U.S. patent number 3,582,656 [Application Number 04/714,954] was granted by the patent office on 1971-06-01 for time base combining radioactive source and solid-state detector.
This patent grant is currently assigned to Bulova Watch Company, Inc.. Invention is credited to Dale R. Koehler.
United States Patent |
3,582,656 |
Koehler |
June 1, 1971 |
TIME BASE COMBINING RADIOACTIVE SOURCE AND SOLID-STATE DETECTOR
Abstract
A radioactive timekeeping standard constituted by a radioactive
source of alpha particles combined with a solid-state radiation
detector, the source being in the form of a backing having a planar
array of discrete islands of a radioactive isotope, the alpha
particles emitted therefrom passing through an apertured mask and
impinging on the sensitive surface of a solid-state radiation
detector, the geometry of the mask apertures, which are in a
matching array, being such as to restrict emanations impinging on
the detector surface to substantially normal angles of incidence
and in addition preventing particles emanating from any one island
from impinging on a neighboring portion of the detector surface
associated with another island.
Inventors: |
Koehler; Dale R. (River Vale,
NJ) |
Assignee: |
Bulova Watch Company, Inc. (New
York, NY)
|
Family
ID: |
24872156 |
Appl.
No.: |
04/714,954 |
Filed: |
March 21, 1968 |
Current U.S.
Class: |
250/370.01;
250/494.1; 257/429; 257/471; 368/155; 968/504; 968/830 |
Current CPC
Class: |
G04F
5/16 (20130101); G04C 10/02 (20130101) |
Current International
Class: |
G04C
10/02 (20060101); G04C 10/00 (20060101); G04F
5/16 (20060101); G04F 5/00 (20060101); G01t
001/24 () |
Field of
Search: |
;250/83.3,83,105,106
(S)/ ;58/23 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Stolwein; Walter
Assistant Examiner: Frome; Morton J.
Claims
What I claim is:
1. A radioactive timekeeping standard adapted to produce
substantially monoenergetic timing pulses and comprising:
a. a planar array of discrete islands of a radioactive isotope
emitting alpha particles, said isotope having a prolonged half-life
whose duration is suitable for timekeeping purposes,
b. a solid-state radiation detector having a sensitive surface in
parallel relationship to said planar array, the area of said
surface being substantially coextensive with the area of said
array, and
c. an alpha particle-absorbing mask interposed between said array
and said surface and having a matching array of alpha
particle-admitting apertures whose geometry is such as to restrict
the emanations impinging on the detector surface through the spaces
in the apertures to nearly normal angles of incidence and
preventing particles emanating from any one island from impinging
on a neighboring portion of the detector surface associated with
another island to obviate a spread in energy distribution.
2. A standard as set forth in claim 1, wherein said array of
islands is deposited on a backing having protective shielding
properties.
3. A standard as set forth in claim 1, wherein said islands are
formed of a thin film of radioactive material to prevent a spread
of energy distribution.
4. A standard as set forth in claim 1, wherein each aperture in
said mask is composed of a first zone adjacent its associated
island having a relatively large cross section and a second zone
adjacent the detector surface having a constricted cross
section.
5. A standard as set forth in claim 4, wherein said second zone of
each aperture is flared outwardly in the direction of the detector
surface.
6. A standard as set forth in claim 1, wherein said radioisotope is
selected from a class consisting of uranium 238, uranium 235,
neptunium 237 and plutonium 239.
7. A standard as set forth in claim 2, wherein said backing is a
metal disc and said mask is composed of at least one circular plate
of the diameter, said detector also having the same
configuration.
8. A standard as set forth in claim 7, wherein said mask is
composed of two circular plates, one having apertures defining the
first zone and the second having apertures defining the second
zone.
9. A standard as set forth in claim 1, wherein said detector is
formed by an array of individual cells, each disposed to intercept
radiation from a respective island, the cells being connected
unidirectionally in parallel.
10. A standard as set forth in claim 9, wherein said cells are
connected in parallel through diodes and are reverse biased.
