Helicity analysis of semileptonic hyperon decays including lepton-mass effects View Full Text


Ontology type: schema:ScholarlyArticle      Open Access: True


Article Info

DATE

2008-11-26

AUTHORS

A. Kadeer, J. G. Körner, U. Moosbrugger

ABSTRACT

Using the helicity method we derive complete formulas for the joint angular decay distributions occurring in semileptonic hyperon decays including lepton-mass and polarization effects. Compared to the traditional covariant calculation, the helicity method allows one to organize the calculation of the angular decay distributions in a very compact and efficient way. In the helicity method the angular analysis is of cascade type, i.e. each decay in the decay chain is analyzed in the respective rest system of that particle. Such an approach is ideally suited as input for a Monte Carlo event generation program. As a specific example we take the decay \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\Xi^{0}\to \Sigma^{+}+l^{-}+\bar{\nu}_{l}$\end{document} (l−=e−,μ−) followed by the nonleptonic decay Σ+→p+π0 for which we show a few examples of decay distributions which are generated from a Monte Carlo program based on the formulas presented in this paper. All the results of this paper are also applicable to the semileptonic and nonleptonic decays of ground-state charm and bottom baryons, and to the decays of the top quark. More... »

PAGES

27-47

References to SciGraph publications

  • 1962-12. The Σ→Λ+e+v decay as a test of the conserved vector current hypothesis in IL NUOVO CIMENTO (1955-1965)
  • 2002-11. Helicity analysis of the decays \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$B \to K^* \ell^+ \ell^-$\end{document} and \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$B \to \rho \ell \nu_\ell$\end{document} in the large energy effective theory in EUROPEAN PHYSICAL JOURNAL C
  • 1998-03. Inclusive semileptonic decays of polarized Λb Baryons into polarized τ-leptons in EUROPEAN PHYSICAL JOURNAL C
  • 1993-03. Joint angular decay distributions in exclusive weak decays of heavy mesons and baryons in ZEITSCHRIFT FÜR PHYSIK C PARTICLES AND FIELDS
  • 1990-06. The semileptonic decaysB→Mτν as a probe of hadron dynamics in ZEITSCHRIFT FÜR PHYSIK C PARTICLES AND FIELDS
  • 1991-12. Semi-leptonic charm baryon decays in the relativistic spectator quark model in ZEITSCHRIFT FÜR PHYSIK C PARTICLES AND FIELDS
  • 1992-09. T-odd andCP-odd triple momentum correlations in the exclusive semi-leptonic charm meson decayD→K*(Kπ)lvl in ZEITSCHRIFT FÜR PHYSIK C PARTICLES AND FIELDS
  • 1990-03. Exclusive semileptonic heavy meson decays including lepton mass effects in ZEITSCHRIFT FÜR PHYSIK C PARTICLES AND FIELDS
  • 1993-03. Complete angular analysis of the decay cascadeB→D** (→D*(→Dπ)+π+W(→lv) in ZEITSCHRIFT FÜR PHYSIK C PARTICLES AND FIELDS
  • 1968-04. Leptonic decays of baryons in ZEITSCHRIFT FÜR PHYSIK A HADRONS AND NUCLEI
  • 1988-09. Exclusive semi-leptonic decays of bottom mesons in the spectator quark model in ZEITSCHRIFT FÜR PHYSIK C PARTICLES AND FIELDS
  • 2007-10-24. Hyperon decay form factors in chiral perturbation theory in JOURNAL OF HIGH ENERGY PHYSICS
  • Identifiers

    URI

    http://scigraph.springernature.com/pub.10.1140/epjc/s10052-008-0801-5

    DOI

    http://dx.doi.org/10.1140/epjc/s10052-008-0801-5

    DIMENSIONS

    https://app.dimensions.ai/details/publication/pub.1011683054


    Indexing Status Check whether this publication has been indexed by Scopus and Web Of Science using the SN Indexing Status Tool
    Incoming Citations Browse incoming citations for this publication using opencitations.net

    JSON-LD is the canonical representation for SciGraph data.

