COMPOSITE MATERIAL DOSIMETERS

Abstract: The present invention is a composite material containing a mix of dosimeter material powder and a polymer powder wherein the polymer is transparent to the photon emission of the dosimeter material powder. By mixing dosimeter material powder with polymer powder, less dosimeter material is needed compared to a monolithic dosimeter material chip. Interrogation is done with excitation by visible light.

Description: COMPOSITE MATERIAL DOSIMETERS FIELD OF THE INVENTION The present invention relates generally to a com¬ posite material for use as a dosimeter, including but not limited to personnel dosimeters, environmental dosim¬ eters, and high dose dosimeters. More specifically the invention is the incorporation of a dosimeter material powder into a polymer powder with subsequent formation of composite material dosimeters. In this patent, the term dosimeter is used to indicate a device that incorporates dosimeter material that absorbs radiation and is subsequently interrogated for indication of radiation dose. In addition to the dosimeter material, the dosimeter may have additional material, for example, packaging or labelling that does not provide any indication of radiation dose. BACKGROUND OF THE INVENTION The present industrial standard personnel dosimeter is a plastic compartment containing a monolithic chip (approximately 3 mm x 3 mm x 1 mm) of a thermoluminescent crystalline material; for example, lithium fluoride doped with titanium and magnesium (LiF:Ti,Mg) . Dosimeters contain one or more compartments with a corresponding thermoluminescent material chip in each compartment. The compartments are used to facilitate handling of the tiny chips, reducing the risk of loss of a chip, and providing a sufficiently large surface upon which identi¬ fying information may be recorded. The chips are normally interrogated after removing them from their compartments by a process referred to as Ther oLuminescent Dosimetry (TLD) . The TLD process entails heating to a peak temperature then observing the light photons emitted as the temperature of the chips approaches the peak temperature. The number of photons are proportional to the level of radiation exposure. Of course, the chips themselves and any other material exposed to the peak temperatures must be able to with- stand the peak temperatures. This requirement generally precludes the use of a composite dosimeter wherein the dosimeter chip material is held in a plastic matrix because most plastic matrices soften or degrade at the peak temperature. Nevertheless, B.E. Bjarngard, R.C. McCall, and I.A. Berstein reported a composite dosimeter in their paper entitled LITHIUM FLUORIDE-TEFLON THERMOLUMINESCENCE DOSIMETERS, published April 1967 in the Proceedings of International Conference on Luminescence Dosimetry, at Stanford University on June 21-23, 1965. Teflon or Polytetrafluoroethylene (PTFE) is one of the few polymers that can withstand the peak temperature necessary to stimulate phosphorescence of the thermoluminescent dosim¬ eter material. Bjarngard et al. report sensitivity of the composite dosimeter from about 50 R. Sensitivity is likely limited by the opacity of the PTFE, and/or back¬ ground signal from the PTFE. Although not tested, use of clear PTFE as is now used as a fiber optic sheath might improve sensitivity of this dosimeter. However, the present cost of the clear PTFE is prohibitive for indus¬ trial dosimeter applications. In addition, R. Bernhardt et al. in their paper RADIATION DOSIMETRY BY OPTICALLY STIMULATED PHOSPHORES¬ CENCE OF CaF 2 :Mn, August 1974 demonstrate optical stimu- lation of a CaF 2 :Mn-TefIon (Teflon is a trade name for the chemical compound polytetrafluoroethylene) dosimeter for exposures from 1 to 10 5 rad. The lower limit of 1 rad is reported as achievable using a measuring time of 0.5 min and a stimulation time of 0.1 in for a total time of 0.6 min. Shorter measuring times result in raising the lower limit, or reducing the sensitivity. The authors conclude that this dosimetric technique is appropriate for accident dosimetry. A more recent method of interrogation was described in U.S. Pat. No. 4,954,707, to Miller et. al. entitled SYSTEM FOR USE WITH SOLID STATE DOSIMETER. In this patent, the method of interrogation is cooling of a solid state material chip and exposing the cooled chip to light for photoconversion of light sensitive traps, then per¬ mitting the chip to warm to ambient temperature wherein during the warming, photons are emitted from the light sensitive traps proportional to the level of radiation exposure. It is important to note that the photon emis¬ sion occurs later in time than the photoconversion. This method is referred to as Cooled Optically Stimulated Luminescence (COSL) . The COSL method is advantageous over the TLD method because the lower temperatures are less harmful to a wider variety of materials than the