11. A radioactive timekeeping standard comprising:
a. a planar array of discrete islands of a radioactive isotope
emitting alpha particles, said isotope having a prolonged
half-life.
b. a solid-state radiation detector having a sensitive surface in
parallel relationship to said planar array, and
c. a mask interposed between said array and said surface, having a
matching array of circular apertures whose geometry is such as to
restrict the emanations impinging on the detector surface to nearly
normal angles of incidence and furthermore preventing particles
emanating from any one island from impinging on a neighboring
portion of the detector surface associated with another island,
wherein the diameter of the circle circumscribing such islands is
not greater than twice the distance between the surface of the
islands and the plane of the detector and furthermore that the
diameter of each of said apertures is not less than the diameter of
said circle.
Description
Related Applications: (A) Ser. No. 651,864, filed July 7, 1967, now
abandoned of Koehler and Grissom, entitled "Timepiece with
Radioactive Timekeeping Standard" and (B) Ser. No. 700.102, filed
Jan. 24, 1968, of Koehler, entitled "Multicellular Solid-State
Radiation Detector Assembly."
This invention relates generally to radioactive time bases, and in
particular to a timekeeping standard constituted by a radioactive
source of alpha particles combined with a solid-state radiation
detector.
In the above-identified application (A), there is disclosed a
timepiece arrangement in which a radioactive source having a
relatively long half-life emits charged particles which are sensed
by a solid-state radiation detector. The detector yields a
relatively large number of electrical pulses per second, the pulses
being scaled down by electronic pulse frequency dividers to produce
a low number of control pulses, such as one per second. The
periodic control pulses are applied to an electronic or
electromechanical time register to actuate or control the register
to indicate time. The combination of the radioactive source and
detector is designated a timekeeping standard, as distinguished
from the associated pulse scaling and indicating stages.
Although nuclear disintegrations are distributed randomly in time,
timing accuracy can be obtained through the accumulation of a
sufficient number of counts. Since the disintegrations obey the
Poisson distribution in accordance with probability theory, one can
calculate the statistical accuracy that can be expected from a
total number of counts, assuming that the counting system
contributes negligible error.
As pointed out in copending application (A), the preferred form of
radioactive source for the timekeeping standard is an isotope which
emits alpha particles and has a prolonged half-life. While gamma
rays are radiated with discrete energies, and in that respect are
nearly monoenergetic and can be used for timing purposes, they are
a highly penetrating form of radiation; hence it would not be
feasible, within the confines of a watch or small timepiece, to
provide the necessary protective shielding. Also, it would not be
possible with gamma rays to control the area of the detector to be
exposed to the radiation source.
Beta particles, on the other hand, are not emitted with discrete
energies, but have a continuous distribution of energies. This
radiation is a high-speed electron that is emitted at the
transformation of a neutron to a proton within the nucleus of an
atom. While it is possible to effect shielding of beta particles
with a few millimeters of aluminum, timing control is very
difficult since the particles are not monoenergetic.
The reason for this is that the output pulse heights of a
solid-state radiation detector are proportional to the ionization
produced by incident radiation. Each nuclear particle of the same
type will lose approximately the same proportion of energy through
the ionization process, thereby establishing a direct relationship
between the pulse height of the detector signal and the energy of
the radiation. Unless the radiation is nearly monoenergetic,
electronic instabilities in the system can cause variations in the
detection of low energy pulses and it becomes difficult to
discriminate between detector output pulses and electrical noise
inherent in solid-state detectors and associated amplifiers. This
gives rise to undesirable variations in timekeeping.
Alpha particles consist of two protons and two neutrons, and
possess a charge twice that of an electron but opposite in sign, as
is also the case for a nucleus of a helium atom. The quantity of
energy released is discrete, its magnitude being characteristic of
the particular alpha particle-emitting radioisotope. Naturally
radiated alpha particles have energies ranging from approximately 4
to 10 m.e.v. The fact that alpha radiation is highly ionizing
accounts for its relatively short range when traversing matter.
This range is only a few centimeters in standard air, and several
sheets of ordinary paper will absorb even the most energetic of
alpha particles. Yet from the characteristic properties of gamma,
beta and alpha particles, it is evident that only alpha particles
are suitable for radioactive timekeeping standards, for not only
are they nearly monoenergetic, but they can be handled in a
practical sense within the confines of a small timepiece.