    TIP: You can open this SciGraph record using an external JSON-LD service: JSON-LD Playground Google SDTT

    [
      {
        "@context": "https://springernature.github.io/scigraph/jsonld/sgcontext.json", 
        "about": [
          {
            "id": "http://purl.org/au-research/vocabulary/anzsrc-for/2008/02", 
            "inDefinedTermSet": "http://purl.org/au-research/vocabulary/anzsrc-for/2008/", 
            "name": "Physical Sciences", 
            "type": "DefinedTerm"
          }, 
          {
            "id": "http://purl.org/au-research/vocabulary/anzsrc-for/2008/0202", 
            "inDefinedTermSet": "http://purl.org/au-research/vocabulary/anzsrc-for/2008/", 
            "name": "Atomic, Molecular, Nuclear, Particle and Plasma Physics", 
            "type": "DefinedTerm"
          }, 
          {
            "id": "http://purl.org/au-research/vocabulary/anzsrc-for/2008/0206", 
            "inDefinedTermSet": "http://purl.org/au-research/vocabulary/anzsrc-for/2008/", 
            "name": "Quantum Physics", 
            "type": "DefinedTerm"
          }
        ], 
        "author": [
          {
            "affiliation": {
              "alternateName": "Institut f\u00fcr Physik, Johannes Gutenberg-Universit\u00e4t Mainz, Staudinger Weg 7, 55099, Mainz, Germany", 
              "id": "http://www.grid.ac/institutes/grid.5802.f", 
              "name": [
                "Institut f\u00fcr Physik, Johannes Gutenberg-Universit\u00e4t Mainz, Staudinger Weg 7, 55099, Mainz, Germany"
              ], 
              "type": "Organization"
            }, 
            "familyName": "Kadeer", 
            "givenName": "A.", 
            "id": "sg:person.07661571307.02", 
            "sameAs": [
              "https://app.dimensions.ai/discover/publication?and_facet_researcher=ur.07661571307.02"
            ], 
            "type": "Person"
          }, 
          {
            "affiliation": {
              "alternateName": "Institut f\u00fcr Physik, Johannes Gutenberg-Universit\u00e4t Mainz, Staudinger Weg 7, 55099, Mainz, Germany", 
              "id": "http://www.grid.ac/institutes/grid.5802.f", 
              "name": [
                "Institut f\u00fcr Physik, Johannes Gutenberg-Universit\u00e4t Mainz, Staudinger Weg 7, 55099, Mainz, Germany"
              ], 
              "type": "Organization"
            }, 
            "familyName": "K\u00f6rner", 
            "givenName": "J. G.", 
            "id": "sg:person.01301453175.98", 
            "sameAs": [
              "https://app.dimensions.ai/discover/publication?and_facet_researcher=ur.01301453175.98"
            ], 
            "type": "Person"
          }, 
          {
            "affiliation": {
              "alternateName": "Institut f\u00fcr Physik, Johannes Gutenberg-Universit\u00e4t Mainz, Staudinger Weg 7, 55099, Mainz, Germany", 
              "id": "http://www.grid.ac/institutes/grid.5802.f", 
              "name": [
                "Institut f\u00fcr Physik, Johannes Gutenberg-Universit\u00e4t Mainz, Staudinger Weg 7, 55099, Mainz, Germany"
              ], 
              "type": "Organization"
            }, 
            "familyName": "Moosbrugger", 
            "givenName": "U.", 
            "id": "sg:person.014505055365.36", 
            "sameAs": [
              "https://app.dimensions.ai/discover/publication?and_facet_researcher=ur.014505055365.36"
            ], 
            "type": "Person"
          }
        ], 
        "citation": [
          {
            "id": "sg:pub.10.1007/bf01565109", 
            "sameAs": [
              "https://app.dimensions.ai/details/publication/pub.1007413953", 
              "https://doi.org/10.1007/bf01565109"
            ], 
            "type": "CreativeWork"
          }, 
          {
            "id": "sg:pub.10.1007/bf01565586", 
            "sameAs": [
              "https://app.dimensions.ai/details/publication/pub.1036453911", 
