Asml Netherlands B.v.

Cymer, Inc.

Daniel Brown

Yezheng Tao

John Tom Stewart, Iv

Jordan Jur

Thomas Patrick Duffey

Robert A Bergstedt

Andrew David LaForge

Alexander Anthony Schafgans

Rajasekhar Rao

Hong Ye

John Viatella

Jason Michael Arcand

James J Ferrell

Slava Rokitski

Rong (Lauren) Liu

Ray Cybulski

Alex Ershov

Richard L Sandstrom

Robert Jay Rafac

Kai-Chung Hou

Michael Anthony Purvis

An initial pulse of radiation is generated; a section of the initial pulse of radiation is extracted to form a modified pulse of radiation, the modified pulse of radiation including a first portion and a second portion, the first portion being temporally connected to the second portion, and the first portion having a maximum energy that is less than a maximum energy of the second portion; the first portion of the modified pulse of radiation is interacted with a target material to form a modified target; and the second portion of the modified pulse of radiation is interacted with the modified target to generate plasma that emits extreme ultraviolet (EUV) light.

Extreme ultraviolet light source

Extreme ultraviolet light source utilizing a target of finite extent

A target material is provided at a target location, the target material including a material that emits extreme ultraviolet light when converted to plasma, and the target material extending in a first extent along a first direction and in a second extent along a second direction; an amplified light beam is directed along a direction of propagation toward the target location; and the amplified light beam is focused in a focal plane, where the target location is outside of the focal plane and an interaction between the amplified light beam and the target material converts at least part of the target material to plasma that emits EUV light.

An aspect of the disclosed subject matter includes a method of reducing the laser absorption of a beam reverser prism consisting of at least one of the following: increasing a first distance between a first incident point and a chamfered corner, wherein the first incident point is on a first reflective surface of the prism and the chamfered corner is formed between the first reflective surface and a second reflective surface of the prism, wherein the chamfered corner has a chamfered surface; increasing a second distance between a second incident point and the chamfered corner, wherein the second incident point is on the second reflective surface of the prism; and increasing a reflectivity of the chamfered surface of the chamfered corner of the prism. A method of determining a prime cut for an optical component is also disclosed. A laser including at least one prime cut optical component is also disclosed.

Very high power laser chamber optical improvements

Growing community of inventors

San Diego, CA, United States of America

Daniel Brown