U.S. patent number 3,628,014 [Application Number 04/887,693] was granted by the patent office on 1971-12-14 for scanning electron microscope with color display means.
This patent grant is currently assigned to The Boeing Company. Invention is credited to Lee R. Grubic, Jr..
| United States Patent |
3,628,014 |
| Grubic, Jr. |
December 14, 1971 |
SCANNING ELECTRON MICROSCOPE WITH COLOR DISPLAY MEANS
Abstract
A scanning electron microscope and system wherein small surface
potential differences are rendered visible as color shifts on a
color CRT (cathode-ray tube) display device. A plurality of
different surface potentials are detected respectively by
scintillation detectors which are coupled to photomultipliers and
then amplifiers. The amplifier output signals representative of
several different means surface potentials at scanned points of the
specimen are coupled respectively to the three signal control grids
of a color CRT in the case of a three scintillating detector-three
channel system and the color combinations of the primary colors
displayed are indicative of surface potentials in between the mean
potentials thus making small differences of the specimen surface
potential readily discernible to the eye as small color shifts.
|
Inventors: |
Grubic, Jr.; Lee R. (Seattle,
WA) |
|
Assignee: |
The Boeing Company (Seattle,
WA)
|
| Family
ID: |
25391661 |
| Appl.
No.: |
04/887,693 |
| Filed: |
December 22, 1969 |
| Current U.S.
Class: |
250/310; 348/34;
250/305; 348/80; 324/754.22 |
| Current CPC
Class: |
H01J
37/22 (20130101); H01J 37/244 (20130101); H01J
37/28 (20130101); H01J 37/266 (20130101); H01J
2237/225 (20130101) |
| Current International
Class: |
H01J
37/22 (20060101); H01J 37/28 (20060101); H01J
37/26 (20060101); H01j 037/28 (); H01j
037/22 () |
| Field of
Search: |
;250/49.5A,49.5E,49.5PE
;178/6.8,DIG.1,5.4R |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Birch; Anthony L.
Claims
What I claim is:
1. In a scanning electron microscope:
beam generating means for emitting a primary electron beam,
support means for supporting a specimen,
at least one focusing electron lens of the magnetic type positioned
between said beam generating means and said support means for
focusing the primary electron beam on the specimen,
first deflecting means positioned between said beam generating
means and said focusing means for deflecting the primary electron
beam to scan the specimen,
first detector means for detecting secondary electrons having a
first constant energy which are emitted from the portion of the
specimen struck by the primary electron beam,
second detector means for detecting secondary electrons having a
second constant energy greater than said first constant energy
which are emitted from the portion of the specimen struck by the
primary electron beam,
a color cathode-ray tube having first and second color control
grids for modulating the intensities of first and second scanning
electron beams in response to the output signals of said first and
second detector means respectively, and
second deflecting means for simultaneously deflecting the first and
second scanning electron beams in the color cathode-ray tube in
synchronous relation with the scanning operation of the primary
electron beam.
2. A scanning electron microscope comprising electron beam
generating means for generating and directing a beam of primary
electrons along a beam path towards a specimen, means for mounting
said specimen, means for focusing said electron beam into a spot on
said specimen, means for raster scanning said focused electron spot
over the surface of said specimen, means for detecting secondary
electrons at different discrete energy levels thereof, a color
cathode-ray tube, and means for coupling the output of said means
for detecting secondary electrons to said color cathode-ray tube
whereby the display intensities of the primary colors thereof are
responsive respectively to the outputs of said detecting means at
said different discrete energy levels thereof.
3. The apparatus of claim 2 wherein said means for detecting
secondary electrons at discrete energy levels comprises a plurality
of photomultiplier-coupled scintillation detectors mounted adjacent
said specimen in position to detect secondary electrons at said
different discrete energy levels.
Description
This invention relates to improvements in scanning electron
microscopes and more particularly to a scanning electron microscope
which is capable of providing a color display derived from
variations in surface potential.
The conventional scanning electron microscope system utilizes a
collector electrode having a slit therein through which pass
secondary electrons emitted from the bombarded point on the
specimen having a certain constant energy. These secondary
electrons are then accelerated to hit a scintillation detector, and
a signal whose amplitude is proportional to the number of electrons
having passed through the slit is detected by a photomultiplier.
This signal is then supplied through an amplifier to a grid of a
cathode-ray tube for effecting modulation of the brightness of the
CRT. Meanwhile, the output of a scanning power source is
simultaneously supplied to the deflecting plates of the scanning
electron microscope, and to the deflecting plates of the cathode
ray tube. By this simultaneous supply of scanning power, a
secondary electron image of the specimen can be observed on the
fluorescent screen of the cathode-ray tube.
Presently, technicians utilizing the above conventional scanning
electron microscope observe the surface characteristics of the
specimen as conveyed by display of surface potential scanning of
the specimen in the form of a black and white picture or display as
seen on the face of the CRT. The single collector of the
above-described conventional SEM (scanning electron microscope)
apparatus is moved to a second position for receiving secondary
electrons having a different constant energy and the greys in the
first and second black and white pictures obtained at the first and
second collector locations are compared.