              "https://doi.org/10.1007/bf01565586"
            ], 
            "type": "CreativeWork"
          }, 
          {
            "id": "sg:pub.10.1007/bf01584403", 
            "sameAs": [
              "https://app.dimensions.ai/details/publication/pub.1030641440", 
              "https://doi.org/10.1007/bf01584403"
            ], 
            "type": "CreativeWork"
          }, 
          {
            "id": "sg:pub.10.1140/epjc/s2002-01040-3", 
            "sameAs": [
              "https://app.dimensions.ai/details/publication/pub.1014979385", 
              "https://doi.org/10.1140/epjc/s2002-01040-3"
            ], 
            "type": "CreativeWork"
          }, 
          {
            "id": "sg:pub.10.1007/bf01245811", 
            "sameAs": [
              "https://app.dimensions.ai/details/publication/pub.1023943104", 
              "https://doi.org/10.1007/bf01245811"
            ], 
            "type": "CreativeWork"
          }, 
          {
            "id": "sg:pub.10.1007/bf01555846", 
            "sameAs": [
              "https://app.dimensions.ai/details/publication/pub.1013553727", 
              "https://doi.org/10.1007/bf01555846"
            ], 
            "type": "CreativeWork"
          }, 
          {
            "id": "sg:pub.10.1088/1126-6708/2007/10/083", 
            "sameAs": [
              "https://app.dimensions.ai/details/publication/pub.1032817681", 
              "https://doi.org/10.1088/1126-6708/2007/10/083"
            ], 
            "type": "CreativeWork"
          }, 
          {
            "id": "sg:pub.10.1007/bf01555745", 
            "sameAs": [
              "https://app.dimensions.ai/details/publication/pub.1005129794", 
              "https://doi.org/10.1007/bf01555745"
            ], 
            "type": "CreativeWork"
          }, 
          {
            "id": "sg:pub.10.1007/bf02440838", 
            "sameAs": [
              "https://app.dimensions.ai/details/publication/pub.1015345804", 
              "https://doi.org/10.1007/bf02440838"
            ], 
            "type": "CreativeWork"
          }, 
          {
            "id": "sg:pub.10.1007/bf02780378", 
            "sameAs": [
              "https://app.dimensions.ai/details/publication/pub.1053529674", 
              "https://doi.org/10.1007/bf02780378"
            ], 
            "type": "CreativeWork"
          }, 
          {
            "id": "sg:pub.10.1007/bf01421916", 
            "sameAs": [
              "https://app.dimensions.ai/details/publication/pub.1046217772", 
              "https://doi.org/10.1007/bf01421916"
            ], 
            "type": "CreativeWork"
          }, 
          {
            "id": "sg:pub.10.1007/bf01556008", 
            "sameAs": [
              "https://app.dimensions.ai/details/publication/pub.1012227930", 
              "https://doi.org/10.1007/bf01556008"
            ], 
            "type": "CreativeWork"
          }
        ], 
        "datePublished": "2008-11-26", 
        "datePublishedReg": "2008-11-26", 
        "description": "Using the helicity method we derive complete formulas for the joint angular decay distributions occurring in semileptonic hyperon decays including lepton-mass and polarization effects. Compared to the traditional covariant calculation, the helicity method allows one to organize the calculation of the angular decay distributions in a very compact and efficient way. In the helicity method the angular analysis is of cascade type, i.e. each decay in the decay chain is analyzed in the respective rest system of that particle. Such an approach is ideally suited as input for a Monte Carlo event generation program. As a specific example we take the decay \n\\documentclass[12pt]{minimal}\n\t\t\t\t\\usepackage{amsmath}\n\t\t\t\t\\usepackage{wasysym}\n\t\t\t\t\\usepackage{amsfonts}\n\t\t\t\t\\usepackage{amssymb}\n\t\t\t\t\\usepackage{amsbsy}\n\t\t\t\t\\usepackage{mathrsfs}\n\t\t\t\t\\usepackage{upgreek}\n\t\t\t\t\\setlength{\\oddsidemargin}{-69pt}\n\t\t\t\t\\begin{document}$\\Xi^{0}\\to \\Sigma^{+}+l^{-}+\\bar{\\nu}_{l}$\\end{document} \n\u2009(l\u2212=e\u2212,\u03bc\u2212) followed by the nonleptonic decay \u03a3+\u2192p+\u03c00 for which we show a few examples of decay distributions which are generated from a Monte Carlo program based on the formulas presented in this paper. All the results of this paper are also applicable to the semileptonic and nonleptonic decays of ground-state charm and bottom baryons, and to the decays of the top quark.", 
