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Statements

Subject Item
n2:RIV%2F00216305%3A26220%2F14%3APU110332%21RIV15-MSM-26220___
rdf:type
n10:Vysledek skos:Concept
dcterms:description
Nuclear quadrupole resonant spectroscopy is method similar to nuclear magnetic resonant spectroscopy also called zero field NMR [1, 2]. The response signal magnitude is very low and it is immersed in to the noise. There can be used some methods to harvest signal from noise it can be matched receiver [3] or averaging. This authors describe detector for Nuclear quadrupole resonant spectroscopy based on statistic methods and probability of distribution, that allow to measure repetitive signals below noise level. The paper presents the mathematical model and practical solution of the detector, and problems such as the dynamic range and signal distortion based on the signal-to-noise ratio are also analyzed in the given context. If the time of signal occurrence is known, the repetitive signal below the noise level can be harvested out of noise by averaging because of the wanted signal is correlated therefor highlighted by averaging contrast to the noise which is not correlated so it is supressed by averagin Nuclear quadrupole resonant spectroscopy is method similar to nuclear magnetic resonant spectroscopy also called zero field NMR [1, 2]. The response signal magnitude is very low and it is immersed in to the noise. There can be used some methods to harvest signal from noise it can be matched receiver [3] or averaging. This authors describe detector for Nuclear quadrupole resonant spectroscopy based on statistic methods and probability of distribution, that allow to measure repetitive signals below noise level. The paper presents the mathematical model and practical solution of the detector, and problems such as the dynamic range and signal distortion based on the signal-to-noise ratio are also analyzed in the given context. If the time of signal occurrence is known, the repetitive signal below the noise level can be harvested out of noise by averaging because of the wanted signal is correlated therefor highlighted by averaging contrast to the noise which is not correlated so it is supressed by averagin
dcterms:title
Detector for Nuclear Quadrupole Resonance Spectroscopy Detector for Nuclear Quadrupole Resonance Spectroscopy
skos:prefLabel
Detector for Nuclear Quadrupole Resonance Spectroscopy Detector for Nuclear Quadrupole Resonance Spectroscopy
skos:notation
RIV/00216305:26220/14:PU110332!RIV15-MSM-26220___
n3:aktivita
n19:S
n3:aktivity
S
n3:dodaniDat
n14:2015
n3:domaciTvurceVysledku
n6:6157165 n6:3429016
n3:druhVysledku
n13:D
n3:duvernostUdaju
n5:S
n3:entitaPredkladatele
n9:predkladatel
n3:idSjednocenehoVysledku
10643
n3:idVysledku
RIV/00216305:26220/14:PU110332
n3:jazykVysledku
n17:eng
n3:klicovaSlova
Nuclear quadrupole resonance, Spectroscopy, Detector, noise, averaging, matched recieving, signal noise ratio.
n3:klicoveSlovo
n7:Detector n7:averaging n7:Spectroscopy n7:noise n7:Nuclear%20quadrupole%20resonance n7:signal%20noise%20ratio. n7:matched%20recieving
n3:kontrolniKodProRIV
[BFE2F784E178]
n3:mistoKonaniAkce
Guangzhou
n3:mistoVydani
Neuveden
n3:nazevZdroje
PIERS 2014 Guangzhou
n3:obor
n4:JA
n3:pocetDomacichTvurcuVysledku
2
n3:pocetTvurcuVysledku
2
n3:rokUplatneniVysledku
n14:2014
n3:tvurceVysledku
Kubásek, Radek Chytil, Jiří
n3:typAkce
n8:WRD
n3:zahajeniAkce
2014-08-25+02:00
s:numberOfPages
4
n18:hasPublisher
Neuveden
n20:isbn
978-1-934142-28-8
n11:organizacniJednotka
26220