When alpha particles are radiated from a relatively thick source,
alpha particle energies are absorbed within the thickness of the
radioisotope deposit itself. Thus a continuous distribution of
energies will result from alpha particles being radiated from
various depths in the thick layer. The spread of this distribution
can be minimized by obtaining the required activity from the
thinnest source possible.
Another cause of spread or departure from monoenergicity, is the
airgap between the radioactive isotope and the detector. While this
can theoretically be overcome by placing the detector and source in
a vacuum, this solution is not practical. A more workable approach
is to place the source in intimate contact with the detector.
However, existing semiconductive solid-state detectors are
physically constructed with a thin entrance window through which
the particulate radiation must pass before entering the sensitive
volume or depletion zone of the detector. Though one can make this
window very thin, the intimate contact geometry results in varying
degrees of energy degradation. At small angles of incidence, this
degradation reaches a level equal to the total energy of the
incident particles.
One solution to the entrance angle effect is to displace the source
from the detector by a distance which is such as to admit only
radiation whose angle of incidence is about normal to the detector
surface. However, this remedy is not practical in a small timepiece
because of physical size limitations.
In view of the foregoing, it is the primary object of my invention
to provide a time base constituted by a radioactive source of alpha
particles in combination with a solid-state radiation detector in
an arrangement which minimizes the airgap therebetween and yet
effectively restricts incident radiation to nearly normal angles of
incidence, thus obviating a spread in energy distribution.
More specifically, it is an object of the invention to provide a
timekeeping standard assembly of the above type in which an
apertured mask or screen is interposed between the radioactive
source of an alpha particle and the detector to so confine
emanation from the source as to maintain it nearly
monoenergetic.
Also an object of the invention is to provide an efficient and
reliable assembly of radioactive source and solid-state radiation
detector.
Briefly stated, these objects are accomplished in a radioactive
time base assembly comprising a backing having an array of discrete
islands thereon of a radioactive isotope emitting alpha particles
and having a relatively protracted half-life, a mask being
interposed between the islands and the surface of a solid-state
radiation detector, the mask having a matching array of apertures
therein whose geometry is such as to confine the particulate energy
impinging on the detector surface to substantially normal angles of
incidence and to prevent particles emanating from any one island
from impinging on a neighboring portion of the detector surface
associated with another island.
For a better understanding of the invention, as well as other
objects and further features thereof, reference is had to the
following detailed description to be read in conjunction with the
accompanying drawing, wherein:
FIG. 1 schematically illustrates an assembly composed of a single
layer of radioactive material and a detector, an apertured mask
being interposed therebetween, this illustration being for purposes
of background analysis;
FIG. 2 schematically illustrates the behavior of the device shown
in FIG. 1;
FIG. 3 schematically shows a radioactive timekeeping standard in
accordance with the invention;
FIG. 4 illustrates the behavior of the standard shown in FIG.
3;
FIG. 5 is an exploded perspective view of an assembly of the type
shown in FIG. 3; and
FIG. 6 is a modified form of standard in accordance with the
invention.
RADIOISOTOPES
The requirements for an alpha-emitting radioactive isotope will now
be considered. Although many radioisotopes with natural alpha
radiation are commercially available, most of them are not suitable
because their half-lives are not sufficiently protracted to satisfy
the half-life requirements for a timekeeping standard as set forth
in copending application (A). The following radioisotopes are
considered suitable for timekeeping purposes, in addition to those
already identified in said copending application: ##SPC1##
As shown in FIG. 1, a layer 10 of the selected radioisotope is
formed on a backing 11, which may be of platinum or aluminum, or
any other material providing adequate support and preferably having
shielding properties. To minimize the spread of energy
distribution, the layer is made as thin and as uniform as possible.
To this end, a deposition technique may be employed, the
radioactive material being laid down in a very dilute solution on
the backing and then allowed to dry, the resultant film adhering to
the backing.