        "genre": "article", 
        "id": "sg:pub.10.1140/epjc/s10052-008-0801-5", 
        "inLanguage": "en", 
        "isAccessibleForFree": true, 
        "isPartOf": [
          {
            "id": "sg:journal.1049394", 
            "issn": [
              "1434-6044", 
              "1434-6052"
            ], 
            "name": "European Physical Journal C", 
            "publisher": "Springer Nature", 
            "type": "Periodical"
          }, 
          {
            "issueNumber": "1", 
            "type": "PublicationIssue"
          }, 
          {
            "type": "PublicationVolume", 
            "volumeNumber": "59"
          }
        ], 
        "keywords": [
          "helicity methods", 
          "method", 
          "complete formula", 
          "formula", 
          "angular decay distributions", 
          "decay distributions", 
          "distribution", 
          "hyperon decays", 
          "decay", 
          "effect", 
          "covariant calculation", 
          "calculations", 
          "efficient way", 
          "way", 
          "angular analysis", 
          "analysis", 
          "cascade type", 
          "types", 
          "decay chain", 
          "chain", 
          "rest system", 
          "system", 
          "particles", 
          "approach", 
          "input", 
          "generation program", 
          "program", 
          "specific examples", 
          "example", 
          "Monte Carlo program", 
          "Carlo program", 
          "results", 
          "bottom baryons", 
          "baryons", 
          "quarks", 
          "helicity analysis", 
          "joint angular decay distributions", 
          "semileptonic hyperon decays", 
          "lepton-mass", 
          "polarization effects", 
          "traditional covariant calculation", 
          "respective rest system", 
          "Monte Carlo event generation program", 
          "Carlo event generation program", 
          "event generation program", 
          "nonleptonic decays", 
          "paper", 
          "ground-state charm", 
          "charm", 
          "top quark", 
          "lepton-mass effects"
        ], 
        "name": "Helicity analysis of semileptonic hyperon decays including lepton-mass effects", 
        "pagination": "27-47", 
        "productId": [
          {
            "name": "dimensions_id", 
            "type": "PropertyValue", 
            "value": [
              "pub.1011683054"
            ]
          }, 
          {
            "name": "doi", 
            "type": "PropertyValue", 
            "value": [
              "10.1140/epjc/s10052-008-0801-5"
            ]
          }
        ], 
        "sameAs": [
          "https://doi.org/10.1140/epjc/s10052-008-0801-5", 
          "https://app.dimensions.ai/details/publication/pub.1011683054"
        ], 
        "sdDataset": "articles", 
        "sdDatePublished": "2021-12-01T19:20", 
        "sdLicense": "https://scigraph.springernature.com/explorer/license/", 
        "sdPublisher": {
          "name": "Springer Nature - SN SciGraph project", 
          "type": "Organization"
        }, 
        "sdSource": "s3://com-springernature-scigraph/baseset/20211201/entities/gbq_results/article/article_464.jsonl", 
        "type": "ScholarlyArticle", 
        "url": "https://doi.org/10.1140/epjc/s10052-008-0801-5"
      }
    ]
     

