Please use this identifier to cite or link to this item:
https://physrep.ff.bg.ac.rs/handle/123456789/625
DC Field | Value | Language |
---|---|---|
dc.contributor.author | Damnjanović, Milan | en |
dc.contributor.author | Milošević, Ivanka | en |
dc.date.accessioned | 2022-07-12T16:23:42Z | - |
dc.date.available | 2022-07-12T16:23:42Z | - |
dc.date.issued | 2010-09-01 | en |
dc.identifier.isbn | 9783642111716 | en |
dc.identifier.issn | 0075-8450 | en |
dc.identifier.uri | https://physrep.ff.bg.ac.rs/handle/123456789/625 | - |
dc.description.abstract | Each physical quantity is a particular type of a line group tensor, i.e., it is changed in a specific way when line group transformations are applied. Quite generally, the transformation is described by a representation of a line group, and its irreducible components single out irreducible tensors. One important class is various functions, in particular quantum mechanical wave functions, among which symmetry-adapted basis consists of harmonics and covariants. Also, irreducible components of polar and axial vectors and second-rank tensors are found. © 2010 Springer-Verlag Berlin Heidelberg. | en |
dc.relation.ispartof | Lecture Notes in Physics | en |
dc.title | Tensors | en |
dc.type | Article | en |
dc.identifier.doi | 10.1007/978-3-642-11172-3_5 | en |
dc.identifier.scopus | 2-s2.0-77956020526 | en |
dc.identifier.url | https://api.elsevier.com/content/abstract/scopus_id/77956020526 | en |
dc.relation.volume | 801 | en |
dc.relation.firstpage | 65 | en |
dc.relation.lastpage | 84 | en |
item.openairetype | Article | - |
item.cerifentitytype | Publications | - |
item.fulltext | No Fulltext | - |
item.openairecristype | http://purl.org/coar/resource_type/c_18cf | - |
item.grantfulltext | none | - |
crisitem.author.orcid | 0000-0001-6885-7201 | - |
Appears in Collections: | Journal Article |
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