Patent Application
20120104256
The technical field relates generally to a method and validation apparatus for authenticating a stationary value document using emitted infrared emission characteristics from one or more covert compositions incorporated on or within a value document when excited by an incident light pulse.
There are many ways to validate or authenticate a value document, from simple to complex. Some methods involve visible, also referred to as overt, features on or incorporated into a document, such as a hologram on a credit card, an embossed image or watermark on a bank note, a security foil, a security ribbon, colored threads or colored fibers within a bank note, or a floating and/or sinking image on a passport. While these features are easy to detect with the human eye and generally do not require equipment for authentication, these overt features are easily identified by a would-be forger and/or counterfeiter. As such, hidden, also referred to as covert, features may be incorporated in value documents, either in lieu of or in addition to overt features. Covert features can include invisible fluorescent fibers, chemically sensitive stains, fluorescent pigments or dyes that are incorporated into the substrate of the value document. Covert features can also be included in the ink that is printed onto the substrate of the value document or within the resin used to make films that are used in laminated value documents. Since covert features are not detectable by the human eye, detectors configured to detect these covert features are needed to authenticate the value document.
Some covert features incorporate taggants that absorb radiation from a light source and emit detectable radiation having properties, such as wavelength and decay time, which can be used to determine whether the value document incorporating the feature is authentic. For example, some covert taggants use rare earth active ions that have been incorporated into oxide crystal lattices. Most oxide crystal lattices are essentially closed packed structures of oxygen ions where metallic ions may be connected to oxygen atoms of the crystal lattice resulting in symmetries of the crystal fields. Oxide crystals typically result in rapid decay of absorbed radiation to a storage energy level followed by decay to lower energy levels. When such covert taggants are illuminated by a light source, they tend to have a peak in their intensity of emitted radiation that corresponds to the point in time when the light source is shut off and thereafter, the emitted radiation exhibits rapid emission decay.
The present technology relates to the use of covert taggants in or on a value document or other article, and particularly to the use of taggants that absorb radiation from an illumination source during an illumination period, and emit radiation in a manner that exhibits a peak intensity at a point in time after the end of an illumination duration, when the illumination source is switched off.
In one aspect, a method of authenticating a value document or other article using an authentication apparatus is provided that includes providing a value document or other article to the authentication apparatus, the value document or other article comprising at least one taggant having a crystal lattice doped with a first rare earth active ion. The method also includes applying radiation having a first wavelength from an illumination source of the authentication apparatus to the value document or other article for an illumination duration. The taggant absorbs radiation from the illumination source and emits infrared radiation having a second wavelength that is greater than the first wavelength of the radiation, the infrared radiation emitted from the taggant having a maximum intensity that occurs at a delay period measured from the end of the illumination duration, the delay period being greater than about 0.1 milliseconds. The method further includes detecting intensity of the emitted infrared radiation over time with a sensor of the authentication apparatus to produce emission data, then processing the emission data with a processor of the authentication apparatus to determine whether the value document or other article is authentic, wherein the processing includes identifying the maximum intensity of the emitted infrared radiation that occurs after the illumination source is switched off and comparing the measure maximum intensity with predetermined authentic data.
In another aspect, a value document or other article is provided that includes a covert feature. The value document or other article comprises at least one taggant having a crystal lattice doped with a first rare earth active ion, the taggant being configured to absorb radiation having a first wavelength from an illumination source during an illumination duration having an end, and to emit infrared radiation having a second wavelength that is greater than the first wavelength of the radiation from the illumination source. The infrared radiation emitted from the taggant has a maximum intensity that occurs at a delay period measured from the end of the illumination duration, the delay period being greater than about 0.1 milliseconds.
In a third aspect, an authentication apparatus is provided that includes an illumination source, a sensor, and a processor. The illumination source applies radiation having a first wavelength to a value document or other article for an illumination duration having an end. The sensor detects intensity of infrared radiation emitted from the value document or other article over time to produce emission data, the infrared radiation emitted from the value document or other article having a second wavelength greater than the first wavelength and having a maximum intensity that occurs at a delay period measured from the end of the illumination duration, the delay period being greater than about 0.1 milliseconds. The processor processes the emission data and identifies the maximum intensity of the emitted infrared radiation that occurs after the delay period in order to compare the emission data to predetermined authentic data to further determine whether the value document or other article is authentic.
Specific examples have been chosen for purposes of illustration and description, and are shown in the accompanying drawings, forming a part of the specification.