The above state of the art method for surface potential studies of
the surfaces of specimens makes small differences in surface
potential very difficult to detect by comparisons of greys in two
or more black and white pictures.
It is therefore a primary object of the present invention to
provide a scanning electron microscope system having increased
sensitivity to surface potential and providing easier visualization
thereof.
It is another object of the present invention to provide a scanning
electron microscope apparatus in which means are provided for
developing a multicolor display on a color cathode-ray tube in
which small differences of surface potential are displayed as small
color shifts in the display.
It is yet another object of the present invention to provide a
scanning electron microscope having a plurality of detection
systems in which the information derived is coupled to a single
display device for the processing thereof.
Other objects, features, and, advantages of the present invention
will become apparent as the detailed description proceeds.
According to one embodiment of the present invention the electron
microscope system comprises means for emitting a primary electron
beam and means for focusing the electrons into a spot on a
specimen. A common scanning power source is provided for
simultaneous scanning of the primary electron beam in the electron
microscope and the plural electron beams in a color cathode-ray
tube. A plurality of slit-shaped collector electrodes are
positioned to receive deflected secondary electrons through the
slits thereof having a corresponding plurality of different
constant energy levels. A scintillation detector is positioned
behind each of the slits and coupled to a photomultiplier which
provides a signal which is then amplified and supplied to the
signal control grids of a color CRT. In accordance with a preferred
embodiment, three channels are provided each including a collector
electrode having a slit, a scintillation detector, a
photomultiplier and amplifier means, the first collector electrode
and slit being positioned to receive secondary electrons having a
first constant energy level and the output signal of the
corresponding amplifier in the first channel is coupled to the
signal control grid of the red gun in the color CRT. The second
collector electrode and slit of the second channel is positioned to
receive secondary electrons having a second constant energy level
higher than said first constant energy level, the output signal
from the amplifier in the second channel being coupled to the
signal control grid of the green electron gun in the color CRT,
while the slit of the third collector electrode in the third
channel is positioned to receive secondary electrons having a third
constant energy level higher than said second constant energy level
and the output signal from the amplifier of the third channel
corresponds to the blue color signal of a color CRT and is coupled
to drive the signal control grid of the blue electron gun of the
color CRT.
More complete understanding of the invention will best be obtained
from consideration of the accompanying description and drawings in
which:
FIG. 1 is a diagrammatic view showing the structure of a prior form
of scanning electron microscope;
FIG. 2 is a diagrammatic view of a scanning electron microscope
structure and apparatus for displaying surface potentials of a
specimen on a color cathode-ray tube in accordance with an
embodiment of the invention;
FIG. 3 is a diagrammatic view of a scanning electron microscope
structure and system for recording and displaying in color
simultaneously surface potentials of a scanned specimen in
accordance with a further embodiment of the invention.
FIG. 1 is illustrative of a prior art scanning electron microscope
and display arrangement as described in FIG. 1 of U.S. Pat. No.
3,474,245 to Kimura et al., which may be referred to for further
detail and explanation thereof.
Briefly, the scanning electron microscope of FIG. 1 includes
electron beam emission means consisting of a cathode 1 in the form
of a hairpin-shaped tungsten filament, a grid 2 generally called
the Wehnelt cylinder, and an anode 3. A voltage of 20 to 30
kilovolts is applied across the anode 3 and the cathode 1, and an
electron beam 4 emitted from the heated tungsten filament is
focused on a specimen 7 to be observed by means of two condenser
lenses 5 and 6. The specimen 7 is placed on a specimen stage 8 and
the speciment position is adjustable in both horizontal and axial
directions. The electron beam 4 is deflected by two pairs of
deflecting plates 9 so as to scan the specimen surface
longitudinally and laterally thereof. When the specimen surface is
bombarded by the primary electron beam 4, a secondary electron beam
10 is emitted from the bombarded point and the amount of the
secondary electrons is variable depending on the material of that
particular bombarded point and the incident angle of the primary
electron beam 4. This secondary electron beam 10 generally has an
energy of less than 50 electron volts. A mesh 11 having a control
aperture for the passage therethrough of the incident beam is
disposed opposite the specimen 7 and is kept at a negative
potential of from several to several tens of volts so that the
secondary electron beam 10 is deflected in a manner as shown and
only those secondary electrons having a certain constant energy are
passed through the slit 12 in collector electrode 12a. These
secondary electrons are then accelerated to hit against a
scintillator 13, and a signal whose amplitude is proportional to
the number of electrons having passed through the slit 12 is
detected by the photomultiplier 14. This signal is then supplied
through an amplifier 15 to grid 17 of the cathode-ray tube 16 for
effecting modulation of the brightness of the tube 16. Meanwhile,
the output of the scanning power source is simultaneously supplied
to the deflecting plates 9 of the scanning electron microscope
column, and to deflecting plates 19 of the cathode-ray tube 16. By
this simultaneous supply of scanning power, a secondary electron
image of the specimen 7 can be observed on the fluorescent screen
of the cathode-ray tube 16.
