Abstract:
Provided is a charged particle beam device that outputs both an ion beam and an electron beam at a sample, has a common detector for both the ion beam and the electron beam in the charged particle beam device that processes and observes the sample, and is able to provide a detection unit to an appropriate position corresponding to the process details and observation technique of the sample. Provided are an electron beam optical column in which an electron beam for observing the observation surface of a sample is generated, an ion beam optical column in which an ion beam that processes the sample is generated, a detection device that detects a secondary signal generated from the sample or transmitted electrons, and a sample stage that is capable of mounting the detection device thereon; is rotatable in a horizontal plane that includes the optical axis of the electron beam and the optical axis of the ion beam about a cross point where both optical axes intersect; and is able to change the distance between the observation surface of the sample and the cross point.

Description:
TECHNICAL FIELD 
     The present invention relates to a charged particle beam device used as a means for observing, analyzing, and evaluating an object to be observed and to a method for observing a sample using a charged particle beam. 
     BACKGROUND ART 
     Miniaturization of semiconductor devices of recent years is making progresses, and scanning electron microscopes (hereinafter abbreviated to SEMs), scanning transmission electron microscopes (hereinafter abbreviated to STEMs), transmission electron microscopes (hereinafter abbreviated to TEMs), and so on are used for analyses of defective portions in manufacturing steps. In order to observe a sample using a STEM or a TEM from among these, it is necessary that a portion of an object to be analyzed be cut out from a sample such as a semiconductor wafer or a semiconductor chip and be machined so thin that an electron beam can penetrate. A focused ion beam (hereinafter abbreviated to FIB) apparatus is used in this application. With the FIB a situation of machining can be observed by detecting and imaging a secondary signal such as secondary electrons generated from the sample by irradiating the sample with an ion beam; however, since the resolution is low and it is impossible to cope with recent miniaturization of subject samples, an apparatus equipped with both of an FIB column and an SEM column for a single sample chamber has been developed. This apparatus is hereinafter referred to as an FIB-SEM. Furthermore, in order to observe a sample of a thin leaf machined by an FIB apparatus using an STEM, an apparatus equipped with both of an FIB column and an STEM column has been developed. This apparatus is hereinafter referred to as an FIB-STEM. 
     In the above-described FIB-SEM and FIB-STEM, because their respective columns occupy large volumes, it is impossible to make their optical axes coaxial with each other. Accordingly, contrivances are made to place the sample at a position and an orientation appropriate relative to the respective optical axes. For example, a high-resolution image can be obtained by rotating the sample such that the machined surface of the sample is placed perpendicular to the optical axis of the SEM (for example, see Patent Literature 1). 
     CITATION LIST 
     Patent Literature 
     Patent Literature 1: JP-A-2002-150990 
     SUMMARY OF INVENTION 
     Technical Problem 
     In an electron microscope in which a sample is irradiated with a finely focused charged particle beam such as an electron beam and a secondary signal such as secondary electrons or transmitted electrons is detected with a detector, the amount of the secondary signal detected by the detector varies when the sample is tilted. Namely, there is an optimum position between the sample and the detector for acquiring intended information. For example, when an image of the bottom of a hole formed in a sample is acquired, where the position of the detector is fixed and only the sample is tilted, the direction of secondary electrons released from the bottom of the hole deviates from the direction of the detector because the side face of the hole in the sample is tilted at the same time. Furthermore, since in the case of an FIB-SEM or an FIB-STEM, machining of the sample and image formation are done at a cross point where the ion beam and the electron beam intersect with each other, the optical axis of the ion beam makes an angle to the optical axis of the electron beam; therefore, the position of the detector for acquiring an image when an ion beam is casted is not the same as the position of the detector for acquiring an image when an electron beam is casted and it is necessary that the detectors be installed at their respective optimum positions. 
