Abstract:
To provide a scanning electron microscope having an electron spectroscopy system to attain high spatial resolution and a high secondary electron detection rate under the condition that energy of primary electrons is low, the scanning electron microscope includes: an objective lens 105; primary electron acceleration means 104 that accelerates primary electrons 102; primary electron deceleration means 109 that decelerates the primary electrons and irradiates them to a sample 106; a secondary electron deflector 103 that deflects secondary electrons 110 from the sample to the outside of an optical axis of the primary electrons; a spectroscope 111 that disperses secondary electrons; and a controller that controls application voltage to the objective lens, the primary electron acceleration means and the primary electron deceleration means so as to converge the secondary electrons to an entrance of the spectroscope.
Abstract:
An aberration corrector includes a mirror that corrects an aberration of a charged particle beam, a beam separator, and a bypass optical system in the beam separator. The beam separator includes an entrance of the charged particle beam and an exit from which the charged particle beam is emitted to an objective lens, and separates an incident trajectory from the entrance to the mirror and a reflection trajectory from the mirror to the exit from each other by deflecting the charged particle beam in an ON state. The bypass optical system is disposed at a position at which the trajectory of the charged particle beam bypasses when the beam separator is in the ON state, and the trajectory of the charged particle beam passes when the beam separator is in an OFF state, and controls the charged particle beam so that objective lens optical conditions in a trajectory via the mirror and a trajectory passing through the bypass optical system coincide with each other.
Abstract:
A simulation device calculates a detection number of electrons generated by charged particles radiated to a sample by a simulation and generates a simulation image of the sample. The simulation device holds penetration length information (272) in which incidence conditions of the charged particles and a penetration length are associated with each other, sample configuration information (271) which shows a configuration of a sample, and emission electron number information in which the incidence conditions of the charged particles and an emission electron number are associated with each other. The simulation device calculates the number of electrons emitted from a predetermined incidence point, on the basis of incidence conditions at the predetermined incidence point, the penetration length information (272), the sample configuration information (271), and the emission electron number information.
Abstract:
In a semiconductor inspection method using a semiconductor inspection device, by selecting an incident energy and a negative potential and scanning an inspection surface of a wafer with primary electrons to detect secondary electrons, a first inspection image is acquired, and a macro defect, stacking faults, a basal plane dislocation and a threading dislocation contained in the first inspection image are discriminated by image processing based on a threshold value of a signal amount of the secondary electrons determined in advance. Moreover, by selecting the incident energy and a positive potential and scanning the inspection surface of the wafer with primary electrons to detect the secondary electrons, a second inspection image is acquired, and a threading screw dislocation of a dot-shaped figure contained in the second inspection image is discriminated by image processing based on a threshold value of a signal amount of the secondary electrons determined in advance.