Abstract:
An apparatus and method for inspecting a surface of a sample, particularly but not limited to a semiconductor device, using an electron beam is presented. The technique is called Secondary Electron Emission Microscopy (SEEM), and has significant advantages over both Scanning Electron Microscopy (SEM) and Low Energy Electron Microscopy (LEEM) techniques. In particular, the SEEM technique utilizes a beam of relatively high-energy primary electrons having a beam width appropriate for parallel, multi-pixel imaging. The electron energy is near a charge-stable condition to achieve faster imaging than was previously attainable with SEM, and charge neutrality unattainable with LEEM. The emitted electrons may be detected using a time delay integration detector.
Abstract:
A scanning photoelectron microscope comprises a stage on which a sample is placed in a state in which gas around the sample is present, a light source emitting light of a wavelength capable of causing photoelectrons to be emitted from the sample, an optical system for condensing the light from the light source on the sample, scanning means for scanning the sample and the light relative to each other, and detecting means capable of applying positive potential to the sample, and detecting the photoelectrons created from the sample by the condensing, through the gas.
Abstract:
A charged particle energy analyser has a magnetic lens such as a snorkel-type lens and a source for directing ionising radiation onto a specimen causing charged particles to be emitted from its surface. The specimen is immersed in the magnetic imaging field of the magnetic lens so that particles having energies in a predetermined energy range are brought to a focus, the energies of the focussed particles being analysed by an energy analyser. An electrode arrangement is provided for enabling the magnetic imaging field of the magnetic lens to utilise unfocussed particles to cause charge neutralisation of the specimen. Alternatively, charged particles from a source are subjected to an electric field which is transverse to the optical axis of the magnetic lens and are guided onto the specimen by the magnetic imaging field of the magnetic lens.
Abstract:
An electron detection apparatus detects information contained in electrons emitted from a sample. For the detection of electron, the apparatus uses a probe disposed in close proximity to the sample. The probe has a first side and a second side between which penetrates an aperture, wherein the first side of the probe confronts the sample. A voltage is applied between the probe and the sample. The voltage applied therebetween is set to a such a level that an electric field effect yields on the surface of the sample. Under the electric field effect yielding on the surface of the sample, light or heat is applied to the surface of the sample to emit the electrons from the sample. The electrons thus emitted is detected by entering electrons into the aperture at the first side, passing through the aperture and exiting from the aperture at the second side.
Abstract:
Atom probe apparatus includes an emission tip from which atoms can be evaporated in atomic emission events, a position sensitive detector for detecting the position and timing of the charge cloud resulting from atomic emission events, and a pulse heating beam for heating the emission tip in short pulses to evaporate atoms essentially one at a time from the emission tip. The heating beam may be formed as an electron beam from an electron gun which is directed to the tip and scanned rapidly back and forth across the tip to be incident upon the tip for short periods of time as the beam is scanned back and forth. The beam may further be produced as a chopped beam of electrons by scanning the beam back and forth across a slit in an aperture plate so that only pulses of electrons pass through the plate as the beam passes across the slit. The electrons passing through the slit are then focused and directed to the tip. The tip may also be heated by light from a pulsed source such as a laser which is passed through a reflecting Schwarzschild objective and focused onto the tip in pulses to provide excitation by light photons. The position sensitive detector, which may include a microchannel plate backed by a position sensitive wedge and strip detector, determines both the time of arrival of a charge pulse from an atomic emission event and the relative position of the charge cloud at the point where it impacts upon the detector. The detector may also be formed as a three-level, trigonal array of pads which allows both one and two atomic events per heating pulse to be resolved.
Abstract:
An apparatus for determining and displaying the time evolution profile of electron carriers present within a submicron or micron device comprises a laser for generating a beam of ultrafast pulses of ultraviolet light. A first beam splitter splits each pulse into a transmitted beam and a reflected beam. The transmitted beam travels through a time delay circuit, and is then converted into a train of ultrafast electrical pulses which are transmitted to the device. The reflected beam is focused on the device. An electron detector, also focused on the device, collects the ejected electrons resulting from the interaction of the light pulse and electrical pulse to produce an electrical signal. The signal is then magnified in intensity by an amplifier and directed at a cathode ray tube to cause an image to appear thereon. A SIT vidicon camera converts the image into an electrical signal and transmits the signal to a computer. The computer generates a time evolution profile from the signal received which is sent to a monitor for display.
Abstract:
A compact charged-particle-beam microscope, weighing less than about 50 kg and having a size of less than about 1 m×1 m×1 m, is provided for imaging a sample. The microscope has a vacuum chamber to maintain a low-pressure environment, a stage to hold a sample in the vacuum chamber, a charged-particle beam source to generate a charged-particle beam, charged-particle beam optics to converge the charged-particle beam onto the sample, and one or more beam scanners to scan the charged-particle beam across the sample. A charged-particle detector is provided to detect charged-particle radiation emanating from the sample and generate a corresponding charged-particle-detection signal. At least one energy dispersive x-ray spectrometer (EDS) is provided to detect x-rays emanating from the sample and generate a corresponding x-ray-detection signal. A controller analyzes the charged-particle-detection signal and the x-ray-detection signal to generate an image of the sample and a histogram of x-ray energies for at least a portion of the sample.