Partial coherence in heavy-ion reactions
First- and second-order interferences are investigated for fluctuating cross sections with average angular distributions <dσ/dΩ> not necessarily symmetric about 90^o. This is expected to be relevant for reactions between light complex nuclei where discrete final states are populated through an...
Ausführliche Beschreibung
Autor*in: |
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Englisch |
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1982 |
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Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 |
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Übergeordnetes Werk: |
in: Nuclear Physics, Section A - Amsterdam : Elsevier, 380(1982), 1, Seite 170-188 |
Übergeordnetes Werk: |
volume:380 ; year:1982 ; number:1 ; pages:170-188 |
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NLEJ181378817 |
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520 | |a First- and second-order interferences are investigated for fluctuating cross sections with average angular distributions <dσ/dΩ> not necessarily symmetric about 90^o. This is expected to be relevant for reactions between light complex nuclei where discrete final states are populated through an intermediate deep-inelastic or precompound process. We obtain <dσ/dΩ> as a sum of coherent and incoherent contributions from either side of the interaction region. The period of the oscillations present in <dσ/dΩ> as well as in the angular cross-correlation function is determined by a characteristic angular momentum Λ. while the damping of these oscillations depends on two angular momentum widths Δ and δ, which characterize the range of contributing partial waves and their phase correlation length, respectively. Using gaussian distributions simple formulae are derived by means of which the quantities Λ, Δ and δ may be extracted directly from the data. In the limit δ = 0 we obtain a transparent description of heavy-ion compound reactions. The excitation function exhibits gross structure whose period is determined by Λ(E). | ||
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(DE-627)NLEJ181378817 (DE-599)GBVNLZ181378817 DE-627 ger DE-627 rakwb eng Partial coherence in heavy-ion reactions 1982 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier First- and second-order interferences are investigated for fluctuating cross sections with average angular distributions <dσ/dΩ> not necessarily symmetric about 90^o. This is expected to be relevant for reactions between light complex nuclei where discrete final states are populated through an intermediate deep-inelastic or precompound process. We obtain <dσ/dΩ> as a sum of coherent and incoherent contributions from either side of the interaction region. The period of the oscillations present in <dσ/dΩ> as well as in the angular cross-correlation function is determined by a characteristic angular momentum Λ. while the damping of these oscillations depends on two angular momentum widths Δ and δ, which characterize the range of contributing partial waves and their phase correlation length, respectively. Using gaussian distributions simple formulae are derived by means of which the quantities Λ, Δ and δ may be extracted directly from the data. In the limit δ = 0 we obtain a transparent description of heavy-ion compound reactions. The excitation function exhibits gross structure whose period is determined by Λ(E). Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Hartmann, K.M. oth Dunnweber, W. oth Frahn, W.E. oth in Nuclear Physics, Section A Amsterdam : Elsevier 380(1982), 1, Seite 170-188 (DE-627)NLEJ177217928 (DE-600)1466542-6 0375-9474 nnns volume:380 year:1982 number:1 pages:170-188 http://linkinghub.elsevier.com/retrieve/pii/0375-9474(82)90588-7 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 380 1982 1 170-188 |
spelling |
(DE-627)NLEJ181378817 (DE-599)GBVNLZ181378817 DE-627 ger DE-627 rakwb eng Partial coherence in heavy-ion reactions 1982 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier First- and second-order interferences are investigated for fluctuating cross sections with average angular distributions <dσ/dΩ> not necessarily symmetric about 90^o. This is expected to be relevant for reactions between light complex nuclei where discrete final states are populated through an intermediate deep-inelastic or precompound process. We obtain <dσ/dΩ> as a sum of coherent and incoherent contributions from either side of the interaction region. The period of the oscillations present in <dσ/dΩ> as well as in the angular cross-correlation function is determined by a characteristic angular momentum Λ. while the damping of these oscillations depends on two angular momentum widths Δ and δ, which characterize the range of contributing partial waves and their phase correlation length, respectively. Using gaussian distributions simple formulae are derived by means of which the quantities Λ, Δ and δ may be extracted directly from the data. In the limit δ = 0 we obtain a transparent description of heavy-ion compound reactions. The excitation function exhibits gross structure whose period is determined by Λ(E). Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Hartmann, K.M. oth Dunnweber, W. oth Frahn, W.E. oth in Nuclear Physics, Section A Amsterdam : Elsevier 380(1982), 1, Seite 170-188 (DE-627)NLEJ177217928 (DE-600)1466542-6 0375-9474 nnns volume:380 year:1982 number:1 pages:170-188 http://linkinghub.elsevier.com/retrieve/pii/0375-9474(82)90588-7 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 380 1982 1 170-188 |
allfields_unstemmed |