     The present invention has an objective to provide a charged particle beam device performing machining and observation of a sample by irradiating the sample with both an ion beam and an electron beam in which a common detector is provided for both the ion beam and the electron beam and the detector can be installed at a position suitable according to the contents of machining of the sample and the observation methods. 
     Solution to Problem 
     To achieve the foregoing objective, an embodiment of the present invention is characterized by having: an electron beam optics column which generates an electron beam for observing an observed surface of a sample; an ion beam optics column which generates an ion beam to machine the sample; a detector which detects a secondary signal or transmitted electrons generated from the sample; and a sample stage on which the detector is mounted, which is capable of rotating with a cross point at which the optical axis of the electron beam and the optical axis of the ion beam intersect as a center and within a plane including both of the optical axes, and which is capable of varying a distance between the observed surface of the sample and the cross point. 
     Furthermore, an embodiment of the present invention is characterized by having: an electron beam optics column which generates an electron beam for observing an observed surface of a sample; an ion beam optics column which generates an ion beam to machine the sample; a first sample stage on which a minute specimen cut out from the sample by machining using the ion beam is mounted; and a second sample stage on which the sample from which the minute specimen is not yet cut out and a detector to detect transmitted electrons from the sample are mounted and which is capable of horizontal movement, vertical movement, and tilt. 
     Advantageous Effects of Invention 
     According to the present invention, it is possible to provide a charged particle beam device having a detector common for both an ion beam and an electron beam and which can be installed at a position suitable according to the contents of machining of a sample and observation methods. 
     Other objects, features, and advantages of the present invention will become apparent from the following description of the embodiments of the invention taken in conjunction with the accompanying drawings. 
    
    
     
       BRIEF DESCRIPTION OF DRAWINGS 
         FIG. 1  is a perspective view showing the internal structure of an FIB-STEM device; 
         FIG. 2  is a longitudinal cross section showing a schematic of the internal structure of an FIB-STEM device viewed from a side; 
         FIG. 3  is a longitudinal cross section showing a schematic of the internal structure of the FIB-STEM device viewed from a side; 
         FIG. 4  is a longitudinal cross section showing a schematic of the internal structure of the FIB-STEM device viewed from a side; 
         FIG. 5  is a longitudinal cross section showing a schematic of the internal structure of the FIB-STEM device viewed from a side; 
         FIG. 6  is a flowchart illustrating a procedure of mounting a second detector on a second stage; 
         FIG. 7  is a longitudinal cross section showing a schematic of the internal structure of the FIB-STEM device viewed from a side; 
         FIG. 8  is a longitudinal cross section showing a schematic of the internal structure of the FIB-STEM device viewed from a side; 
         FIG. 9  is a longitudinal cross section showing a schematic of the internal structure of the FIB-STEM device viewed from a side; 
         FIG. 10  is a longitudinal cross section showing a schematic of the internal structure of the FIB-STEM device viewed from a side; 
         FIG. 11A  is a side view where the portion of the electron beam optics system of  FIG. 10  is extracted; 
         FIG. 11B  is a side view where the portion of the electron beam optics system of  FIG. 10  is extracted; 
         FIG. 12  is a flowchart of movement processing of the second detector; 
         FIG. 13  is a perspective view showing the internal structure of an FIB-STEM device; 
         FIG. 14  is an enlarged perspective view of a second sample stage; 
         FIG. 15  is a perspective view showing the internal structure of the FIB-STEM device; 
         FIG. 16  is a perspective view showing the internal structure of the FIB-STEM device; 
         FIG. 17  is a perspective view showing the internal structure of the FIB-STEM device; 
         FIG. 18  is a perspective view showing the internal structure of the FIB-STEM device; 
         FIG. 19  is a perspective view showing the internal structure of the FIB-STEM device; 
         FIG. 20  is a perspective view showing the internal structure of the FIB-STEM device; 
         FIG. 21  is a perspective view showing the internal structure of the FIB-STEM device; 
         FIG. 22  is a perspective view showing the internal structure of the FIB-STEM device; 
         FIG. 23  is a perspective view showing the internal structure of the FIB-STEM device; 
         FIG. 24  is a flowchart describing a sequence of operations until a thin-film sample to which a bulk sample is thinned down is observed with an STEM. 
