Rare earth spatial/spectral barcodes for multiplexed biochemical testing
US-9528145-B2 · Dec 27, 2016 · US
US2016200972A1 · US · A1
| Field | Value |
|---|---|
| Publication number | US-2016200972-A1 |
| Application number | US-201615077042-A |
| Country | US |
| Kind code | A1 |
| Filing date | Mar 22, 2016 |
| Priority date | Oct 28, 2012 |
| Publication date | Jul 14, 2016 |
| Grant date | — |
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A scintillation crystal can include Ln (1-y) RE y X 3 , wherein Ln represents a rare earth element, RE represents a different rare earth element, y has a value in a range of 0 to 1, and X represents a halogen. In an embodiment, the scintillation crystal is doped with a Group 1 element, a Group 2 element, or a mixture thereof, and the scintillation crystal is formed from a melt having a concentration of such elements or mixture thereof of at least approximately 0.02 wt. %. In another embodiment, the scintillation crystal can have unexpectedly improved proportionality and unexpectedly improved energy resolution properties. In a further embodiment, a radiation detection apparatus can include the scintillation crystal, a photosensor, and an electronics device. Such a radiation detection apparatus can be useful in a variety of applications.
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What is claimed is: 1 . A method, comprising: placing into a crucible precursors including: a rare earth halide precursor; and a dopant precursor that includes a halide of a Group 1 element or a Group 2 element; melting the precursors to form a melt, wherein a concentration of all Group 1 and Group 2 halides is at least approximately 0.02 wt. %; and forming a scintillation crystal including Ln (1-y) RE y X 3 :Me, wherein: Ln represents a rare earth element; RE represents a different rare earth element; y has a value in a range of 0 to 1; X represents a halogen; Me represents a Group 1 element, a Group 2 element, or any mixture thereof; and optically coupling an optical interface to the scintillation crystal. 2 . The method of claim 1 , wherein Me is Ca. 3 . The method of claim 1 , wherein Me is Li. 4 . The method of claim 1 , wherein the concentration of all Group 1 and Group 2 halides in the melt is no greater than approximately 1.0 wt. %. 5 . The method of claim 1 , wherein y is no greater than approximately 0.5 and at least approximately 0.005. 6 . The method of claim 1 , wherein y is in a range of approximately 0.01 to approximately 0.09. 7 . The method of claim 1 , wherein Ln is La, RE is Ce, and X is Br. 8 . The method of claim 1 , wherein y is approximately 1.0 f.u. 9 . The method of claim 1 , wherein for a radiation energy range of 13 keV to 30 keV, the scintillation crystal has a PR dev average of no greater than approximately 14%, or for a radiation energy range of 30 keV to 60 keV, the scintillation crystal has a PR dev average of no greater than approximately 8.0% 10 . The method of claim 1 , wherein: for a radiation energy range of 11 keV to 30 keV, the scintillation crystal has a PR dev average of no greater than approximately 8.0%; or for a radiation energy range of 30 keV to 60 keV, the scintillation crystal has the PR dev average of no greater than approximately 3.6%. 11 . The method of claim 1 , wherein an energy resolution ratio is an energy resolution of the scintillation crystal divided by a different energy resolution of a different scintillation crystal of a different composition, wherein the energy resolution ratio is: no greater than approximately 0.95 for an energy of 8 keV; no greater than approximately 0.95 for an energy of 13 keV; no greater than approximately 0.95 for an energy of 17 keV; no greater than approximately 0.95 for an energy of 22 keV; no greater than approximately 0.95 for an energy of 26 keV; no greater than approximately 0.95 for an energy of 32 keV; or no greater than approximately 0.97 for an energy of 44 keV. 12 . The method of claim 11 , wherein the energy resolution ratio is no greater than approximately 0.95 for the energy of 8 keV. 13 . The method of claim 11 , wherein the energy resolution ratio is no greater than approximately 0.95 for the energy of 13 keV. 14 . The method of claim 11 , wherein the energy resolution ratio is no greater than approximately 0.95 for the energy of 17 keV. 15 . The method of claim 11 , wherein the energy resolution ratio is no greater than approximately 0.95 for the energy of 22 keV. 16 . The method of claim 11 , wherein the energy resolution ratio is no greater than approximately 0.95 for the energy of 26 keV. 17 . The method of claim 11 , wherein an energy resolution ratio is no greater than approximately 0.95 for the energy of 32 keV. 18 . The method of claim 1 , further comprising optically coupling a photosensor to the optical interface. 19 . A method, comprising: placing into a crucible precursors including: a rare earth halide precursor; and a dopant precursor that includes a strontium halide, a barium halide, or any combination thereof; melting the precursors; forming a scintillation crystal including a rare earth halide, wherein: for a radiation energy range of 11 keV to 30 keV, the scintillation crystal has an nPR dev average of no greater than approximately 8.0%; or for a radiation energy range of 30 keV to 60 keV, the scintillation crystal has the nPR dev average of no greater than approximately 3.6%; and optically coupling an optical interface to the scintillation crystal. 20 . The method of claim 19 , further comprising optically coupling a photosensor to the optical interface.
Conversion screens for the conversion of the spatial distribution of X-rays or particle radiation into visible images, e.g. fluoroscopic screens (photographic processes using X-ray intensifiers G03C5/17; discharge tubes comprising luminescent screens H01J1/62; cathode ray tubes for X-ray conversion with optical output H01J31/50) · CPC title
with a phosphor layer · CPC title
using a combination of a scintillator and photodetector which measures the means radiation intensity · CPC title
Halogenides (C09K11/7767 takes precedence) · CPC title
with alkali or alkaline earth metal · CPC title
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