In one embodiment, a multi charged particle beam writing apparatus includes a blanking aperture array substrate provided with a plurality of blankers configured to respectively perform blanking deflection on a plurality of charged particle beams included in a multi-beam, and a first shield member which is disposed downstream of the blanking aperture array substrate with respect to a travel direction of the multi-beam, has a cylindrical part in which the multi-beam passes through, and is composed of a high magnetic permeability material.

A charged particle beam system may include a detector. A package for a detector may have a package body that includes two sets of pins, each of the sets of pins including two pins. Each pin of the sets of pins may be configured to be connected to one of two terminals of a sensing element. Pins of different sets may be configured to be connected to a different one of the two terminals of the diode. The sets of pins may be arranged with a symmetry such that magnetic fields generated when current passes through the sets of pins is reduced due to the symmetry.

A plasma processing apparatus includes a plasma processing chamber whose wall has a multi-layer structure including a layer made of a material having a permeability higher than a permeability of aluminum and a loading/unloading port disposed on the wall of the plasma processing chamber to load/unload a substrate into/from the plasma processing chamber. The plasma processing apparatus includes a substrate support disposed in the plasma processing chamber.

Methods, systems, apparatuses, and computer programs are presented for controlling etch rate and plasma uniformity using magnetic fields. A semiconductor substrate processing apparatus includes a vacuum chamber including a processing zone for processing a substrate using capacitively coupled plasma (CCP). The apparatus further includes a magnetic field sensor configured to detect a signal representing a residual magnetic field associated with the vacuum chamber. At least one magnetic field source is configured to generate one or more supplemental magnetic fields through the processing zone of the vacuum chamber. A magnetic field controller is coupled to the magnetic field sensor and the at least one magnetic field source. The magnetic field controller is configured to adjust at least one characteristic of the one or more supplemental magnetic fields, causing the one or more supplemental magnetic fields to reduce the residual magnetic field to a pre-determined value.

Disclosed herein are electron microscopes with improved imaging. An example electron microscope at least includes an illumination system, for directing a beam of electrons to irradiate a specimen, an elongate beam conduit, through which the beam of electrons is directed; a multipole lens assembly configured as an aberration corrector, and a detector for detecting radiation emanating from the specimen in response to said irradiation, wherein at least a portion of said elongate beam conduit extends at least through said aberration corrector and has a composite structure comprising intermixed electrically insulating material and electrically conductive material, wherein the elongate beam conduit has an electrical conductivity σ and a thickness t, with σt<0.1 Ω.sup.−1.

A board includes a first magnetic conductive plate and a second magnetic conductive plate. The first magnetic conductive plate has a first magnetic conductive direction. The second magnetic conductive plate overlaps with the first magnetic conductive plate. The second magnetic conductive plate has a second magnetic conductive direction. The first magnetic conductive direction and the second magnetic conductive direction cross.

A lens element of a charged particle system comprises an electrode having a central opening. The lens element is configured for functionally cooperating with an aperture array that is located directly adjacent said electrode, wherein the aperture array is configured for blocking part of a charged particle beam passing through the central opening of said electrode. The electrode is configured to operate at a first electric potential and the aperture array is configured to operate at a second electric potential different from the first electric potential. The electrode and the aperture array together form an aberration correcting lens.

A plasma chamber includes a chamber body having a processing region therewithin, a liner disposed on the chamber body, the liner surrounding the processing region, a substrate support disposed within the liner, a magnet assembly comprising a plurality of magnets disposed around the liner, and a magnetic-material shield disposed around the liner, the magnetic-material shield encapsulating the processing region near the substrate support.

An e-beam apparatus is disclosed, the tool comprising an electron optics system configured to project an e-beam onto an object, an object table to hold the object, and a positioning device configured to move the object table relative to the electron optics system. The positioning device comprises a short stroke stage configured to move the object table relative to the electron optics system and a long stroke stage configured to move the short stroke stage relative to the electron optics system. The e-beam apparatus further comprises a magnetic shield to shield the electron optics system from a magnetic disturbance generated by the positioning device. The magnetic shield may be arranged between the positioning device and the electron optics system.

An ion implantation system has a mass analyzing magnet having interior and exterior region and defining a first entrance, second entrance, and an exit. A first ion source defines a first ion beam directed toward the first entrance along a first beam path. A second ion source defines a second ion beam directed toward the second entrance along a second beam path. A magnet current source supplies a magnet current to the mass analyzing magnet. Magnet control circuitry controls a polarity of the magnet current based on a formation of the first or second ion beam. The mass analyzing magnet mass analyzes the respective first or second ion beam to define defining a mass analyzed ion beam along a mass analyzed beam path. At least one shield in the interior or exterior region prevents line-of-sight between the first and second ion sources. Beamline components modify the mass analyzed ion beam.