higher temperatures of the TLD process. The photocon¬ version in the COSL method as practiced using CaF 2 :Mn or CaF 2 :Dy is accomplished using ultraviolet (UV) light because the UV light produces the most photons per unit of ionizing radiation exposure thereby producing sensi¬ tivities on the order of about 1 milliRoentgen (mR) . A yet more recent method of interrogation was described in U.S. Pat. No. 5,272,348 to Miller, entitled METHOD FOR RADIATION DETECTION AND MEASUREMENT, wherein the dosimeter material is stimulated by light energy at one wavelength to produce photons at another wavelength at ambient temperatures. The emitted photons are propor- tional to the level of radiation exposure. This ambient temperature method is referred to as Optically Stimulated Luminescence (OSL) . The OSL process has the advantage that no heating or cooling is necessary to obtain emitted photons. In the OSL process, photon emission occurs nearly simultaneously with light stimulation. The optical stimulation of the OSL process is practiced using light in the visible and infrared. It is preferred to use light at a wavelength that is near the excitation wavelength of the dosimeter material traps. Regardless of the method of interrogation, however, the chips still required compartments for handling and interrogation independent of the compartment. The com¬ partment plus chip cost along with the handling cost for interrogation made it prohibitive to perform large scale population dosimetry studies. Also, because of the cost of the chips, in industrial employee applications it was necessary to re-use the chips because the' additional handling was less costly than replacement of the chips. SUMMARY OF THE INVENTION The present invention is based upon the discovery that certain plastic/dosimeter material combinations provide sufficient sensitivity that rapid readings (less than 10 sec) are possible and it is not necessary to remove the dosimeter material from the plastic for purposes of interrogation. Thus, a composite material containing a mix of dosimeter material powder and a polymer powder can be molded, extruded, or otherwise formed into dosimeters of various shapes. The polymer must be transparent to the photon emission of the dosimeter material powder. The dosimeter is useful for measuring radiation dose from ionizing radiation includ¬ ing but not limited to beta and gamma rays as well as non-ionizing short wave radiation, for example x-rays. By mixing dosimeter material powder with polymer powder, less dosimeter material is needed compared to a monolithic dosimeter material chip. Moreover, the composite chip exhibits greater dosimeter-to-dosimeter uniformity compared to monolithic chip dosimeters. Thus, the composite dosimeter is sufficiently less costly that re-use is not necessary and overall cost of dosimetric interrogations is reduced. Because interrogation by heating is generally done at temperatures in excess of softening or melting points of polymer materials, this invention is particularly suited for interrogation by non-heating methods. How¬ ever, to avoid the loss of sensitivity due to high background signals from plastics exposed to ultraviolet light, it was discovered that optically transmissive sensitized metal oxides or alkali-metal halides provide sufficient photons when excited by a visible light, preferably a blue light, that they can be incorporated into a plastic or polymer matrix. As used herein, the term optically transmissive includes a broad range of transmissivities from optically clear for the wavelengths of interest to optically trans¬ lucent for the wavelengths of interest. Another term considered synonymous is non-opaque. The subject matter of the present invention is particularly pointed out and distinctly claimed in the concluding portion of this specification. However, both the organization and method of operation, together with further advantages and objects thereof, may best be understood by reference to the following description taken in connection with accompanying drawings wherein like reference characters refer to like elements. BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a graph of intensity versus wavelength for a range of ultraviolet wavelengths. FIG. 2 is a graph of intensity versus wavelength for a range of violet to red optical wavelengths. FIG. 3 is a graph of COSL Response of A1 2 0 3 versus wavelength. FIG. 4 is a graph of Response versus time for the short time constant decay of A1 2 0 3 . FIG. 5 is a graph of OSL Intensity versus time for the long time constant decay of A1 2 0 3 . FIG. 6 is a graph of COSL response versus exposure for CaF 2 :Mn in PMMA. DESCRIPTION OF THE PREFERRED EMBODIMENT(S) The present invention is a dosimeter for measuring radiation exposure having an amount of an optically transmissive sensitized metal based bi-element compound powder dispersed throughout a volume of a polymer matrix. In