A sample may be inspected by making particles traverse the sample. The particles that have traversed the sample hit a detector one-by-one. In response thereto, the detector provides a sequence of respective detection outputs. The sequence of respective detection outputs is processed so as to identify respective locations where respective incident particles have hit the detector. An image is generated on the basis of the respective locations that have been identified. In order to determine a location where an incident particle has hit the detector, an evaluation is made with regard to pre-established respective associations between, on the one hand, respective locations where incident particles have hit the detector and, on the other hand, respective detection outputs.

A charged particle beam device for imaging and/or inspecting a sample is described. The charged particle beam device includes a beam emitter for emitting a primary charged particle beam; a retarding field device for retarding the primary beam before impinging on the sample, the retarding field device including an objective lens and a proxy electrode; and a first detector for off-axial backscattered particles between the proxy electrode and the objective lens. The charged particle beam device is adapted for guiding the primary beam along an optical axis to the sample for releasing signal particles. The proxy electrode includes one opening allowing a passage of the primary charged particle beam and of the signal particles, wherein the one opening is sized to allow a passage of charged particles backscattered from the sample at angles from 0° to 20° or above relative to the optical axis. Further, a method for imaging and/or inspecting a sample with a charged particle beam device is described.

A charged particle beam apparatus includes: an electromagnetic wave generation source 16 that generates an electromagnetic wave with which a sample is irradiated; a charged particle optical system that includes a pulsing mechanism 3 and irradiates the sample with a focused charged particle beam; a detector 10 that detects an emitted electron emitted by an interaction between the charged particle beam and the sample; a first irradiation control unit 15 that controls the electromagnetic wave generation source and irradiates the sample with a pulsed electromagnetic wave to generate an excited carrier; a second irradiation control unit 14 that controls the pulsing mechanism and irradiates an electromagnetic wave irradiation region of the sample with a pulsed charged particle beam; and a timing control unit 13. While the emitted electrons are detected by the detector in synchronization with irradiation of the pulsed charged particle beam, the timing control unit controls the first irradiation control unit and the second irradiation control unit, and controls an interval time between the pulsed electromagnetic wave and the pulsed charged particle beam to the electromagnetic wave irradiation region. As a result, based on a transient change in an electron emission amount, it is possible to detect sample information with nano spatial resolution.

A charged particle beam device for imaging and/or inspecting a sample is described. The charged particle beam device includes a beam emitter for emitting a primary charged particle beam, the charged particle beam device adapted for guiding the primary charged particle beam along an optical axis to the sample for releasing signal particles; a retarding field device for retarding the primary charged particle beam before impinging on the sample, the retarding field device including an objective lens and a proxy electrode, wherein the proxy electrode includes an opening allowing a passage of the primary charged particle beam and of the signal particles; a first detector for off-axial backscattered particles between the proxy electrode and the objective lens; and a pre-amplifier for amplifying a signal of the first detector, wherein the pre-amplifier is at least one of (i) integrated with the first detector, (ii) arranged adjacent to the first detector inside a vacuum housing of the charged particle beam device, and (iii) fixedly mounted in a vacuum chamber of the charged particle beam device. Further, a method for imaging and/or inspecting a sample with a charged particle beam device is described.

Disclosed herein is an inspection tool and a method for identifying defects in a sample. The method includes steps of scanning a first area of a sample with a first detector-beam and scanning a second area of the sample with a second detector-beam, then receiving first and second signals that are derived from the first and second detector-beams. The first and second signals are compared to determine whether a defect is present in the sample.

A charged particle beam apparatus for inspecting a sample is provided. The apparatus includes a pixelized electron detector to receive signal electrons generated in response to an incidence of an emitted charged particle beam onto the sample. The pixelized electron detector includes multiple pixels arranged in a grid pattern. The multiple pixels may be configured to generate multiple detection signals, wherein each detection signal corresponds to the signal electrons received by a corresponding pixel of the pixelized electron detector. The apparatus further includes a controller includes circuitry configured to determine a topographical characteristic of a structure within the sample based on the detection signals generated by the multiple pixels, and identifying a defect within the sample based on the topographical characteristic of the structure of the sample.

The disclosure relates to a method of imaging a specimen using a transmission charged particle microscope, said method comprising providing a specimen, and providing a charged particle beam and directing said charged particle beam onto said specimen for generating a flux of charged particles transmitted through the specimen. The method comprises the step of generating and recording a first energy filtered flux of charged particles transmitted through the specimen, wherein said first energy filtered flux of charged particles substantially consists of non-scattered and elastically scattered charged particles. The method as disclosed herein comprises the further step of generating and recording a second energy filtered flux of charged particles transmitted through the specimen, wherein said second energy filtered flux of charged particles substantially consists of inelastically scattered charged particles. Said first and second recorded energy filtered flux are then used for imaging said specimen with increased contrast.

The present invention overcomes a trade-off between throughput, SNR, and spatial resolution in a charged particle beam device. Accordingly, a computer 18 sets at least one of a charged particle optical system and a detection system so as to modulate the intensity of signal charged particles or an electromagnetic wave detected by a detector 12 at a prescribed frequency. The charged particle optical system scans a specimen with a charged particle beam. The computer 18 generates an image or a signal profile by associating an irradiation position of the charged particle beam with a DC component of a signal acquired through synchronous detection of a detection signal from the detector at the irradiation position with a reference signal having a prescribed frequency.

Capacitive sensors and capacitive sensing data integration for plasma chamber condition monitoring are described. In an example, a plasma chamber monitoring system includes a plurality of capacitive sensors, a capacitance digital converter, and an applied process server coupled to the capacitance digital converter, the applied process server including a system software. The capacitance digital converter includes an isolation interface coupled to the plurality of capacitive sensors, a power supply coupled to the isolation interface, a field-programmable gate-array firmware coupled to the isolation interface, and an application-specific integrated circuit coupled to the field-programmable gate-array firmware.

To correct a difference in signal intensity due to a difference in hardware, for example, temporal deterioration of the hardware in the same device, or a difference in signal intensity between different devices. An adjustment method according to the disclosure specifies an amplification gain with which the same detection signal intensity as that of a comparison target is obtained by comparing correspondence relationships between the detection signal intensity and the amplification gain at different time points in the same charged particle beam device or among different charged particle beam devices.