A method of forming an optical device comprises applying a laser beam to a target area of the surface so as to selectively heat material of the surface thereby to provide transfer of material due to a surface tension gradient, wherein the surface is such that, when liquid, parts of the surface at hi
A method of forming an optical device comprises applying a laser beam to a target area of the surface so as to selectively heat material of the surface thereby to provide transfer of material due to a surface tension gradient, wherein the surface is such that, when liquid, parts of the surface at higher temperatures have a higher surface tension than adjacent parts of the surface at lower temperatures.
대표청구항▼
1. A method of forming a diffractive optical device, the method comprising: applying a laser beam to a plurality of target areas located at different positions on a surface of a substrate so as to selectively melt material of the surface; andcontrolling at least one of atmospheric conditions at the
1. A method of forming a diffractive optical device, the method comprising: applying a laser beam to a plurality of target areas located at different positions on a surface of a substrate so as to selectively melt material of the surface; andcontrolling at least one of atmospheric conditions at the surface and composition of the surface such that the application of the laser beam causes a melt pool at each of the plurality of target areas to exhibit a surface tension gradient, with higher temperature areas of the melt pool having a higher surface tension than lower temperature areas of the melt pool, that results in a transfer of molten material to build up profiles on the surface, the profiles forming a diffractive structure of the diffractive optical device. 2. The method according to claim 1, comprising controlling the atmosphere at the surface such that the higher temperature areas of the melt pool have a higher surface tension than the lower temperature areas of the melt pool. 3. The method according to claim 2, wherein the controlling of the atmosphere comprises providing an atmosphere at the surface rich in a gas, relative to the concentration of the gas in air, that causes at least one of oxidation, phosphorus evaporation, carbide formation and chromium migration. 4. The method according to claim 2, wherein the controlling of the atmosphere comprises providing a CO2-rich atmosphere, relative to the concentration of CO2 in air, at the surface during the application of the laser beam to the surface. 5. The method according to claim 1, comprising providing material at the surface having a composition such that the higher temperature areas of the melt pool have a higher surface tension than the lower temperature areas of the melt pool. 6. The method according to claim 5, comprising treating the surface of the substrate with a surface active agent that reacts with material of the substrate to provide the composition. 7. The method according to claim 6, wherein the surface active agent causes at least one of oxidation, phosphorus evaporation, carbide formation and chromium migration. 8. The method according to claim 5, wherein the composition comprises one or more elements from groups 13, 14, 15 and 16 of the periodic table. 9. The method according to claim 8, wherein the composition comprises one or more elements from periods 2 and 3 of the periodic table. 10. The method according to claim 8, wherein the material comprises a high period metal and the composition comprises one or more elements from periods 4 and 5. 11. The method according to claim 5, wherein the composition comprises one or more elements selected from calcium, sulphur, manganese, silicon, titanium, zirconium, aluminium, magnesium, nitrogen, oxygen and phosphorus. 12. The method according to claim 5, wherein the material has a selected oxygen or sulphur content. 13. The method according to claim 1, comprising controlling at least one parameter of the laser beam to obtain the transfer of material. 14. The method according to claim 13, wherein the at least one parameter comprises at least one of intensity, wavelength, pulse length, and pulse repetition time. 15. The method according to claim 1, wherein, for at least one of the plurality of target areas, the laser beam has a greater intensity at a first part of the at least one target area than at a second part of the at least one target area. 16. The method according to claim 15, wherein the laser beam has an intensity above a threshold intensity thereby to reduce the transfer of material to the first part of the at least one target area in comparison to the transfer of material to the second part of the at least one target area. 17. The method according to claim 16, wherein the laser beam has an intensity above the threshold intensity at the first part of the at least one target area and an intensity below the threshold intensity at the second part of the at least one target area. 18. The method according to claim 16, wherein the threshold intensity is an intensity at which radiation of the laser beam ablates the surface. 19. The method according to claim 16, wherein the threshold intensity is a minimum intensity for which radiation of the laser beam acts to oppose the transfer of material due to the surface tension gradient. 20. The method according to claim 16, comprising applying both the laser beam and a further laser beam to the at least one target area, wherein the laser beam has an intensity above the threshold intensity and the further laser beam has a maximum intensity below the threshold intensity. 21. The method according to claim 20, wherein the method comprises: applying one of the laser beam and the further laser beam to the at least one target area;allowing the surface at the at least one target area to at least partially solidify; andapplying the other of the laser beam and the further laser beam to the at least one target area. 22. The method according to claim 21, wherein application of the further laser beam to the at least one target area fills in with material at least a portion of the profile of surface material formed by application of the laser beam, or vice versa. 23. The method according to claim 22, wherein application of the laser beam forms a two peaked profile of surface material and application of the further laser beam subsequently at least partially fills a well between the two peaks, or application of the further laser beam forms a single peaked profile of surface material and application of the laser beam subsequently at least partially broadens the single peak. 24. The method according to claim 20, wherein the laser beam and the further laser beam have parameters that are controlled such as to produce a profile of material at the at least one target area that has a flat top. 25. The method according to claim 1, comprising applying a further laser beam to a plurality of further target areas, each of the further target areas being at a respective, different position on the surface, thereby to create a further melt pool at each further target area and build up the profiles of the diffractive optical device. 26. The method according to claim 25, wherein the method comprises applying the laser beam to the plurality of target areas in a sequence, wherein at least some of the target areas that are spatially adjacent to each other on the surface are temporally non-adjacent in the sequence. 27. The method according to claim 1, comprising applying the laser beam to at least one target area of the plurality of target areas a plurality of times thereby to build up material at the target area. 28. The method according to claim 27, further comprising: controlling the atmosphere at the surface such that the higher temperature areas of the melt pool have a higher surface tension than the lower temperature areas of the melt pool; andvarying a composition of gas above the surface, so that the composition of the gas is different for at least some of the times that the laser beam is applied to the at least one target area than for at least some other of the times that the laser beam is applied to the at least one target area. 29. The method according to claim 1, wherein the method comprises blocking an outer part of the laser beam from reaching the surface. 30. The method according to claim 1, wherein the method comprises passing the laser beam through a beam shaper before applying it to the surface. 31. The method according to claim 30, wherein the beam shaper is configured to redistribute power from higher intensity parts of the laser beam to lower intensity parts of the laser beam. 32. The method according to claim 1, wherein the laser beam has an intensity such as to provide transfer of material due to the surface tension gradient without removal of material from the substrate. 33. The method according to claim 1, wherein the diffractive optical device comprises at least one of a metrological device, a phase scale, a hologram and a diffraction grating. 34. The method according to claim 10, wherein the high period metal is a metal selected from the group of silver, tungsten, platinum and gold. 35. The method according to claim 6, wherein the surface active agent comprises one or more elements selected from calcium, sulphur, manganese, silicon, titanium, zirconium, aluminium, magnesium, nitrogen, oxygen and phosphorus. 36. The method according to claim 25, comprising applying the further laser beam to the plurality of further target areas in a sequence, wherein at least some of the further target areas that are spatially adjacent to each other on the surface are temporally non-adjacent in the sequence. 37. The method according to claim 25, comprising applying the further laser beam to at least one further target area of the plurality of further target areas a plurality of times thereby to build up material at the at least one further target area. 38. The method according to claim 37, comprising: controlling the atmosphere at the surface such that higher temperature areas of the further melt pool have a higher surface tension than lower temperature areas of the further melt pool; andvarying a composition of gas above the surface, so that the composition of the gas is different for at least some of the times that the further laser beam is applied to the at least one further target area than for at least some other of the times that the further laser beam is applied to the at least one further target area.
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