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 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: 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: An atom probe includes a specimen mount that can hold a specimen to be analyzed. A detector is spaced apart from the specimen mount. Between the detector and specimen mount Is a local electrode with an aperture. A laser is oriented to emit a laser beam toward the specimen mount at a nonzero angle with respect to the aperture plane, the aperture plane being oriented perpendicular to an ion travel path defined through the aperture between the specimen mount and detector.

Abstract: A method for aligning an energy beam to an object in an atom probe is disclosed. The method comprises monitoring at least one parameter indicative of an interaction between the energy beam and the object. A signal is generated in response to the interaction of the energy beam and the object. The signal is then used to effectuate control of the alignment of the energy beam to the object.

Abstract: A laser atom probe (100) situates a counter electrode between a specimen mount and a detector (106), and provides a laser (116) having its beam (122) aligned to illuminate the specimen (104) through the aperture (110) of the counter electrode (108). The detector, specimen mount (102), 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.