摘要:
The invention provides a charged particle device (1) comprising: a particle source (2) for providing a charged particle beam (4), an objective lens (10) for directing the particle beam onto a specimen (8), said objective lens (10) having an optical axis (6); a particle mirror (14) located on the optical axis (6) of the objective lens (10), said particle mirror having a front surface, a back surface, a drift region (26) reaching from the back surface to the front surface for letting the charged particle beam pass from the back surface to the front surface, said drift region (26) being positioned away from the optical axis (6), and a deflecting region located on the front surface for deflecting charge particles coming from the specimen towards a detector (16).
摘要:
The SEM according to the invention is arranged to detect scattered electrons transmitted by the specimen (22). The detector is constructed so as to have a flat detector surface (26) for a large angular range. In order to select a given angular range, a mask (24) with an eccentric opening (40) is arranged between the specimen and the detector surface and it is also arranged so as to be rotatable. An optimum angle relative to a given direction in the specimen can thus be selected for a given type of contrast. The mask is preferably displaceable in the specimen direction, the detector surface being subdivided into a plurality of parts (26a, 26b) and the assembly formed by the specimen and the detector surface is tiltable through an angle relative to the optical axis (4). A high degree of flexibility is thus achieved for the selection of the electrons to be detected which are scattered by the specimen, so that adjustments can be made so as to achieve an optimum contrast situation.
摘要:
A structure and associated method for detecting secondary and backscatter electrons in a microcolumn. A secondary electron detector and a backscatter electron detector, both located upstream of the Einzel (objective) lens in the microcolumn, provide a highly efficient axially symmetric electron detector, short column length, and short working distance. The secondary electron detector is located between the deflection system and the Einzel lens, between the suppressor plate and the Einzel lens, or between the deflection system and the beam-limiting aperture. The backscatter electron detector is located between a beam-limiting aperture and the deflection system and can be incorporated into the aperture. A secondary electron extractor placed between the sample and the Einzel lens further improves the spatial resolution caused by surface imperfection or local surface potential on the sample surface.
摘要:
An electron detector is proposed particularly for detecting secondary electrons in a micro electron column based e-beam tool such as e.g. a scanning electron microscope. The electron detector has a flat detector body (10) and a plurality of trench-shaped channels (12) extending parallel to the body surface and being e.g. open on this surface. The channels (12) extend radially from an opening (11) for the primary electron beam (1) of the tool. Furthermore, the detector comprises an inner and an outer ring electrode (15, 16) for generating an electric field which is rotationally symmetrical in relation to the axis of the opening (11) and by which the secondary electrons are accelerated along the length of the channels (12). The rotational symmetry of the electric field prevents unwanted interaction with the primary electron beam. The preferred embodiment of the electron detector is manufactured by micro-machining, starting from a silicon on insulator wafer.
摘要:
A scanning electron microscope using a retarding-field formation technique and still capable of high-efficient separation and detection of secondary electrons. The scanning electron microscope comprises an electron source, a converging lens for converging a primary electron beam emitted from the electron source, a detector for detecting electrons derived from the irradiation of a sample with the converged primary electron beam, first retarding means for slowing down the primary electron beam directed to the sample, second retarding means for slowing down the electrons emitted from the sample, and a deflector for directing the electrons from the second retarding means toward the detector.
摘要:
An environmental scanning electron microscope is provided which is capable of only detecting backscattered electron signals emanating from the specimen with the detector assembly being positioned within the gaseous environment of the ESEM specimen chamber. This detector assembly includes a biased converter plate and a collection grid/collection plate/collector ring arrangement. The primary beam passes through the final pressure limiting aperture formed in the converter plate and then through a central aperture of the collection grid/plate/ring before striking the sample. The collection grid is held at ground potential and therefore does not collect secondary electron signals generated at the sample. The backscattered electrons are not collected by the collector grid/plate/ring and strike the converter plate creating converted backscattered electrons. The converted backscattered electrons are amplified in the gas by the electric field created between the converter plate and the collection grid. As a result, the collection grid/plate/ring will not collect secondary electron signals from the sample but will collect only an amplified converted backscattered electron signal. This dedicated gaseous backscattered electron detector can also be utilized to make a simple, low cost electron detector that can easily be switched between secondary electron detection, backscattered electron detection or both together.
摘要:
The current of secondary electrons emanating from the specimen (14) in an ESEM is amplified by an avalanche-like ionization of the molecules (41) of the gas atmosphere. However, in order to achieve an adequate number of successive ionizations, a comparatively high voltage is required at the detector electrode (30) and, because of the risk of electric breakdowns, the distance between the specimen and the detector may not be smaller than a comparatively large minimum distance. Consequently, the number of successive ionizations is limited and hence also the current amplification. In order to achieve a higher amplification, the invention proposes the application of an additional magnetic field B in the ionization space. The path length of the secondary electrons is thus substantially increased so that a significantly larger number of ionizations takes place and hence a higher amplification is achieved.
摘要:
The detection system of the scanning electron microscope with the tube separated from the sample chamber (11) by means of the differential chamber (2) consists of the single-crystal scintillator (6) with the aperture stop (9); said single-crystal scintillator (6) is divided into two halves, and based on double yttrium-aluminium oxides or on yttrium silicate activated by trivalent cerium, and having the central conical opening (46), smaller base of which is on the side near to incidence of the primary electron beams, and forms the aperture stop (9). Said conical opening (46) is coated with the reflecting metal layer (37) on the contact areas of the both halves, and with the reflective layer (34) of dielectric and heavy metal on its inner surface. The single-crystal scintillator (6) is placed between the left and the right lightguides (18, 19) in space of the sample chamber (11) above the sample (10). From the external bottom (3) of the differential chamber, it is separated with the sealing (45), and from the side of the sample (10) placing, it is equipped with the circular electrode system (7) consisting of at least two electrodes (27, 28) symmetrical around the axis (47) of the primary electron beams (33).
摘要:
A solid state electron or x-ray detector is mounted within the time-varying magnetic deflection fields of a charged particle beam system. A minimum volume of high resistivity conductors and insulating materials are used in the mounting to minimize eddy currents that otherwise cause dynamic deflection distortions. Segmented conductive elastomer members make electrical and mechanical contact with the active surface of the detector. A flexible PC board connects the detector active areas to external signal processing electronics.
摘要:
Method and apparatus for material analysis in which X-rays generated pursuant to incidence of an electron beam on the material are detected by a detector (24) which generates signals representative of X-ray intensity. A first single channel analyser (SCA-1) is connected to receive the signals from the detector (24) and to pass to an associated first counter (CTR-1) a count signal whenever the signal applied to the first single channel analyser is representative of an X-ray energy within a relatively narrow range of such energies. A second single channel analyser (BG-1) is also connected to receive the signals from the detector (24) and to pass to an associated second counter (B-1) a count signal whenever the signal applied to the second analyser (BG-1) is representative of an X-ray energy falling within a much broader range of such energies than the first-mentioned range. The first and second counters (CTR-1 and B-1) accumulate the count signals applied thereto. The count in the second counter (B-1) is compared by a comparator (C-1) with a pre-established count in a third counter (A-1) and when the count in the second counter (B-1) assumes the same value as the count in the third counter (A-1) the counts in the first and second counters (CTR-1 and B-1) are held. The so held count in the first counter (CTR-1) then itself represents a normalized ratio of X-ray energy within the narrow range to the X-ray energy for the energy spectrum represented by the broad range of energies. On the basis of this normalized ratio information as to the makeup of the material can be derived.