Abstract:
A particle beam, such as that generated by a scanning electron microscope, impinges upon the specimen to be analyzed. The beam produces X-rays, the energy of which enables the various elements contained in the specimen to be identified. The detected X-ray energy is converted to rectangular electrical pulses, the height of which is proportional to the detected X-ray energy and hence characteristic of the element or elements present in the specimen. The pulse signals are coded so as to trigger or energize the several guns of a conventional color cathode ray tube, such as that used in a color televison receiver. The resulting multicolor map displayed on the screen of the cathode ray tube thus visually indicates to the observer the presence of certain elements and their relative position in the specimen being investigated.
Abstract:
A scanning ion microscope is described in which the prior arts of scanning microscopy and achromatic quadrupole lens design as perfected for electrons are utilized for massive high-energy positive ions. Because the DeBroglie wavelength of the massive ions is smaller than the wavelength of electrons, diffraction in the objective lens is reduced. In principle resolution better than one Angstrom can be achieved. Because of the copious production of X-rays and Auger electrons in the specimen by such ions, specimens of atomic dimensions can be examined with a minimum of radiation damage by the ions. The specifically new, novel, and useful feature of this invention is the use of properly focused high-energy heavy-ion beams and the detection of single atomic events in the specimen, which together enable much greater sensitivity and resolution than attainable by other means.
Abstract:
A raster scanning ion microscope for determining, with a large field of view, the lateral distribution of elements, isotopes and compounds at the surface and in the bulk of solid specimens and for displaying the surface topography of the sample. The scanning ion microscope consists of an ion gun to produce a primary ion beam, a means to focus and raster scan the primary ion beam over the surface of the specimen, a means to form a beam of secondary ions out of all particles sputtered from the specimen, an energy analyzer and a mass spectrometer for secondary ion analysis and a means for optimum transport of the secondary ions from the specimen to the mass spectrometer. Use of a quadrupole mass filter as a mass analyzer reduces restrictions usually faced with magnetic type mass analyzer and allows imaging of the specimen with a large field of view. Moreover non-normal secondary ion extraction and/or non-normal primary ion incidence in combination with low secondary ion extraction voltages result in the capability of the instrument of displaying the surface topography of the specimen.
Abstract:
An X-ray scan area mapping system for a scanning electron microscope provides a spacial area map display of X-ray events emitted from a specimen within at least one energy range as the specimen is scanned at scanning electron microscope rates by an electron beam. A background X-ray noise reduction circuit enables intensification of the scanning electron microscope cathode-ray tube display upon the occurrence of an X-ray event within the energy range and disables intensification when the time between consecutive X-ray events within the energy range exceeds a predetermined time period. Background X-ray events occur at much slower rates than the X-ray events emitted from the specimen within the energy range, and therefor, a substantial reduction in background noise on the scanning electron microscope display is obtained.
Abstract:
An electron-beam micro-analyzer for investigating solid test specimens and radiation penetrable test specimens is disclosed. The micro-analyzer has an electron-beam generator for directing a focussed electron beam unto the test specimen to release Auger electrons therefrom. An electron spectrometer then separates the released Auger electrons according to the respective kinetic energies thereof and an electron detector detects the Auger electrons of specified energy separated in the spectrometer. The electron-beam generator has a field-emission point cathode having a small radius of curvature and an anode having an opening for passing the electron beam therethrough. A voltage supply applys a voltage to develop an electric field between the anode and the point cathode of sufficient strength to excite the cathode to electron field emission. A deceleration lens disposed intermediate the anode and the test specimen reduces the velocity of the electrons of the electron beam passing from the opening of the anode.
Abstract:
An electron microprobe has a holder for a sample to be analyzed. The holder is movable along an X-axis and a Y-axis, each at right angles to the electron beam directed at the sample. Drives, each including an electric motor, are operatively connected to the holder to adjust the position of the holder along the respective axis. There are also electron beam position controls for positioning the beam in a path oriented as desired with respect to the X and Y axes. An electron beam current control enables the quantity of electrons in the beam to be adjusted. A third drive includes an electric motor, and is connected to a reflector to position the reflector with respect to the X-rays emitted from the sample, and with respect to X-ray detectors. The controls and drives are connected to a control matrix through which signals are supplied to the respective controls and drives, as dictated by a computer. Each of the controls and drives produces an analogue feedback signal indicative of the setting thereof. These feedback signals are sent to a selector matrix from which a specific signal is selected, as dictated by the computer, with the selected signal being delivered to the computer through an analogue to digital converter. The X-ray detectors also produce signals which are ultimately delivered to the computer either directly or through the analogue to digital converter. By appropriately programming the computer, the apparatus automatically analyzes the sample for constituents as desired.
Abstract:
In micro-analyzer apparatus of the kind in which material to be analyzed is arranged as a target of an ion probe and ionized particles obtained from the target are analyzed in a mass spectrometer, accuracy of analysis is improved by analyzing not secondary ions sputtered from the target but neutral atoms which are collected and passed to the mass spectrometer through an ionizer. Several possible forms of ionizer for ionizing the sputtered neutrals are also disclosed.
Abstract:
An electron energy loss spectrometer is described having a direct detection sensor, a high speed shutter and a sensor processor wherein the sensor processor combines images from individual sensor read-outs and converts a two dimensional image from said sensor into a one dimensional spectrum and wherein the one dimensional spectrum is output to a computer and operation of the high speed shutter is integrated with timing of imaging the sensor. The shutter is controlled to allow reduction in exposure of images corresponding to the individual sensor readouts. A plurality of images are exposed by imaging less than the full possible exposure and wherein the plurality of images are combined to form a composite image. The plurality of images can be comprised of images created by exposing the sensor for different exposure times.
Abstract:
A device for imparting an orbital angular momentum to a charged particle wave propagating along a beam axis in a charged particle beam generating apparatus is described. The device comprises a support element having a target region adapted for transmitting a charged particle wave propagating along a beam axis and an induction means for inducing a magnetic flux along an elongated profile having a free end portion located in the target region and the induction means is adapted for providing a magnetic flux in the elongated profile in order to induce an angular gradient, relative to the beam axis, of the phase of the charged particle wave when transmitted through the target region. A corresponding method is also disclosed, as well as the use thereof in electron microscopy.