Femtosecond laser-induced forward transfer (LIFT): a technique for versatile micro-printing applications
Femtosecond laser-induced forward transfer (LIFT): a technique for versatile micro-printing applications
The Laser-Induced Forward Transfer (LIFT) method exists as a relatively simple and versatile additive surface micropatterning technology. Material is transferred from a supported thin film to a receiver substrate by irradiating the rear side of the film with a single laser pulse. Typically transfer is effected either through melting through of the source film or by ablation of the film at a constrained interface with a resultant pressure build-up propelling a piece of the film to the receiver. Both of these processes have inherent advantages and disadvantages; by melting the source film during transfer, sub-laser spot size features can be produced, but the choice of available materials is reduced and control of deposit morphology is limited. Ablation-driven transfer is less material selective but resultant deposits are typically broken during transfer and scattered over relatively large areas.
Banks, D.P.
134b4e3e-9c17-4155-a3e6-bd16d5f94be4
Grivas, Christos
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Eason, R.W.
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Zergioti, I.
97fd5ac7-1c63-4bc3-a2b6-3ecea9dd86f1
June 2007
Banks, D.P.
134b4e3e-9c17-4155-a3e6-bd16d5f94be4
Grivas, Christos
7f564818-0ac0-4127-82a7-22e87ac35f1a
Eason, R.W.
e38684c3-d18c-41b9-a4aa-def67283b020
Zergioti, I.
97fd5ac7-1c63-4bc3-a2b6-3ecea9dd86f1
Banks, D.P., Grivas, Christos, Eason, R.W. and Zergioti, I.
(2007)
Femtosecond laser-induced forward transfer (LIFT): a technique for versatile micro-printing applications.
Conference on Lasers and Electro-Optics (CLEO)-Europe/International Quantum Electronics Conference (IQEC) 2007, , Munich, Germany.
17 - 22 Jun 2007.
1 pp
.
Record type:
Conference or Workshop Item
(Paper)
Abstract
The Laser-Induced Forward Transfer (LIFT) method exists as a relatively simple and versatile additive surface micropatterning technology. Material is transferred from a supported thin film to a receiver substrate by irradiating the rear side of the film with a single laser pulse. Typically transfer is effected either through melting through of the source film or by ablation of the film at a constrained interface with a resultant pressure build-up propelling a piece of the film to the receiver. Both of these processes have inherent advantages and disadvantages; by melting the source film during transfer, sub-laser spot size features can be produced, but the choice of available materials is reduced and control of deposit morphology is limited. Ablation-driven transfer is less material selective but resultant deposits are typically broken during transfer and scattered over relatively large areas.
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Published date: June 2007
Venue - Dates:
Conference on Lasers and Electro-Optics (CLEO)-Europe/International Quantum Electronics Conference (IQEC) 2007, , Munich, Germany, 2007-06-17 - 2007-06-22
Identifiers
Local EPrints ID: 47792
URI: http://eprints.soton.ac.uk/id/eprint/47792
PURE UUID: 5913f8d9-fe16-4bbb-b125-ffb3807b3d13
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Date deposited: 10 Aug 2007
Last modified: 16 Mar 2024 02:38
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Contributors
Author:
D.P. Banks
Author:
Christos Grivas
Author:
R.W. Eason
Author:
I. Zergioti
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