     
    
    
     DESCRIPTION OF EMBODIMENTS 
     Embodiments of the present invention are hereinafter described with reference to the drawings. 
     Embodiment 1 
     A first embodiment is described.  FIG. 1  is a perspective view showing the internal structure of an FIB-STEM device. It has a structure in which a column for irradiating a sample with an ion beam, a column for irradiating it with an electron beam, a detector for detecting secondary electrons generated at the sample, and a detector for detecting transmitted electrons transmitted through the sample are provided. 
     In  FIG. 1 , it has an ion beam optics system  2  for irradiating a sample  1  with an ion beam, an electron beam optics system  3  for irradiating the sample  1  with an electron beam, a first sample stage  6  having a sample holder on which the sample  1  is mounted, a second sample stage  7  on which the sample  1  and detectors can be mounted, a first detector  9  for detecting secondary electrons or the like emitted from the sample  1  by irradiation of the ion beam or the electron beam, a second detector  8  attachable/detachable to the second sample stage  7 , a probe driving mechanism  11  for driving a probe  10  used when the sample  1  is taken out after being machined, a deposition gas source  4  for supplying a gas for ion-beam-assisted deposition, a transport mechanism  12  for transporting the sample  1 , the second detector  8 , or the like into a sample chamber  5  of the device, and a central control-and-display unit, which is not shown, for controlling these instruments. 
     The first sample stage  6  contains a not-shown sample holder on which the sample  1  is mounted. The sample holder has an area on which the sample  1  is directly mounted or a mesh area in which a mesh is arranged, on which the sample  1  of a thin piece is mounted. The sample holder may have both an area on which the sample  1  is directly mounted and a mesh area in which a mesh having the thin piece mounted thereon is arranged. Further, the first sample stage  6  is capable of planar movement, tilt movement, and rotation of the sample  1  so that it can cause a certain location of the sample  1  move into a position of ion beam irradiation or an observation position of the electron beam. Since the first sample stage  6  can move with high accuracy and is highly vibration-resistant, it is often used for observations of high accuracy. 
     The second sample stage  7  can have the sample  1  and the second detector  8  mounted thereon and is capable of planar movement and, tilt movement and movement in the height direction with the cross point of the ion beam and the electron beam as the center. Furthermore, the second detector  8  can be arranged in a prescribed position. The second sample stage  7  has the feature that a large sample such as a semiconductor wafer can be mounted thereon. 
     The second detector  8  can be attached to and detached from the second sample stage  7 , and secondary electrons, secondary ions, backscattered electrons, X-rays, reflected electrons, transmitted electrons, or the like are objects to be detected, which are generated from the sample  1 , the probe  10 , or the like due to irradiation of an ion beam or an electron beam. 
     The central control-and-display unit can process signals from the first detector  9  and the second detector  8 , image them, and display them on a not-illustrated display unit. Furthermore, it can control the ion beam optics system  2 , the electron beam optics system  3 , the first sample stage  6 , the second sample stage  7 , the first detector  9 , the second detector  8 , the probe driving mechanism  11 , the deposition gas source  4 , the transport mechanism  12 , and so on, respectively. 
