http://rdf.ncbi.nlm.nih.gov/pubchem/patent/EP-1265064-A1

Outgoing Links

Predicate Object
assignee http://rdf.ncbi.nlm.nih.gov/pubchem/patentassignee/MD5_9fb288f65e96bd2f0160b7b73b0c94e5
classificationCPCAdditional http://rdf.ncbi.nlm.nih.gov/pubchem/patentcpc/G01N2021-6463
classificationCPCInventive http://rdf.ncbi.nlm.nih.gov/pubchem/patentcpc/G01N21-6452
classificationIPCInventive http://rdf.ncbi.nlm.nih.gov/pubchem/patentipc/G01N21-64
filingDate 2002-05-22-04:00^^<http://www.w3.org/2001/XMLSchema#date>
inventor http://rdf.ncbi.nlm.nih.gov/pubchem/patentinventor/MD5_c3035b208b9ee565dff12599607e1832
publicationDate 2002-12-11-04:00^^<http://www.w3.org/2001/XMLSchema#date>
publicationNumber EP-1265064-A1
titleOfInvention Device for optically exciting fluorescence of selected samples on a multi-sample carrier
abstract The invention relates to an arrangement for reading out the fluorescent radiation fromnSample carriers with a large number of individual samples, for the excitation of thenFluorescence radiation in selected individual samples is a switchable electro-opticalnThere is a matrix for locally limited lighting.n n n The task of finding a new possibility for a locally differentiated illumination of a sample carrier (5) with a large number of samples using an electro-optical matrix (2) which, with high-resolution imaging of the electro-optical matrix (2) on the sample carrier (5) the excitation radiation contributing to the fluorescence signal is minimized, in an arrangement for reading out the fluorescence radiation of selected individual samples from multiprobe carriers (5) with a switchable electro-optical matrix (2) for generating a locally defined limited illumination, an optical system (3) for imaging the electro-optical matrix ( 2) on the sample carrier (5) and a highly sensitive photo receiver (7) for integral measurement of the fluorescence radiation of excited individual samples of the sample carrier (5), solved according to the invention by the electro-optical matrix (2) and the sample carrier (5) with respect to the optical axis (31 ) of the optical system (3) g are inclined and subject to a Scheimpflug condition and the inclination angle (α; β) of the electro-optical matrix (2) and of the sample carrier (5) are so large that the excitation radiation imaged by the light source unit (1) is reflected on the sample carrier (5) in such a way that essentially no excitation radiation reaches the detection beam path (53) ,
isCitedBy http://rdf.ncbi.nlm.nih.gov/pubchem/patent/WO-2008010182-A3
http://rdf.ncbi.nlm.nih.gov/pubchem/patent/WO-2008010182-A2
http://rdf.ncbi.nlm.nih.gov/pubchem/patent/TW-I493175-B
priorityDate 2001-06-07-04:00^^<http://www.w3.org/2001/XMLSchema#date>
type http://data.epo.org/linked-data/def/patent/Publication

Incoming Links

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isCitedBy http://rdf.ncbi.nlm.nih.gov/pubchem/patent/WO-0214838-A2
isDiscussedBy http://rdf.ncbi.nlm.nih.gov/pubchem/substance/SID226395793
http://rdf.ncbi.nlm.nih.gov/pubchem/compound/CID4911

Total number of triples: 18.