Radiant energy – Inspection of solids or liquids by charged particles – Electron probe type
Reexamination Certificate
2002-06-27
2004-08-10
Lee, John R. (Department: 2881)
Radiant energy
Inspection of solids or liquids by charged particles
Electron probe type
C250S307000
Reexamination Certificate
active
06774363
ABSTRACT:
BACKGROUND OF THE INVENTION
The present invention relates to a charged particle beam technique for irradiating a sample with a charged particle beam, to observe, analyze, and process the sample.
An apparatus for a charged particle beam for irradiating a sample with a charged particle beam and observing, analyzing, and processing the sample is widely used. In the case where a sample contains an insulating material, when the surface of the sample is scanned with a charged particle beam, the surface of the sample may be charged. The charging disturbs observation, analysis, and processing due to drift of an emitted beam and decrease in a discharge amount of secondary particles. Consequently, a method of preventing the charging is important.
Conventional charging preventing methods include a method of preventing charging by irradiating the surface of a sample with a charged particle beam, a method of making charges escape by forming a conductive layer on the surface of a sample by irradiation of an ultraviolet ray or charged particle beam, a method of making charges escape by covering the surface of a sample with a conductive film, and a method of making charges escape by using conductive foil, conductive paste or a conduction terminal.
As a method of preventing charging by irradiation of a charged particle beam, there is, as prior art
1
, “charged particle beam processing apparatus and method (Japanese Patent Application Laid-Open (JP-A) No. 8-138617)”. The prior art
1
discloses an apparatus and method for detecting secondary electrons from the surface of a sample without extracting electrons emitted from an electron gun for preventing charging by a secondary electron detector by disposing the nozzle-shaped tip of the electron gun near the surface of the sample at the time of preventing charging of the sample with an ion beam, by using an electron beam.
The method of making charges escape by forming a conductive layer on the surface of a sample by irradiation with an ultraviolet ray or charged particle beam includes, as prior art
2
, “secondary electron image detecting method and apparatus, and processing method and apparatus using focusing charged particle beam (JP-A-11-154479)” and “charged particle beam processing apparatus and method (JP-A-8-138617)”. The prior art
2
discloses an apparatus and method realizing processing of 1.0 &mgr;m or less in such a manner that charging is stably avoided irrespective of the state and kind of a sample, a secondary electron image of the sample is detected at high resolution in a real time manner, and observation of the pattern of the sample, positioning of the focused charged particle beam, and the like are realized with high accuracy by the method of inducing a conductive layer and making charges escape by irradiating a region including a focused charged particle beam irradiation region on the surface of a sample with a positive ion beam.
As the method of covering the surface of a sample with a conductive film, there is, as prior art
3
, “method of manufacturing conductive resist film and semiconductor device (JP-A-7-74076)”. The prior art
3
discloses a method of suppressing charging as much as possible by a method of forming a conductive film under a resin film which is sensitive to charged particles and a method of exposing a pattern with high accuracy while reducing a charged particle beam curved irradiation phenomenon.
The method of making charges escape by a conductive terminal includes, as prior art
4
, “sample charging eliminating apparatus (JP-A-2000-173525)”. The prior art
4
discloses an apparatus preventing hindrances to observation, analysis, and processing due to a charging phenomenon and realizing a high-sensitivity, high-resolution, and high-precision work by making charges generated during the process of observation, analysis, and processing escape via an earth line by allowing a terminal to come into contact with the periphery of at least 180 degrees of an observation, analysis, and processing region by a remote control.
The method of capturing charges by a conductive probe includes, as prior art
5
, “micropattern measuring apparatus (JP-A-7-94562)”. The prior art
5
discloses a micropattern measuring apparatus which prevents a charge-up phenomenon in such a manner that negative charges generated by an electron beam are captured either by directly contact of a probe with a micropattern or by applying a positive voltage of 5000V to a probe from a position apart from the micropattern by 30 &mgr;m.
According to the prior arts, by the method of covering the surface of a sample with a conductive substance or making a conductive substance come into contact with the surface of a sample, the method of irradiating the surface of a sample with a charged particle beam, or the like, charging which occurs at the time of irradiating the sample with a charged particle beam is eliminated.
According to the charging preventing methods of the prior arts
1
and
2
, if the irradiation amount of an electron or ion beam used for preventing charging does not coincide with that of the charged particle beam used for observation, analysis, and processing, charging occurs. In this case, to improve resolution of an observed image by improving the precision of an irradiation position of a charged particle beam and to improve contrast of an observation image by increase in an emission amount of secondary electrons generated by irradiation of the charged particle beam, the irradiation amount of an electron or ion beam has to be controlled by means for detecting a charging preventing condition by using a reference. Further, control of the irradiation amount by the charging preventing condition detecting means requires experience of the operator.
Further, secondary electrons emitted by irradiation with an electron or ion beam are detected by a secondary electron detector. At this time, the secondary electrons overlap with secondary electrons emitted from the surface of a sample irradiated with the charged particle beam, so that the secondary electrons emitted by the irradiation of the electron or ion beam deteriorate an observation image very much. In order to suppress an emission amount of the secondary electrons emitted by the irradiation of the electron or ion beam, the irradiation amount has to be regulated. When a charging amount of the surface of a sample is large, the charging preventing method by irradiation of an electron or ion beam is not effective.
Generally, secondary electrons generated by the irradiation of a charged particle beam are emitted 10 to 100 times as much as secondary ions. Consequently, the resolution of an observation image based on a secondary electron signal is higher than that of an observation image based on secondary ions. However, in the case of emitting an electron or ion beam in order to prevent charging, due to generation of secondary electrons, the resolution of an observation image based on the secondary electron signals deteriorates more than that of an observation image based on secondary ions. Therefore, in the apparatus for a charged particle beam, a secondary ion detector is widely used.
In the charging preventing method of the prior art
3
, a coating with a conductive layer is formed on the surface of a sample. When the surface of a sample is covered, however, the structure of the surface cannot be observed with a charged particle beam, and a problem occurs in determination of a position of observation, analysis, and processing with a charged particle beam. Further, in order to avoid contamination of a sample, the charging preventing film formed on the surface of the sample has to be removed after observation, analysis, and processing with the charged particle beam.
According to the method of making charges escape by the conductive terminal disclosed in the prior art
4
, the terminal has to be made come into contact with the periphery of at least 180 degrees of the region of observation, analysis, and processing by a remote control. By making the terminal come into contact with the periphery of a
Fukuda Muneyuki
Shichi Hiroyasu
Tomimatsu Satoshi
Gill Erin-Michael
Hitachi , Ltd.
Lee John R.
Mattingly Stanger & Malur, P.C.
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