       FIGS. 2-5  are longitudinal cross sections showing schematics of the internal structure of an FIB-STEM device viewed from a side.  FIG. 6  is a flowchart illustrating a procedure of mounting the second detector  8  on the second stage  7 . The following procedure is carried out by a processor of the central control-and-display unit, which is not shown, executing a preset control program. In  FIG. 2 , in the state where a gate between the sample chamber  5  and the transport mechanism  12  is closed, a gate of the atmospheric side of the transport mechanism  12  is opened and the second detector  8  is introduced into the transport mechanism  12  (S 101 ). Then, the gate of the atmospheric side of the transport mechanism  12  is closed and the inside of the transport mechanism  12  is evacuated to the same degree of vacuum as the inside of the sample chamber  5  (S 102 ). Next, as shown in  FIG. 3 , the gate between the transport mechanism  12  and the sample chamber  5  is opened (S 104 ) and the second detector  8  is introduced into the sample chamber  5  by a transport arm  13  of the transport mechanism  12  (S 105 ). At this time, in order to make the moving distance of the transport arm  13  short, the second sample stage  7  may be brought close to the transport mechanism  12  (S 103 ). And, as shown in  FIG. 4 , the transport arm  13  pushes a connector  20  into a plug part of a connector  21  provided on the second sample stage  7 . When the second detector  8  is pushed in, the connector  20  provided to the second detector  8  and the connector  21  provided to the second sample stage  7  are connected together so that, the second detector  8  becomes ready to use as shown in  FIG. 5 . 
     Mounting the second detector  8  on the second sample stage  7  is detected by a sensor  22  (S 106 ). Where the second detector  8  cannot be detected by the sensor  22 , upon verifying whether the transport mechanism  12 , the second detector  8 , and the second sample stage  7  have no abnormalities (S 107 ), it returns to S 101  and the second detector  8  is again set to the transport mechanism  12 . Where the second detector  8  can be detected by the sensor  22 , the central control-and-display unit confirms the completion of setting of the second detector  8  to the second sample stage  7  (S 108 ), the transport arm  13  detaches the second detector  8  from itself and moves back to the transport mechanism  12  as shown in  FIG. 5 , and the gate between the transport mechanism  12  and the sample chamber  5  is closed (S 109 ). With this method, the second detector  8  can be introduced to the inside of the device without opening the sample chamber  5  to the atmosphere. 
     When the second detector  8  is taken out of the device, the reversed procedure is carried out. Also, this method can be implemented similarly in the case of a sample as well as in the case of the detector. When the sample  1  is mounted on the second sample stage  7 , observation, machining, or the like of the sample  1  can be carried out using the first detector  9  fixed in the sample chamber  5  shown in  FIG. 1 . Incidentally, a procedure may also be gone through consisting of taking the second sample stage  7  per se out of the sample chamber  5  and returning it into the sample chamber  5  after attaching the sample  1  and the second detector  8  to the second sample stage  7 . In this case, the transport mechanism  12  having a size permitting the second sample stage  7  to be taken in and out is prepared. 
       FIGS. 7-10  are longitudinal cross sections showing schematics of the internal structure of the FIB-STEM device viewed from a side.  FIG. 7  shows the position of the second sample stage  7  when an image acquired by the second detector  8  while irradiating with an electron beam  30  during machining of the sample  1  using an ion beam  40  is observed. The second detector  8  is so positioned that the optical axis of the electron beam optics system  3  and the principal axis  31  of the second detector  8  are in line symmetry with respect to the optical axis of the ion beam optics system  2 . Assuming that the second sample stage  7  on which the second detector  8  is disposed can be rotated around the cross point at which the optical axis of the electron beam optics system  3  and the optical axis of the ion beam optics system  2  intersect with each other as the center and within a plane including both the optical axes, the sample  1  can be tilted to any arbitrary position. Furthermore, the distance between the observed surface of the sample  1  and the cross point can be varied. In this way, the tilt and the distance of the sample  1  can be adjusted and, therefore, the location where the second detector  8  is placed may be selected to be a location where a secondary signal such as reflected electrons released from the sample  1  is detected strong. In addition, an adjustment is made with the first sample stage  6  such that the observed surface of the sample  1  faces the direction of the ion beam optics system  2 . 
