A pulsed generator of electrically charged particles includes a vacuum chamber; wherein the vacuum chamber is configured to maintain an internal operating pressure between 10-6 mbar and atmospheric pressure; the vacuum chamber is configured to accommodate a photocathode and an anode, the photocathode and the anode being separated by an adjustable distance less than or equal to 30 mm; the vacuum chamber includes a window enabling pulsed light to reach firstly a rear face of the photocathode; the anode is arranged downstream of the photocathode and has an orifice suitable for the passage of electrically charged particles; the generator of electrically charged particles includes a system to apply a difference in potential between the photocathode and the anode, the voltage being configured to accelerate the charged particles.

A pulsed generator of electrically charged particles includes a vacuum chamber; wherein the vacuum chamber is configured to maintain an internal operating pressure between 10-6 mbar and atmospheric pressure; the vacuum chamber is configured to accommodate a photocathode and an anode, the photocathode and the anode being separated by an adjustable distance less than or equal to 30 mm; the vacuum chamber includes a window enabling pulsed light to reach firstly a rear face of the photocathode; the anode is arranged downstream of the photocathode and has an orifice suitable for the passage of electrically charged particles; the generator of electrically charged particles includes a system to apply a difference in potential between the photocathode and the anode, the voltage being configured to accelerate the charged particles.

The present disclosure is related to a Schottky thermal field (TFE) source for emitting an electron beam. Electron optics can adjust a shape of the electron beam before the electron beam impacts a scintillator screen. Thereafter, the scintillator screen generates an emission image in the form of light. An emission image can be adjusted and captured by a camera sensor in a camera at a desired magnification to create a final image of the Schottky TFE source's tip. The final image can be displayed and analyzed to for defects.

The present disclosure is related to a Schottky thermal field (TFE) source for emitting an electron beam. Electron optics can adjust a shape of the electron beam before the electron beam impacts a scintillator screen. Thereafter, the scintillator screen generates an emission image in the form of light. An emission image can be adjusted and captured by a camera sensor in a camera at a desired magnification to create a final image of the Schottky TFE source's tip. The final image can be displayed and analyzed to for defects.

Multiple electron beamlets are split from a single electron beam. The electron beam passes through an acceleration tube, a beam-limiting aperture, an anode disposed between an electron beam source and the acceleration tube, a focusing lens downstream from the beam-limiting aperture, and a micro aperture array downstream from the acceleration tube. The micro aperture array generates beamlets from the electron beam. The electron beam can be focused from a divergent illumination beam into a telecentric illumination beam.

Multiple electron beamlets are split from a single electron beam. The electron beam passes through an acceleration tube, a beam-limiting aperture, an anode disposed between an electron beam source and the acceleration tube, a focusing lens downstream from the beam-limiting aperture, and a micro aperture array downstream from the acceleration tube. The micro aperture array generates beamlets from the electron beam. The electron beam can be focused from a divergent illumination beam into a telecentric illumination beam.

The invention is to simplify operations performed when imaging an electron diffraction pattern by using a transmission electron microscope. As a solution to the problem, a transmission electron microscope includes a detector to which an electron diffraction pattern is projected, a mask for zero-order wave configured to be inserted into and pulled out from between a sample and the detector, and a current detector configured to be inserted into and pulled out from a detection region of the zero-order waves in a state where the mask is inserted. An amount of current of electron beams emitted to the mask is measured in real time, and the measurement result is automatically reflected in settings of imaging conditions of an imaging camera provided in the transmission electron microscope.

The invention is to simplify operations performed when imaging an electron diffraction pattern by using a transmission electron microscope. As a solution to the problem, a transmission electron microscope includes a detector to which an electron diffraction pattern is projected, a mask for zero-order wave configured to be inserted into and pulled out from between a sample and the detector, and a current detector configured to be inserted into and pulled out from a detection region of the zero-order waves in a state where the mask is inserted. An amount of current of electron beams emitted to the mask is measured in real time, and the measurement result is automatically reflected in settings of imaging conditions of an imaging camera provided in the transmission electron microscope.

An object is to provide an electron gun that makes it possible to verify whether or not an electron beam emitted form a photocathode is misaligned from a designed emission center axis. The object can be achieved by an electron gun including: a light source; a photocathode; and an anode. The electron gun includes an intermediate electrode arranged between the photocathode and the anode, an electron beam shielding member configured to block a part of an electron beam, a measurement unit configured to measure an intensity of an electron beam blocked by the electron beam shielding member, and an electron beam emission direction deflector arranged between the anode and the electron beam shielding member and configured to change a position where an electron beam that passed through the anode reaches the electron beam shielding member. The intermediate electrode has an electron beam passage hole and a drift space.

Presented systems and methods facilitate efficient and effective monitoring of particle beams. In some embodiments, a radiation gun system comprises: a particle beam gun that generates a particle beam, and a gun control component that controls the gun particle beam generation characteristics, including particle beam fidelity characteristics. The particle beam characteristics can be compatible with FLASH radiation therapy. Resolution control of the particle beam generation can enable dose delivery at an intra-pulse level and micro-bunch level. The micro-bunch can include individual bunches per each 3 GHz RF cycle within the 5 to 15 μsec pulse-width. The FLASH radiation therapy dose delivery can have a bunch level resolution of approximately 4.4×10{circumflex over ( )}-6 cGy/bunch.