order to achieve a dosimeter material/polymer matrix combination, the problem of polymer matrix back¬ ground signal had to be overcome. FIG. 1 illustrates the problem. For a dosimeter material dispersed throughout a polymer matrix, when exposed to ultraviolet light, the first background signal 1 from the polymer matrix is so much more intense than the first peak signal 2 from the dosimeter material, that the combination is inoperative as a means or method of making measurements of radiation dose less than about 1 R of gamma radiation exposure as demonstrated by R. Bernhardt et al. (op. cit.) . In FIG. 2, according to the present invention, exposure of a dosimeter of optically transmissive sensitized bi-element metal based compound dispersed in a polymer matrix, wherein the dosimeter is exposed to a light in the violet to red (350 n to 700 nm) , results in the second background signal 21 having much smaller intensity than the second peak signal 22 which is operative as a means and/or method of making sensitive measurements of radiation dose less than about 1 R of gamma radiation exposure, but more preferably less than about 10 mR of gamma radiation exposure. The metal based compound is a bi-element compound wherein the term bi-element is defined as containing two chemical elements substantially stoichiometrically bonded together. The term substantially is used because there are occasionally excesses and deficiencies of one or the other element in a powder that are not strictly stoichio- metric. There may be multiple atoms of one or both elements, but the compound still has the two chemical elements. The metal oxides are preferably selected from the group of zirconium oxide, barium oxide, strontium oxide, aluminum oxide and silicon oxide. Although there is debate as to whether silicon is a metal, it is included herein as a metal for purposes of definition of the metal based compound. The metal based compound may be non-stoichiomet- rically doped with one or more additional element(s) . Bi-element compounds are selected from the group of metal oxides and metal halides, or combinations thereof. Dopants may be any element(ε) but are preferably selected from the group of manganese, dysproprium, titanium, mag¬ nesium, silicon and carbon. The polymer matrix selected depends upon the method of interrogating the dosimeter material. When using the COSL method, there is time between photoconversion (resulting from photoexcitation) and photon emission (resulting from warming the dosimeter material) . The time lag is controllable or selectable by keeping the dosimeter material at a low temperature until it is desired to obtain a reading. That time lag permits the use of a wide range of plastics because the background signal from the photoexcitation of the plastic decays as a function of time sooner than the photon emission decays from the dosimeter material. It is preferred that the plastic be optically transmissive to the photons released by the dosimeter material powder and optically trans¬ missive to the photoconversion. Polymer matrices found to exhibit these characteristics include, for example, methyl-pentene (PTX) , polyethylene, polypropylene, polycarbonate, poly-methyl-methacrylate (PMMA) or Lucite, polystyrene, and most thermoset polymers. In addition to the time lag for the response of the dosimeter material, there is also a time lag for the response of the plastic matrix. Thus, for best readout sensitivity, it is best to permit the plastic matrix background signal to decay before reading the dosimeter material response. Addi¬ tional improvement was discovered by using aluminum oxide as the dosimeter material. Aluminum oxide need only be cooled to dry ice temperatures compared to calcium fluoride that must be cooled to about liquid nitrogen temperatures. Use of the dry ice temperature permits the plastic matrix background signal to decay more quickly and requires less time to bring the dosimeter to room temperature. At liquid nitrogen temperatures, the time constant for the plastic background signal is on the order of hundreds of milliseconds whereas at room temper¬ ature, the plastic background signal time constant is from tens of nanoseconds to hundreds of nanoseconds. Use of warmer dry ice temperatures theoretically would affect sensitivity. In practice, it was discovered that if there is reduced sensitivity, it is within 10% of the liquid nitrogen temperature sensitivity. When using OSL interrogation of alkali halide thermoluminescent materials, for example LiF, NaF, and NaCl, the light stimulation immediately produces emitted photons. Because both occur simultaneously, the background signal from the plastic induced by the light stimulation cannot be differentiated from the OSL emitted photons and therefore limits the potential sensitivity of the dosimeter. Nevertheless, it was discovered that stress relieved or cast PMMA has sufficiently low background