Optical Grating Crystal

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We have succeeded in fabricating the optical gratings on the surface and inside of the diamond plates even though only partial material in the irradiated region phase-transforms from single crystal phase to amorphous phase. The gratings can be used as terahertz polarizers likewise. What if Factorio mind-melded with Satisfactory, producing a hybrid offspring with Astroneer, then danced with Stellaris? Welcome to Dyson Sphere Program: th. Custom Diffraction Gratings In optics, a diffraction grating is an optical component with a periodic structure that splits and diffracts light into several beams traveling in different directions. The directions of the beams depend on the spacing of the grating and the wavelength of the light so that the grating acts as the dispersive element. Optical grating. Graphene and Carbon materials. Polymers and Thin Organic Films. Life Sciences and Biotechnology.

Optical axis gratings (OAGs) are gratings of optical axis of a birefringent material. In OAGs, the birefringence of the material is constant, while the direction of optical axis is periodically modulated in a fixed direction. In this way they are different from the regular phase gratings, in which the refractive index is modulated and the direction of the optical axis is constant.

The optical axis in OAGs can be modulated in either transverse or the longitudinal direction, which causes it to act as a diffractive or a reflective component. Numerous modulation profiles allow variation in the optical properties of the OAGs.

Examples of OAGs

TUNABLE DIFFRACTION GRATING WITH TRANSPARENT INDIUM-TIN OXIDE ELECTRODES

ON A LITHIUM NIOBATE X-CUT CRYSTAL

V.D. Paranin1, S.V. Karpeev12, K.N. Tukmakov1, B.O. Volodkin1 1 Image Processing Systems Institute of RAS, - Branch of the FSRC 'Crystallography and Photonics ' RAS, Samara, Russia,

2 Samara National Research University, Samara, Russia

Abstract

A tunable diffraction grating based on an electrooptic X-cut lithium niobate crystal has been manufactured and experimentally analyzed. The period of electrodes is 290 pm, the electrode width is 117.5 pm, and the thickness of an electrode is 150 - 160 nm. The electrodes are made of a transparent conducting indium-tin oxide that serves as an antireflection coating with the aim of increasing the optical transmission. In order to prevent crystal polarization switching and electrical breakdown an optimized electrode topology with end ellipticity 1: 1 and increased interelectrode gap is used.

The optical diagram of the tunable grating with alternating electrode potentials for various gap voltages is analyzed. The intensity of the zero order of diffraction is shown to decrease by 40 % at a voltage of 800 V. At the same time, the origination of new diffraction orders at angles ± X / (2d) is noted. The measurement of the forward-bias and reverse-bias regions of the modulation characteristic reveals the absence of hysteresis, which confirms the correctness of the electrode topology design.

Keywords: tunable diffraction grating, linear electro-optical effect, lithium niobate.

Citation: Paranin VD, Karpeev SV, Tukmakov KN, Volodkin BO. Tunable diffraction grating with transparent indium-tin oxide electrodes on a lithium niobate X-cut crystal. Computer Optics 2016; 40(5): 685-688. DOI: 10.18287/2412-6179-2016-40-5-685-688.

Acknowledgements: The work was funded by the Russian Foundation for Basic Research (RFBR grants 16-29-11698 and 14-02-97033 r_povolzhiye_a).

Introduction

Tunable diffraction gratings based on the electroopti-cal effect remain the subject of various studies. Part of publications is devoted predominantly to synthesis and application of highly sensitive electrooptical materials for the production of substrates [1 - 7]. In other studies more attention is given to the design of control electrodes. Thus, in papers [7, 8] a three-element electrode is discussed that forms a quasitriangular phase profile of the grating causing deflection of transmitted light. This approach, however, can be applied only to thin electroopti-cal layers comparable to the interelectrode gap of, for instance, liquid crystals. In the case of thick crystals (about 1 mm) the electric field of the electrodes is concentrated near the surface they are located on and the interaction of the lower and upper electrodes is insignificant.

In [9] improvement of transmission of the tunable grating due to the use of transparent 130 nm thick indium-tin oxide In2Ü3-SnO2 (ITO) electrodes is discussed. According to the results presented in the specified paper the resistivity of ITO-electrodes is quite high, approximately 48 Q / sq. This fact caused the necessity of evaporating narrow aluminum stripes on top of the ITO-electrode. This approach complicates the fabrication process, it causes origination of higher diffraction orders and undesirable scatter of optical light. It is necessary to reduce the resistance of indium tin-oxide by maintaining stoichiometry of the film in the process of evaporation or at the postprocessing stage.

It should be noted that the design of electrodes determines the processes of polarization switching of the lithium niobate surface layer (with the electrical field higher than coercive). These effects can be observed mostly in the vicinity of rectangular electrode ends and

to a smaller degree in interelectrode gaps [10]. Origination and growth of needle-shaped domains determines the hysteresis of tunable gratings and reduces the diffraction efficiency due to the depolarization of transmitted light [11].

The aim of the study was to develop improved electrode topology characterized by improved optical transmission due to the use of transparent indium-tin oxide. Other tasks included reduction of the film resistance and optimization of electrode form and dimensions to prevent polarization switching of the crystal surface layer.

