Isotope tagging for workpiece authentication

Abstract

A method of assisting with authenticating a workpiece is provided. In another aspect, ions are generated, accelerated in an accelerator, an isotope is created, and then the isotope is implanted within a workpiece to assist with authenticating of the workpiece. A further aspect includes a workpiece substrate, a visual marker and an isotope internally located within the substrate adjacent the visual marker.

Claims

1. A method of assisting with authenticating a workpiece, the method comprising: (a) generating ions; (b) accelerating the ions in an accelerator with an energy of at least 100 A-MeV and a beam power of at least 1 kW; (c) creating an accelerated isotope from the accelerated ions; and (d) implanting the accelerated isotope in the workpiece to assist with the authenticating of the workpiece.

2. The method of claim 1, wherein the accelerating of the ions occurs by using a facility comprising a superconducting cyclotron accelerator.

3. The method of claim 2, wherein the generating of the ions occurs by using one of: (a) an electron cyclotron resonance source or (b) an electron beam ion source.

4. The method of claim 2, wherein the generating of the ions occurs by using one of: (a) microwaves in a low pressure gas, or (b) thermionic emissions of electrons to ionize a base material in its gaseous state.

5. The method of claim 2, wherein the ions are rare heavy ions.

6. The method of claim 1, further comprising using a gamma ray detector with keV energy resolution to nondestructively identify at least one of: (a) the isotope, or (b) a position of the isotope, to assist in the authenticity of the workpiece after the implanting step.

7. The method of claim 1, further comprising placing a removable mask, having a unique hole pattern, against the workpiece and emitting the accelerated isotope through the hole pattern before the implanting step.

8. The method of claim 1, further comprising using different combinations of rare isotopes to create customizable workpiece identifiers in additional workpieces.

9. The method of claim 1, further comprising applying a visual marker to the workpiece adjacent to a location of the isotope implantation.

10. The method of claim 1, wherein the creating of the accelerated isotope comprises fragmenting the accelerated ions to create a fragmented isotope and then re-accelerating the fragmented isotope.

11. The method of claim 1, wherein the workpiece includes a painting on canvas and the isotope penetrates into and is implanted inside the workpiece between 5 mm and 1 micron deep from an entry surface thereof.

12. The method of claim 1, wherein the workpiece is metallic and the isotope penetrates into and is implanted inside the workpiece between 5 mm and 1 micron deep from an entry surface thereof.

13. A method of assisting with authenticating workpieces, the method comprising: (a) generating ions; (b) accelerating the ions in a superconducting cyclotron accelerator; (c) creating a first combination of rare isotopes and a second combination of rare isotopes; (d) transmitting the first combination of rare isotopes through holes in at least one removable mask toward a first of the workpieces; (e) transmitting the second combination of rare isotopes through the holes in the at least one removable mask toward a second of the workpieces; and (f) causing the first and second combinations of rare isotopes to penetrate into the respective workpieces between 5 mm and 1 micron deep from an entry surface of each of the workpieces adjacent the mask, wherein the first and second combinations of rare isotopes are different, which creates unique authenticating indications.

14. The method of claim 13, wherein each of the rare isotopes has a measurable and precise alpha or gamma decay emission, but not a beta decay emission.

15. The method of claim 13, wherein the generating of the ions occurs by using one of: (a) an electron cyclotron resonance source or (b) an electron beam ion source.

16. The method of claim 13, wherein the generating of the ions occurs by using one of: (a) microwaves in a low pressure gas, or (b) thermionic emissions of electrons to ionize a base material in its gaseous state.

17. The method of claim 13, further comprising using an isotope ratio mass spectrometer to nondestructively identify at least one of: (a) the first or second combinations of rare isotopes, or (b) a position of the first or second combinations of rare isotopes, to assist in the authenticity of the workpieces after the implanting step.

18. The method of claim 13, further comprising applying a visual marker to each of the workpieces adjacent to a location of implantation of the first or second combinations of rare isotopes.

