Position shifts caused by charging phenomena can be corrected with high accuracy. A charged particle beam writing apparatus includes an exposure-amount distribution calculator calculating an exposure amount distribution of a charged particle beam using a pattern density distribution and a dose distribution, a fogging charged particle amount distribution calculator calculating a plurality of fogging charged particle amount distributions by convoluting each of a plurality of distribution functions for fogging charged particles with the exposure amount distribution, a charge-amount distribution calculator calculating a charge amount distribution due to direct charge using the pattern density distribution, the dose distribution, and the exposure amount distribution, and calculating a plurality of charge amount distributions due to fogging charge using the plurality of fogging charged particle amount distributions, a position shift amount calculator calculating a position shift amount of a writing position based on the charge amount distribution due to direct charge and the plurality of charge amount distributions due to fogging charge, a corrector correcting an exposure position using the position shift amount, and a writer exposing the corrected exposure position to a charged particle beam.

A method includes: producing a light beam made up of pulses having a wavelength in the deep ultraviolet range, each pulse having a first temporal coherence defined by a first temporal coherence length and each pulse being defined by a pulse duration; for one or more pulses, modulating the optical phase over the pulse duration of the pulse to produce a modified pulse having a second temporal coherence defined by a second temporal coherence length that is less than the first temporal coherence length of the pulse; forming a light beam of pulses at least from the modified pulses; and directing the formed light beam of pulses toward a substrate within a lithography exposure apparatus.

A method includes: producing a light beam made up of pulses having a wavelength in the deep ultraviolet range, each pulse having a first temporal coherence defined by a first temporal coherence length and each pulse being defined by a pulse duration; for one or more pulses, modulating the optical phase over the pulse duration of the pulse to produce a modified pulse having a second temporal coherence defined by a second temporal coherence length that is less than the first temporal coherence length of the pulse; forming a light beam of pulses at least from the modified pulses; and directing the formed light beam of pulses toward a substrate within a lithography exposure apparatus.

Vacuum ultraviolet rays are emitted to a surface to be processed of a substrate to be processed by a light source. During an emission period in which the vacuum ultraviolet rays are emitted from the light source to the substrate, part of the vacuum ultraviolet rays is received by an illuminometer, and illuminance of the received vacuum ultraviolet rays is measured. A light receiving surface of the illuminometer is located at a constant height that is based on the surface to be processed of the substrate during the emission period of the vacuum ultraviolet rays. An exposure amount of the substrate is calculated based on the illuminance measured by the illuminometer. Emission of the vacuum ultraviolet rays from the light source to the substrate is stopped based on the calculated exposure amount of the substrate.

A method for generating a radiation light in a lithography exposure system is provided. The method includes connecting a first nozzle assembly coupled to a support to an outlet of a storage member that receives a target fuel inside. The method further includes guiding the target fuel flowing through the first nozzle assembly and supplying a droplet of the target fuel into an excitation zone via the first nozzle assembly. The method also includes moving the support to connect a second nozzle assembly coupled to the support with the outlet. In addition, the method includes guiding the target fuel flowing through the second nozzle assembly and supplying a droplet of the target fuel into the excitation zone via the second nozzle assembly. The method further includes irradiating the droplet of the target fuel in the excitation zone with a laser pulse.

A method of patterning lithographic substrates, the method comprising using a free electron laser to generate EUV radiation and delivering the EUV radiation to a lithographic apparatus which projects the EUV radiation onto lithographic substrates, wherein the method further comprises reducing fluctuations in the power of EUV radiation delivered to the lithographic substrates by using a feedback-based control loop to monitor the free electron laser and adjust operation of the free electron laser accordingly.

A method of patterning lithographic substrates, the method including using a free electron laser to generate EUV radiation and delivering the EUV radiation to a lithographic apparatus which projects the EUV radiation onto lithographic substrates, wherein the method further includes reducing fluctuations in the power of EUV radiation delivered to the lithographic substrates by using a feedback-based control loop to monitor the free electron laser and adjust operation of the free electron laser accordingly.

An optical device is described. At least a portion of the optical device includes ferroelectric non-linear optical material(s) and is fabricated utilizing ultraviolet lithography. In some aspects the at least the portion of the optical device is fabricated using deep ultraviolet lithography. In some aspects, the short range root mean square surface roughness of a sidewall of the at least the portion of the optical device is less than ten nanometers. In some aspects, the at least the portion of the optical device has a loss of not more than 2 dB/cm.

An electron beam lithography apparatus-includes: a density set storage unit that stores, for each of pieces of figure information, a set of pieces of first density information corresponding to areas occupied by a figure in first small regions divided from a figure region specified by the piece of figure information; a density set acquisition unit that acquires first density sets respectively corresponding to the pieces of figure information from the density set storage unit; a correction amount acquisition unit that acquires correction amounts corresponding to the first density sets for each of the pieces of figure information, and are for the second small regions; an emission amount acquisition unit that acquires, for the second small regions, emission amounts of an electron beam with intensities corresponding to the correction amounts for the second small regions; and a drawing unit that emits an electron beam according to the emission amounts.

An object of the present invention is to provide a resin membrane filter having excellent separation accuracy and excellent toughness, and a manufacturing method of the resin membrane filter.

The resin membrane filter of the present invention includes a first main surface, a second main surface, and a plurality of through-holes, in which, in the through-hole, in a case where an average area of an opening portion at a position A which is located at a distance of 10% of a thickness of the resin membrane filter from the first main surface is denoted as Sva and an average area of an opening portion at a position B which is located at a distance of 90% of the thickness of the resin membrane filter from the first main surface is denoted as Svb, 0.8?Sva/Svb?1.25, a number ratio Ra of through-holes in which an area of the opening portion at the position A is more than 1.25 times Sva is 3.0% or less, and a number ratio Rb of through-holes in which an area of the opening portion at the position B is more than 1.25 times Svb is 3.0% or less.