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1. ITO tunable grating technology

Polished chips of congruent lithium niobate with the dimensions 15 x 15 x 1 mm were used as substrates. An oxide of indium-tin alloy of electronic grade deposited in vacuum by magnetron sputtering served as the material of electrodes.

The substrates were cleaned by rinsing in an alkaline solution, soaking in a chrome solution H2SO4:K2CrO7 for 5 minutes and rinsing in deionized water. The lift-off process was used to produce a diffraction mask. A layer of FP-051K photoresist 0.4 mkm thick was spin-deposited in two stages: 20 seconds at the rate of 500 rev / min, and then 45 seconds at the rate of 4500 rev / min. The photoresist was air-dried for 2 minutes and then dried on a heater for 12 minutes at the temperature 95 °C. Immediately after the inverse photomask exposure the photoresist was developed in UBP-1F developer solution for 1 minute, rinsed in deionized water and dried by pure dried air flow.

In order to accomplish vacuum deposition of the indium-tin layer the substrates with the photoresist inverse mask were fixed on a heating substrate holder of the ETNA-100-MT vacuum unit. Reactive sputtering in oxy-

gen environment with additional heating is necessary for successful formation of indium-tin oxide. The temperature of heating is limited by photomask degradation in such aggressive conditions. Download autocad 2003 free full version free. It was experimentally established that heating up to the temperature of 200 °C in the presence of argon-oxygen mixture does not cause any significant degradation of the photoresist used and the resulting mask is completely washed off with acetone at a later step.

After evacuation to marginally hard vacuum of the order of 10-4 Pa heating of the substrate holder was switched on with the help of a resistive helix. The temperature was tunable by an automatic PID-regulator. The rate of temperature growth did not exceed 10 °C / min and the nominal temperature of the substrate holder was not higher than 200 °C. This temperature was maintained during the whole process of ITO deposition.

The process of sputtering itself started with spraying of the upper layer of the target material, indium-tin alloy of electronic grade (target diameter 3') onto the closed shutter under the following conditions: atmosphere - argon with the chamber pressure 0.5 mTorr, the rate of supply through the magnetron - 9 cm3 / sec; the magnetron power increased up to 200 W in the course of 30 seconds and then was maintained at this level for 5 minutes in direct current conditions. Let us note that the closed magnetron shutter and the supply of gas from the bottom of the magnetron determined higher argon working pressure in the magnetron as compared to that in the main chamber, which ensured stable operation of the magnetron.

After the target was cleaned the shutter was opened, the flow of argon through the magnetron increased up to 22 cm3 / sec and oxygen was additionally supplied to the substrate at a rate of consumption 9 cm3 / sec (the pressure in the chamber therewith grew up to 1.1 mTorr). The magnetron power decreased down to 110 W and its operation condition changed to the intermittent current mode with a periodic inverted pulse to minimize the effect of anode loss. The film thickness was measured with the help of a quartz thickness gage using a check test piece placed near the samples. The rate of ITO oxide formation on the test piece is somewhat different, consequently, the film density may also differ from that on the sample film. Therefore, to control the process the rate of film growth was used (it amounted to 0.26 nm / sec), the constancy of which meant the process was stable.

To improve the conductivity of the ITO-film deposited a higher temperature (300 - 500 °C) is required [13 -14]. Therefore, additional annealing was used after the completion of the lift-off process. The crystals were air heated with the help of a heater at a rate of 30 °C / min from 20 °C to 250 °C, which was maintained for 2 min. Both the crystals and the heater were cooled down to room temperature by air convection. Annealing resulted in considerable decrease of the film surface resistivity from 50 Q / sq to 26 Q / sq.

The refraction index of the ITO-film was measured by the method of ellipsometry using a J.A. Woollam V-VASE automatic spectral ellipsometer. The wavelength was as-

signed to be equal to 632.8 nm, the width of the light spectrum did not exceed 2.3 nm. To reduce the impact of reflection from the back surface of the substrate it was mat-finished. The refraction indices determined with the help of the ellipsometer software were as follows: n = 1.8841 ± 0.0027, k=0.0176 ± 0.0030 according to the data of^-polarization.

A tunable diffraction grating made of indium-tin oxide on X-cut lithium niobate was formed in the way described. Fig. 1 shows a fragment of topology in the form of interdigital electrodes that ensure alternating distribution of potentials of the 0V0V kind. The coordinate axis z corresponds to the crystal optical axis. The electrode tips are rounded so as to reduce maximum intensity of the electric field Ez acting along the optical axis. The impact of the field results in the origination of microdomains that change the crystal's optical properties and contribute to electrical breakdown of the interelectrode gap [10, 11]. As modeling showed [12], tip ellipticity 1:1 yields twofold reduction of the maximum field Ez .