The present technology relates to authentication features that can be incorporated into or onto value documents or other articles, and can be detected using authentication apparatuses as described herein. The authentication features use one or more taggants that absorb radiation from an illumination source that is switched on during an illumination duration and is switched off at the end of the illumination duration. The illumination source is then kept off during an off duration. Once radiation is absorbed, the taggants emit infrared radiation in a manner having a maximum intensity that occurs after the end of the illumination duration (i.e., when the illumination source is switched off). The illumination source can function in a periodic pulsed manner, providing a plurality of illumination durations, where each illumination duration is separated by an off duration, during which the illumination source is switched off. The length of time of each illumination duration is preferably identical, and the length of time of each off duration is also preferably identical. The length of time of each illumination duration may be selected based upon the properties of the authentic taggant, and is preferably sufficiently short to facilitate the occurrence of the maximum emission intensity at a detectable delay period after the end of the illumination period. The length of time of each off duration may also be selected based upon the properties of the authentic taggant, and is preferably sufficiently long to allow for the taggant emission to decay to zero before repeating the illumination duration. The use of periodic pulsed illumination allows for numerous data sets to be measured and recorded in the emission data that is collected by the authentication apparatus. The emission data having a number of data sets can then be statistically analyzed to achieve a higher degree of temporal accuracy.
Taggants of the present technology are incorporated into or onto an article, such as a value document (e.g., a banknote, a check, a stock certificate) or other article (e.g., an identification card, a driver's license, a passport, identity papers, a document, a paper, a packaging component, a credit card, a bank card, a label, a seal, a postage stamp, a token, a liquid, a human, an animal, and a biological sample), in various embodiments. The taggants may be in the form of particles, for example, which may be mixed with substrate material, ink (e.g., a clear or colored ink) or other printed feature material (e.g., a pigment or paint), a coating, or other components of the value document or article. The value documents or other articles can include a substrate, a carrier, an embedded feature, a surface-applied feature, and/or a printed material. For example, but not by way of limitation,
Taggants of the present technology comprise a crystalline composition that includes a host crystal lattice doped with at least a first rare earth active ion. In some examples, the crystal lattice is doped with a second rare earth active ion. The host crystal lattice material, first rare earth active ion, and any second rare earth active ion can be selected and incorporated as the taggant in order to provide the desired properties of the taggant. For example, the taggant may be selected to exhibit a relatively rapid absorption of the radiation from the illumination source during the illumination duration, and may initially store the absorbed radiation in a first storage energy level, which may be a transient storage energy level. The taggant may then transfer absorbed energy from the first storage energy level to a second storage energy level, which may be an emitting storage energy level, and may then emit infrared radiation from that second storage energy level. Since there can be a difference in the decay values of Tau between the two energy levels, it is possible to see the population of the second storage energy level increase after the illumination has been turned off. This can occur when the decay constant of the second level is less than the decay rate of the level supplying it. In at least one such example, the intensity of the emitted radiation continues to build after the end illumination duration, during the off duration when the illumination source is switched off, building to a maximum, or peak, intensity over a delay period, and then decaying. The delay period is measured from the end of the illumination duration, and is the amount of time that it takes for the intensity of the emitted radiation to reach its maximum. The decay of the intensity of the emitted radiation after the delay period can be an exponential decay combined with any residual energy flow continuing into the second storage level.
When the maximum, or peak, intensity of the infrared radiation emitted from the taggant occurs at a sufficient delay period, the maximum intensity can be detected by conventional infrared detectors and is processed by conventional electronics. The delay period is preferably greater than about 0.1 milliseconds, greater than about 0.2 milliseconds, or greater than about 0.5 milliseconds. For example, the delay period can be from about 0.1 milliseconds to about 5 milliseconds.
Suitable crystalline lattices that can be used as host materials include inorganic crystalline lattices selected from oxyfluorides, fluorides, and oxysulfides, while other crystalline lattices may be used in some examples. Without being bound by any particular theory, it is believed that at least some of the temporal behavior of the taggants is a result of using crystal lattices in which other atoms such as sulfur or fluorine replace oxygen ions thereby resulting in a corresponding lattice distortion. In some examples, the crystalline lattice can be yttrium oxysulfide, sodium ytterbium fluoride, or sodium yttrium fluoride.
The first rare earth active ion can be selected such that it absorbs radiation having a first wavelength from the illumination source into a first storage energy level and transfers non-radiatively the absorbed radiation to a second storage energy level, which can be a storage energy level of the first or second rare earth ion. The second storage energy level can decay radiatively to a lower energy level by emitting infrared radiation having a second wavelength as a down converter. The second wavelength is greater than the first wavelength of the radiation from the illumination source that is absorbed by the first rare earth active ion.