Detector 12, which is used to intercept alpha particles emanating
from layer 10, may be of the surface barrier or diffused-junction
type commercially available. While the present invention resides in
the use of an apertured mask in combination with a radioactive
source in the form of an array of separate islands of radioisotope
material, the mask 13 in FIG. 1 is shown in combination with a
single, continuous radioactive layer 10, and is provided with an
array of apertures 13A, 13B, 13C, etc., defining parallel passages
of uniform cross section for the emanations. This combination is
not in accordance with the invention, but is shown only for
purposes of background analysis.
FIG. 2 indicates the trajectories of particles emanating at various
angles from different points on source 10, and traveling toward the
surface of detector 12. Path P.sub.1 is normal to the surface of
detector 12. This is the shortest and most direct path and provides
maximum energy. The angle of incidence of path P.sub.2 is such that
it passes through the upper edge of the mask, some energy being
absorbed therein, whereby the remaining energy of the particles
arriving at the detector is reduced. Path P.sub.3, which cuts
through the lower edge of the mask, is even further reduced in
energy. Similarly, paths P.sub.4, P.sub.5 and P.sub.6 are
intercepted by varying thickness of the solid body of the mask, and
are more or less reduced in energy by absorption.
Thus the particles in path P.sub.1 will produce a relatively large
output pulse in the detector, whereas those in the other paths will
produce pulses having lesser and varying degrees of amplitude.
Hence while the alpha-emitting source is nearly monoenergetic, the
detector responds as if the source had a spread of energy
distribution, which is undesirable for timekeeping purposes.
OPERATING PRINCIPLES OF THE TIMEKEEPING STANDARD
Referring now to FIGS. 3 and 4, there is schematically shown a
timekeeping standard in accordance with the invention and
comprising a backing 11 on which is deposited a planar array of
thin islands 14A, 14B, 14C, etc., of a radioisotope emitting alpha
particles. Interposed between this radioactive source and the
exposed surface of the solid-state radiation detector 12 is a mask,
generally designated by numeral 15, having an upper section I and a
lower section II to form a matching array of apertures 15A, 15B,
15C, etc.
Each island 14A, 14B, etc. is centered with respect to the upper
zone of the corresponding aperture defined by the upper section I,
which upper zone has a relatively large and uniform cross section,
the diameter of the island being equivalent to or less than that of
the upper zone. The lower zone of the aperture defined by the lower
section II, has at its top side a smaller diameter preferably equal
to or greater than the diameter of the associated island, the
underside of the aperture being chamfered to provide a flared mouth
of increasing cross section.
The preferred geometry of the mask structure eliminates those
events which would cause an energy loss in the aperture edge
adjacent the radioactive island. Thus it will be seen that the
trajectories indicated by emission paths Pa, Pb and Pc normal to
the detector surface, are unobstructed by the mask. Paths Pd and
Pe, which represent very low angles of incidence are intercepted by
the upper section I of the mask and completely absorbed
thereby.
Because of the flared lower edges of the apertures, paths Pf, Pg
and Ph, which are not normal but which have relatively high angles
of incidence, go directly to the detector surface without striking
an aperture edge and hence without being degraded. Virtual
elimination of the detector-side aperture edge by flaring causes a
minimization of the solid angle subtended by absorptive mask
material at the source, thus minimizing the number of particles
that can actually be energy degraded in the mask material.
Thus the apertured mask in accordance with the invention prevents
particles from any one island from impinging on a neighboring
portion of the detector surface at a low angle of incidence, and
provides an entrance aperture subtending an optimum angle at the
detector. The geometry of the aperture in the mask is such as to
minimize edge effects as well as to reduce airgap losses.
STRUCTURE OF TIMEKEEPING STANDARD
Referring now to FIG. 5, there is shown a practical embodiment of a
timekeeping standard in accordance with the invention. Backing 11
for the radioactive source is in the form of a thin disc of
suitable shielding material on which is deposited a uniform array
of thin circular islands 14A, 14B, etc., of radioactive material
possessing alpha-particle-emitting properties. The islands are
constituted by the deposits of radioactive material substantially
equispaced from each other.