     The electron beam  30  emitted from the electron beam optics system  3  impinges on the sample  1  and is scanned, and a secondary signal such as secondary electrons is detected by the second detector  8 . Since observations can be made without directing the sample surface of the sample  1  toward the direction of the electron beam optics system  3  during machining with the ion beam  40 , the throughput of machining with the ion beam  40  can be improved. 
       FIG. 8  shows the arrangement of the second sample stage  7  when the sample  1  is machined into a thin film and the end point of the machining is detected. The position of the sample  1  is adjusted by the first sample stage  6  (not shown) so that the machined surface of the sample  1  becomes parallel to the optical axis of the ion beam optics system  2  and the sample  1  is scraped down to a thin film from right to left in the figure by the ion beam  40 . The second sample stage  7  is rotated as indicated by the two-dot chain line with respect to the embodiment shown in  FIG. 7  and the second detector  8  is arranged at a lower right of the figure, namely in such a way that the optical axis of the electron beam optics system  3  and the principal axis  31  of the second detector  8  are in line symmetry about the line normal to the machined surface of the sample  1 . Since the second sample stage  7  on which the second detector  8  is disposed is adjustable in rotation within the plane of the paper of the figure and in a distance with respect to the sample  1 , the arrangement location of the second detector  8  may be selected at a location where a secondary signal such as reflected electrons released from the sample  1  is detected strong. 
     The electron beam  30  emitted from the electron beam optics system  3  is made to impinge on the sample  1  and scanned, and a secondary signal is detected by the second detector  8 . The observed surface of the sample  1  can be observed with the electron beam optics system  3  while the sample  1  is being made into a thin film by the ion beam  40  emitted from the ion beam optics system  2 ; detection of the end point of the machining with the ion beam  40  can be carried out with high accuracy. 
       FIG. 9  shows the arrangement of the second detector  8  in a case where a secondary signal generated from the sample  1  by irradiating the sample  1  with the ion beam  40  is detected so that the situation of the machining with the ion beam  40  is imaged and observed. Observation using the ion beam  40  is referred to as SIM (Scanning Ion Beam Microscope) observation. SIM observation is convenient because machining can be made to proceed while verifying the situation of machining of the sample  1 ; however, images with an ion beam are lower in resolution than images with an electron beam and applications using SIM observation are limited. The first sample stage  6  is adjusted so that the observed surface of the sample  1  faces the electron beam optics system  3  and it is arranged so that the optical axis of the ion beam optics system  2  and the principal axis  41  of the second detector  8  are in line symmetry about the line normal to the observed surface of the sample  1 . 
     The ion beam  40  emitted from the ion beam optics system  2  is made to impinge on the sample  1  and scanned, and a secondary signal is detected by the second detector  8 . This arrangement is suitable for SIM observation during machining of the sample with an ion beam. The second sample stage  7  on which the second detector  8  is disposed is adjustable in rotation within the plane of the paper of the figure and in the distance with respect to the sample  1 . 
       FIG. 10  is a longitudinal cross section showing a schematic of the internal structure of the FIB-STEM device viewed from a side. The first sample stage  6  is so adjusted that the observed surface of the sample  1  faces the electron beam optics system  3 , the second sample stage  7  is so adjusted that the second detector  8  faces the electron beam optics system  3 , and the sample  1  and the second detector  8  are arranged on the optical axis of the electron beam  30  of the electron beam optics system  3 . Transmitted electrons  51  transmitted through the sample  1  are detected by the second detector  8  so that STEM observation of the sample  1  can be performed. Because the second sample stage  7  on which the second detector  8  is disposed can adjust rotation within the plane of the plane of the figure and the distance with respect to the sample  1 , the arrangement location of the second detector  8  may be selected at a location where transmitted electrons transmitted through the sample  1  are detected strong. 