The first rare earth active ion preferably absorbs radiation from the illumination source by narrow or broad band absorption. The absorption by the first rare earth active ion is preferably very rapid, such as being below about 0.01 milliseconds. The first rare earth active ion can transfer the absorbed radiation to the second storage energy level at a lifetime τ1, and the second storage energy level can have a lifetime τ2. The lifetime τ1 is preferably from about 50% of τ2 to about 95% of τ2. In at least one example, τ2 can be from about 1.5 milliseconds to about 10 milliseconds, and τ1 can be from about 1 millisecond to about 9 milliseconds. Given the rapid absorption of the radiation from the illumination source, illumination duration is preferably for an amount of time τ3, which can be from about 0.1 milliseconds to about 1 millisecond, or that is from about 4% of τ2 to about 10% of τ2.
Periodic pulsed illumination is preferably used, wherein the illumination source is turned on and off in a repetitive, periodic pulsed manner to provide a plurality of illumination durations separated by a plurality of off durations, and data is gathered during each repetition. Repetitive periodic pulsed illumination allows for a plurality of data sets to be measured and recorded in the emission data, which can then be analyzed, and can allow the use of statistics in the computation section of the authentication apparatus through signal averaging techniques. The off duration, which is the amount of time that the illumination source is turned off between illumination durations, should be greater than the delay period, and should be greater than the delay period and the decay period combined, and is preferably greater than the time during which the intensity of the radiation emitted from the taggant falls to zero.
Erbium (Er) is one example of a preferred first rare earth active ion for use in the taggants of the present technology. The use of erbium allows taggants to absorb visible or infrared radiation from the illumination source as a narrow or a band absorber. A band or line absorber absorbs incident infrared radiation over a wide or narrow spectral range depending on the absorption characteristics of the ions, and therefore can be sufficiently excited by infrared illumination sources such as, for example, a 660 nanometer (nm) red LED light source, which targets one the 4F9/2 strong absorption bands of erbium. The emission from the first storage energy level of the erbium rare earth active ion can be at about 980 nm using the 4I11/2 to 4I15/2 transition, which is in the infrared wavelength range whose energy storage arises from the non-radiative decay of the 4F9/2 absorption band to the 4I11/2 storage level.
Ytterbium (Yb) is one example of a preferred second rare earth active ion for use in the taggants of the present technology. Ytterbium acts well as an acceptor ion for energy transfer from other rare earth or transition metal ions (e.g., erbium).
Both erbium and ytterbium exhibit a long lifetime storage energy level that is charged at slow enough rates so that the decay constant of the second level is less than the decay rate of the level supplying it. Thus, the second storage level continues to charge after the illumination duration, when the illumination source is switched off, producing a maximum in the emitted intensity after a delay period measured from the end of the illumination duration. In examples where erbium and ytterbium are incorporated in yttrium oxysulfide, sodium yttrium fluoride or sodium ytterbium fluoride crystal lattices, erbium tends to emit at about 980 nm characteristic wavelength, while ytterbium tends to emit emits at about 1030 nm characteristic wavelength. In this case, the absorption can take place in the 4F9/2 level typically using a 660 nm LED as the illumination source. The energy from the 4F9/2 level non-radiatively decays the 4I11/2 erbium level. The energy from that erbium level can then non-radiatively transfer to the 2F5/2 level of ytterbium. Emission at about 1030 nm then takes place on the radiative 2F5/2 to the 2F7/2 ytterbium transition. The amount of emission on the various transitions depends upon the dopant levels of the substitute ions.
In view of the properties designed into the taggants of the present technology, authentication apparatuses 1000 of the present technology can include an illumination source 1002, a sensor 1004, and a processor 1006, as shown in
From the foregoing, it will be appreciated that, although specific examples have been described herein for purposes of illustration, various modifications may be made without deviating from the spirit or scope of this disclosure. It is therefore intended that the foregoing detailed description be regarded as illustrative rather than limiting, and that it be understood that it is the following claims, including all equivalents, that are intended to particularly point out and distinctly claim the claimed subject matter.
This application claims priority to co-pending, U.S. Provisional Application Ser. No. 61/408,817, filed on Nov. 1, 2010.
| Number | Date | Country | |
|---|---|---|---|
| 61408817 | Nov 2010 | US |