that the emitted photons can be measured to sensitivities of ionizing radiation exposure below 100 R. Measurements may be made from about 10 R to about 10 7 R. This range is useful for high dose dosimetry and for radiation sterilization carried out from about 10 3 R to about 10 6 R. For OSL, it is preferred to use metal halides, for example lithium fluoride and/or sodium fluoride. Alternatively, it was discovered according to the present invention that aluminum oxide, specifically, has a decay time that is longer than the decay time of the plastic matrix for visible light and near visible light. Near visible light is in the ranges considered near infrared and near ultraviolet. For ultraviolet light, however, there was such a strong signal from the plastic, that it was not possible to make readings as sensitive as with light exposure substantially free of ultraviolet light. Thus, for a composite dosimeter of aluminum oxide in plastic, use of a room temperature pulsed laser readout permits the background signals from the plastic to decay to a low level before the signal from the aluminum oxide has decayed. In other words, by using visible light substantially free of ultraviolet light, the measurement of the aluminum oxide signal may be made substantially after decay of the background signal from the plastic matrix. Further, a combination of aluminum oxide stimulated with visible light substantially free of ultraviolet light together with cooling to a temperature below ambient temperature to about dry ice temperature results in improved sensitivity of radiation measurements. The sensitization of the metal based compound powders is presently uncharacterized. It was found that certain batches of similar compounds behaved very dif¬ ferently. For example, a batch of chromatography grade sapphire (aluminum oxide) did not provide sufficient photon signal for dosimetric performance, whereas a batch of substrate grade sapphire polished crystals obtained from the Adolf-Meller Co. (now Meller Optics, Inc., Providence, Rhode Island) did provide sufficient photon signal for dosimetric performance. Although it is not yet known how to control the sensitization of a partic¬ ular batch of a certain powder, sensitized batches are easily identified. Further, it is not yet known what the material parameters are that develop sensitization. One clue was the observation that the chromatography grade sapphire had a low anion deficiency concentration based upon measurements which exhibited essentially no photon emission whereas the commercial sapphire had an anion deficiency from about 10 16 to about 10 18 anion defi¬ ciencies per cubic centimeter. An anion deficiency is defined as a lattice defect wherein one or more oxygen atoms is/are missing. Anion deficiency is measured using optical absorption techniques wherein characteristic absorption occurs between from about 200 nm to about 260 nm in the ultraviolet. It is postulated that element or ion charge compensation may contribute to sensitiza¬ tion, but that is not certain. Because both powders of metal oxides and metal halides can be interrogated using either COSL or OSL, the dosimeters are not limited to a particular interrogation method. In certain applications, it may be desirable to use one or the other depending upon required sensitivity of measurement or cost considerations. The COSL process is presently sensitive to as low as about 1 microR while the OSL process is presently sensitive to as low as about 1 mR without a plastic matrix. Addition of the plastic or polymer matrix provides a source of background signal that raises the lower limit from about 1 mR to from between above 1 mR to about 20 mR and most likely between about 10 mR and about 20 mR. The interrogation method may also include annealing the bi-element material. Annealing may be accomplished by exposure to heat or light. It is preferred when using a metal oxide to anneal by exposure to light substan- tially free of ultraviolet light. It is further prefer¬ red that the light be white light substantially free of ultraviolet light. White light is preferred because it is easily available, inexpensive, and effective to anneal the metal oxide. The annealing procedure requires a certain amount of light energy from about 10 Joules/cm 2 to about 1000 Joules/cm 2 depending upon the degree of annealing required or desired for a particular applica¬ tion. More sensitive measurements require a greater degree or amount of annealing. For annealing aluminum oxide for sensitive measurements, an amount of light of about 200 Joules/cm 2 is preferred. The light energy may be delivered quickly or slowly. In the lab, room lights have been found to provide a limited level of annealing. A Cermax lamp source delivering 500 mW of light applied for from about 4 to about 8 hours provided adequate annealing for sensitive measurements. According to the present invention, it was dis¬ covered that aluminum oxide powder exhibits a long time constant phosphorescence at ambient temperatures (about 24°C) . Moreover, the photon emission of aluminum oxide at ambient temperatures was as intense or more intense than calcium fluoride doped with manganese. Thus, aluminum oxide is a preferred dosimeter powder. The proportions of dosimeter material powder and polymer matrix material may vary according to a partic¬ ular dosimetric application. According to the present invention, a ratio of dosimeter material powder to poly¬ mer matrix material may range from about 0.1% by weight to about 40% by weight. Below about 0.1% by weight, there is insufficient amount of dosimeter material to provide sufficient signal for making readings especially at low doses. Above about 40% by weight, the mechanical properties of the composite are reduced. A preferred range is from about 1% to about 10% by weight of dosim¬ eter material and more preferred is a range from about 5% to about 10% by weight. In addition, the dosimeter mate¬ rial powder particle size distribution may vary as well. Dosimeter material particle size may range from about 1 micrometer (μm) to about 250 μm. Below from about 1 μ to about 250 μm. Below from about 1 μm to about 10 μm, the dosimeter material exhibits a loss of ionizing radiation sensitivity. Above about 250 μm, it is difficult to achieve uniform dispersion in the polymer matrix. Thus, it is preferred that the dosimeter material particles are from about 40 μm to about 150 μm to provide good sensitivity and satisfactory mixing or dispersion within the polymer matrix. Ideally, the more individual particles homogeneously distributed throughout the polymer matrix, the better. That is because each powder particle acts as an individual dosimeter. However, because it is impossible to make the number of photon emission traps the same in each powder particle, it is necessary to have a statistically large number of powder particles in a dosimeter so that photon emission for a given radiation dose is consistent from dosimeter to dosimeter within acceptable limits. It is preferred to be consistent with a deviation of one standard deviation from the mean of about a 10%, and more preferred to be consistent within about 5%, and most preferred to be consistent within less than 5%. This makes it possible to achieve greater uniformity between dosimeters than is possible between monolithic chips of dosimeter material which exhibit a deviation from about 15% for LiF samples to greater than or equal to about 25% for unsorted A1 2 0 3 single crystals samples. By utilizing a polymer matrix, it is easier to form the dosimeter into a variety of shapes and sizes for example, finger rings or small discs. By using COSL or OSL, the interrogation is done without removing a chip of dosimeter material from the finger ring as is presently done using the TLD process. Moreover, it is easier to use presently available miniature marking technology to place identifying marks on a polymer matrix dosimeter so that chain of custody is maintained without the need for a separate container. This is important for increasing reliability of measurements should the detection element become separated from its container. By using a composite of aluminum oxide in a polymer matrix in combination with a room temperature readout, there are two fundamental options for room temperature readout, one based upon a short time constant decay and another based upon a long time constant decay. A preferred embodiment utilizes the long time constant decay in a two step process wherein a dosimeter is first exposed to a photoexcitation, then mechanically moved to a photomultiplier for readout of the dosimeter material photon emission. Advantages of the two-step process include avoiding exposure of the photomultiplier tube to an initial strong photon emission without electrical switching of the photomultiplier tube, and inexpensive light sources may be used. It will be apparent to those skilled in the art of dosimetry that the mechanical movement may be omitted. Any light source may be used, but it is preferred to use light sources substantially free of ultraviolet light. Examples of light sources include but are not limited to continuous or pulsed sources and laser and non-laser sources. It is preferred to utilize laser light sources because they are more easily adjusted to exclude ultraviolet light. One way to utilize the short time constant decay option is with a fast pulsed laser with energy from about 1 to about 1000 mJ (millijoule) per pulse. Alterna¬ tively, a shuttered continuous wave laser delivering from about 1 to about 1000 mJ in an open shutter period wherein the open shutter period is approximately or about 1 ms may be used. A flash lamp or other pulsed or shuttered light source may be used instead of a laser. METHOD OF MEASURING RADIATION DOSE According to the present invention, a