       FIGS. 11A and 11B  are side views where the portion of the electron beam optics system  3  of  FIG. 10  is extracted. The electron beam  30  emitted from the electron beam optics system  3  is made to impinge on the sample  1  and scanned, and transmitted electrons are detected by the second detector  8 . The transmitted electrons are classified into bright-field transmitted electrons  52  transmitted without being scattered or diffracted within the sample  1  and dark-field transmitted electrons  53  transmitted while undergoing scattering or diffraction within the sample  1 . Within the second detector  8 , the bright-field transmitted electrons  52  are detected by a bright-field detection portion  54  and the dark-field transmitted electrons  53  are detected by a dark-field detection portion  55 . The distance between the second detector  8  and the sample  1  can be varied by moving the second sample stage  7  up and down.  FIG. 11A  shows a case where the distance between the second detector  8  and the sample  1  is short, and  FIG. 11B  shows a case where the distance between the second detector  8  and the sample  1  is long; it can be seen that the detection angle of scattered electrons of the dark-field transmitted electrons  53  changes when the distance between the sample  1  and the second detector  8  is varied. Z-contrast observation can be carried out by bringing the second detector  8  mounted on the second sample stage  7  closer to the sample  1  so as to increase the detection angle of the scattered electrons. 
       FIG. 12  is a flowchart of movement processing of the second detector  8 . The flow from setting the sample  1  on the first sample stage  6  to a start of an observation is explained. First, the sample  1  is set on the first sample stage  6  (S 201 ). Then, an optics system used for the observation is selected (S 202 ). Then, the angle of the observed surface of the sample  1  is set using the first sample stage  6  (S 203 ). Then, the second detector  8  is moved into an optimum position using the second sample stage  7  based on the used optics system and information on the angle of the observed surface of the sample  1  (S 204 ). 
     Since in the above-described Embodiment the position of the second detector  8  can be varied with the sample  1  as the center and the height can be varied, the optimum position for signal detection which is determined according to the attitude and the shape of the sample  1  can be adjusted and, further, detection of a desired signal such as secondary electrons, secondary ions, or transmitted electrons can be selectively acquired. 
     While the ion beam optics system  2  is arranged vertically and the electron beam optics system  3  is arranged obliquely in Embodiment 1 , the ion beam optics system  2  may be arranged obliquely and the electron beam optics system  3  may be arranged vertically. Moreover, both of the ion beam optics system  2  and the electron beam optics system  3  may be arranged obliquely. Additionally, a structure of a triple-beam optics system comprising a gallium ion beam optics system, a gas ion beam optics system, and an electron beam optics system may be adopted. 
     Embodiment 2 
     A second embodiment is described. 
       FIG. 13  is a perspective view showing the internal structure of an FIB-STEM device. Embodiment 2 is similar in the fundamental structure to Embodiment 1; the sample  1  can be mounted on the second sample stage  7  in addition to the second detector  8 . 
       FIG. 14  is an enlarged perspective view of the second sample stage  7  and the sample  1  is mounted on a rotary stage that turns independently. 
       FIGS. 15-23  are perspective views showing the internal structure of the FIB-STEM device. Furthermore,  FIG. 24  is a flowchart describing a sequence of operations until a thin-film sample  73  to which a bulk sample  71  is thinned down is observed with an STEM. 
