crystals at elevated temperature Appl. Phys. Lett. 82 4602 - 4604
Fujimura M , Sohmura T , Suhara T 2003 Fabrication of domain-inverted gratings in MgO:LiNbO3 by applying voltage under ultraviolet irradiation through photomask at room temperature Electron. Lett. 39 719 - 721
Batchko R. G , Shur V. Y , Fejer M. M , Byer R. L 1999 Backswitch poling in lithium niobate for high-fidelity domain patterning and efficient blue light generation Appl. Phys. Lett. 75 1673 - 1675
Missey M. J , Russell S , Dominic V , Batchko R. G , Schepler K. L 2000 Real-time visualization of domain formation in periodically poled lithium niobate Opt. Express 6 186 - 195
Gopalan V , Jia Q. X , Mitchell T. E 1999 In situ video observation of 180°domain kinetics in congruent LiNbO3 crystals Appl. Phys. Lett. 75 2482 - 2484
Jeon O. Y “Broadband optical parametric interactions in periodically poled lithium niobate crystals” Pusan National University Ph.D. Thesis
Miller G. D 1998 “Periodically poled lithium niobate : modeling fabrication and nonlinear-optical performance” Stanford University Ph.D. Thesis
Ro J. H 2001 “Poling dynamics of lithium niobate crystals fornonlinear optical applications” Pusan National University Ph.D. Thesis
Yu N. E , Ro J. H 2009 In-situ visualization method of domain boundary for stoichiometric lithium niobate crystal Jpn. J. Appl. Phys. 48 121407 -
Jin M.-J , Jeon O.-Y , Kim B.-J , Cha M 2005 Fabrication of periodically poled lithium niobate crystal and poling-quality evaluation by diffraction measurement J. Korean Phys. Soc. 47 S336 - S339
Pandiyan K , Kang Y.-S , Lim H.-H , Kim B.-J , Prakash O , Cha M 2008 Poling quality evaluation of periodically poled lithium niobate using diffraction method J. Opt. Soc. Korea 12 205 - 209
Pandiyan K , Kang Y.-S , Lim H.-H , Kim B.-J , Cha M 2009 Nondestructive quality evaluation of periodically poled lithium niobate crystals by diffraction Opt. Express 17 17862 - 17867