A method of using a Charged Particle Microscope, comprising: A specimen holder, for holding a specimen; A source, for producing an irradiating beam of charged particles; An illuminator, for directing said beam so as to irradiate the specimen; A detector, for detecting a flux of emergent radiation emanating from the specimen in response to said irradiation,
additionally comprising the following steps: In said illuminator, providing an aperture plate comprising an array of apertures; Using a deflecting device to scan said beam across said array, thereby alternatingly interrupting and transmitting the beam so as to produce a train of beam pulses; Irradiating said specimen with said train of pulses, and using said detector to perform positionally resolved (temporally discriminated) detection of the attendant emergent radiation.

Systems and methods for implementing a detector array are disclosed. According to certain embodiments, a substrate comprises a plurality of sensing elements including a first element and a second element. The detector comprises a switching element configured to connect the first element and the second element. The switching region may be controlled based on signals generated in response to the sensing elements receiving electrons with a predetermined amount of energy.

A multi-beam scanning electron microscope (charged particle beam device) 100 includes an electron gun (charged particle irradiation source) 101 configured to irradiate a sample 104 with an electron beam (charged particle beam) 103, a detector 106 having a detection region corresponding to the charged particle beam 103 and configured to output an electrical signal 107 corresponding to a reaching position when secondary particles 105 generated from the sample 104 by irradiating the sample 104 with the charged particle beam 103 reach the detection region, and a signal processing block 115 configured to perform measurement of a charge amount of the sample 104 by the charged particle beam 103 and generation of an inspection image of the sample 104 in parallel based on the electrical signal 107 output from the detector 106.

Charged particle beam systems and methods, such as a multi beam charged particle beam system and related methods, can compensate sample charging.

A method for calibration including determining a temperature induced offset in a pedestal of a process module under a temperature condition for a process. The method includes delivering a wafer to the pedestal of the process module by a robot, and detecting an entry offset. The method includes rotating the wafer over the pedestal by an angle. The method includes removing the wafer from the pedestal by the robot and measuring an exit offset. The method includes determining a magnitude and direction of the temperature induced offset using the entry offset and exit offset.

A scanning electron microscope incorporates a multi-pixel solid-state electron detector. The multi-pixel solid-state detector may detect back-scattered and/or secondary electrons. The multi-pixel solid-state detector may incorporate analog-to-digital converters and other circuits. The multi-pixel solid state detector may be capable of approximately determining the energy of incident electrons and/or may contain circuits for processing or analyzing the electron signals. The multi-pixel solid state detector is suitable for high-speed operation such as at a speed of about 100 MHz or higher. The scanning electron microscope may be used for reviewing, inspecting or measuring a sample such as unpatterned semiconductor wafer, a patterned semiconductor wafer, a reticle or a photomask. A method of reviewing or inspecting a sample is also described.

The present disclosure relates to an apparatus and methods for generating a hybrid image by high-dynamic-range counting. In an embodiment, the apparatus includes a processing circuitry configured to acquire an image from a pixelated detector, obtain a sparsity map of the acquired image, the sparsity map indicating low-flux regions of the acquired image and high-flux regions of the acquired image, generate a low-flux image and a high-flux image based on the sparsity map, perform event analysis of the acquired image based on the low-flux image and the high-flux image, the event analysis including detecting, within the low-flux image, incident events by an event counting mode, multiply, by a normalization constant, resulting intensities of the high-flux image and the detected incident events of the low-flux image, and generate the hybrid image by merging the low-flux image and the high-flux image.

An electron detector comprises a sensor module comprising a sensor for detecting electrons, and an electronics module comprising circuitry for processing signals received from the sensor module. Wiring is provided for electrically connecting the sensor module to the electronics module. An adaptor is arranged between the sensor module and the electronics module. The adaptor comprises a passage for the wiring, and shielding elements for shielding from radiation.

According to one aspect of the present invention, a multi-beam image acquisition apparatus, includes: an objective lens configured to image multiple primary electron beams on a substrate by using the multiple primary electron beams; a separator configured to have two or more electrodes for forming an electric field and two or more magnetic poles for forming a magnetic field and configured to separate multiple secondary electron beams emitted due to the substrate being irradiated with the multiple primary electron beams from trajectories of the multiple primary electron beams by the electric field and the magnetic field formed; a deflector configured to deflect the multiple secondary electron beams separated; a lens arranged between the objective lens and the deflector and configured to image the multiple secondary electron beams at a deflection point of the deflector; and a detector configured to detect the deflected multiple secondary electron beams.

A multi-beam apparatus for observing a sample with high resolution and high throughput and in flexibly varying observing conditions is proposed. The apparatus uses a movable collimating lens to flexibly vary the currents of the plural probe spots without influencing the intervals thereof, a new source-conversion unit to form the plural images of the single electron source and compensate off-axis aberrations of the plural probe spots with respect to observing conditions, and a pre-beamlet-forming means to reduce the strong Coulomb effect due to the primary-electron beam.