Abstract:
Methods and apparatus provide for: a first source of plasma, wherein the plasma includes a first species of ions; a second source of plasma, wherein the plasma includes a second species of ions; selection of the plasma from the first and second sources; and acceleration the first species of ions or the second species of ions toward a semiconductor wafer.
Abstract:
There is provided an ion beam generating apparatus capable of reducing power consumption and obtain highly-accurate uniformity in a substrate process without providing a mechanism to rotate a substrate. Each of ion beam generating apparatuses 1a and 1b includes a discharging tank for generating plasma, an extraction electrode including an inclined portion arranged so as to be inclined with respect to an irradiated surface for extracting an ion generated in the discharging tank, a rotating driving unit 30 provided out of the discharging tank for rotating the extraction electrode, and a rotation supporting member 31 for coupling the rotating driving unit 30 and the extraction electrode 7, wherein an insulator block 34 arranged around the rotation supporting member 31 is included in the discharging tank.
Abstract:
A masking apparatus includes a mask positioned upstream of a target positioned for treatment with ions. The mask is sized relative to the target to cause a first half of the target to be treated with a selective treatment of ions through the mask and a second half of the target to be treated with a blanket treatment of ions unimpeded by the mask during a first time interval. The masking apparatus also includes a positioning mechanism to change a relative position of the mask and the target so that the second half of the target is treated with the selective treatment of ions and the first half of the target is treated with the blanket implant during a second time interval. An ion implanter having the masking apparatus is also provided.
Abstract:
The present invention generally relates to a detection unit of a charged particle imaging system. More particularly, portion of the detection unit can move into or out of the detection system as imaging condition required. With the assistance of a Wein filter (also known as an E×B charged particle analyzer) and a movable detector design, the present invention provides a stereo imaging system that suitable for both low current, high resolution mode and high current, high throughput mode. Merely by way of example, the invention has been applied to a scanning electron beam inspection system. But it would be recognized that the invention could apply to other system using charged particle beam as an observation tool.
Abstract:
A masking apparatus includes a mask positioned upstream of a target positioned for treatment with ions. The mask is sized relative to the target to cause a first half of the target to be treated with a selective treatment of ions through the mask and a second half of the target to be treated with a blanket treatment of ions unimpeded by the mask during a first time interval. The masking apparatus also includes a positioning mechanism to change a relative position of the mask and the target so that the second half of the target is treated with the selective treatment of ions and the first half of the target is treated with the blanket implant during a second time interval. An ion implanter having the masking apparatus is also provided.
Abstract:
A substrate processing apparatus includes: a cylindrical shaped chamber configured to accommodate a substrate; a movable electrode capable of moving along a central axis of the cylindrical shaped chamber within the cylindrical shaped chamber; a facing electrode facing the movable electrode within the cylindrical shaped chamber; and an expansible/contractible partition wall connecting the movable electrode with an end wall on one side of the cylindrical shaped chamber. In the substrate processing apparatus, a high frequency power is applied to a first space between the movable electrode and the facing electrode, a processing gas is introduced thereto, and the movable electrode is not in contact with a sidewall of the cylindrical shaped chamber. At least one low dielectric member is provided in a second space between the movable electrode and the end wall on one side of the cylindrical shaped chamber.
Abstract:
Charged particle beam equipment having a rotary mechanism in which shift of the observing/machining position incident to the rotary operation of the equipment having the rotary mechanism can be corrected conveniently with high precision in a plane perpendicular to the optical axis of the optical system of charged particle beam or in a slightly inclining plane. An X-Y shift incident to rotation in a plane is determined from the angular information of a rotary mechanism such as a sample holder, diaphragms or biprisms in the charged particle beam equipment, and then driving or controlling is performed to cancel the X-Y shift.
Abstract:
Techniques for reducing contamination during ion implantation is disclosed. In one particular exemplary embodiment, the techniques may be realized by an apparatus for reducing contamination during ion implantation. The apparatus may comprise a platen to hold a workpiece for ion implantation by an ion beam. The apparatus may also comprise a mask, located in front of the platen, to block the ion beam and at least a portion of contamination ions from reaching a first portion of the workpiece during ion implantation of a second portion of the workpiece. The apparatus may further comprise a control mechanism, coupled to the platen, to reposition the workpiece to expose the first portion of the workpiece for ion implantation.
Abstract:
A charged particle beam apparatus includes: a charged particle beam generator which generates a charged particle beam; a projection optical system which generates a lens field to focus the charged particle beam on an external substrate; and deflectors arranged so as to surround an optical axis of the charged particle beam; the deflectors generating a deflection field which is superposed on the lens field to deflect the charged particle beam and to control a position to irradiate the substrate, and being configured so that intensity of the deflection field in a direction of the optical axis is changed in accordance with an angle with which the charged particle beam should fall onto the substrate.
Abstract:
In a particle-optical projection system a pattern is imaged onto a target by means of energetic electrically charged particles. The pattern is represented in a patterned beam of said charged particles emerging from the object plane through at least one cross-over; it is imaged into an image with a given size and distortion. To compensate for the Z-deviation of the image position from the actual positioning of the target (Z denotes an axial coordinate substantially parallel to the optical axis), without changing the size of the image, the system includes a position detector for measuring the Z-position of several locations of the target, and a controller for calculating modifications of selected lens parameters of the final particle-optical lens and controlling said lens parameters according to said modifications.