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pubmed-article:17919022rdf:typepubmed:Citationlld:pubmed
pubmed-article:17919022lifeskim:mentionsumls-concept:C0028158lld:lifeskim
pubmed-article:17919022lifeskim:mentionsumls-concept:C0009264lld:lifeskim
pubmed-article:17919022lifeskim:mentionsumls-concept:C1521991lld:lifeskim
pubmed-article:17919022lifeskim:mentionsumls-concept:C0337196lld:lifeskim
pubmed-article:17919022lifeskim:mentionsumls-concept:C0681019lld:lifeskim
pubmed-article:17919022pubmed:issue13lld:pubmed
pubmed-article:17919022pubmed:dateCreated2007-10-8lld:pubmed
pubmed-article:17919022pubmed:abstractTextTheory and experiment are combined in a novel approach aimed at establishing a set of two-body state-to-state rates for elementary processes ij --> lm in low temperature N(2):N(2) collisions involving the rotational states i,j,l,m. First, a set of 148 collision cross sections is calculated as a function of the collision energy at the converged close-coupled level via the MOLSCAT code, using a recent potential energy surface for N(2)-N(2). Then, the corresponding rates for the range of 2 < or = T < or = 50 K are derived from the cross sections. The link between theory and experiment, aimed at assessing the calculated rates, is a master equation which accounts for the time evolution of rotational populations in a reference volume of gas in terms of the collision rates. In the experiment, the evolution of rotational populations is measured by Raman spectroscopy in a tiny reference volume (approximately 2 x 10(-3) mm(3)) of N(2) traveling along the axis of a supersonic jet. The calculated collisional rates are assessed experimentally in the range of 4 < or = T < or = 35 K by means of the master equation, and then are scaled by averaging over a large set of experimental data. The scaled rates account accurately for the evolution of the rotational populations measured in a wide range of conditions. Accuracy of 10% is estimated for the main scaled rates.lld:pubmed
pubmed-article:17919022pubmed:languageenglld:pubmed
pubmed-article:17919022pubmed:journalhttp://linkedlifedata.com/r...lld:pubmed
pubmed-article:17919022pubmed:statusPubMed-not-MEDLINElld:pubmed
pubmed-article:17919022pubmed:monthOctlld:pubmed
pubmed-article:17919022pubmed:issn0021-9606lld:pubmed
pubmed-article:17919022pubmed:authorpubmed-author:MonteroSSlld:pubmed
pubmed-article:17919022pubmed:authorpubmed-author:RamosAAlld:pubmed
pubmed-article:17919022pubmed:authorpubmed-author:FernándezJ...lld:pubmed
pubmed-article:17919022pubmed:authorpubmed-author:ThibaultFFlld:pubmed
pubmed-article:17919022pubmed:authorpubmed-author:TejedaGGlld:pubmed
pubmed-article:17919022pubmed:authorpubmed-author:FonfríaJ PJPlld:pubmed
pubmed-article:17919022pubmed:issnTypePrintlld:pubmed
pubmed-article:17919022pubmed:day7lld:pubmed
pubmed-article:17919022pubmed:volume127lld:pubmed
pubmed-article:17919022pubmed:ownerNLMlld:pubmed
pubmed-article:17919022pubmed:authorsCompleteYlld:pubmed
pubmed-article:17919022pubmed:pagination134305lld:pubmed
pubmed-article:17919022pubmed:year2007lld:pubmed
pubmed-article:17919022pubmed:articleTitleInelastic collisions in molecular nitrogen at low temperature (2 < or = T < or = 50 K).lld:pubmed
pubmed-article:17919022pubmed:affiliationInstituto de Estructura de la Materia, CSIC, Serrano 121, 28006 Madrid, Spain.lld:pubmed
pubmed-article:17919022pubmed:publicationTypeJournal Articlelld:pubmed