(DE-627)NLEJ181378817 (DE-599)GBVNLZ181378817 DE-627 ger DE-627 rakwb eng Partial coherence in heavy-ion reactions 1982 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier First- and second-order interferences are investigated for fluctuating cross sections with average angular distributions <dσ/dΩ> not necessarily symmetric about 90^o. This is expected to be relevant for reactions between light complex nuclei where discrete final states are populated through an intermediate deep-inelastic or precompound process. We obtain <dσ/dΩ> as a sum of coherent and incoherent contributions from either side of the interaction region. The period of the oscillations present in <dσ/dΩ> as well as in the angular cross-correlation function is determined by a characteristic angular momentum Λ. while the damping of these oscillations depends on two angular momentum widths Δ and δ, which characterize the range of contributing partial waves and their phase correlation length, respectively. Using gaussian distributions simple formulae are derived by means of which the quantities Λ, Δ and δ may be extracted directly from the data. In the limit δ = 0 we obtain a transparent description of heavy-ion compound reactions. The excitation function exhibits gross structure whose period is determined by Λ(E). Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Hartmann, K.M. oth Dunnweber, W. oth Frahn, W.E. oth in Nuclear Physics, Section A Amsterdam : Elsevier 380(1982), 1, Seite 170-188 (DE-627)NLEJ177217928 (DE-600)1466542-6 0375-9474 nnns volume:380 year:1982 number:1 pages:170-188 http://linkinghub.elsevier.com/retrieve/pii/0375-9474(82)90588-7 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 380 1982 1 170-188 |
allfieldsGer |
(DE-627)NLEJ181378817 (DE-599)GBVNLZ181378817 DE-627 ger DE-627 rakwb eng Partial coherence in heavy-ion reactions 1982 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier First- and second-order interferences are investigated for fluctuating cross sections with average angular distributions <dσ/dΩ> not necessarily symmetric about 90^o. This is expected to be relevant for reactions between light complex nuclei where discrete final states are populated through an intermediate deep-inelastic or precompound process. We obtain <dσ/dΩ> as a sum of coherent and incoherent contributions from either side of the interaction region. The period of the oscillations present in <dσ/dΩ> as well as in the angular cross-correlation function is determined by a characteristic angular momentum Λ. while the damping of these oscillations depends on two angular momentum widths Δ and δ, which characterize the range of contributing partial waves and their phase correlation length, respectively. Using gaussian distributions simple formulae are derived by means of which the quantities Λ, Δ and δ may be extracted directly from the data. In the limit δ = 0 we obtain a transparent description of heavy-ion compound reactions. The excitation function exhibits gross structure whose period is determined by Λ(E). Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Hartmann, K.M. oth Dunnweber, W. oth Frahn, W.E. oth in Nuclear Physics, Section A Amsterdam : Elsevier 380(1982), 1, Seite 170-188 (DE-627)NLEJ177217928 (DE-600)1466542-6 0375-9474 nnns volume:380 year:1982 number:1 pages:170-188 http://linkinghub.elsevier.com/retrieve/pii/0375-9474(82)90588-7 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 380 1982 1 170-188 |
allfieldsSound |
(DE-627)NLEJ181378817 (DE-599)GBVNLZ181378817 DE-627 ger DE-627 rakwb eng Partial coherence in heavy-ion reactions 1982 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier First- and second-order interferences are investigated for fluctuating cross sections with average angular distributions <dσ/dΩ> not necessarily symmetric about 90^o. This is expected to be relevant for reactions between light complex nuclei where discrete final states are populated through an intermediate deep-inelastic or precompound process. We obtain <dσ/dΩ> as a sum of coherent and incoherent contributions from either side of the interaction region. The period of the oscillations present in <dσ/dΩ> as well as in the angular cross-correlation function is determined by a characteristic angular momentum Λ. while the damping of these oscillations depends on two angular momentum widths Δ and δ, which characterize the range of contributing partial waves and their phase correlation length, respectively. Using gaussian distributions simple formulae are derived by means of which the quantities Λ, Δ and δ may be extracted directly from the data. In the limit δ = 0 we obtain a transparent description of heavy-ion compound reactions. The excitation function exhibits gross structure whose period is determined by Λ(E). Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Hartmann, K.M. oth Dunnweber, W. oth Frahn, W.E. oth in Nuclear Physics, Section A Amsterdam : Elsevier 380(1982), 1, Seite 170-188 (DE-627)NLEJ177217928 (DE-600)1466542-6 0375-9474 nnns volume:380 year:1982 number:1 pages:170-188 http://linkinghub.elsevier.com/retrieve/pii/0375-9474(82)90588-7 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 380 1982 1 170-188 |
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abstract |
First- and second-order interferences are investigated for fluctuating cross sections with average angular distributions <dσ/dΩ> not necessarily symmetric about 90^o. This is expected to be relevant for reactions between light complex nuclei where discrete final states are populated through an intermediate deep-inelastic or precompound process. We obtain <dσ/dΩ> as a sum of coherent and incoherent contributions from either side of the interaction region. The period of the oscillations present in <dσ/dΩ> as well as in the angular cross-correlation function is determined by a characteristic angular momentum Λ. while the damping of these oscillations depends on two angular momentum widths Δ and δ, which characterize the range of contributing partial waves and their phase correlation length, respectively. Using gaussian distributions simple formulae are derived by means of which the quantities Λ, Δ and δ may be extracted directly from the data. In the limit δ = 0 we obtain a transparent description of heavy-ion compound reactions. The excitation function exhibits gross structure whose period is determined by Λ(E). |