19. A workpiece comprising: (a) a pre-made workpiece substrate; (b) a visual marker; and (c) rare isotopes internally located within the pre-made substrate adjacent the visual marker, the rare isotopes providing a customized identifier based on at least one of: a pattern, quantity, isotope combinations, or half-life; (d) the rare isotopes having: the half-life of at least three months; a precise and measurable alpha or gamma decay emission; a unique isotope signature; and wherein the rare isotopes are a combination of rare isotopes including at least one of: .sup.148.sub.64Gd, .sup.194.sub.76Os, .sup.60.sub.26Fe, .sup.126.sub.50Sn, .sup.228.sub.88Ra, or .sup.210.sub.82Pb.

20. The workpiece of claim 19, wherein: the combination of the rare isotopes is arranged in a unique pattern implanted within the substrate between 5 mm and 1 micron deep from an entry surface thereof.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

(1) FIG. 1 is a diagrammatic view showing superconducting cyclotron equipment used with the present method and system;

(2) FIG. 2 is an enlarged side elevational view showing the present system including isotopes implanted within a workpiece;

(3) FIG. 3 is an enlarged back elevational view showing the present system including a visual marker and/or mask located on the workpiece;

(4) FIG. 4A is a graph showing predicted rare isotope charge versus isotope neutron number rates expected after completion of the Facility for Rare Isotope Beams;

(5) FIG. 4B is a table showing values associated with isotope .sub.64.sup.148Gd of FIG. 4A;

(6) FIG. 4C is a table showing values associated with isotope .sub.76.sup.194Os of FIG. 4A;

(7) FIG. 4D is a table showing values associated with isotope .sub.26.sup.60Fe of FIG. 4A;

(8) FIG. 4E is a table showing values associated with isotope .sub.50.sup.126Sn of FIG. 4A; and

(9) FIG. 4F is a table showing values associated with isotope .sub.88.sup.228Ra of FIG. 4A.

DETAILED DESCRIPTION

(10) The present method, workpiece and system are shown in FIGS. 1-3. A superconducting cyclotron facility 21 includes an ion source 23, a K500 cyclotron 25, a K1200 cyclotron 27, an A1900 fragment separator 29, a momentum compression ANL gas catcher 31, an optional cryogenic gas stopper 33, a low energy beam line EBIT cooler buncher helium jet 35, an optional linear reaccelerator 37, and an isotope tagging station 39. The preceding items are all computer controlled. Ion source 23 includes an electron cyclotron resonance (ECR) source or an electron beam ion source (EBIS), such a using an ion gun employing microwaves in a low pressure gas or thermionic emissions of electrons to ionize the base material in its gaseous state. Superconducting cyclotron facility 21 is of the type disclosed in Hausmann, M., et al., Design of the Advanced Rare Isotope Separator ARIS at FRIB, Nucl. Instr. Meth. B 317 (Jul. 4, 2013) 349-353; and Experimental Equipment Needs for the Facility for Rare Isotope Beams (FRIB)whitepaper (Feb. 13, 2015). Facility 21 uses projectile fragmentation and induced in-flight fission of heavy-ion primary beams at energies of 100 MeV and preferably at least 200 MeV/u and at a beam power of at least 1 kW and preferably at least 400 kW, to generate rare isotope beams. More particularly, reaccelerator 37 is a superconductingRF driver, linear accelerator. Fragment separator 29 is preferably a three-stage fragment separator including a first stage vertically bending preseparator followed by two horizontally-bending second and third stages using multiple superferric magnet dipoles and quadruples to focus the beam and/or correct image aberrations. FIG. 1 illustrates the equipment layout of the National Superconducting Cyclotron Laboratory with the proposed location of the isotope tagging station within the accelerator complex, but alternate layouts may be employed.

