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Energy Materials Testing Laboratory EVALUATION FROM

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Preparing the Target<br />

With K(OC 2 H 5 ) 5 (95%), Nb(OC 2 H 5 ) 5<br />

(99.8%) and Ta(OC 2 H 5 ) 5 (99.8%) as the<br />

starting materials, we prepared<br />

KTa 0.65 NB 0.35 O 3 powder that included<br />

the excessive K(OC 2 H 5 ) 5 , ≈1%, by the<br />

sol-gel method.<br />

We then pressed the powder into a<br />

30-mm diameter disk. When the temperature<br />

reached 1100°C, we sintered<br />

it for 45 h in the Kali atmosphere.<br />

Details are given in the literature. 8<br />

Preparing the Films<br />

We used Lamda EMG201MSC quasimolecular<br />

laser equipment in the<br />

experiment. The output wavelength<br />

was 308 nm. The repeat frequency<br />

rate was 20 Hz. The single pulsed<br />

laser energy density was 1.6 J/cm 2 ,<br />

2.0 J/cm 2 and 2.4 J/cm 2 , respectively.<br />

The system's automatic scanning of<br />

the beam focuses the laser beam into<br />

a 3 mm 2 flare, after it passes through<br />

a lens. The scanning speed is 20 rpm,<br />

which generates the best proportional<br />

films.<br />

KTN, or K(Ta 1-x Nb x )O 3 , has many<br />

good properties, including electrooptic<br />

characteristics, nonlinear optic<br />

characteristics and pyroelectricity. It<br />

also has a high K. When x = 0.35, it<br />

can be applied in a wide variety of<br />

fields with the highest electro-optic<br />

coefficient.<br />

During deposition and the addition<br />

of oxygen atmosphere, the pressure<br />

was kept between 10 and 15 pa. The<br />

substrate was the simple quartz crystal<br />

(100). The target was the potassium-rich<br />

ceramics. The distance from<br />

the substrate to the target was about<br />

5 cm.<br />

From the experiment, we found<br />

that when the temperature of the<br />

substrate exceeds 350°C, the simple<br />

quartz crystal breaks. The reason was<br />

that the thermal-dilatation coefficient<br />

of quartz differs greatly from<br />

that of the substrate.<br />

The substrate’s temperature must<br />

be controlled at ≈300°C, and the<br />

depositing time at 30 min. At the end<br />

of the experiments, the temperature<br />

of the films must be cooled slowly to<br />

room temperature under a certain<br />

pressure of oxygen.<br />

After analyzing the prepared films<br />

by XRD, we found that the films were<br />

I/I °<br />

100<br />

80<br />

60<br />

40<br />

20<br />

0<br />

(3.993)<br />

20 40 60 80 100<br />

The X-ray diffraction diagram of the polycrystal KTa 1-x Nb x O 3 powder.<br />

in an amorphous state. According to<br />

the theory of the growth of films,<br />

amorphous films belong to the structure<br />

of the metastable state, which<br />

has high internal energy. Under the<br />

action of neighbor energy, e.g., illumination,<br />

heating, etc., the amorphous<br />

state can conquer the<br />

potential energy hill and transform<br />

into a homeostatic state, namely<br />

crystal.<br />

The literature has reported that the<br />

best substrate temperature (TS) for<br />

preparing the LiTaO 3 electrical waveguide<br />

by PLD is 650°C. 10 Amorphous<br />

films prepared at

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