Abstract: An atom probe directs two or more pulsed laser beams onto a specimen, with each laser beam being on a different side of the specimen, and with each laser beam supplying pulses at a time different from the other laser beams. The laser beams are preferably generated by splitting a single beam provided by a laser source. The laser beams are preferably successively aligned incident with the specimen by one or more beam steering mirrors, which may also scan each laser beam over the specimen to achieve a desired degree of specimen ionization.

Abstract: An atom probe directs two or more pulsed laser beams onto a specimen, with each laser beam being on a different side of the specimen, and with each laser beam supplying pulses at a time different from the other laser beams. The laser beams are preferably generated by splitting a single beam provided by a laser source. The laser beams are preferably successively aligned incident with the specimen by one or more beam steering mirrors, which may also scan each laser beam over the specimen to achieve a desired degree of specimen ionization.

Abstract: In an atom probe having a vacuum chamber containing a specimen mount and a detector for receiving ions emitted from the specimen, a high vacuum subchamber is provided about the specimen mount, with an aperture in the subchamber allowing passage of emitted ions to the detector. The high vacuum subchamber may be pumped to higher vacuum (lower pressure) than the vacuum chamber, and so long as the pressure in the vacuum chamber is below about 10?1 Pa, very little gas diffusion takes place through the aperture, allowing higher vacuum to be maintained in the subchamber despite the aperture opening to the chamber. The higher vacuum in the subchamber about the specimen assists in reducing noise in atom probe image data. The aperture may conveniently be provided by the aperture in a counter electrode, such as a local electrode, as commonly used in atom probes.

Abstract: In an atom probe having a specimen mount spaced from a detector, and preferably having a local electrode situated next to the specimen mount, a lens assembly is insertable between the specimen (and any local electrode) and detector. The lens assembly includes a decelerating electrode biased to decelerate ions from the specimen mount and an accelerating mesh biased to accelerate ions from the specimen mount. The decelerating electrode and accelerating mesh cooperate to divert the outermost ions from the specimen mount—which correspond to the peripheral areas of a specimen—so that they reach the detector, whereas they would ordinarily be lost. Because the detector now detects the outermost ions, the peripheral areas of the specimen are now imaged by the detector, providing the detector with a greatly increased field of view of the specimen, as much as 100 degrees (full angle) or more.

Abstract: In an atom probe having a specimen mount spaced from a detector, and preferably having a local electrode situated next to the specimen mount, a lens assembly is insertable between the specimen (and any local electrode) and detector. The lens assembly includes a decelerating electrode biased to decelerate ions from the specimen mount and an accelerating mesh biased to accelerate ions from the specimen mount, with the decelerating electrode being situated closer to the specimen mount and the decelerating electrode being situated closer to the detector. The decelerating electrode and accelerating mesh cooperate to divert the outermost ions from the specimen mount—which correspond to the peripheral areas of a specimen—so that they reach the detector, whereas they would ordinarily be lost.

Abstract: The present invention is directed generally toward atom probe and TEM data and associated systems and methods. Other aspects of the invention are directed toward combining APT data and TEM data into a unified data set. Other aspects of the invention are directed toward using the data from one instrument to improve the quality of data obtained from another instrument.

Abstract: An atom probe includes a detector which registers the time of flight of ions evaporated from a specimen, as well as the positions on the detector at which the ions impact and the kinetic energies of the ions. The detected position allows the original locations of the ions on the specimen to be mapped, and the times of flight and kinetic energies can be spectrally analyzed (e.g., binned into sets of like values) to determine the elemental identities of the ions. The use of kinetic energy data as well as time of flight data can allow more accurate identification of composition than where time of flight data are used alone, as in traditional atom probes.

Abstract: Aspects of the present invention are directed generally toward atom probe and three-dimensional atom probe microscopes. For example, certain aspects of the invention are directed -toward an atom probe or a three-dimensional atom probe that includes a sub-nanosecond laser to evaporate ions from a specimen under analysis and a reflectron for reflecting the ions. In further aspects of the invention, the reflectron can include a front electrode and a back electrode. At least one of the front and back electrodes can be capable of generating a curved electric field. Additionally, the front electrode and back electrodes can be configured to perform time focusing and resolve an image of a specimen.

Abstract: A mass analysis device with wide angular acceptance, notably of the mass spectrometer or atom probe microscope type, includes means for receiving a sample, means for extracting ions from the surface of the sample, and a reflectron producing a torroidal electrostatic field whose equipotential lines are defined by a first curvature in a first direction and a first center of curvature, and a second curvature in a second direction perpendicular to the first direction and a second center of curvature, the sample being positioned close to the first center of curvature.

Abstract: An achromatic magnetic mass spectrometer, for example of the SIMS type with double focusing, comprises means for canceling the four aberrations of the second order, and means for canceling the off-axis achromatism and for modulating the dispersion in mass.