method of measuring radiation dose has the steps of: (a) exposing a dosimeter having a bi-element dosimeter material within a polymer matrix to radiation; (b) stimulating the irradiated dosimeter with visible light substantially free of ultraviolet light; and (c) counting photons emitted from the bi- element dosimeter material as a result of the light stimulation. Ultraviolet light is light of wavelengths of less than about 326 nm. It is most preferred that the amount of ultraviolet light in the visible light used for interrogation be zero so that background noise from the polymer is minimized. However, in applications measuring moderate to high doses, or where low dose sensitivity is less important, a certain amount of ultraviolet light producing a corresponding background signal may be tolerable thereby permitting the use of a lamp or filtered lamp source. The method can be carried out at room temperature or with a step of cooling the irradiated dosimeter to cryo¬ genic temperatures prior to light stimulation. In a preferred embodiment, the polymer has a visible light background signal decay time of less than a visible OSL light decay time of the bi-element material thereby permitting rapid readings. Preferably, readings are obtained in less than about 10 sec, and more preferably less than about 5 sec, and most preferably less than about 1 sec. Rapid readings are obtained by using a laser emit¬ ting in the near visible to visible range, preferably blue, to stimulate the dosimeter material to phosphor¬ escence at a wavelength within the range from about 380 nm to about 500 nm. In applications wherein the stimulating wavelength is different from the response wavelength, an optical filter may be used to exclude scattered stimulation light from a photomultiplier tube used to count the response. In applications wherein the stimulating and emission wavelengths overlap, a short time constant laser excitation technique may be used with time gating to eliminate the scattered light from the excitation source. The laser may be a pulsed laser or a continuous wave laser. In the method of the present invention, it is neces¬ sary that the stimulating light be substantially free of ultraviolet light. EXAMPLE 1 An experiment was done to quantify the response versus wavelength behavior of sensitized aluminum oxide (A1 2 0 3 ) . Twenty one wavelengths between 300 nm and 700 nm were selected for the experiment. A combination of com¬ mercially available lasers and filtered light sources was used to provide excitation at the various wavelengths. At each wavelength, about ten excitations were done thereby permitting estimation of an error band about each data point. Each excitation transferred the same amount of energy independent of wavelength. The COSL interrogation method was used to quantify the response of the aluminum oxide at each wavelength. Cooling was accomplished with liquid nitrogen and emitted photons were detected and counted by a photomultiplier tube model RCA 8575, RCA Burle, Massachusetts. Results are shown in FIG. 3 confirming a sensitive response between about 400 nm and about 520 nm. EXAMPLE 2 A second experiment was performed to quantify decay constants for sensitized aluminum oxide. For quantifica¬ tion of the fast decay (FIG. 4) data were obtained with a frequency doubled Nd:YAG laser operating at 532 nm (green) and generating 25 mJ at 2 Hz. The pulse duration of the laser was about 10 ns. A narrow-band pass 420 nm filter was used with the photomultiplier tube of Example 1 to eliminate the 532 nm light. For quantification of the slow decay (FIG. 5) a 600 ps nitrogen dye laser manufactured by Laser Photonics, Orlando, Florida was used to provide a burst of energy to the sensitized aluminum oxide at room temperature. The photomultiplier tube used in Example 1 was used in this example to count photon emission over time after the burst. Results are shown in FIGS. 4 and 5 for a first lumi¬ nescent center and a second luminescent center respec¬ tively. The first luminescent center data provided in FIG. 4 shows data points 41 of actual data and a first smooth fit line 42 through the data. Although short, the time of up to 0.1 sec is sufficient to obtain a reading at room temperature which has significant advantages over readings required to be obtained at either high or low temperatures. The second luminescent center data provided in FIG. 5 shows data points 51 of actual data and a second smooth fit line 52 through the data. This second lumi¬ nescent center exhibits a much longer decay time than the first luminescent center. EXAMPLE 3 An experiment was conducted to demonstrate the response versus wavelength behavior of sensitized aluminum oxide interrogated by the OSL method at room temperature. Results are shown in Table 3.1. Table! 