Mask 13 includes a circular upper plate I having relatively large
apertures in a configuration matching the array of the islands, the
diameter of the plate being equal to that of the backing 11. Mask
13 is provided also with a lower plate II having a corresponding
array of smaller apertures whose underside (not shown) is flared,
as indicated in connection with FIG. 3. Finally, below plate II is
a disc-shaped solid-state radiation detector 12.
When the four discs are brought together, the resultant wafer
constitutes a highly compact and efficient timekeeping standard
which may readily be incorporated in a small timepiece or watch. In
a structure of this type, the geometry of the mask is such as to
restrict emanations impinging on the detector surface to nearly
normal angles of incidence and furthermore preventing particles
emanating from any one island from impinging on a neighboring
portion of the detector surface associated with another island.
Preferably, the diameter of each island or the diameter of the
circle circumscribing the island, should the island not be
circular, is no greater than twice the distance between the surface
of the island and the plane of the detector, the diameter of each
mask aperture being not less than the diameter of the island or the
circle.
MODIFIED FORM OF TIMEKEEPING STANDARD
In the conventional solid-state radiation detector, an electric
field is set up across a low-conductivity region, which region is
the charge depletion layer at the diode junction operating at
reverse bias. When a charged particle passes through the
semiconductive medium, electron hole pairs are produced therein.
These charges are caused to separate by the electric field and the
resultant electrical signal can be transmitted to a measuring
system to afford useful information respecting the particles
detected.
The principal drawback in existing solid-state detectors is that
its sensitivity, especially to low-energy particles, tends to be
very low, for there is an appreciable probability of absorption of
such particles before they reach the depletion layer, and even if a
pair of charges is produced in the depletion layer, the quantum
efficiency is limited to one pair per particle, with no chance of
multiplication such as is effectively obtained in Geiger-Muller
tubes and proportional counters.
The low sensitivity dictates the use of high-gain amplifiers. Thus
in the case of detectors 12 shown in the previous figures high-gain
amplication is necessary. However, the output signal from a
conventional solid-state radiation detector lies in the millivolt
range and is not much more pronounced in amplitude than the noise
level in the associated electronic amplifying circuits for
elevating the signal to a level suitable for measurement and
analysis. This noise may give rise to spurious signals which cannot
readily be distinguished from the radiation signals, thus adversely
affecting the sensitivity and energy resolution of the detection
system.
In my copending application (B), there is disclosed a
multicellular, solid-state radiation detector assembly adapted to
produce exceptionally large signals in response to incident
radiation, the detector being constituted by an array of individual
surface-barrier or diffused-junction, radiation-sensitive,
semiconductive cells, each of which has a small area and a low
internal capacitance.
The cells in the array are unidirectionally connected in parallel
relation with respect to current flow, but are otherwise
electrically isolated from each other, whereby the overall
capacitance of the array is low while the detection efficiency
thereof is substantially equal to a unitary radiation detector
whose surface area is equivalent to the aggregate area of the
cells, the signal output from the multicellular detector being far
greater than that yielded by the unitary detector.
In the arrangement shown in FIG. 6, the multicellular solid-state
radiation detector is combined with an array of radioactive islands
14A, 14B, etc., and an apertured mask 13 of the type shown in FIG.
3. The multicellular detector is constituted by an array of tiny
radiation detector cells 16A, 16B, 16C, 16D, etc., whose diameters
are substantially the same as that of the radioactive islands and
which are positioned in registration therewith.
Cells 16A, 16B, etc., are unidirectionally connected in parallel
relation with respect to current flow by diodes 17A, 17B, 17C,
etc., but are otherwise electrically isolated from each other,
whereby the overall capacitance of the array of cells is low,
whereby the detection efficiency thereof is substantially equal to
a unitary radiation detector, such as detector 12, whose surface
area is equivalent to the aggregate area of the cells. However, the
signal output from the multicellular detector is far greater than
that yielded by the unitary detector. In practice, the
parallel-connected detector cells are connected to an output
circuit which imposes a reverse bias thereon.
While there have been shown and described preferred embodiments of
my invention, it will be appreciated that many changes and
modifications may be made therein without, however, departing from
the essential spirit of the invention as defined in the annexed
claims.
* * * * *