(11) A high value workpiece 51 is an original artwork, such as a painting, print, photograph, sculpture, vase, tapestry, document or the like. Alternately, workpiece is an antique, jewelry, watch, vintage automobile component such as an engine block, or other such expensive or one-of-a-kind object that is prone to having forgeries or false reproductions made thereof. In the painting workpiece 51 example used herewith, a substrate 53 is canvas with an aesthetic painted layer 55 on a front surface. If a sculpture, substrate 53 includes the clay or ceramic material. If jewelry or an automobile component, substrate 53 may be a metal structure.

(12) First, a visual marker 57 is placed in a small area on a backside of workpiece 51, such as by printing, painting or any other manner which will last for decades without significant degradation or harm to aesthetic painted layer 55. Marker 57 provides a visual point for the authenticator to begin seeking the isotope tag. One or more metallic masks 59 are temporarily placed against marker 57. Each mask 59 is a lead plate of about 2-10 mm thick with one or more holes 61 therethrough. Workpiece 51 is then placed in a fixture within isotope tagging station 39. A hollow and elongated beam pipe 63 is sealed against mask 59.

(13) A beam of heavy ions is generated from source 23 and accelerated to approximately half the speed of light by cyclotrons 25 and 27. Nuclear reactions occur at the beginning of the fragment separator 29 to create the desired isotope. The desired isotope 71 is selected by the fragment separator and then transported for use in a beam pipe or optionally travel through catcher 31 and are slowed down in helium gas stopper 33. Optionally, isotopes 71 are thereafter re-accelerated in linear accelerator 37 to create a precise workpiece-penetration speed. Isotopes from the fragment separator or optionally reaccelerated isotopes 71 then travel through pipe 63 and those isotopes aligned with holes 61 in mask 59, penetrate into and are implanted between 5 mm and 1 micron deep, and more preferably at or between 1 mm and 10 microns inside workpiece 51 relative to the backside surface thereof adjacent pipe 63.

(14) Multiple masks 59 with different hole quantities or patterns (as shown in FIG. 3) may be employed to provide unique or customized identifiers. Moreover, different combinations of rare isotopes 71 may be implanted through a single or different combinations of mask holes 61 to provide unique or customized identifiers. In the example shown in FIG. 3, at least four and more preferably sixteen different isotope locations are provided for a single workpiece. The identifier may be published in a reference guide for each original workpiece. Since a rare isotope is chosen that can only be implanted in expensive accelerator facilities (i.e., >$500 million (2015 USD)), the present approach is too expensive and technically difficult for a forger. However, the present approach is feasible for a physicist with legitimate access to such a system. The authenticator uses a gamma ray detector 73 with keV energy resolution or the like to identify the type of isotope and position of the isotope in a nondestructive manner, to assist in authentication (which includes identification) of the workpiece.

(15) Referring to FIGS. 4A-4F, desired rare isotopes are those that are accelerated with an energy of at least 100 A-MeV and with a beam power of at least 1 kW. Furthermore, the desired rare isotopes have a half-life decay rate of at least three months, have a measurable and precise alpha or gamma decay emission (but not a beta decay emission), and have a unique and repeatable isotope signature which cannot be imitated by other isotopes. Nonlimiting exemplary desired isotopes include .sub.64.sup.148Gd, .sub.76.sup.194Os, .sub.26.sup.60Fe, .sub.50.sup.126Sn, .sub.88.sup.228Ra, .sub.82.sup.210Pb, and the like. Other such rare isotopes may be employed beyond those specifically identified. However, .sub.14.sup.32Si, for example, is not desired since it is a pure beta emitter which makes it difficult to identify the specific isotope due to a lack of unique energies.

(16) While various embodiments have been disclosed, other embodiments may fall within the scope of the present invention. For example, the mask can have alternate external and/or hole shapes, such as elongated slots of straight or curved shapes. Additional or alternate accelerator, separator, catcher, stopper and jet equipment may be used as long as the facility is not commonly available and can produce rare isotopes accelerated with the above-specified energies and beam powers; such alternate equipment may lead to difference rates of isotope production as compared to FIGS. 4B-4F discussed hereinabove. Additional modifications can be made which fall within the scope and spirit of the present invention.