Abstract:
A charged particle apparatus includes: a charged particle source unit; a blanking electrode unit that blanks a charged particle beam launched from the charged particle source unit; a deflecting electrode unit that deflects the charged particle beam launched from the charged particle source unit and passing through the blanking electrode unit; an objective lens unit that converges the charged particle beam deflected by the deflecting electrode unit and radiates the charged particle beam to a surface of a sample; a secondary charged particle detection unit that detects a secondary charged particle generated from the sample irradiated with the charged particle beam; a signal processing unit that processes a signal obtained by detecting the secondary charged particle by the secondary charged particle detection unit; and a control unit that controls the entire apparatus. The control unit includes a transient signal correction unit that corrects a transient signal when the blanking of the charged particle beam is turned off by the blanking electrode. Thus, an image with no distortion can be obtained even when the blanking electrode is operated to turn on and off at a high speed and it is possible to perform measurement or inspection of a minute pattern with high precision.
Abstract:
To provide a charged particle beam apparatus capable of obtaining an image with high contrast and high visibility, the apparatus has: a charged particle optical system; a detection part to detect secondary charged particles generated from the sample; an image formation part to receive a detection signal from the detection part and form an image of the sample; an image processing part to process the image formed with the image formation part; and a display part to display the result of processing with the image processing part, wherein the image formation part has a pulse-count signal processing part to generate cumulative histogram information on a pulse signal component in the detection signal, set a threshold value for pulse signal detection using information on the generated cumulative histogram, and output a detection signal having a value higher than the set threshold value as a pulse signal.
Abstract:
A charged-particle beam system comprises: a charged-particle beam device containing a detection unit for detecting electrons generated by irradiating a sample with a charged-particle beam released from a charged particle source; and a signal detection unit in which a detection signal from the detection unit is input through a wiring. The signal detection unit comprises: a separation unit for separating into a rising signal and a falling signal the detection signal from the detection unit; a falling signal processing unit for at least eliminating ringing in the falling signal; and a combination unit generating and delivering a combined signal produced by combining the rising signal, which has been separated by the separation unit, with the falling signal wherefrom the ringing has been eliminated by the falling signal processing unit.
Abstract:
The scanning charged particle beam microscope according to the present application is characterized in that, in acquiring an image of the FOV (field of view), interspaced beam irradiation points are set, and then, a deflector is controlled so that a charged particle beam scan is performed faster when the charged particle beam irradiates a position on the sample between each of the irradiation points than when the charged particle beam irradiates a position on the sample corresponding to each of the irradiation points (a position on the sample corresponding to each pixel detecting a signal). This allows the effects from a micro-domain electrification occurring within the FOV to be mitigated or controlled.
Abstract:
In an image forming method of charged particle beam apparatus for scanning a sample by irradiating the sample with a converged charged particle beam and detecting secondary charged particles generated from the sample by a detection unit, receiving and processing an output signal from the detection unit, and receiving the processed signal and forming an image of the sample, receiving and processing the output signal are performed by analogically processing the output signal and by performing pulse-count processing on the output signal, and pulse-count processing is performed by removing a ringing pulse in the output signal and counting pulses in the signal from which the ringing pulse has been removed.
Abstract:
A processing apparatus and a processing method are provided, which use a charged particle beam device that achieves defection of secondary electrons/reflected electrons at a large angle and cancels out noises of an electromagnetic deflector and an electrostatic deflector to suppress a position shift of a primary electron beam caused by circuit noises of a primary beam/secondary beam separation circuit. In the charged particle beam device that includes an electronic optical system radiating a concentrated electron beam onto a sample placed on a stage to perform scanning and captures an image of the sample, a reference signal and a signal generation unit of a voltage-source control signal applied to the electrostatic deflector generating the electrostatic deflector and a reference signal and a signal generation unit of a current-source control signal applied to the electromagnetic deflector generating a magnetic field are made common in an overlapping-electromagnetic-deflector control unit that controls a path of the secondary electrons/reflected electrons incident on a detector, and frequency characteristics and phase characteristics of the voltage control signal are coincident with those of the current-source control signal.
Abstract:
The scanning charged particle beam microscope according to the present invention is characterized in that, in acquiring an image of the FOV (field of view), interspaced beam irradiation points are set, and then, a deflector is controlled so that a charged particle beam scan is performed faster when the charged particle beam irradiates a position on the sample between each of the irradiation points than when the charged particle beam irradiates a position on the sample corresponding to each of the irradiation points (a position on the sample corresponding to each pixel detecting a signal). This allows the effects from a micro-domain electrification occurring within the FOV to be mitigated or controlled.
Abstract:
The present invention relates to a measurement and inspection device of a scanning-type electron beam system, and provides a technique for achieving a measuring/inspecting process with high precision in accordance with a scanning speed. A secondary electron signal detection system in the present measurement and inspection device is suitably applicable to a scanning control with a plurality of scanning speeds, and the device is provided with a detector 107 for detecting a secondary electron signal (SE) derived from an irradiation onto a sample 110 with an electron beam by a scanning control process, a preamplifier 30 for current-to-voltage converting and pre-amplifying the output, an analog signal processing and amplifying unit 51 to which the output of the preamplifier 30 is inputted to carry out an analog processing and amplifying process thereon as a secondary electron signal detection unit 50, an ADC 52 for analog-to-digital converting the output thereof, and an image processing unit 205 for generating an image for use in measurements or inspections based upon the output. A control unit 210 carries out a switching control of respective units including an LPF (12) inside the analog signal processing and amplifying unit 51, in accordance with a scanning speed or the like.
Abstract:
Technique capable of achieving shortening of settling time, which is caused by ringing, etc. of a blanking control signal is provided. A measuring/inspecting apparatus is configured to have a main blanking unit and a correction blanking control unit as a high-speed switching control unit of an electron beam. During the period of switching of a main blanking control signal from ON to OFF, a correction blanking control signal is applied in real time in synchronization with the switching. The ringing, etc. caused by the main blanking are corrected so as to be cancelled out by that, the settling time is shortened as a result.
Abstract:
Provided is a charged particle beam device to enable determination of a noise source of a charged particle beam device that can cause a noise frequency component superimposed on a measurement image. The charged particle beam device includes a unit that extracts information regarding a noise source. The unit that extracts information regarding a noise source includes: a control signal monitoring unit that observes a control signal of a control unit which controls an electron optical system of the charged particle beam device and outputs the observed signal; a first frequency conversion processing unit that executes frequency conversion processing on the signal output from the control signal monitoring unit; a second frequency conversion processing unit that executes frequency conversion processing on an image signal output from a detector of the electron optical system; and a frequency analysis and comparison processing unit that receives an output signal of the first frequency conversion processing unit and an image signal of the second frequency conversion processing unit, and associates a peak frequency of a superimposed noise of the image signal with a noise source of the control unit which generates a noise having a peak frequency corresponding to the peak frequency of the superimposed noise within the image signal.