IP Library Granted Patent US 8,367,971
Granted Patent B2
US 8,367,971 · App. 12/621,123 · Granted Feb 5, 2013

Method of working material with high-energy radiation

Inventors: Arne Koops (Neu-Lankau, DE); Sven Reiter (Hamburg, DE)
Assignee: tesa SE
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Quick Facts
Patent No.
US 8,367,971
App. No.
12/621,123
Granted
Feb 5, 2013
Kind
B2
Abstract

According to the present invention, a method of working material with high-energy radiation is provided, wherein a polymer matrix ( 1 ) is irradiated with high-energy radiation, in particular with a laser beam ( 9 ), wherein the radiation is focused onto a focal point ( 11 ) and the focal point ( 11 ) is set such that the focal point ( 11 ) lies behind the surface ( 3 ) of the polymer matrix ( 1 ) facing the radiation, and material removal is brought about at the polymer matrix ( 1 ), and consequently a reaction space ( 13 ) is created within the polymer matrix ( 1 ).

Claims (47)

1. A method of working material with high-energy radiation, comprising the steps of

irradiating a polymer matrix ( 1 ) with high-energy radiation,

focusing the radiation onto a focal point ( 11 ),

setting the focal pint ( 11 ) such that the focal point ( 11 ) lies behind the surface ( 3 ) of the polymer matrix ( 1 ) facing the radiation,

removing material removal at the polymer matrix ( 1 ),

creating a reaction space ( 13 ) within the polymer matrix ( 1 )

providing reactants ( 15 , 17 ) in the reaction space ( 13 ) after the removal of material,

obtaining reaction in the reaction space ( 13 ) of the reactants ( 15 , 17 ) under irradiation with high-energy radiation to form a product ( 19 ).

2. The method according to claim 1 , wherein the product ( 19 ) is deposited on the workpiece ( 7 ) which is in contact with the polymer matrix ( 1 ) and is transparent to the radiation wavelength when the reaction space ( 13 ) is irradiated with high-energy radiation.

3. The method according to claim 1 , wherein the reaction space ( 13 ) has a spatial extent with a diameter in the range of 20-200 μm, and a depth in the range of 10-100 μm.

4. The method according to claim 3 , wherein the depth is in the range of approximately 40 μm.

5. The method according to claim 3 , wherein the diameter is in the range of approximately 70 μm.

6. The method according to claim 1 , wherein the reaction space ( 13 ) is created by a first pulse of a pulsed laser beam ( 9 ) and the reaction space ( 13 ) is irradiated with a second pulse of the pulsed laser beam ( 9 ).

7. The method according to claim 1 , wherein the reaction space ( 13 ) is a plurality of reaction spaces arranged locally next to one another and are created within the polymer matrix ( 1 ) by means of irradiating the polymer matrix ( 1 ) with high-energy radiation.

8. The method according to claim 7 , wherein the radiation is a pulsed laser beam ( 9 ) and, during the irradiation, the pulsed beam ( 9 ) is moving laterally in relation to the polymer matrix ( 1 ), or the polymer matrix ( 1 ) is made to move laterally in relation to the pulsed beam ( 9 ).

9. The method according to claim 7 , wherein the reaction spaces ( 13 ) are created such that neighbouring reaction spaces ( 13 ) overlap by at least 25% of their spatial extent.

10. The method according to claim 1 , wherein the radiation is generated with a pulsed laser ( 9 ) and a pulse rate of 10 kHz-300 kHz.

11. The method according to claim 1 , wherein the focal point ( 11 ) lies in the reaction space ( 13 ), in the polymer matrix ( 1 ) or behind the polymer matrix ( 1 ).

12. The method according to claim 1 , wherein the irradiating the polymer matrix ( 1 ) is accomplished with a laser beam ( 9 ).

13. A method of working material with high-energy radiation, comprising the steps of

irradiating a polymer matrix ( 1 ) with high-energy radiation,

focusing the radiation onto a focal point ( 11 ),

setting the focal point ( 11 ) such that the focal point ( 11 ) lies behind the surface ( 3 ) of the polymer matrix ( 1 ) facing the radiation,

removing material removal at the polymer matrix ( 1 ),

creating a reaction space ( 13 ) within the polymer matrix ( 1 ),

wherein the reaction space ( 13 ) is spatially bounded by the polymer matrix ( 1 ) and by a workpiece ( 7 ) which is in contact with the polymer matrix ( 1 ) and is transparent to the radiation wavelength, preferably a glass substrate ( 7 ), and the radiation passes through the workpiece ( 7 ) before it impinges on the polymer matrix ( 1 ).

14. A method of working material with high-energy radiation, comprising the steps of

irradiating a polymer matrix ( 1 ) with high-energy radiation,

focusing the radiation onto a focal point ( 11 ),

setting the focal point ( 11 ) such that the focal point ( 11 ) lies behind the surface ( 3 ) of the polymer matrix ( 1 ) facing the radiation,

removing material removal at the polymer matrix ( 1 ),

creating a reaction space ( 13 ) within the polymer matrix ( 1 )

wherein the focal point ( 11 ) is set such that the radiation power density at the surface ( 3 ) of the polymer matrix ( 1 ) is less than 3 J/cm 2 .

15. A method of working material with high-energy radiation, comprising the steps of

irradiating a polymer matrix ( 1 ) with high-energy radiation,

focusing the radiation onto a focal point ( 11 ),

setting the focal point ( 11 ) such that the focal point ( 11 ) lies behind the surface ( 3 ) of the polymer matrix ( 1 ) facing the radiation,

removing material removal at the polymer matrix ( 1 ),

creating a reaction space ( 13 ) within the polymer matrix ( 1 ),

wherein the focal point ( 11 ) is set such that the maximum radiation power density within the reaction space ( 13 ) is at least 5 J/cm 2 .

16. A method of working material with high-enemy radiation, comprising the steps of

irradiating a polymer matrix ( 1 ) with high-energy radiation,

focusing the radiation onto a focal point ( 11 ),

setting the focal point ( 11 ) such that the focal point ( 11 ) lies behind the surface ( 3 ) of the polymer matrix ( 1 ) facing the radiation,

removing material removal at the polymer matrix ( 1 ),

creating a reaction space ( 13 ) within the polymer matrix ( 1 )

wherein the maximum radiation power density within the reaction space ( 13 ) is at least 10 J/cm 2 .

Assignments (2)
CHANGE OF ADDRESS Recorded Dec 17, 2015
From: TESA SE
To: TESA SE
Reel/Frame 037317/0675 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Dec 11, 2009
From: KOOPS, ARNE; REITER, SVEN
To: TESA SE
Reel/Frame 023640/0923 →
Priority Claims (1)
DE 10 2008 058 535 · Nov 21, 2008 · national
Continuity (1)
Related Publication 20100126975A1 · May 27, 2010