A scanning electron microscope objective lens system is disclosed, which includes: a magnetic lens, a deflection device, a deflection control electrode, specimen to be observed, and a detection device; in which, The opening of the pole piece of the magnetic lens faces to the specimen; the deflection device is located in the magnetic lens, which includes at least one sub-deflector; the deflection control electrode is located between the detection device and the specimen, and the deflection control electrode is used to change the direction of the primary electron beam and the signal electrons generating from the specimen; the detection device comprises the first sub-detector for detecting the back-scattered electrons and the second sub-detector for detecting the second electrons. A specimen detection method is also disclosed.

An integrated transmission electron microscope comprising multiple electron sources for tuned beams of ultrafast, scanning probe, and parallel illumination in varied beam energies can be alternated within sub-microseconds onto a sample with dynamic ‘transient state’ processes to acquire atomic-scale structural/chemical data with site specificity. The various electron sources and condenser optics enable high-resolution imaging, high-temporal resolution imaging, and chemical imaging, using fast-switching magnets to direct the different electron beams onto a single maneuverable objective pole piece where the sample resides. Such multimodal in situ characterization tools housed in a single microscope have the potential to revolutionize materials science.

Provided is a scanning electron microscope which can perform high-speed focus correction even when an electron beam having high energy is used. The scanning electron microscope includes an electron optical system including an electron source 100 that emits an electron beam and an objective lens 113, a sample stage 1025 which is disposed on a stage 115 and on which a sample 114 is placed, a backscattered electron detector 1023 which is disposed between the objective lens and the sample stage and is configured to detect backscattered electrons 1017 emitted due to interaction between the electron beam and the sample, a backscattered electron detection system control unit 138 which is provided corresponding to the backscattered electron detector and is configured to apply a voltage to the backscattered electron detector, and a device control calculation device 146. The objective lens has an opening in a stage direction, and the device control calculation device performs focus correction of the electron beam by controlling the voltage applied to the backscattered electron detector from the backscattered electron detection system control unit.

A supply unit for driving an electrode of a charged particle beam column, the supply unit includes a first amplifier and a second amplifier that are configured to receive an input signal, an output of the first amplifier is coupled, via the first resistor, to a signal line of the coaxial cable, an output of the second amplifier is coupled, via the second resistor, to a main shield of the coaxial cable, one port of the first amplifier and one port of the second amplifier are coupled to a power supply return port. The signal line is configured to provide a first driving signal to an that is coupled between the signal line and the power supply return port.

A method for measuring an electron signal or an electron induced signal may be provided. The method may include providing a threshold number of events or a threshold event rate for a pixel on a detector. The method may include collecting from the detector the threshold number of events or determining that the threshold event rate is achieved, wherein a signal at the detector is an electron signal or an electron induced signal from a sample. The method may include modulating an intensity of an electron source directed to the sample in response.

A scanning electron microscope objective lens system is disclosed, which includes: a magnetic lens, a deflection device, a deflection control electrode, specimen to be observed, and a detection device; in which, The opening of the pole piece of the magnetic lens faces to the specimen; the deflection device is located in the magnetic lens, which includes at least one sub-deflector; the deflection control electrode is located between the detection device and the specimen, and the deflection control electrode is used to change the direction of the primary electron beam and the signal electrons generating from the specimen; the detection device comprises the first sub-detector for detecting the back-scattered electrons and the second sub-detector for detecting the second electrons. A specimen detection method is also disclosed.

The focused ion beam apparatus includes: an ion source configured to generate ions; a first electrostatic lens configured to accelerate and focus the ions to form an ion beam; a beam booster electrode configured to accelerate the ion beam to a higher level; one or a plurality of electrodes, which are placed in the beam booster electrode, and are configured to electrostatically deflect the ion beam; a second electrostatic lens, which is provided between the one or plurality of electrodes and a sample table, and is configured to focus the ion beam applied with a voltage; and a processing unit configured to obtain a measurement condition, and set at least one of voltages to be applied to the one or plurality of electrodes or a voltage to be applied to each of the first electrostatic lens and the second electrostatic lens, based on the obtained measurement condition.

An integrated transmission electron microscope comprising multiple electron sources for tuned beams of ultrafast, scanning probe, and parallel illumination in varied beam energies can be alternated within sub-microseconds onto a sample with dynamic transient state processes to acquire atomic-scale structural/chemical data with site specificity. The various electron sources and condenser optics enable high-resolution imaging, high-temporal resolution imaging, and chemical imaging, using fast-switching magnets to direct the different electron beams onto a single maneuverable objective pole piece where the sample resides. Such multimodal in situ characterization tools housed in a single microscope have the potential to revolutionize materials science.

A Wien filter and a charged particle beam imaging apparatus are provided. The Wien filter Wien filter, including a Wien filter body which includes: an electrostatic deflector, including at least one pair of electrodes, respective two electrodes in each pair of which are opposite to each other, each electrode including an electrode body constructed in an arc-shaped form, and respective electrode bodies of respective two electrodes in each pair of the at least one pair of electrodes being arranged concentrically with and opposite to each other in a diameter direction, and the at least one pair of electrodes being configured to generate respective electric fields by cooperation of the respective two electrodes in each pair of the at least one pair of electrodes, in the condition of respective bias voltages applied individually thereon; and a magnetic deflector, including at least one pair of magnetic poles, respective two magnetic poles in each pair of which are opposite to each other, each magnetic pole including a magnetic pole body constructed in an arc-shaped form, and respective magnetic pole bodies of respective two magnetic poles in each pair of the at least one pair of magnetic poles being arranged concentrically with and opposite to each other in the diameter direction, and the magnetic pole bodies of the at least one pair of magnetic poles in the magnetic deflector and the electrode bodies of the at least one pair of electrodes in the electrostatic deflector being arranged concentrically and spaced apart from each other in a circumferential direction, and the at least one pair of magnetic poles being configured to generate respective magnetic fields by cooperation of respective two magnetic poles in each pair of the at least one pair of magnetic poles; a resultant electric field formed collectively by all of the respective electric fields is perpendicular to a resultant magnetic field formed collectively by all of the respective magnetic fields; and each electrode is also provided with a respective first protrusion extending radially inwards from a radial inner side of the respective electrode body thereof, and each magnetic pole is also provided with a second protrusion extending radially inwards from a radial inner side of the respective magnetic pole body thereof.

A charged particle beam device includes a charged particle source which emits a charged particle beam radiated on a sample; a condenser lens system which has at least one condenser lens focusing the charged particle beam at a predetermined demagnification; a deflector which is positioned between a condenser lens of a most downstream side and a charged particle source in the condenser lens system, and moves a virtual position of the charged particle source; and a control unit which controls the deflector and the condenser lens system. The control unit controls the deflector to move the virtual position of the charged particle source to a position of suppressing a deviation, which is caused by a change of the demagnification of the condenser lens system, of a center trajectory of the charged particle beam downstream of the condenser lens system.