Abstract:
There is provided a lithographic apparatus comprising an illumination system IL for providing a beam B of extreme ultra-violet radiation, a masking device MB for controlling the illumination of a patterning device MA by the beam of radiation, a support MT for supporting the patterning device, the patterning device configured to impart a pattern to the beam of radiation, a substrate table WT for holding a substrate W, and a projection system PL for projecting the patterned beam of radiation onto a target portion of the substrate, wherein the masking device MD comprises a masking blade MB configured to reflect extreme ultra-violet radiation incident on the masking blade such that at least a portion of the reflected radiation is not captured by the projection system.
Abstract:
A collector module (SO) is disclosed comprising: a collector (14) for collecting radiation generated by a radiation generating plasma (10), and for directing at least a portion of the generated radiation to a focal point (16); a structure (30) upstream of the focal point and extending at least partially around an expected position of a beam comprising the at least a portion of the collected radiation (B); a diffractive element being arranged to diffract infrared radiation that is reflected from the plasma formation location. When the plasma formation location is at an intended location, m = +1 diffracted infrared radiation (32) is directed towards a first region of the structure. At m = -1 diffracted infrared radiation is directed towards a second region of the structure. Also disclosed is an infra-red detector with increased dynamic range obtained by providing a screen for forming an image of a hotspot and a camera directed on to the screen. The dynamic range of the detector is improved either by heating the screen such that a low intensity hotspot is raised above a camera threshold, or by dividing the image into multiple images of differing intensities.
Abstract:
A lithographic apparatus comprising a source of EUV radiation, an illumination system configured to condition a radiation beam, and a projection system configured to project the radiation beam onto a substrate, wherein the apparatus further comprises a filter configured to prevent or reduce the transmission of unwanted radiation and an apparatus configured to detect damage of the filter, wherein the damage detection apparatus comprises an antenna configured to receive radio waves and an analysis apparatus configured to determine the presence of filter damage based upon the received radio waves.
Abstract:
A radiation source includes a nozzle configured to direct a stream of fuel droplets along a droplet path towards a plasma formation location, and is configured to receive a gaussian radiation beam having gaussian intensity distribution, having a predetermined wavelength and propagating along a predetermined trajectory, and further configured to focus the radiation beam on a fuel droplet at the plasma formation location. The radiation source includes a phase plate structure including one or more phase plates. The phase plate structure has a first zone and a second zone. The zones are arranged such that radiation having the predetermined wavelength passing through the first zone and radiation having the predetermined wavelength passing through the second zone propagate along respective optical paths having different optical path lengths. A difference between the optical path lengths is an odd number of times half the predetermined wavelength.
Abstract:
A beam delivery apparatus is used with a laser produced plasma source. The beam delivery apparatus comprises variable zoom optics (550) operable to condition a beam of radiation so as to output a conditioned beam having a configurable beam diameter (b) and a plurality of mirrors (530a, 530b) operable to direct the conditioned beam of radiation to a plasma generation site. The beam delivery apparatus enables control of the axial position of the beam where the beam has a particular diameter, with respect to the beam's focus position (570). Also, a method is used to control the axial position of the location at a plasma generation site where a beam has a particular diameter, with respect to the beam's focus position.