    Download the RDF metadata as:  json-ld nt turtle xml License info

    HOW TO GET THIS DATA PROGRAMMATICALLY:

    JSON-LD is a popular format for linked data which is fully compatible with JSON.

    curl -H 'Accept: application/ld+json' 'https://scigraph.springernature.com/pub.10.1140/epjc/s10052-008-0801-5'

    N-Triples is a line-based linked data format ideal for batch operations.

    curl -H 'Accept: application/n-triples' 'https://scigraph.springernature.com/pub.10.1140/epjc/s10052-008-0801-5'

    Turtle is a human-readable linked data format.

    curl -H 'Accept: text/turtle' 'https://scigraph.springernature.com/pub.10.1140/epjc/s10052-008-0801-5'

    RDF/XML is a standard XML format for linked data.

    curl -H 'Accept: application/rdf+xml' 'https://scigraph.springernature.com/pub.10.1140/epjc/s10052-008-0801-5'


     

    This table displays all metadata directly associated to this object as RDF triples.

    175 TRIPLES      22 PREDICATES      89 URIs      68 LITERALS      6 BLANK NODES

    Subject Predicate Object
    1 sg:pub.10.1140/epjc/s10052-008-0801-5 schema:about anzsrc-for:02
    2 anzsrc-for:0202
    3 anzsrc-for:0206
    4 schema:author Nbcc5c7fb368046c797d6f338aa2a936f
    5 schema:citation sg:pub.10.1007/bf01245811
    6 sg:pub.10.1007/bf01421916
    7 sg:pub.10.1007/bf01555745
    8 sg:pub.10.1007/bf01555846
    9 sg:pub.10.1007/bf01556008
    10 sg:pub.10.1007/bf01565109
    11 sg:pub.10.1007/bf01565586
    12 sg:pub.10.1007/bf01584403
    13 sg:pub.10.1007/bf02440838
    14 sg:pub.10.1007/bf02780378
    15 sg:pub.10.1088/1126-6708/2007/10/083
    16 sg:pub.10.1140/epjc/s2002-01040-3
    17 schema:datePublished 2008-11-26
    18 schema:datePublishedReg 2008-11-26
    19 schema:description Using the helicity method we derive complete formulas for the joint angular decay distributions occurring in semileptonic hyperon decays including lepton-mass and polarization effects. Compared to the traditional covariant calculation, the helicity method allows one to organize the calculation of the angular decay distributions in a very compact and efficient way. In the helicity method the angular analysis is of cascade type, i.e. each decay in the decay chain is analyzed in the respective rest system of that particle. Such an approach is ideally suited as input for a Monte Carlo event generation program. As a specific example we take the decay \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\Xi^{0}\to \Sigma^{+}+l^{-}+\bar{\nu}_{l}$\end{document}  (l−=e−,μ−) followed by the nonleptonic decay Σ+→p+π0 for which we show a few examples of decay distributions which are generated from a Monte Carlo program based on the formulas presented in this paper. All the results of this paper are also applicable to the semileptonic and nonleptonic decays of ground-state charm and bottom baryons, and to the decays of the top quark.
    20 schema:genre article
    21 schema:inLanguage en
    22 schema:isAccessibleForFree true
    23 schema:isPartOf N4e4bc119ba794c7f8a7f7d135d3e05ad
    24 Nffe1f9aadb1c40c1adba354fdd834361
    25 sg:journal.1049394
    26 schema:keywords Carlo event generation program
    27 Carlo program
    28 Monte Carlo event generation program
    29 Monte Carlo program
    30 analysis
    31 angular analysis
    32 angular decay distributions
    33 approach
    34 baryons
