Abstract:
In order to correct measurement magnification and measurement position of a spectral image with high efficiency and with high accuracy using an electronic spectroscope and a transmission electron microscope regarding the spectral image formed in two orthogonal axes which are an amount of energy loss axis and a measurement position information axis; a method for correcting magnification and position and a system for correcting magnification and position, both of which are capable of correcting measurement magnification and measurement position of a spectral image with high efficiency and with high accuracy using an electronic spectroscope and a transmission electron microscope regarding the spectral image formed in two orthogonal axes which are an amount of energy loss axis and a measurement position information axis, are provided.
Abstract:
An electron microscopy system (1) and an electron microscopy method for detection of time dependencies of secondary electrons generated by primary electrons is provided, in which the primary electron pulses are directed onto a sample surface (9) and electrons emanating from the sample surface are detected, time resolved. To this end the system comprises in particular a cavity resonator (53, 5). A cavity resonator can also be used to reduce aberrations of focusing lenses.
Abstract:
In order to correct measurement magnification and measurement position of a spectral image with high efficiency and with high accuracy using an electronic spectroscope and a transmission electron microscope regarding the spectral image formed in two orthogonal axes which are an amount of energy loss axis and a measurement position information axis; a method for correcting magnification and position and a system for correcting magnification and position, both of which are capable of correcting measurement magnification and measurement position of a spectral image with high efficiency and with high accuracy using an electronic spectroscope and a transmission electron microscope regarding the spectral image formed in two orthogonal axes which are an amount of energy loss axis and a measurement position information axis, are provided.
Abstract:
The present invention provides an electron spectroscopy apparatus (12) comprising a high energy particle source (12) for irradiating a sample, an electron detector system (16) (e.g. including a delay line detector) for detecting electrons emitted from the sample and an ion gun (8) for delivering a polycyclic aromatic hydrocarbon (PAH) ion beam to the sample, wherein the ion gun comprises a polycyclic aromatic hydrocarbon ion source, for example comprising coronene. In an embodiment, the PAH is located in a heated chamber (22) and vaporised to produce gas phase PAH. The gas phase PAH molecules are then ionised by electron impact, extracted from the ion source via an extraction field and focussed using ion optics. The PAH ion beam can be used for surface cleaning and depth analysis.
Abstract:
The invention describes a particle source in which energy selection occurs. The energy selection occurs by sending a beam of electrically charged particles 103 eccentrically through a lens 107. As a result of this, energy dispersion will occur in an image formed by the lens. By projecting this image onto a slit 109 in an energy selecting diaphragm 108, it is possible to allow only particles in a limited portion of the energy spectrum to pass. Consequently, the passed beam 113 will have a reduced energy spread. Deflection unit 112 deflects the beam to the optical axis 101. One can also elect to deflect a beam 105 going through the middle of the lens toward the optical axis and having, for example, greater current. The energy dispersed spot is imaged on the slit by a deflector 111. When positioning the energy dispersed spot on the slit, central beam 105 is deflected from the axis to such an extent that it is stopped by the energy selecting diaphragm. Hereby reflections and contamination resulting from this beam in the region after the diaphragm are avoided. Also electron-electron interaction resulting from the electrons from the central beam interacting with the energy filtered beam in the area of deflector 112 is avoided.
Abstract:
An electron microscope has an electron beam energy analyzer (energy filter) (11) to observe electron beam energy loss spectra and element distribution images. This electron microscope further includes a deflection coil (8) provided on the upstream side of a magnetic prism (9) to correct for the electron beam path in a plane normal to the optical axis and make the electron beam incident to the energy filter, a deflection coil (14) for correcting for the electron beam path in the energy axis direction of an energy dispersion surface (12) formed by the magnetic prism (9), and a control unit (21) for controlling the exciting conditions of the deflection coils (8,14).
Abstract:
A multipurpose ion implanter beam line configuration constructed for enabling implantation of common monatomic dopant ion species and cluster ions, the beam line configuration having a mass analyzer magnet defining a pole gap of substantial width between ferromagnetic poles of the magnet and a mass selection aperture, the analyzer magnet sized to accept an ion beam from a slot-form ion source extraction aperture and to produce dispersion at the mass selection aperture in a plane corresponding to the width of the beam, the mass selection aperture capable of being set to a mass-selection width sized to select a beam of the cluster, the mass selection aperture also capable of being set to a substantially narrower mass-selection width and the analyzer magnet having a resolution at the mass selection aperture sufficient to enable selection of a beam of monatomic dopant ions of substantially a single atomic or molecular weight.
Abstract:
The present invention provides for an irradiation system with an ion beam/charged particle beam having an energy filter (17) formed by deflection electrodes (24-1, 24-2) and a deflection magnet (22) and means for switching therebetween wherein the deflection magnet has a general window-frame shape and is formed with a hollow portion at its centre and the deflection electrodes are installed, along with suppression electrodes (31-1, 31-2), in a vacuum chamber (23) arranged in the hollow portion of the deflection magnet. The deflection electrodes are installed with respect to the deflection magnet such that a deflection trajectory of a beam caused by a magnetic field and a deflection trajectory of a beam caused by an electric field overlap each other and since the deflection electrodes or the deflection magnet can be selectively used by way of a switching means the system can function with a wide range of beam conditions and thus is widely usable.