A scanning electron microscope device for a sample to be detected and an electron beam inspection apparatus are provided, the scanning electron microscope device being configured to project electron beam to a surface of the sample to generate backscattered electrons and secondary electrons, and comprising: an electron beam source, a deflection mechanism, and an objective lens assembly. The deflection mechanism comprises a first deflector located downstream the electron beam source and a second deflector located downstream the first deflector. The objective lens assembly comprises: an excitation coil; and a magnetic yoke, formed by a magnetizer material as a housing which opens towards the sample and comprising a hollow body defining an internal chamber where the excitation coil is accommodated, and at least one inclined portion extending inward from the hollow body at an angle with reference to the hollow body and directing towards the optical axis, with an end of the at least one inclined portion being formed into a pole piece. The deflection mechanism further comprises a third deflector located between the second deflector and the objective lens assembly and disposed in an opening delimited and circumscribed by the pole piece, and each of the first deflector, the second deflector and the third deflector is an electrostatic deflector.

The present invention provides a charged particle beam apparatus capable of efficiently reducing the effect of a residual magnetic field when SEM observation is performed. The charged particle beam apparatus according to the present invention includes a first mode for passing a direct current to a second coil after turning off a first coil, and a second mode for passing an alternating current to the second coil after turning off the first coil.

A multiple particle beam system comprises a magnetic immersion lens and a detection system. A cross-over of the second individual particle beams is provided in the secondary path between the beam switch and the detection system, and a contrast aperture with a central cutout for cutting out the secondary beams is arranged in the region of the cross-over. A contrast correction lens system with a first magnetic contrast correction lens is arranged between the objective lens and the contrast aperture. The contrast correction lens system is configured to generate a magnetic field with an adjustable strength and correct beam tilts of the secondary beams in the cross-over in relation to the optical axis of the multiple particle beam system. It is possible to obtain a more uniform contrast for different individual images and the contrast can be improved overall.

A charged particle beam system can include a vacuum chamber, a specimen holder for holding a specimen within the vacuum chamber, and a charged particle column. The charged particle column can include a charged particle source for producing a beam of charged particles along an optical axis and a magnetic immersion lens for focusing the beam of charged particles. The magnetic immersion lens can include a first lens pole disposed adjacent a first surface of the specimen, an excitation coil surrounding the first lens pole, and a counterpole disposed adjacent a second surface of the specimen, the counterpole including one or more magnets disposed on the counterpole.

An adjustable magnetic field free objective lens for a charged particle microscope is disclosed herein. An example charged particle microscope at least includes first and second optical elements arranged on opposing sides of a sample plane, a third optical element arranged around the sample plane, and a controller coupled to control the first, second and third optical elements. The controller coupled to excite the first and second optical elements to generate first and second magnetic lenses, the first and second magnetic lenses formed on opposing sides of the sample plane and oriented in the same direction, and excite the third optical element to generate a third magnetic lens at the sample plane that is oriented in an opposite direction, where a ratio of the excitation of the third optical element to the excitation of the first and second optical elements adjusts a magnetic field at the sample plane.

An adjustable magnetic field free objective lens for a charged particle microscope is disclosed herein. An example charged particle microscope at least includes first and second optical elements arranged on opposing sides of a sample plane, a third optical element arranged around the sample plane, and a controller coupled to control the first, second and third optical elements. The controller coupled to excite the first and second optical elements to generate first and second magnetic lenses, the first and second magnetic lenses formed on opposing sides of the sample plane and oriented in the same direction, and excite the third optical element to generate a third magnetic lens at the sample plane that is oriented in an opposite direction, where a ratio of the excitation of the third optical element to the excitation of the first and second optical elements adjusts a magnetic field at the sample plane.

The invention provides a charged particle beam device that prevents a leakage of an unnecessary magnetic field to a trajectory of a charged particle beam with which a sample is irradiated in a sample observation according to a boosting method. The charged particle beam device includes: a charged particle source configured to generate the charged particle beam with which the sample is irradiated; an object lens configured to generate the magnetic field for focusing the charged particle beam; and a boosting electrode that is provided inside the object lens and to which a voltage for accelerating the charged particle beam is applied. The boosting electrode is formed of a magnetic material.

A charged particle beam system can include a vacuum chamber, a specimen holder for holding a specimen within the vacuum chamber, and a charged particle column. The charged particle column can include a charged particle source for producing a beam of charged particles along an optical axis and a magnetic immersion lens for focusing the beam of charged particles. The magnetic immersion lens can include a first lens pole disposed adjacent a first surface of the specimen, an excitation coil surrounding the first lens pole, and a counterpole disposed adjacent a second surface of the specimen, the counterpole including one or more magnets disposed on the counterpole.

A particle beam system includes a multi-beam particle source for generating a multiplicity of charged individual particle beams, and a magnetic multi-deflector array for deflecting the individual particle beams in the azimuthal direction. The magnetic multi-deflector array includes a magnetically conductive multi-aperture plate having a multiplicity of openings, which is arranged in the beam path of the particle beams such that the individual particle beams substantially pass through the openings of the multi-aperture plate. The magnetic multi-deflector array also includes a magnetically conductive aperture plate having an individual opening. The aperture plate is arranged in the beam path of the particle beams such that the individual particle beams substantially pass through the first aperture plate. The multi-aperture plate and the first aperture plate are connected to each other such that a cavity is formed between the two plates. A first coil for generating a magnetic field is arranged in the cavity between the first aperture plate and the multi-aperture plate such that the multiplicity of individual particle beams substantially pass through the coil.

A scanning electron microscope with a composite detection system and a specimen detection method. The scanning electron microscope includes a composite objective lens system including an immersion magnetic lens and an electro lens, configured to focus an initial electron beam to a specimen to form a convergent beam spot; a composite detection system located in the composite objective lens system; and a detection signal amplification and analysis system. A magnetic field of the immersion magnetic lens is immersed in the specimen; the electro lens is configured to decelerate the initial electron beam and focus the initial electron beam onto the specimen, and separate BSEs from a transmission path of an X-ray; the composite detection system is located below an inner pole piece of the immersion magnetic lens, is located above the control electrode, and includes an annular BSE detector and an annular X-ray detector that have a same axis center.