Patent classifications
H01J2237/057
Beam Deflection Device, Aberration Corrector, Monochromator, and Charged Particle Beam Device
The present disclosure pertains to a beam deflection device capable of properly deflecting a beam. The present disclosure provides a beam deflection device for deflecting a beam inside a charged particle beam device, said beam deflection device being provided with: one or more electrostatic deflectors (207, 208) each having a pair of electrodes disposed so as to face each other across a beam path in a first direction orthogonal to the beam path; and one or more magnetic deflectors (209) each having a pair of magnetic poles disposed so as to face each other across the beam path in a second direction orthogonal to the beam path and to the first direction. When viewed from an incident direction of the beam, the one or more electrostatic deflectors and the one or more magnetic deflectors are stacked along the beam path such that the pair of electrodes at least partially overlap with the pair of magnetic poles and with a gap between the pair of magnetic poles.
WIEN FILTER AND CHARGED PARTICLE BEAM IMAGING APPARATUS
A Wien filter and a charged particle beam imaging apparatus are provided. The Wien filter Wien filter, including a Wien filter body which includes: an electrostatic deflector, including at least one pair of electrodes, respective two electrodes in each pair of which are opposite to each other, each electrode including an electrode body constructed in an arc-shaped form, and respective electrode bodies of respective two electrodes in each pair of the at least one pair of electrodes being arranged concentrically with and opposite to each other in a diameter direction, and the at least one pair of electrodes being configured to generate respective electric fields by cooperation of the respective two electrodes in each pair of the at least one pair of electrodes, in the condition of respective bias voltages applied individually thereon; and a magnetic deflector, including at least one pair of magnetic poles, respective two magnetic poles in each pair of which are opposite to each other, each magnetic pole including a magnetic pole body constructed in an arc-shaped form, and respective magnetic pole bodies of respective two magnetic poles in each pair of the at least one pair of magnetic poles being arranged concentrically with and opposite to each other in the diameter direction, and the magnetic pole bodies of the at least one pair of magnetic poles in the magnetic deflector and the electrode bodies of the at least one pair of electrodes in the electrostatic deflector being arranged concentrically and spaced apart from each other in a circumferential direction, and the at least one pair of magnetic poles being configured to generate respective magnetic fields by cooperation of respective two magnetic poles in each pair of the at least one pair of magnetic poles; a resultant electric field formed collectively by all of the respective electric fields is perpendicular to a resultant magnetic field formed collectively by all of the respective magnetic fields; and each electrode is also provided with a respective first protrusion extending radially inwards from a radial inner side of the respective electrode body thereof, and each magnetic pole is also provided with a second protrusion extending radially inwards from a radial inner side of the respective magnetic pole body thereof.
Systems and methods for continuously supplying negative ions using multi-pulsed plasma sources
The present disclosure relates to a system and method for continuously supplying negative ions using multi-pulsed plasma sources. The system includes a plurality of plasma generators each to generate plasma by applying pulsed power to the electronegative gas from a gas source; a negative ion supply unit connected to the plasma generators to receive the plasmas transferred therefrom and to continuously supply ions; and a controller connected to the plurality of plasma generators and configured to control characteristics of the pulsed powers delivered to the respective plasma generators and to adjust phase shift associated with the pulsed power envelopes. By adjusting the phase shift, the controller enables a plasma in one of the plasma generators to be in an after-glow state when a plasma in another plasma generator is in an active-glow state.
APPARATUS FOR AND METHOD OF CONTROLLING AN ENERGY SPREAD OF A CHARGED-PARTICLE BEAM
Disclosed among other aspects is a charged particle inspection system including an absorbing component and a programmable charged-particle mirror plate arranged to modify the energy distribution of electrons in a beam and shape the beam to reduce the energy spread of the electrons and aberrations of the beam, with the absorbing component including a set of absorbing structures configured as absorbing structures provided on a transparent conductive layer and a method using such an absorbing component and with the programmable charged-particle mirror plate including a set of pixels configured to generate a customized electric field to shape the beam and using such a programmable charged-particle mirror plate.