Turning now to FIG. 2 wherein the same numerals represent parts
corresponding to those of the SEM of FIG. 1 it will be observed
that the output display device of the system is a color cathode-ray
tube 16a rather than a black and white picture tube 16 as shown in
the prior art system of FIG. 1. An electromagnetic deflection coil
19a is shown for purposes of simultaneously deflecting the
plurality of electron beams of the tube 16a and causing them to
scan a raster on the faceplate of tube 16a. In FIG. 2, there are
three collector electrodes 23a, 24a, and 25a each having a
corresponding slit 23, 24, and 25. Slit 23 in collector electrode
23a comprises the input to the secondary electron detection system
of the first channel. Secondary electrons in secondary electron
beam 33 having the lowest certain constant energy are deflected by
the field formed in the region of the beam along a curved path in
the manner shown and received by scintillator 13a after passage
through slit 23. Coupled to scintillator 13a is photomultiplier 14a
which provides an output signal whose amplitude is proportional to
the number of electrons having passed through the slit 23. This
signal is then supplied through an amplifier 15a to feed the red
signal control grid 17a. Secondary electrons in secondary electron
beam 34 which have a certain constant energy higher than the
secondary electrons of beam 33 are deflected further in the field
formed in the beam deflection region along a curved path and pass
through slit 24 in collector electrode 24a and are then detected by
scintillator 13b coupled to photomultiplier 14b, the output of
scintillation detection 13b and photomultiplier 14b then being fed
to amplifier 15b and the amplified signal being the green color
signal supplied to drive green signal control grid 17b at the
output of the second channel between the SEM and color cathode-ray
tube 16a. The third channel input is provided by collector
electrode 25a which receives through slit 25 therein secondary
electrons in secondary electron beam which have a constant energy
level higher than the secondary electrons of beam 34 and which are
consequently deflected further through the deflection field between
the specimen 7 and collector electrode 25a. These secondary
electrons which reach and pass through slit 25 strike scintillator
13c which is coupled to photomultiplier 14c. The output of
scintillation detector 13c and photomultiplier 14c is then
amplified in amplifier 15c and the amplifier output in the third
channel is coupled to signal control grid 17c. While the several
collector electrodes 23a, 24a, and 25a are shown spaced
successively further away from the specimen and parallel to mesh 11
which is kept at a negative potential of several to several tens of
volts to provide the deflection of secondary electron beams 33, 34,
and 35 as shown, it should be recognized that other deflecting
fields and electrode geometry, as for example as is shown in the
embodiment of FIG. 3, may be utilized to provide detection of
secondary electron beams at selected energy levels to furnish the
three inputs to the three channels shown. While a three-color CRT
coupled to the three channel outputs is shown, it should be
recognized that a two-color display device at the output of two
channels using two collectors at the input of the channels may be
utilized to provide a two-color display of surface potentials of a
scanned specimen. A penetration-type color CRT of known type may be
utilized as the output display device in a two-channel arrangement
of the system.
A further embodiment of the invention is shown now in FIG. 3. The
collector structure of this embodiment differs from that of FIG. 2
in that instead of separate collectors 23a, 24a, and 25a
insulatively separated from each other there is included in FIG. 3
a single collector plate 26 having corresponding slits 23, 24, and
25 therein. Thus the individual collectors of the three channels
are seen to be maintained at the same potential because of the
integral collector plate 26 common to the three channel inputs.
Light pipes 43, 44, and 45 are coupled between scintillators 13a,
13b, and 13c and photomultipliers 14a, 14b, and 14c, respectively.
This manner of light transmission from scintillators to
photomultipliers in each channel permits close positioning of
scintillators behind closely spaced slits 23, 24, and 25 in
collector plate 26. Photomultipliers 14a, 14b, and 14c are thus not
required to be mounted directly behind and in the limited space
available to the rear of scintillator buttons 13a, 13b, and 13c. It
should be noted that collector plate 26 having a plurality of slits
23, 24, and 25 is positioned at right angles to mesh 11 and also
parallel to the primary electron beam 4 for collecting deflected
secondary electron beams 23, 24, and 25. Recording means 75 is
shown coupled to record the third channel output signal obtained
through switching means 76 shown in the third channel position
making connection to terminal 79 for sensing the output of
amplifier 15c. In the same manner, the output signals representing
scanned surface potentials derived in the second and first channels
may be recorded when switch 76 is connected respectively to
terminals 78 and 77. Alternatively, plural channel recording means
may be coupled to output terminals 77, 78, and 79 when it is
desired to analyze and compare the three channel output voltages
available at output terminals 77, 78 and 79 to obtain more exact
surface potential variations than can be observed visually on the
screen of color CRT 16a. Small differences of surface potential are
displayed as small color shifts. The measurement of potentials in
between those primarily measured by each collector and the ability
to see small potential differences as color shifts are possible
because of the Gaussian distribution of electron trajectories for
any one surface potential. Other color combinations than those in
the embodiments shown wherein the highest surface potentials show
up as blue and the lowest potentials as red may be utilized to
provide the display.
* * * * *