Abstract:
A method for regulating sample surface charge has been proposed in this invention. The processes of applying a charged particle beam to a first area and applying a flood energized beam gun with gaseous molecules to a second area are executed in the method when the sample is in both continuous and Leap & Scan movements. The second area is located at a predetermined distance from the first area behind or ahead of the first area being scanned with respect to the movement of the sample. Thus, the surface of the sample may be regulated.
Abstract:
A plasma electron flood system, comprising a housing configured to contain a gas, and comprising an elongated extraction slit, and a cathode and a plurality of anodes residing therein and wherein the elongated extraction slit is in direct communication with an ion implanter, wherein the cathode emits electrons that are drawn to the plurality of anodes through a potential difference therebetween, wherein the electrons are released through the elongated extraction slit as an electron band for use in neutralizing a ribbon ion beam traveling within the ion implanter.
Abstract:
Methods and apparatus for electron beam treatment of a substrate are provided. An electron beam apparatus that includes a vacuum chamber, at least one thermocouple assembly in communication with the vacuum chamber, a heating device in communication with the vacuum chamber, and combinations thereof are provided. In one embodiment, the vacuum chamber comprises an electron source wherein the electron source comprises a cathode connected to a high voltage source, an anode connected to a low voltage source, and a substrate support. In another embodiment, the vacuum chamber comprises a grid located between the anode and the substrate support. In one embodiment the heating device comprises a first parallel light array and a second light array positioned such that the first parallel light array and the second light array intersect. In one embodiment the thermocouple assembly comprises a temperature sensor made of aluminum nitride.
Abstract:
According to the present invention, a charged particle beam device has an unlimitedly rotatable sample stage and an electric field control electrode for correcting electric field distortion at a sample peripheral part. A voltage is applied to a sample on the unlimitedly rotatable sample stage through a retarding electrode that is in contact with a holder receiver at a rotation center of a rotary stage. An equipotential plane on the electric field control electrode is varied by applying a voltage to the electric field control electrode, and following this the equipotential plane at a sample edge is corrected, which enables the sample to be observed as far as its edge.
Abstract:
Electrification affected on a surface of a sample which is caused by irradiation of a primary charged particle beam is prevented when plural frames are integrated to obtain an image of a predetermined area of the sample in a charged particle beam apparatus. The predetermined area of the sample is scanned with a primary electron beam from an electron gun, and plural frames are generated and integrated while detecting generated secondary electrons with a detector to obtain the image of the predetermined area. If it is determined by a detection signal of the detector that an electrification amount at the predetermined area becomes a specified value when generating plural frames, an electricity removal voltage is applied to a boosting electrode to remove or reduce the electrification, prior to generation of the next frame. Accordingly, the signal-to-noise ratio of the image obtained by integrating plural frames can be improved.
Abstract:
A system for ion beam neutralization includes a beamguide configured to transport an ion beam through a dipole field, a first array of magnets and a second array of magnets configured to generate a multi-cusp magnetic field, the first array of magnets being on a first side of the ion beam path and the second array of magnets being on a second side of the ion beam path. The system may further include a charged particle source having one or more apertures configured to inject charged particles into the ion beam. The system may furthermore align the one or more apertures with at least one of the first array of magnets and the second array of magnets to align the injected charged particles from the charged particle source with one or more magnetic regions for an effective charged particle diffusion into the ion beam.
Abstract:
Techniques for confining electrons in an ion implanter are disclosed. In one particular exemplary embodiment, the techniques may be realized as an apparatus for confining electrons in an ion implanter. The apparatus may comprise a first array of magnets and a second array of magnets positioned along at least a portion of a beam path, the first array being on a first side of the beam path and the second array being on a second side of the beam path, the first side opposing the second side. At least one magnet in the first array may have a pole facing an opposite pole of a corresponding magnet in the second array.
Abstract:
When the surface of a semiconductor wafer, a photomask or the like sample is charged by irradiation with a charged particle beam, the charging is liable to hamper image observation, inspection and handling. Therefore, the sample and the surface or vicinity of the sample being charged by an electron beam or the like is held in an atmosphere or a reduced pressure atmosphere or in a predetermined gaseous atmosphere within a preliminary evacuation chamber, a sample chamber or the like, containing a soft X-ray generator which irradiates the sample or the vicinity thereof with soft X-rays which are controlled to generate positive ions and negative ions and remove charges on the surface of the sample.
Abstract:
A dual beam system includes an ion beam system and a scanning electron microscope with a magnetic objective lens. The ion beam system is adapted to operate optimally in the presence of the magnetic field from the SEM objective lens, so that the objective lens is not turned off during operation of the ion beam. An optional secondary particle detector and an optional charge neutralization flood gun are adapted to operate in the presence of the magnetic field. The magnetic objective lens is designed to have a constant heat signature, regardless of the strength of magnetic field being produced, so that the system does not need time to stabilize when the magnetic field is changed.
Abstract:
An ultra low-k dielectric material layer is formed on a semiconductor substrate. In one embodiment, a grid of wires is placed at a distance above a top surface of the ultra low-k dielectric material layer and is electrically biased such that the total electron emission coefficient becomes 1.0 at the energy of electrons employed in electron beam curing of the ultra low-k dielectric material layer. In another embodiment, a polymeric conductive layer is formed directly on the ultra low-k dielectric material layer and is electrically biased so that the total electron emission coefficient becomes 1.0 at the energy of electrons employed in electron beam curing of the ultra low-k dielectric material layer. By maintaining the total electron emission coefficient at 1.0, charging of the substrate is avoided, thus protecting any device on the substrate from any adverse changes in electrical characteristics.