Patent Number: 
Section: claims

1. A method comprising:forming a first remaining plasma that at least partially coincides with a target region, the first remaining plasma being formed from a previous extreme ultraviolet (EUV)-light producing interaction between target material and an amplified light beam;providing a target comprising target material in a first spatial distribution to the target region, the target material comprising material that emits EUV light when converted to plasma;allowing the first remaining plasma and the initial target to interact, the interaction rearranging the target material from the first spatial distribution to a shaped target distribution to form a shaped target in the target region, the shaped target comprising the target material arranged in the shaped target distribution, the shaped target distribution comprising sides that define a concave region;directing the amplified light beam toward the concave region of the shaped target in the target region, an interaction between the amplified light beam and the target material of the shaped target converting at least some of the target material in the shaped target to a plasma that emits EUV light, and the sides of the concave region confining at least some of the plasma that emits EUV light; andallowing a second remaining plasma to form in the target region. 2. The method of claim 1, wherein the sides of the shaped target distribution extend from a vertex, and the concave region is a recess defined by the sides and the vertex. 3. The method of claim 1, wherein the amplified light beam is a pulsed amplified light beam. 4. The method of claim 1, wherein providing a target comprising target material in a first spatial distribution to the target region comprises providing a disk-shaped target to the target region. 5. The method of claim 4, wherein providing a disk-shape target comprises:releasing a target material droplet comprising target material from a target material supply apparatus toward the target region;directing a pulse of radiation toward the target material droplet to interact the pulse of radiation with the target material droplet while the target material droplet is between the target material supply apparatus and the target region, the first pulse of radiation having an energy sufficient to initiate a modification of a spatial distribution of the target material of the target material droplet; andallowing the target material droplet to expand in two dimensions after the interaction between the pulse of radiation and the target material droplet to form the disk-shaped target. 6. The method of claim 5, wherein the target material droplet expands in two dimensions by expanding in a plane that is perpendicular to a direction of propagation of the amplified light beam. 7. The method of claim 6, wherein the target material droplet narrows in a direction that is parallel to the direction of propagation to form the disk-shaped spatial distribution of target material. 8. The method of claim 6, wherein the first pulse of radiation comprises a pulse of laser light having a wavelength of 1.06 microns (μm) and the amplified light beam is a pulsed laser beam having a wavelength of 10.6 μm. 9. The method of claim 1, further comprising:providing a second target comprising target material in the first spatial distribution to the target region;allowing the second remaining plasma and the second target to interact, the interaction arranging the target material in the first spatial distribution to the shaped target distribution to form a second shaped target in the target region;directing the amplified light beam toward the target region to convert at least some of the second shaped target to a plasma that emits EUV light; andallowing a third remaining plasma to form in the target region, the third remaining plasma being formed from converting at least some of the second shaped target to the plasma that emits EUV light. 10. The method of claim 8, wherein the amplified light beam is directed toward the target region and the second shaped target no more than 25 microseconds (μs) after the amplified light beam is directed toward the first shaped target. 11. The method of claim 10, wherein a first burst of EUV light is produced after directing the amplified light beam toward the target region and the shaped target, and a second burst of EUV light is produced after directing the amplified light beam toward the target region and the second shaped target, the first and second EUV bursts occurring no more than 25 μs apart. 12. The method of claim 6, wherein the first pulse of radiation and the amplified light beam have the same wavelength. 13. The method of claim 1, wherein the confined plasma heats the target material in the sides of the shaped target to produce EUV light. 14. A method comprising:forming a remaining plasma that at least partially coincides with a target region, the remaining plasma being a plasma formed from a previous extreme ultraviolet (EUV)-light producing interaction between target material and an amplified light beam, the interaction between the target material and the amplified light beam occurring in the target region;providing a target comprising target material in a first spatial distribution to an initial target region, the target material comprising material that emits EUV light when converted to plasma, the initial target region being spatially distinct from the target region;initiating a modification of the first spatial distribution of target material in two dimensions by interacting the target with a first pulse of radiation in the initial target region;allowing the first spatial distribution of target material to change in the two dimensions after interacting the target with the first pulse of radiation to form a modified target;shaping the modified target in three dimensions by allowing the modified target to enter into the target region and interact with the remaining plasma in the target region to form a shaped target; anddirecting an amplified light beam toward the target region and the shaped target to form a plasma that emits EUV light. 15. The method of claim 14, wherein the two dimensions comprise two dimensions that extend in a plane that is perpendicular to the direction of propagation of the amplified light beam. 16. The method of claim 14, wherein initiating a modification of the first spatial distribution in two dimensions comprises directing a pulsed laser beam toward the target such that a pulse of the laser beam interacts with the target. 17. The method of claim 16, wherein the two dimensions comprise two dimensions that extend in a plane that is perpendicular to the direction of propagation of the pulsed laser beam. 18. The method of claim 17, wherein the modified target has a larger cross-sectional area in the plane that is perpendicular to the direction of propagation of the pulsed laser beam than the target. 19. The method of claim 15, wherein the shaped target distribution comprises a concave region that is open to the amplified light beam. 20. The method of claim 14, wherein the target region is in an interior of a vacuum chamber of an EUV light source. 21. The method of claim 14, wherein directing the amplified light beam toward the target region comprises directing the amplified light beam in a direction of propagation, and focusing the amplified light beam to a focus, the focus being in a plane that is perpendicular to the direction of propagation. 22. The method of claim 14, wherein the shaped target distribution comprises sides that extend from a vertex, the sides forming an open region, and the open region being oriented toward the amplified light beam. 23. The method of claim 21, wherein the focus is in a plane that is different from a parallel plane that includes the shaped target in the target region.