abstractGer |
First- and second-order interferences are investigated for fluctuating cross sections with average angular distributions <dσ/dΩ> not necessarily symmetric about 90^o. This is expected to be relevant for reactions between light complex nuclei where discrete final states are populated through an intermediate deep-inelastic or precompound process. We obtain <dσ/dΩ> as a sum of coherent and incoherent contributions from either side of the interaction region. The period of the oscillations present in <dσ/dΩ> as well as in the angular cross-correlation function is determined by a characteristic angular momentum Λ. while the damping of these oscillations depends on two angular momentum widths Δ and δ, which characterize the range of contributing partial waves and their phase correlation length, respectively. Using gaussian distributions simple formulae are derived by means of which the quantities Λ, Δ and δ may be extracted directly from the data. In the limit δ = 0 we obtain a transparent description of heavy-ion compound reactions. The excitation function exhibits gross structure whose period is determined by Λ(E). |
abstract_unstemmed |
First- and second-order interferences are investigated for fluctuating cross sections with average angular distributions <dσ/dΩ> not necessarily symmetric about 90^o. This is expected to be relevant for reactions between light complex nuclei where discrete final states are populated through an intermediate deep-inelastic or precompound process. We obtain <dσ/dΩ> as a sum of coherent and incoherent contributions from either side of the interaction region. The period of the oscillations present in <dσ/dΩ> as well as in the angular cross-correlation function is determined by a characteristic angular momentum Λ. while the damping of these oscillations depends on two angular momentum widths Δ and δ, which characterize the range of contributing partial waves and their phase correlation length, respectively. Using gaussian distributions simple formulae are derived by means of which the quantities Λ, Δ and δ may be extracted directly from the data. In the limit δ = 0 we obtain a transparent description of heavy-ion compound reactions. The excitation function exhibits gross structure whose period is determined by Λ(E). |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">NLEJ181378817</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20210706151959.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">070505s1982 xx |||||o 00| ||eng c</controlfield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)NLEJ181378817</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)GBVNLZ181378817</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Partial coherence in heavy-ion reactions</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1982</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zzz</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">z</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zu</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">First- and second-order interferences are investigated for fluctuating cross sections with average angular distributions <dσ/dΩ> not necessarily symmetric about 90^o. This is expected to be relevant for reactions between light complex nuclei where discrete final states are populated through an intermediate deep-inelastic or precompound process. We obtain <dσ/dΩ> as a sum of coherent and incoherent contributions from either side of the interaction region. The period of the oscillations present in <dσ/dΩ> as well as in the angular cross-correlation function is determined by a characteristic angular momentum Λ. while the damping of these oscillations depends on two angular momentum widths Δ and δ, which characterize the range of contributing partial waves and their phase correlation length, respectively. Using gaussian distributions simple formulae are derived by means of which the quantities Λ, Δ and δ may be extracted directly from the data. In the limit δ = 0 we obtain a transparent description of heavy-ion compound reactions. The excitation function exhibits gross structure whose period is determined by Λ(E).</subfield></datafield><datafield tag="533" ind1=" " ind2=" "><subfield code="f">Elsevier Journal Backfiles on ScienceDirect 1907 - 2002</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Hartmann, K.M.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Dunnweber, W.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Frahn, W.E.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">in</subfield><subfield code="t">Nuclear Physics, Section A</subfield><subfield code="d">Amsterdam : Elsevier</subfield><subfield code="g">380(1982), 1, Seite 170-188</subfield><subfield code="w">(DE-627)NLEJ177217928</subfield><subfield code="w">(DE-600)1466542-6</subfield><subfield code="x">0375-9474</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:380</subfield><subfield code="g">year:1982</subfield><subfield code="g">number:1</subfield><subfield code="g">pages:170-188</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">http://linkinghub.elsevier.com/retrieve/pii/0375-9474(82)90588-7</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_H</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">ZDB-1-SDJ</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_NL_ARTICLE</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">380</subfield><subfield code="j">1982</subfield><subfield code="e">1</subfield><subfield code="h">170-188</subfield></datafield></record></collection>
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