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 mountwhich correspond to the peripheral areas of a specimenso 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.

In one aspect, the present invention provides a method of generating an electron beam in a transmission electron microscopy device. The method includes: generating an electron pulse [306] by a pulsed electron source [300], accelerating the electron pulse in a first resonant microwave cavity [302], passing the accelerated electron pulse through a drift space [314], and correcting the energy spread of the accelerated electron pulse in a second resonant microwave cavity [304] by operating it out of phase by 90 degrees from the first resonant cavity [302].

The present disclosure hereinafter proposes a charged particle beam device and a method for adjusting a charged particle beam device which aim to appropriately set device conditions independently of a state of a sample. The present disclosure proposes a method and a system for adjusting contrast and brightness of an image, comprising: adjusting offset (step 112) of a signal processing device of the charged particle beam device so that the brightness of a pattern in an image obtained by scanning with a first charged particle beam (first intermittent condition beam) becomes a predetermined value; and adjusting a gain (step 114) of the signal processing device so that the brightness of a pattern in an image obtained by scanning with a second charged particle beam, which is a pulse beam (second intermittent condition beam) different from the first charged particle beam in at least one of irradiation time, irradiation distance, interval time between irradiation points, and distance between irradiation points, becomes a predetermined value.

In one aspect, the present invention provides a method of generating an electron beam in a transmission electron microscopy device. The method includes: generating an electron pulse [306] by a pulsed electron source [300], accelerating the electron pulse in a first resonant microwave cavity [302], passing the accelerated electron pulse through a drift space [314], and correcting the energy spread of the accelerated electron pulse in a second resonant microwave cavity [304] by operating it out of phase by 90 degrees from the first resonant cavity [302].

An apparatus for performing charged particle spectroscopy, comprising: A source, for producing a pulsed beam of charged particles that propagate along a beam path; A specimen holder, for holding a specimen at an irradiation position in said beam path; A detector arrangement, for performing energy-differentiated detection of charged particles that traverse said specimen,
wherein, between said source and said detector arrangement, said beam path successively traverses: An energizing cavity, for applying a time-dependent accelerating field to said beam; A primary drift space; Said irradiation position; A temporal focusing cavity, for converting an energy differential in said beam into a time-of-flight differential; A secondary drift space.

An apparatus for performing charged particle spectroscopy, comprising: A source, for producing a pulsed beam of charged particles that propagate along a beam path; A specimen holder, for holding a specimen at an irradiation position in said beam path; A detector arrangement, for performing energy-differentiated detection of charged particles that traverse said specimen,
wherein, between said source and said detector arrangement, said beam path successively traverses: An energizing cavity, for applying a time-dependent accelerating field to said beam; A primary drift space; Said irradiation position; A temporal focusing cavity, for converting an energy differential in said beam into a time-of-flight differential; A secondary drift space.

A method of time-resolved pump-probe electron microscopy, comprises the steps of irradiating a sample (1) with a photonic pump pulse (2) being directed on a pump pulse path (3) from a photonic source to the sample (1), irradiating the sample (1) with an electron probe pulse (4) being directed on an electron pulse path (5) from an electron pulse source (10) to the sample (1), wherein the photonic pump pulse (2) and the electron probe pulse (4) arrive at the sample (1) with a predetermined temporal relationship relative to each other, and detecting a sample response to the electron probe pulse (4) irradiation with a detector device (20), wherein the photonic source comprises a photonic lattice structure (30) being arranged adjacent to the electron pulse path (5), and the photonic pump pulse (2) is created by an interaction of the electron probe pulse (4) with the photonic lattice structure (30). Furthermore, an electron microscopy apparatus, configured for time-resolved pump-probe electron microscopy, and a sample supply device (200) for an electron microscopy apparatus (100) are described.

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 mountwhich correspond to the peripheral areas of a specimenso 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.

A tomographic atom probe includes an analysis chamber intended to analyze a sample of material in the form of a nanotip mounted on an anti-vibration support, the nanotip being brought to a temperature of between 0 kelvin and ambient temperature, the nanotip being biased at an adjustable voltage of between 1 kV and 15 kV, the analysis chamber comprising a position-sensitive and time of flight-sensitive ion detector. The atom probe comprises a generator for generating high-peak-intensity single-cycle ultrashort terahertz pulses, the analysis chamber comprising optical means for focusing the terahertz pulses, the focusing of the terahertz pulses causing the atoms of the nanotip to evaporate through the field effect without thermal effects. The terahertz pulses are generated by a femtosecond pulsed laser emitting very high-power ultrashort optical pulses at a high rate.