Radiant energy – With charged particle beam deflection or focussing – With detector
Reexamination Certificate
2001-03-21
2004-10-12
Lee, John R. (Department: 2881)
Radiant energy
With charged particle beam deflection or focussing
With detector
C250S488100, C250S486100, C250S487100
Reexamination Certificate
active
06803583
ABSTRACT:
BACKGROUND OF THE INVENTION
This invention relates to electron microscopes and more particularly to scintillators for electron microscopes and a method of making scintillators. General principles of electron microscopy, and particularly scanning electron microscopy (SEM), is explained in “Scanning Electron Microscopy”, by Postek, Howard, Johnson and McMichael, particularly pages 26, 27 and 28 (incorporated herein by reference). A beam of electrons is focussed onto a specimen producing a scattering of two types referred to as secondary and backscatterd electrons emitted outward from the specimen surface in all directions. These may be detected by a further known system as shown schematically in
FIG. 1
wherein the microscope column includes a collector
1
, scintillator
2
, light pipe (or guide)
3
and detector base
4
together with other components forming the detector assembly. Scintillator
2
is mounted on the end of light pipe
3
covered by collector
1
supported by small screws on detector base
4
so that the scintillator is within the specimen chamber
5
when detector base
4
is mounted on a wall thereof
6
such as shown schematically in FIG.
2
. This figure shows parts of the microscope that are positioned outside the specimen chamber, such as photomultiplier
7
(PMT) in case
8
mounted such as by PMT cover mount
9
on the side of detector base
4
opposite to that on which the detector assembly is mounted. A rubber light shield
10
may also be used as shown and a preamplifier case
11
is mounted at the outer end of the PMT. A collector voltage cable
12
extends through the detector base and is connected at its end
13
to collector
1
. A scintillator high tension cable
14
is similarly connected at its end
15
to a ring
15
around the scintillator so that when the cables are energized the collector is positively biased to draw electrons to the scintillator. The scintillator is a thin plastic disc coated with a special phosphor and also coated with aluminum which serves as a mirror to direct the photons toward the PMT
7
. The positive bias accelerates low energy secondary electrons toward the detector, but does not influence higher energy backscattered electrons. Electrons strike the scintillator and the phosphors thereon produce photons (small flashes of light), several photons being emitted, theoretically, for each incoming electron. The photons are transported through light pipe
3
from the evacuated microscope column. Light pipes are generally made of plexiglass or polished quartz for example. Photons carried by the light pipe are converted by the PMT and a photocathode (not shown) to an amplified electronic signal outside the microscope column which can then be displayed on a cathode ray tube with the brightness on the screen being proportional to the number of secondary electrons emitted from the specimen. The amplification of the signal with the PMT is far less efficient than that of the scintillator, in that noise is greatly amplified with the PMT.
Scintillators for the SEM of the type of this invention are discussed in my article “Scintillators For The Sem”, by M. E. Taylor, published in “Microscopy Today”, July, 1998 (incorporated herein by reference), which states, inter alia, that without a properly functioning scintillator images tend to be noisy, weak, or exhibit other signs of degradation. This article also states that there are three types of scintillators generally used in the SEM: organic/polymeric, phosphor powder, and crystalline (single or poly). Also, plastic scintillators are currently used less frequently mainly because they are subject to radiation damage which causes a short lifetime, although this type of scintillator has the shortest decay time (about 2.2-5 ns) and very low noise. Using a quartz substrate the scintillator material, in liquid form, is spin coated to produce a uniform thin film, which makes a more robust product and introduces a minimum of organic material to the high vacuum system. The films may be over coated with aluminum for conductivity. Various phosphor powders have been used, but the P47 line of materials appears to be most preferred. They are generally produced by settling in proprietary sollutions, with or without binders, on glass/quartz. Grain size of the phosphor, thickness of the layer, and other additives to the settlement tank can vary the results. The phosphors have a somewhat longer decay time (about 20-40 ns), but these are still within the bounds to be used at fast scan rates. They last 2-3 times longer than plastic scintillators, as long as the vacuum is clean. A contamination layer on the surface of a scintillator will reduce its efficiency.
Scintillators should be handled with the utmost care scince they are very fragile. The main problem in production is getting the material thin enough for optimum resolution. The coated surface should never be touched. They must be installed so that the active/coated side is facing toward the sample chamber and held securely in place with the scintillator retaining ring which must be in contact with the surface for optimum conductivity. Application of silver paint at this interface is no longer recommended.
Unless used in the backscatter mode, the scintillator has a 9-12 KV bias voltage applied. If arcing occurs in the area of the scintillator, damage could result. Furthermore, if scintillator material is removed in any way to produce pin holes, the underlying substrate may also charge up.
Scintillators are also discussed in my article “An Improved Light Pipe for the Scanning Electron Microscope”, by M. E. Taylor, in “The Review Of Scientific Instruments”, Vol. 43, No. 12, December 1972 (incorporated herein by reference).
U.S. Pat. No. 5,932,880 shows an SEM and a scintillator used therein in which electrodes are formed on the electron beam output plane and scintillation radiation plane and a high d.c. voltage is applied between the electrodes to control the scatter direction of an electron beam which has entered the scintillator to be in the direction of the scintillator radiation direction. In one embodiment, a transparent electrode of tin oxide, indium oxide, titanium oxide or the like is between the scintillator and a glass substrate, and the other electrode is deposited over the other side of the device and may be made of Al, Au, Ag, or Pt.
U.S. Pat. No. 5,517,033 shows an SEM using a scintillator comprised of an Al foil having a coating of scintillating material on the underside, and a mirror made of Al coated with a thin layer of Au to prevent oxidation. U.S. Pat. No. 5,536,941 shows a camera and prism assembly for electron microscopes having a scintillator of phosphor applied onto the surface of a glass prism mounted on a movable block. U.S. Pat. No. 5,491,339 shows a charged particle detection device used in addition to a scintillator for detecting a secondary electron signal from a sample using a semiconductor having on one side an oxide film covered with an Al film and a Au pad arranged around the detector in contact with the Al film, and on the inner surface of a hole therethrough an oxide film covered with a conductive film of Au, Pt, Ni, Ti or the like. All the above patents are incorporated herein by reference.
BRIEF SUMMARY OF THE INVENTION
It is a principle object of the invention to provide a scintillator for an electron microscope with improved qualities over previously known scintillators by having enhanced electrical contact, a reduction in pinhole interference, and a reduction of signal to noise ratio, and by eliminating the requirement for an aluminum coating.
It is a further object of the invention to provide an improved scintillator which is easier to handle than other known scintillators and that can be recoated.
It is also an object of the invention to provide a method of making a scintillator having the above advantages over known scintillators.
The above objects are achieved by the scintillator of this invention having a generally disc shape wherein a scintillator material of phosphor, organic, or single crystal is ele
Erdley Randall G.
Fernandez Kalimah
Lee John R.
M.E. Taylor Engineering Inc.
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