    35 bottom baryons
    36 calculations
    37 cascade type
    38 chain
    39 charm
    40 complete formula
    41 covariant calculation
    42 decay
    43 decay chain
    44 decay distributions
    45 distribution
    46 effect
    47 efficient way
    48 event generation program
    49 example
    50 formula
    51 generation program
    52 ground-state charm
    53 helicity analysis
    54 helicity methods
    55 hyperon decays
    56 input
    57 joint angular decay distributions
    58 lepton-mass
    59 lepton-mass effects
    60 method
    61 nonleptonic decays
    62 paper
    63 particles
    64 polarization effects
    65 program
    66 quarks
    67 respective rest system
    68 rest system
    69 results
    70 semileptonic hyperon decays
    71 specific examples
    72 system
    73 top quark
    74 traditional covariant calculation
    75 types
    76 way
    77 schema:name Helicity analysis of semileptonic hyperon decays including lepton-mass effects
    78 schema:pagination 27-47
    79 schema:productId Nc7dee86fe9204918b229b841c5b440dd
    80 Nd6ca340f442145b9834ce74c7f03adf3
    81 schema:sameAs https://app.dimensions.ai/details/publication/pub.1011683054
    82 https://doi.org/10.1140/epjc/s10052-008-0801-5
    83 schema:sdDatePublished 2021-12-01T19:20
    84 schema:sdLicense https://scigraph.springernature.com/explorer/license/
    85 schema:sdPublisher N151c33592c264fd3b743452229d80698
    86 schema:url https://doi.org/10.1140/epjc/s10052-008-0801-5
    87 sgo:license sg:explorer/license/
    88 sgo:sdDataset articles
    89 rdf:type schema:ScholarlyArticle
    90 N151c33592c264fd3b743452229d80698 schema:name Springer Nature - SN SciGraph project
    91 rdf:type schema:Organization
    92 N4ac65939b0b04e2bb30c979beb53f91d rdf:first sg:person.014505055365.36
    93 rdf:rest rdf:nil
    94 N4e4bc119ba794c7f8a7f7d135d3e05ad schema:issueNumber 1
    95 rdf:type schema:PublicationIssue
    96 Nbcc5c7fb368046c797d6f338aa2a936f rdf:first sg:person.07661571307.02
    97 rdf:rest Nc9dfe7478cc441878d43cde41806f737
    98 Nc7dee86fe9204918b229b841c5b440dd schema:name doi
    99 schema:value 10.1140/epjc/s10052-008-0801-5
    100 rdf:type schema:PropertyValue
    101 Nc9dfe7478cc441878d43cde41806f737 rdf:first sg:person.01301453175.98
    102 rdf:rest N4ac65939b0b04e2bb30c979beb53f91d
    103 Nd6ca340f442145b9834ce74c7f03adf3 schema:name dimensions_id
    104 schema:value pub.1011683054
    105 rdf:type schema:PropertyValue
    106 Nffe1f9aadb1c40c1adba354fdd834361 schema:volumeNumber 59
    107 rdf:type schema:PublicationVolume
    108 anzsrc-for:02 schema:inDefinedTermSet anzsrc-for:
    109 schema:name Physical Sciences
    110 rdf:type schema:DefinedTerm
    111 anzsrc-for:0202 schema:inDefinedTermSet anzsrc-for:
    112 schema:name Atomic, Molecular, Nuclear, Particle and Plasma Physics
    113 rdf:type schema:DefinedTerm
    114 anzsrc-for:0206 schema:inDefinedTermSet anzsrc-for:
    115 schema:name Quantum Physics
    116 rdf:type schema:DefinedTerm
    117 sg:journal.1049394 schema:issn 1434-6044
    118 1434-6052
    119 schema:name European Physical Journal C
    120 schema:publisher Springer Nature
    121 rdf:type schema:Periodical
    122 sg:person.01301453175.98 schema:affiliation grid-institutes:grid.5802.f
    123 schema:familyName Körner
    124 schema:givenName J. G.