Abstract: A tomographic atom probe uses electrical pulses applied to an electrode in order to carry out evaporation of the sample being analyzed. In order to produce these electrical pulses, the tomographic atom probe comprises a high-voltage generator connected to an electrode by an electrical connection comprising a chip of semiconductor material. The probe also comprises a light source which can be controlled in order to generate light pulses which are applied to the semiconductor chip. Throughout the illumination, the chip is rendered conductive, which puts the high-voltage generator and the electrode in electrical contact so that a potential step is applied to the latter. The probe also comprises means for applying a voltage step of opposite amplitude to the previous step at the end of a time interval ?t0, so that the electrode finally receives a voltage pulse of duration ?t0.

Abstract: A wide spectral band laser pulse generating device capable of covering a spectrum formed of given wavelengths is provided, including: a monochromatic laser light source whose intensity is adjustable; non-linear optical means, a photonic crystal or a microstructured optical fiber for example, for carrying out spectral widening of the wave emitted by the light source; the light source and the non-linear optical means are configured and arranged so as to create a white supercontinuum whose continuous spectrum contains the wavelengths considered. The invention relates to the general field of the analysis of the composition of material specimens, and in particular to laser tomographic atom probes.

Abstract: A laser atom probe situates a counter electrode between a specimen mount and a detector, and provides a laser having its beam aligned to illuminate the specimen through the aperture of the counter electrode. The detector, specimen mount, and/or the counter electrode may be charged to some boost voltage and then be pulsed to bring the specimen to ionization. The timing of the laser pulses may be used to determine ion departure and arrival times allowing determination of the mass-to-charge ratios of the ions, thus their identities. Automated alignment methods are described wherein the laser is automatically directed to areas of interest.

Abstract: A reflectron (1) for deflecting an ion from a specimen in a time-of-flight mass spectrometer comprises a front electrode (2) and a back electrode (3). At least one of the front and back electrodes (2, 3) is capable of generating a curved electric field. The front and back electrodes are configured to perform time focusing and resolve an image of a specimen.

Abstract: An achromatic magnetic mass spectrometer, for example of the SIMS type with double focusing, comprises means for canceling the four aberrations of the second order, and means for canceling the off-axis achromatism and for modulating the dispersion in mass.

Abstract: A mass analysis device with wide angular acceptance, notably of the mass spectrometer or atom probe microscope type, includes means for receiving a sample, means for extracting ions from the surface of the sample, and a reflectron producing a torroidal electrostatic field whose equipotential lines are defined by a first curvature in a first direction and a first center of curvature, and a second curvature in a second direction perpendicular to the first direction and a second center of curvature, the sample being positioned close to the first center of curvature.

Abstract: The present invention concerns the enhancing of the mass resolution of wide angle tomographic atom probes. The invention consists of an atom probe also comprising a sample-holding device and a detector which are separated from one another by a distance L and enclosed in a chamber, an “Einzel” type electrostatic lens consisting of three electrodes arranged inside the chamber between the sample and the detector, to which electrical potentials are applied so as to form an electrical field that strongly focuses the beam of ions emitted by the sample under test when the probe is operating. According to the invention, the geometry of the electrodes is defined precisely so as to greatly limit the effects of the spherical aberration that affects the “Einzel” lens on the beam of ions, said spherical aberration being clearly sensitive when the lens is greatly polarized. The invention applies more particularly to the atom probes known as 3D atom probes.

Abstract: A tomographic atom probe uses electrical pulses applied to an electrode in order to carry out evaporation of the sample being analyzed. In order to produce these electrical pulses, the tomographic atom probe comprises a high-voltage generator connected to an electrode by an electrical connection comprising a chip of semiconductor material. The probe also comprises a light source which can be controlled in order to generate light pulses which are applied to the semiconductor chip. Throughout the illumination, the chip is rendered conductive, which puts the high-voltage generator and the electrode in electrical contact so that a potential step is applied to the latter. The probe also comprises means for applying a voltage step of opposite amplitude to the previous step at the end of a time interval ?t0, so that the electrode finally receives a voltage pulse of duration ?t0.

Abstract: A wide spectral band laser pulse generating device capable of covering a spectrum formed of given wavelengths is provided, including: a monochromatic laser light source whose intensity is adjustable; non-linear optical means, a photonic crystal or a microstructured optical fiber for example, for carrying out spectral widening of the wave emitted by the light source; the light source and the non-linear optical means are configured and arranged so as to create a white supercontinuum whose continuous spectrum contains the wavelengths considered. The invention relates to the general field of the analysis of the composition of material specimens, and in particular to laser tomographic atom probes.

Abstract: The present invention relates generally to atom probes, atom probe specimens, and associated methods. For example, certain aspects are directed toward methods for analyzing a portion of a specimen that includes selecting a region of interest and moving a portion of material in a border region proximate to the region of interest so that at least a portion of the region of interest protrudes relative to at least a portion of the border region. The method further includes analyzing a portion of the region of interest. Other aspects of the invention are directed toward a method for applying photonic energy in an atom probe process by passing photonic energy through a lens system separated from a photonic device and spaced apart from the photonic device. Yet other aspects of the invention are directed toward a method for reflecting photonic energy off an outer surface of an electrode onto a specimen.