     First, in  FIG. 15 , the bulk sample  71  and the second detector  8  are mounted on the second sample stage  7  within the device using the transport mechanism  12 . Then, as shown in  FIG. 16 , the second sample stage  7  is moved in such a way that the bulk sample  71  is brought into the position of the cross point of the optical axis of the ion beam optics system  2  and the optical axis of the electron beam optics system  3  (S 301 ). Next, the bulk sample  71  is cut out with an ion beam  60  emitted from the ion beam optics system  2  as shown in  FIG. 17  (S 302 ), and a minute specimen  72  in the bulk sample  71  and the probe  10  are made to adhere to each other using the ion beam  60  and a deposition gas  61  as shown in  FIG. 18  (S 303 ). Then, as shown in  FIG. 19 , the junction portion between the bulk sample  71  and the minute specimen  72  is cut off (S 304 ), and the minute specimen  72  is taken out of the bulk sample  71  and transported to the sample holder of the first sample stage  6  using the probe  10  and the probe driving mechanism  11  (S 305 ). Next, as shown in  FIG. 20 , the second sample stage  7  is retracted, the sample holder of the first sample stage  6  is moved to the cross point of the two optical axes, and the minute specimen  72  is mounted onto an area of the sample holder of the first sample stage  6  where a sample is directly mounted or onto a mesh on a mesh area using the ion beam  60 , the deposition gas  61 , and the probe  10  (S 306 ). Then, as shown in  FIG. 21 , the second detector  8  is moved into a position where a situation of thinning down of the minute specimen  72  can be observed with the SEM in order to carry out an end-point detection with the accuracy of the FIB machining when the minute specimen  72  is thinned down into a thin film with the ion beam (S 307 ). Next, as shown in  FIG. 22 , the minute specimen  72  on the first sample stage  6  is thinned down using the ion beam  60  (S 308 ). Then, as shown in  FIG. 23 , in order to perform STEM observation of the thin-film sample  73 , which has been thinned down, the position of the first sample stage  6  is so adjusted that the observed surface of the thin-film sample  73  faces the electron beam optics system  3  (S 309 ), and the second sample stage  7  is so adjusted that the second detector  8  is on the optical axis of the electron beam optics system  3  and faces the electron beam optics system  3  (S 310 ). Then, the electron beam  62  emitted from the electron beam optics system  3  is made to impinge on the thin-film sample  73  and scanned, and generated transmitted electrons  65  are detected by the second detector  8  (S 311 ). 
     In the above-described Embodiment 2 , the minute specimen  72  and the probe  10  are made to adhere to each other, and the sample  1  and the minute specimen  72  are separated at the end using the ion beam. The probe  10  may be made to adhere to the minute specimen  72  after a specific portion of the sample  1  is cut out so that the minute specimen  72  cut out from the sample  1  is completely separated. 
     Furthermore, in Embodiment 2 , it is not necessary to take in and out the sample and the second detector from the preparation of the sample until the STEM observation and, therefore, a time period until observation can be reduced. Furthermore, since no stage dedicated for the detector is needed, there is an advantage that the sample chamber can be made small in size. Because of reduction in size of the sample chamber, the time to evacuate the inside of the sample chamber can be reduced and the time from startup of the device to observation can also be reduced. Additionally, because no stage dedicated for the detector is needed, the manufacturing cost can be reduced. Also, since attaching/detaching of the second detector to the second sample stage is easy, periodic maintenance of the second detector is easy; further, because movement of the second detector can be accomplished by moving the second sample stage, no extra moving mechanism for the second detector is required, and the number of parts to be replaced is reduced, leading to an improvement of the maintainability. 
     While embodiments of the present invention have been described concretely so far, the invention is not limited to the above embodiments; those skilled in the art would easily appreciate that various changes and modifications are possible within the scope of the invention set forth in the claims. 
     REFERENCE SIGNS LIST 
       1 : sample 
       2 : ion beam optics system 
       3 : electron beam optics system 
       4 : deposition gas source 
       5 : sample chamber 
       6 : first sample stage 
       7 : second sample stage 
       8 : second detector 
       9 : first detector 
       10 : probe 
       11 : probe driving mechanism 
       12 : transport mechanism 
       13 : transport arm 
       20 ,  21 : connectors 
       22 : sensor 
       30 ,  62 : electron beams 
       31 ,  41 : principal axes 
       40 ,  60 : ion beams 
       51 ,  65 : transmitted electrons 
       52 : bright-field transmitted electrons 
       53 : dark-field transmitted electrons 
       54 : bright-field detection portion 
       55 : dark-field detection portion 
       61 : deposition gas 
       71 : bulk sample 
       72 : minute specimen 
       73 : thin-film sample