Abstract:
An apparatus may include an electrodynamic mass analysis (EDMA) assembly disposed downstream from the convergent ion beam assembly. The EDMA assembly may include a first stage, comprising a first upper electrode, disposed above a beam axis, and a first lower electrode, disposed below the beam axis, opposite the first upper electrode. The EDMA assembly may also include a second stage, disposed downstream of the first stage and comprising a second upper electrode, disposed above the beam axis, and a second lower electrode, disposed below the beam axis. The EDMA assembly may further include a deflection assembly, disposed between the first stage and the second stage, the deflection assembly comprising a blocker, disposed along the beam axis, an upper deflection electrode, disposed on a first side of the blocker, and a lower deflection electrode, disposed on a second side of the blocker.
Abstract:
A retarding potential type energy analyzer including a front grid electrode, reference grid electrode and rear grid electrode sequentially arranged, with a predetermined amount of potential difference given between the reference grid electrode and the front grid electrode to form an upward potential gradient as well as a potential difference given between the reference grid electrode and the rear grid electrode to form a downward potential gradient, the grid electrodes are arranged so that the distance between the reference grid electrode and the rear grid electrode is shorter than the distance between the reference grid electrode and the front grid electrode, or the potential difference between the reference grid electrode and the rear grid electrode is made to be greater than the potential difference between the reference grid electrode and the front grid electrode.
Abstract:
When an electrode (29) such as a grid applied with a negative voltage is installed in front of an objective lens (23), low energy electrons among secondary electrons (25) generated from a sample (24) by an electron beam or the like is reflected by the electrode to come into a detector (22) installed in the sample (24) side, while electrons of higher energy are not detected, since they are not reflected by the electrode. Accordingly, since only the electrons of lower energy of the secondary electrons can be detected by discriminating the secondary electrons by the energy, it is possible to obtain a detection signal, e.g., rich in the information on the surface state of the sample.
Abstract:
A deceleration apparatus capable of decelerating a short spot beam or a tall ribbon beam is disclosed. In either case, effects tending to degrade the shape of the beam profile are controlled. Caps to shield the ion beam from external potentials are provided. Electrodes whose position and potentials are adjustable are provided, on opposite sides of the beam, to ensure that the shape of the decelerating and deflecting electric fields does not significantly deviate from the optimum shape, even in the presence of the significant space-charge of high current low-energy beams of heavy ions.
Abstract:
The invention provides for a method of improving bioactivity of a surface of an implantable object. The invention also provides for a method of improving bioactivity of a surface of biological laboratory ware. The invention further provides a method of attaching cells to an object. The invention even further provides for a method of preparing an object for medical implantation. The invention also provides for an article with attached cell, and for an article for medical implantation. Improvements result from the application of gas-cluster ion beam technology and from the application of neutral beam technology, wherein neutral beams are derived from accelerated gas-cluster ion beams.
Abstract:
Applicants have found that the asymmetrical energy distribution of ions from an ion source allow chromatic aberration to be reduced by filtering ions in the low energy beam tail without significantly reducing processing time. A preferred embodiment includes within an ion beam column a filter that removes the low energy ions from the beam.
Abstract:
An ion energy analyzer is described for use in diagnosing the ion energy distribution (IED) of ions incident on a radio frequency (RF) biased substrate immersed in plasma. The ion energy analyzer comprises an entrance grid exposed to the plasma, an ion selection grid disposed proximate to the entrance grid, an electron rejection grid disposed proximate to the ion selection grid, and an ion current collector disposed proximate to the electron rejection grid. The ion selection grid is coupled to an ion selection voltage source configured to positively bias the ion selection grid by an ion selection voltage, and the electron rejection grid is coupled to an electron rejection voltage source configured to negatively bias the electron rejection grid by an electron rejection voltage. Furthermore, an ion current meter is coupled to the ion current collector to measure the ion current.
Abstract:
An electroscope system excites a certain area of a surface of a sample to emit electrons with a characteristic distribution of kinetic energies. The analyzed area of the sample is excited by an electron beam produced by a field emission source. A monochromator energy filter for the electron beam is down-stream of the field emission source. The field emission electron source is preferably a Schottky source, and a monochromator energy filter reduces energy dispersion of the electrons of the electron beam to less than 0.2 eV. Microareas of linear dimensions on the order of ten nanometers may be analyzed while observing them. Information on the chemical state of the detected elements present at the surface of the examined microarea of the sample is gathered.
Abstract:
One embodiment disclosed relates to a scanning electron beam apparatus including an objective lens, scan deflectors, de-scan deflectors, an energy-filter drift tube, and a segmented detector. The objective lens may be an immersion lens configured with a high extraction field so as to preserve azimuthal angle discrimination of the electrons scattered from the specimen surface. The de-scan deflectors may be used to compensate for the scanning of the incident electron beam. The energy-filter drift tube is configured to align the scattered electrons according to polar angles of trajectory from the specimen surface.
Abstract:
A scanning electron microscope with an energy filter which can positively utilize secondary electrons and/or reflected electrons which collide against a mesh electrode and are lost. The scanning electron microscope which has a porous electrode for producing an electric field for energy-filtering electrons produced by applying a primary electron beam to a sample and a 1st electron detector which detects electrons passing through the porous electrode is characterized by further having a porous structure provided near the sample, a deflector which deflects electrons from the axis of the primary electron beam, and a 2nd electron detector which detects the electrons deflected by the deflector.