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Online proceedings - EDA Publishing Association

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In our work, we proposed an innovated dry process for<br />

PZT-electrode fine pattern fabrication [12]. This process use<br />

conventional ICP-RIE system and Ar/SF 6 mixed gas as the<br />

etchant. AFM images of the PZT film before and after the<br />

dry-etching revealed that the grain-boundary and the shape<br />

of the PZT crystallites were more identifiable when using<br />

lower Ar concentration in Ar/SF 6 mixed etchant. It suggested<br />

that the etching is reactive-physical combined process. As<br />

shown in Fig. 3, the highest PZT etching-rate (58 nm/min)<br />

and the best etching-selectivity (PZT:Pt=1.14) was achieved<br />

at 66.7% of Ar in Ar/SF 6 mixture. We also confirmed that the<br />

remanent polarization and the dielectric constant of the PZT<br />

film were 16.5 μC/cm 2 and 1019 before the etching, 15.5<br />

μC/cm 2 and 1013 after the etching. It demonstrated that the<br />

proposed dry-etching process did not degrade the properties<br />

of the PZT film. As shown in insert of Fig. 3, a<br />

PZT-electrode fine pattern with the feature size of 2 μm was<br />

successfully obtained by this process.<br />

2.3 Low temperature bonding of PZT film<br />

For most of the MEMS and IC devices, process<br />

temperature of more than 400 °C is fatal. However, to obtain<br />

well-crystallized and (100)-oriented PZT film by sol-gel<br />

method, high annealing temperature in the range of 600–750<br />

°C is usually required. Even the transforming temperature of<br />

PZT perovskite-phase (~530 °C) is beyond that of most<br />

MEMS and ICs can withstand. Although adding modifiers<br />

into PZT solution [13], or using seeding layers to enhance<br />

PZT nucleation [14] has been reported effective to reduce the<br />

PZT annealing temperature, their benefits to piezoelectric<br />

MEMS fabrication are limited. Z.Wang et al. proposed the<br />

bonding of bulk PZT with silicon wafer, and then thin down<br />

the PZT to less than 10 μm by using chemical mechanical<br />

polishing [15]. This method is complicated, time-consuming,<br />

and high-cost. Therefore, it is hard to be used for MEMS<br />

mass production.<br />

Ti: 50 nm<br />

Cr: 50 nm<br />

PZT film: 1 μm<br />

Pt/Ti: 200/50 nm<br />

SiO 2 : 2 μm<br />

Si: 500 μm<br />

Si: 400 μm<br />

4-inch<br />

11-13 <br />

May 2011, Aix-en-Provence, France<br />

<br />

Au film 100/300 nm<br />

Au film: 300 nm<br />

film low temperature integration on silicon substrate. We use<br />

Au film as the intermediate layer. Fig. 4 shows schematic<br />

view of the sample and its SAM image after bonded at 150<br />

°C. Die-shear test revealed that the bonding strength is ~75<br />

MPa at the bonding pressure of 325 MPa [16]. This<br />

technique effectively avoids the damage of PZT high<br />

temperature annealing to other MEMS components and ICs.<br />

It also enables the fabrication of piezoelectric material,<br />

piezoelectric MEMS components, and ICs separately by<br />

different wafers, and then bonded them together for<br />

integrated MEMS/ICs mass production.<br />

2.4 Energy dissipation in piezoelectric MEMS device<br />

Piezoelectric MEMS device offers great self-actuation<br />

and self-sensing capabilities, but it always suffers from low<br />

device performance in sensitivity. To investigate the energy<br />

dissipation mechanism, various cantilevers with different<br />

layers are designed and fabricated, which includes SiO 2<br />

elastic layer, Pt/Ti bottom electrode layer, PZT film, Ti/Pt/Ti<br />

upper electrode layer, and SiO 2 top electric passivation layer.<br />

The measured quality-factors (Q-factor) of those cantilevers<br />

were analyzed by theoretical calculation. Fig. 5 summarized<br />

the difference between measured Q-factors and theoretical<br />

calculated Q-factors. It clearly revealed that the energy<br />

dissipation by the PZT film and the multi-layered structure is<br />

extremely large. It is comparable to air dumping under<br />

atmospheric pressure and becomes dominating under<br />

reduced pressures [17].<br />

Q-factor decreases to calculated value (%)<br />

10<br />

0<br />

-10<br />

-20<br />

-30<br />

-40<br />

-50<br />

-60<br />

-70<br />

SiO 2<br />

SiO 2<br />

+Ti/Pt<br />

SiO 2<br />

+Ti/Pt+PZT+Ti/Pt/Ti+SiO 2<br />

SiO 2<br />

+Ti/Pt+PZT<br />

Length: 200 μm<br />

Length: 250 μm<br />

Length: 300 μm<br />

1 2 3 4 5<br />

Number of structure layer<br />

Fig.5 Q-factor of the cantilever decreased with the increasing of structure<br />

layers, especially after PZT film integration.<br />

Fig. 4 PZT bonding on silicon substrate by surface activated bonding (SAB)<br />

using Au film as the intermediate layer: schematic view of the sample (left)<br />

and SAM images of the sample bonded at 150 °C (right).<br />

To promote the PZT application in case >400 °C<br />

temperature cannot been used, surface activated bonding<br />

(SAB) was introduced in our work for the first time for PZT<br />

Based on above results, a piezoelectrically-actuated<br />

micro cantilever [18] and a piezoelectrically-transduced disk<br />

resonator [19] were designed and fabricated in our work as<br />

resonant-based ultra-sensitive mass sensor for human<br />

healthcare and other applications. The device fabrication was<br />

done by 4-inch SOI wafers using above large area PZT film<br />

219

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