Abstract:
A device for mass selective determination of at least one ion or of a plurality of ions is used, for example, in a measuring apparatus having an ion trap. The ion trap has a ring electrode having a first opening. A first electrode is arranged at the first opening. Furthermore, an amplifier for providing a radio-frequency storage signal for the ion trap and a first transformer are provided, said first transformer being connected to the amplifier and the first electrode in such a way that the radio-frequency storage signal is coupled into the first electrode via the first transformer.
Abstract:
There is a limit in range and distance in which an electron beam can interfere and electron interference is implemented within a range of a coherence length. Therefore, interference images are consecutively recorded for each interference region width from an interference image of a reference wave and an observation region adjacent to the reference wave by considering that a phase distribution regenerated and observed by an interference microscopy is a differential between phase distributions of two waves used for interference and a differential image between phase distributions of a predetermined observation region and a predetermined reference wave is acquired by acquiring integrating phase distributions acquired by individually regenerating the interference images. This work enables a wide range of interference image which is more than a coherence length by arranging phase distribution images performed and acquired in the respective phase distributions in a predetermined order.
Abstract:
Rheology system. The system includes a first piezoelectric actuator assembly for providing microscale displacement of a sample and a second piezoelectric actuator assembly for oscillating the sample at a nano/micro scale displacement in a selected frequency range extended significantly as compared to the frequency range available on the commercial AFMs. A preferred sample is cartilage and the disclosed system can distinguish between normal cartilage and GAG-depleted cartilage.
Abstract:
A probe arrangement with a probe for local electrophysiological analysis of cells (4) such as patch-clamp techniques for use with atomic force microscopy, has a probe with a cantilever arm (2) connected to a probe holder (3). The probe has a probe tip (4) at a probing end (5) of the cantilever arm (2) and a fluid channel (6) in the cantilever arm (2) connecting a probe tip aperture (7) with a fluid reservoir (8) via a duct (9). The fluid channel (6), the duct (9) and the fluid reservoir (8) are adapted to be filled with a fluid solution (10) enabling ion transport for electrophysiological analysis. A first electrode (15) for electrophysiological analysis is placed in the fluid reservoir (8) and/or in the duct (9) and/or in the fluid channel (6).
Abstract:
An apparatus configured to control a magnetic field strength of a magnetic lens is provided. The apparatus may include a magnetic sensor configured to generate an output signal responsive to a first magnetic field strength of the magnetic lens. The apparatus may also include a control circuit coupled to the magnetic sensor and the magnetic sensor. The control circuit may be configured to receive the output signal from the magnetic lens and to receive an input signal responsive to a predetermined magnetic field strength. The control circuit may be further configured to generate a control signal responsive to the output signal and the input signal. Additionally, the control circuit may be configured to apply a current to the magnetic lens such that a second magnetic field strength may be generated within the magnetic lens closer to the predetermined magnetic field strength than the first magnetic strength.
Abstract:
A lattice strain measuring method comprising the steps of: using a scanning transmission electron microscope 12 to apply convergent electron beams 34 to a sample 32 and obtain a convergent-beam electron diffraction image 36 of the sample 32; computing a lattice strain magnitude of the sample 32, based on the obtained convergent-beam electron diffraction image; and displaying the computed lattice strain magnitude, associated with an electron microscope image of the sample 32. A scanning transmission electron microscope 12 is used, whereby electron beams 34 are caused to scan to thereby suitably set an incidence position. Accordingly, the incidence position of the electron beams can be displaced at a nanometer-order pitch accurately in a short period of time. The use of a scanning transmission electron microscope 12 requires no image forming lens below the sample 32, and the convergent-beam electron diffraction image is free from the distortion due to the influence of an image forming lens. Thus, a distribution of lattice strains in an electronic device having, e.g., a micronized structure can be displayed in an image with high resolving power and with high accuracy and furthermore in a short period of time.
Abstract:
A photoemission electron microscopy having a light source system for carrying out a high-resolution measurement such as work function distribution measurement or magnetic domain distribution with reliability, and a high-sensitivity measurement method using the photoemission electron microscopy. A photoemission electron microscopy having an excitation light source system in which a specimen is irradiated with irradiation light from a light source uses a vacuum chamber in which the specimen is placed and an objective lens which collects the irradiation light on a specimen surface. The objective lens is accommodated in the vacuum chamber. The light source may be placed outside the vacuum chamber. A condenser lens which makes the irradiation light from the light source generally parallel may be placed between the light source and the vacuum chamber. A transmission window which transmits the irradiation light while the vacuum chamber is sealed may be placed between the condenser lens and the objective lens. If a diffraction grating for selecting the wavelength of the irradiation light or a polarizing filter for selecting the direction of circularly polarized light in the irradiation light is used between the condenser lens and the transmission window, a high-resolution measurement of a work function distribution or a magnetic domain distribution on the specimen surface can be carried out.
Abstract:
A time-of-flight secondary ion mass spectrometer instrument comprises a pulsed source of a beam of ions, directed through a focusing device onto a sample to be analyzed. Ions emitted from the sample are collected, and mass spectrometry performed thereon to analyze the sample. Both the source and emitted beams may be focused by the same focusing device. This allows the instrument to be mounted to a single port in a vacuum chamber.
Abstract:
Electron microscope provided, in the direction of the longitudinal axis, with at least one electron beam generation system, a condenser and objective lens system, a specimen chamber with a specimen mount, a projection lens system with imaging screen for the purpose of transmission electron microscopy (TEM) and/or an electron detector for the purpose of scanning electron microscopy (SEM) . The microscope is used in combination with an externally positioned Raman spectrometer and an associated light source for injecting and extracting, via a window in the microscope wall, a light beam to be directed at the specimen, and specimen-related Raman radiation, respectively. In the specimen chamber, a light beam and Raman radiation guide system is provided with an optical guide to guide the light beam to--and the Raman radiation from--the specimen. The guide system and the specimen mount are displaceable with respect to one another for mutual alignment of the specimen and the optical axis of the Raman spectrometer.
Abstract:
A surface analyzing method comprising an ion generation step for generating multiply-charged ions of specific ion species and specific charge state; a deceleration step for decelerating the generated multiply-charged ions to a lower kinetic energy than an energy of threshold of sputtering of an objective material; an irradiation step for irradiating the decelerated multiply-charged ions on the surface of a sample; and an analysis step for analyzing particles or light emitted from the surface of said sample by the irradiation of said multiply-charged ions. Apparatus is provided for carrying out the method. Since the ions irradiated on the sample surface are multiply-charged ions having a lower kinetic energy than that of threshold of sputtering of materials constituting a sample, the irradiated ions interact merely with the top surface layer of the sample whereby analyzed information merely from the top surface layer of the sample can be obtained, and as a result, the kind of atoms of the top surface layer of the sample and the bonding state of said atoms can be analyzed with high sensitivity and high resolution.