    125 schema:sameAs https://app.dimensions.ai/discover/publication?and_facet_researcher=ur.01301453175.98
    126 rdf:type schema:Person
    127 sg:person.014505055365.36 schema:affiliation grid-institutes:grid.5802.f
    128 schema:familyName Moosbrugger
    129 schema:givenName U.
    130 schema:sameAs https://app.dimensions.ai/discover/publication?and_facet_researcher=ur.014505055365.36
    131 rdf:type schema:Person
    132 sg:person.07661571307.02 schema:affiliation grid-institutes:grid.5802.f
    133 schema:familyName Kadeer
    134 schema:givenName A.
    135 schema:sameAs https://app.dimensions.ai/discover/publication?and_facet_researcher=ur.07661571307.02
    136 rdf:type schema:Person
    137 sg:pub.10.1007/bf01245811 schema:sameAs https://app.dimensions.ai/details/publication/pub.1023943104
    138 https://doi.org/10.1007/bf01245811
    139 rdf:type schema:CreativeWork
    140 sg:pub.10.1007/bf01421916 schema:sameAs https://app.dimensions.ai/details/publication/pub.1046217772
    141 https://doi.org/10.1007/bf01421916
    142 rdf:type schema:CreativeWork
    143 sg:pub.10.1007/bf01555745 schema:sameAs https://app.dimensions.ai/details/publication/pub.1005129794
    144 https://doi.org/10.1007/bf01555745
    145 rdf:type schema:CreativeWork
    146 sg:pub.10.1007/bf01555846 schema:sameAs https://app.dimensions.ai/details/publication/pub.1013553727
    147 https://doi.org/10.1007/bf01555846
    148 rdf:type schema:CreativeWork
    149 sg:pub.10.1007/bf01556008 schema:sameAs https://app.dimensions.ai/details/publication/pub.1012227930
    150 https://doi.org/10.1007/bf01556008
    151 rdf:type schema:CreativeWork
    152 sg:pub.10.1007/bf01565109 schema:sameAs https://app.dimensions.ai/details/publication/pub.1007413953
    153 https://doi.org/10.1007/bf01565109
    154 rdf:type schema:CreativeWork
    155 sg:pub.10.1007/bf01565586 schema:sameAs https://app.dimensions.ai/details/publication/pub.1036453911
    156 https://doi.org/10.1007/bf01565586
    157 rdf:type schema:CreativeWork
    158 sg:pub.10.1007/bf01584403 schema:sameAs https://app.dimensions.ai/details/publication/pub.1030641440
    159 https://doi.org/10.1007/bf01584403
    160 rdf:type schema:CreativeWork
    161 sg:pub.10.1007/bf02440838 schema:sameAs https://app.dimensions.ai/details/publication/pub.1015345804
    162 https://doi.org/10.1007/bf02440838
    163 rdf:type schema:CreativeWork
    164 sg:pub.10.1007/bf02780378 schema:sameAs https://app.dimensions.ai/details/publication/pub.1053529674
    165 https://doi.org/10.1007/bf02780378
    166 rdf:type schema:CreativeWork
    167 sg:pub.10.1088/1126-6708/2007/10/083 schema:sameAs https://app.dimensions.ai/details/publication/pub.1032817681
    168 https://doi.org/10.1088/1126-6708/2007/10/083
    169 rdf:type schema:CreativeWork
    170 sg:pub.10.1140/epjc/s2002-01040-3 schema:sameAs https://app.dimensions.ai/details/publication/pub.1014979385
    171 https://doi.org/10.1140/epjc/s2002-01040-3
    172 rdf:type schema:CreativeWork
    173 grid-institutes:grid.5802.f schema:alternateName Institut für Physik, Johannes Gutenberg-Universität Mainz, Staudinger Weg 7, 55099, Mainz, Germany
    174 schema:name Institut für Physik, Johannes Gutenberg-Universität Mainz, Staudinger Weg 7, 55099, Mainz, Germany
    175 rdf:type schema:Organization
     




    Preview window. Press ESC to close (or click here)


    ...