US2004197816A1PendingUtilityA1

Two-dimensional spectral imaging system

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Assignee: QUANTUM DOT CORPPriority: Apr 6, 2000Filed: Apr 26, 2004Published: Oct 7, 2004
Est. expiryApr 6, 2020(expired)· nominal 20-yr term from priority
B01L 3/5025C40B 40/06B01J 2219/00677G01N 2035/00752G01N 21/272B82Y 30/00G01N 21/6456B01J 2219/00585B01L 2400/0457B01J 2219/00596G01N 21/6486G01N 21/6452G01N 2015/0092G01N 21/274B01L 2200/0668B01J 2219/00432B01J 2219/00659B01J 2219/00707G01N 2015/1497G01N 21/6428G01N 2021/6482B01J 2219/00743G01N 2035/00158G01N 2015/1472B01L 3/545B01L 2300/021B01J 2219/005G01N 21/6489B01J 2219/00578B01J 2219/00574G01N 2201/04B01J 2219/00657B01J 2219/00317B01L 2300/0819B01J 2219/00576G01N 2035/00742B01L 2400/0454G01N 2021/6441B01L 3/5085G01N 33/54373G01N 2201/06113B01L 3/502715G01N 21/278B01J 2219/00648C40B 60/14B01L 2300/0829B01J 2219/00722B01L 3/502761G01N 21/253G01N 21/25G01N 2201/12
55
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Claims

Abstract

Improved devices, systems, and methods for sensing and/or identifying signals from within a signal detection region are well-suited for identification of spectral codes. Large numbers of independently identifiable spectral codes can be generated by quite small bodies, and a plurality of such bodies or probes may be present within a detection region. Simultaneously imaging of identifiable spectra from throughout the detection region allows the probes to be identified. As the identifiable spectra can be treated as being generated from a point source within a much larger detection field, a prism, diffractive grading, holographic transmissive grading, or the like can spectrally disperse the images of the labels across a sensor surface. A CCD can identify the relative wavelengths of signals making up the spectra. Absolute signal wavelengths may be identified by determining positions of the labels, by an internal wavelength reference within the spectra, or the like.

Claims

exact text as granted — not AI-modified
What is claimed is:  
     
         1 . A method for identifying signals of differing strengths, the method comprising: 
 generating a plurality of signals in response to excitation energy, the signals comprising higher intensity signals and lower intensity signals;    sensing the lower intensity signals by simultaneously imaging the signals on a sensor; and    sequentially sensing at least some of the higher intensity signals.    
     
     
         2 . The method of  claim 1 , wherein at least one of the signals is generated by a semiconductor nanocrystal.  
     
     
         3 . The method of  claim 1 , wherein sensing the lower intensity signals comprises imaging for a first integration time, and wherein sequentially sensing the higher intensity signals comprises sequentially imaging for a second integration time shorter than the first integration time.  
     
     
         4 . The method of  claim 1 , further comprising filtering the higher intensity signals from the simultaneously imaged signals.  
     
     
         5 . The method of  claim 4 , wherein the higher intensity signals have wavelengths that are different than wavelengths of the lower intensity signals, and wherein the filtering step comprises wavelength filtering the higher intensity signals.  
     
     
         6 . The method of  claim 1 , wherein the higher intensity signals are sequentially sensed by scanning markers generating the signals, and wherein the markers generating the higher intensity signals are spatially intermingled with the markers generating the lower intensity signals.  
     
     
         7 . The method of  claim 6 , wherein the scanning step comprises scanning an aperture relative to the markers.  
     
     
         8 . The method of  claim 7 , wherein the scanning step comprises scanning a slit relative to the markers.  
     
     
         9 . The method of  claim 1 , wherein the excitation energy comprises a first energy, the first energy exciting high-energy markers to generate the high energy signals, and a second energy, the second energy exciting low-energy markers to generate the lower energy signals.  
     
     
         10 . The method of  claim 9 , wherein the second energy is less than the first energy, and wherein the second energy selectively excites the low energy markers.  
     
     
         11 . The method of  claim 1 , wherein the high intensity signals are generated by label markers and define an identifiable spectral code, and wherein the low intensity signals are generated by assay markers and indicate results of a plurality of assays, each assay having an associated spectral code.  
     
     
         12 . The method of  claim 11 , wherein the markers are supported by probe bodies to define probes, each probe comprising a label with at least one label marker to generate the spectral code, wherein at least one assay marker is associated with the probe to indicate results of an associated assay, and further comprising determining each assay result by identifying each label and correlating the label with the associated marker signal.

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