Fig. 1. Topology of a tunable diffraction grating

The electrode dimensions were measured using a Bi-omed-5P microscope and a WLI-DMR white light interferometer. The period was 290 ^m, the electrode width was 117.5 ^m, the thickness was 150.160 nm. The film thickness and refraction index determined approximately similar transmission of the electrodes and the substrate at the wavelength 632.8 nm, equal to 83 - 84 % with account for the influence of acrylic layer on the output surface. The roughness of the electrodes corresponded to the roughness of a polished substrate Ra< 1.2 nm.

2. Experimental study of ITO tunable grating

Crystal
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The optical diagram of the ITO-grating was analyzed with the help of an optical setup that comprised a heliumneon laser, a spatial filter- beam expander, a Glan-Taylor polarizer, an experimental sample, an image-forming cylindrical lens and a CCD-matrix. The illumination of the tunable diffraction grating was close to uniform. The negative photos of diffraction orders for various voltages are shown in fig. 2.

It follows from the data obtained that a diffraction grating on the basis of indium-tin oxide is an amplitudephase one. The fact is confirmed by the presence of the first diffraction orders in the absence of voltage. As the electrical voltage increases the intensities of the zero and first diffraction orders decrease. At the same time the intensity of new ± 01 orders located between the zero and the first ones at the angles ± X / (2d) increases.

The dependence of the zero order intensity on voltage was measured with the help of a PM100D secondary converter equipped with a temperature-compensated S120C sensor. To improve spatial resolution quartz fiber with the core diameter 62.5 ^m was used. The center of the fiber was made coincident with the zero diffraction order image with the help of a positioning stage by the maximum value of intensity. In fig. 3 the measured normalized modulation characteristic is shown.

Fig. 2. Diffraction orders of a tunable grating at different voltages: a) 0 V, b) 400 V, c) 800 V

Intensity, r.u. —^-

Volta, V

0,9 0,8 0,7 0,6 0,5

0 200 400 600 800

Fig. 3. Dependence of intensity of zero-order diffraction on electrical voltage

The modulation characteristic is of the typical kind I=cos2(kuU) where ku is a constant determined by the electo-optical material, the electrode period and width. The analysis of the forward-bias and the reverse-bias regions of the characteristic revealed absence of hysteresis observed earlier [11]. This is due to the fact that the electrodes are rounded, which reduces maximum of the electric field near the electrode ends, as well as to a greater interelectrode gap (172.5 ^m instead of 140 ^m in [11]). Since crystal polarization switching is a threshold process domains of the kind of optical nonuniformities do not originate. The analysis of the tunable grating by the polarization optical method confirmed absence of microdomains after carrying out experiments in the vicinity of electrode ends and in the interelectrode gap.

Conclusion

A tunable diffraction grating with improved topology of control electrodes has been developed and experimentally analyzed. Intensity of diffraction zero order is shown to decrease by 40 % at interelectrode voltage of 800 V. A two-fold increase of optical transmission is achieved at the operating wavelength 632.8 nm due to the use of transparent conducting indium-tin oxide of half-wave thickness instead of chrome-copper electrodes [10, 11].

Electrode's surface resistivity is shown to decrease from 50 Q / sq to 26 Q / sq in the case of air annealing at 250 °C for 2 min. The intensity of the electric field is reduced due to the increase of the interelectrode gap from 140 ^m go 172.5 ^m and rounding of electrode ends in the 1:1 proportion. Formation of needle-shaped domains in the crystal surface layer and hysteresis of dependence of diffraction order intensity on voltage is prevented.

References

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[6] Volk TR, Ivanov NR, Isakov DV, Ivleva LI, Lykov PA. Electro-optical properties of strontium-barium niobate crystals and their relation to the domain structure of the crystals. Phys Solid State 2005; 47(2): 305-311. DOI: 10.1134/1.1866411.

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Optical Grating Crystal Dyson Sphere Program

[8] Paranin VD, Matyunin SA. Modeling tunable diffractive elements based on the linear electro-optic effect. Proc SPIE 2010; 7523: 75230E. DOI: 10.1117/12.852958.

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[10] Paranin VD. Formation of needle-shaped domains in a surface layer of x-cut lithium niobate. Technical Physics 2014; 59(12): 1869-1873. DOI: 10.1134/S1063784214120226.

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Authors' Information

Vyacheslav Dmitrievich Paranin (b. 1986) graduated from Samara State Aerospace University in 2010, majoring in Design and Technology of Radio-Electronic Equipment. Currently he works as an assistant professor at the Nanoen-gineering department of Samara National Research University. Research interests are methods and devices for controlling of laser radiation. E-mail: [email protected] .

Diffraction grating crystal definition

Optical Grating Crystal

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Sergei Vladimirovich Karpeev, Doctor of Physical and Mathematical Sciences; Professor of Samara National Research University. He is a leading researcher of the IPSI RAS - Branch of the FSRC 'Crystallography and Photonics' RAS. Research interests: diffractive optics, singular optics, mode and polarization transformations, optical manipulations, optical and digital image processing. E-mail: [email protected] .

The information about authors Konstantin Nickolaevich Tukmakov and Boris Olegovich Volodkin you can find on page 672 of this issue.

Code of State Categories Scientific and Technical Information (in Russian - GRNTI)): 29.31.15. Received September 30, 2016. The final version - October 24, 2016.