3.1 OSL Response of A1 2 0 3 Wavelencfth (nm) Response (counts) 326 190 442 850 488 816 514 611 630 37 It was observed that the peak of greatest intensity occurred also between 400 nm and 520 nm, specifically at about 450 nm. EXAMPLE 4 An experiment was conducted to identify polymers having low background for light at various wavelengths. Data for polymers exposed to 390 nm stimulation are given in Table 4.1. Table 4.1 Response of Polymers to 390 nm Light Polymer Response (counts) Polyethylene 11.3 Polyvinylchloride (PVC) 10.9 PMMA 6.67 Teflon 5.1 Urethane Acrylate 500. Fluroacrylates 150-300. A similar test was performed but with wavelengths of 326 nm and wavelengths less than 326 nm with resulting background signals of 300 to 400 counts and in some instances, as high as 600 counts compared to the 11.3, etc. counts in Table 4.1. (The counts in Example 3 do not correspond to the counts in Example 4.) A test exposing PMMA to blue light at 442 nm resulted in a background signal of about 5 counts, that is much quieter than the 390 nm exposure. In addition, it was surprising to discover that the decay of the background signal from the plastic matrix was faster than the decay from the aluminum oxide material. This permits rapid reading within 30 sec and preferably within about 1 or 2 sec (FIG. 5) or within about 0.1 sec (FIG. 4) . EXAMPLE 5 An experiment was conducted to demonstrate the response of calcium fluoride manganese (CaF 2 :Mn) in PMMA. FIG. 6 shows response versus exposure obtained using the COSL process cooled with liquid nitrogen and a light source with bandpass filter producing light at 390 nm ±10 nm. CLOSURE While a preferred embodiment of the present inven¬ tion has been shown and described, it will be apparent to those skilled in the art that many changes and modifica- tions may be made without departing from the invention in its broader aspects. The appended claims are therefore intended to cover all such changes and modifications as fall within the true spirit and scope of the invention.

Claims: I claim: 1. A method of measuring radiation dose, compris¬ ing the steps of: (a) exposing a dosimeter having a bi-element dosimeter material in a polymer matrix to radiation; (b) maintaining the exposed dosimeter at a temperature; (c) stimulating the irradiated dosimeter with visible light substantially free of ultraviolet light; and (d) counting photons emitted from the bi- element dosimeter material as a result of the light stimulation. 2. The method as recited in claim 1, further comprising the step of annealing the bi-element material after the step of counting. 3. The method as recited in claim 2, wherein annealing is done with light substantially free of ultraviolet light. 4. The method as recited in claim 1, wherein the temperature is ambient temperature. 5. The method as recited in claim 1, wherein the temperature is below ambient temperature. 6. The method as recited in claim 5, wherein the temperature is dry ice temperature. 7. The method as recited in claim 1, wherein the polymer has a visible light decay time of less than a visible light decay time of the bi-element material. 8. The method as recited in claim 1, wherein the bi-element dosimeter material is selected from the group of alkali-metal halides. 9. The method as recited in claim 8, wherein the alkali-metal is selected from the group of lithium and sodium. 10. The method as recited in claim 1, wherein the bi-element dosimeter material is a metal oxide. 11. The method as recited in claim 10, wherein the metal oxide is selected from the group consisting of zirconium oxide, barium oxide, strontium oxide, aluminum oxide and silicon oxide or any combination thereof. 12. The method as recited in claim 11, wherein the bi-element dosimeter material is sensitized aluminum oxide. 13. The method as recited in claim 12, wherein sensitization is anion deficiency. 14. The method as recited in claim 13, wherein the anion deficiency is from about 10 16 to about 10 18 anion deficiencies per cubic centimeter of aluminum oxide. 15. The method as recited in claim 1, wherein the polymer is stress relieved poly-methyl-methacrylate. 16. The method as recited in claim 1, wherein the visible light is blue light. 17. The method as recited in claim 1, wherein the light is provided by a laser. 18. The method as recited in claim 17, wherein the laser is a pulsed laser. 19. The method as recited in claim 1, wherein the visible light is laser light in the range from above about 326 nm to about 700 nm. 20. The method as recited in claim 19, wherein the light has a wavelength between 326 and 630 nm. 20. The method as recited in claim 7, wherein counting is done after waiting for a background signal from the polymer matrix to decay. 21. The method as recited in claim 1, wherein the bi-element dosimeter material is in the form of particles dispersed throughout the volume of the polymer.

Inventors: MILLER STEVEN D, MILLER, STEVEN, D.
Applicants: BATTELLE MEMORIAL INSTITUTE
Application year: 1995
Main classification: G01T1
IPC codes: G01T1