METHOD OF DETERMINING AN ENERGY WIDTH OF A CHARGED PARTICLE BEAM
The disclosure relates to a method of determining an energy width of a charged particle beam, comprising the steps of providing a charged particle beam, directing said beam towards a specimen, and forming an energy-dispersed beam from a flux of charged particles transmitted through the specimen. As defined herein, the method comprises the steps of providing a slit element in a slit plane, and using said slit element for blocking a part of said energy-dispersed beam, as well as the step of modifying said energy-dispersed beam at the location of said slit plane in such a way that said energy dispersed beam is partially blocked at said slit element. The unblocked part of said energy-dispersed beam is imaged and an intensity gradient of said imaged energy-dispersed beam is determined, with which the energy width of the charged particle beam can be determined.
ELECTRODYNAMIC MASS ANALYSIS WITH RF BIASED ION SOURCE
Provided herein are approaches for performing electrodynamic mass analysis with a radio frequency (RF) biased ion source to reduce ion beam energy spread. In some embodiments, a system may include an ion source including a power supply, the ion source operable to generate a plasma within a chamber housing, and an extraction power assembly including a first power supply and a second power supply electrically coupled with the chamber housing of the ion source, wherein the first power supply and the second power supply are operable to bias the chamber housing of the ion source with a time modulated voltage to extract an ion beam from the ion source. The system may further include an electrodynamic mass analysis (EDMA) assembly operable to receive the ion beam and perform mass analysis on the ion beam.
Apparatus and method for measuring energy spectrum of backscattered electrons
The present invention relates to an apparatus and method for analyzing the energy of backscattered electrons generated from a specimen. The apparatus includes: an electron beam source (101) for generating a primary electron beam; an electron optical system (102, 105, 112) configured to direct the primary electron beam to a specimen while focusing and deflecting the primary electron beam; and an energy analyzing system configured to detect an energy spectrum of backscattered electrons emitted from the specimen. The energy analyzing system includes: a Wien filter (108) configured to disperse the backscattered electrons; a detector (107) configured to measure the energy spectrum of the backscattered electrons dispersed by the Wien filter (108); and an operation controller (150) configured to change an intensity of a quadrupole field of the Wien filter (108), while moving a detecting position of the detector (107) for the backscattered electrons in synchronization with the change in the intensity of the quadrupole field.
Mass separator using retractable magnetic yoke on a beam bending path
Provided is a mass separator (100) for performing mass separation for an ion beam (IB). The mass separator (100) includes a transfer structure (30) that is a component of a yoke (13) and move at least one of an upper yoke (13a) positioned over the beam path (L), a lower yoke (13b) positioned under the beam path (L), and a side yoke (13c, 13d) positioned at a side of the beam path (L) between a normal position (P) in the traveling of the ion beam (IB) and a retracted position (Q) that does not overlap with at least a part of the normal position (P); the yoke (13) is surrounding the beam path (L) and is made of a magnetic body.
Scanning electron microscope
Provided is a scanning electron microscope provided with an energy selection and detection function for a SE.sub.1 generated on a sample while suppressing the detection amount of a SE.sub.3 excited due to a BSE in the scanning electron microscope that does not apply a deceleration method. Provided are: an electron optical system that includes an electron source 21 generating an irradiation electron beam and an objective lens 12 focusing the irradiation electron beam on a sample; a detector 13 that is arranged outside an optical axis of the electron optical system and detects a signal electron generated when the sample is irradiated with the irradiation electron beam; a deflection electrode that forms a deflection field 26 to guide the signal electron to the detector; a disk-shaped electrode 23 that is arranged to be closer to the electron source than the deflection field and has an opening through which the irradiation electron beam passes; and a control electrode arranged along the optical axis to be closer to the sample than the deflection field. The sample and the objective lens are set to a reference potential. A potential lower than the reference potential is applied to the disk-shaped electrode, and a potential higher than the reference potential is applied to the control electrode.
Magnetic filter tube
The present invention discloses a magnetic filter tube, and relates to the technical field of magnetic filters. The magnetic filter tube includes a first rectangular tube and a second rectangular tube, where one end of the first rectangular tube is fixedly connected to one end of the second rectangular tube; the other end of the first rectangular tube forms an inlet of the magnetic filter tube; the inlet of the magnetic filter tube is connected with a cathode target flange; the other end of the second rectangular tube forms an outlet of the magnetic filter tube; the outlet of the magnetic filter tube is connected with a vacuum chamber; an inner wall of the first rectangular tube and an inner wall of the second rectangular tube are each provided with a protrusion and a groove; the protrusion is filled with cold water.