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Laser generated patterns for fluidic driven self-alignment

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Confocal microscopy: receptor site in AuPdNi

L

ASER

G

ENERATED

P

ATTERNS FOR

FLUIDIC DRIVEN SELF

-

ALIGNMENT

Gert-willem R.B.E. Römer, Daniel Arnaldo del Cerro, Ralph Pohl , Bert Huis in ‘t Veld

University of Twente, Chair of Applied Laser Technology, g.r.b.e.romer@utwente.nl

Background

Fluidic self-alignment of micro components relies on a locally confined liquid droplet (e.g. water) on top of which the component is “dropped”. Next, capillary action provides the driving force for self-alignment.

Approach

Exploitation of Gibb’s inequality to impede the droplet from leaving a receptor site, by creating a “sharp” trench around the site.

Gibbs inequality:

Trench was created by Laser Ablation using an Ultra Short Pulsed laser source.

Experimental setup

• Yb:YAG laser source (Trumpf TruMicro 5050) =1030nm, pulse duration 6.7ps • A THG unit converting the IR radiation

to =343nm (UV)

• Galvano-scanner (IntelliScan14 of ScanLab) & telecentric 100 mm f-lens (Ronar of Linos)

• Gaussian fluence profile, spot diameter =16 µm (2nd moment diameter)

Two substrate materials were studied

1. Thin Au-Pd-Ni multilayer on Copper 2. Polyimide (Kapton) foil

Results on Au-Pd-Ni layer on Copper

Trenches in Au-Pd-Ni : SEM & Confocal microscopy. Laser settings: 0.15µJ/pulse, 94%pulse overlap,

200kHz, 50 (left) & 100 (right) overscans (OS).

Acknowledgements

Mark Jorritsma & the European Union, grant FP7-2010-NMP-ICT-FoF, No. 260079.

http://www.fab2asm.eu Initial surface roughness, Ra=1.5µm,

li-mits high values of edge angle , which reduces robust self-alignment.

Results on Polyimide foil

Confocal microscopy: trench profile, with characteristic

“humps” at edges. 1µJ per pulse, 94% overlap, 400kHz, 4 overscans.

Edges as sharp as =95º were obtained. Self-alignment tests with SU8 chips on distilled water on 200×200 µm2 receptor

sites showed 100% success rate.

Optical microscopy: SU8 chip prior to (left) and after (right) self-alignment.

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