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  <ref-type name="Journal Article">17</ref-type>
  <contributors>
    <authors>
      <author>Avigo, R.</author>
      <author>Wieland, O.</author>
      <author>Bracco, A.</author>
      <author>Camera, F.</author>
      <author>Ameil, F.</author>
      <author>Arici, T.</author>
      <author>Ataç, A.</author>
      <author>Barrientos, D.</author>
      <author>Bazzacco, D.</author>
      <author>Bednarczyk, P.</author>
      <author>Benzoni, G.</author>
      <author>Birkenbach, B.</author>
      <author>Blasi, N.</author>
      <author>Boston, H. C.</author>
      <author>Bottoni, S.</author>
      <author>Brambilla, S.</author>
      <author>Bruyneel, B.</author>
      <author>Ciemała, M.</author>
      <author>Clément, E.</author>
      <author>Cortes, Martha Liliana</author>
      <author>Crespi, F. C. L.</author>
      <author>Cullen, D. M.</author>
      <author>Curien, D.</author>
      <author>Didierjean, F.</author>
      <author>Domingo-Pardo, C.</author>
      <author>Duchêne, G.</author>
      <author>Eberth, J.</author>
      <author>Görgen, A.</author>
      <author>Gadea, A.</author>
      <author>Gerl, J.</author>
      <author>Goel, N.</author>
      <author>Golubev, P.</author>
      <author>González, V.</author>
      <author>Górska, M.</author>
      <author>Gottardo, A.</author>
      <author>Gregor, E.</author>
      <author>Guastalla, Giulia</author>
      <author>Habermann, T.</author>
      <author>Harkness-Brennan, L. J.</author>
      <author>Jungclaus, A.</author>
      <author>Kmiecik, M.</author>
      <author>Kojouharov, I.</author>
      <author>Korten, W.</author>
      <author>Kurz, N.</author>
      <author>Labiche, M.</author>
      <author>Lalović, N.</author>
      <author>Leoni, S.</author>
      <author>Lettmann, M.</author>
      <author>Maj, A.</author>
      <author>Menegazzo, R.</author>
      <author>Mengoni, D.</author>
      <author>Merchan, Edana</author>
      <author>Million, B.</author>
      <author>Morales, A. I.</author>
      <author>Napoli, D. R.</author>
      <author>Nociforo, C.</author>
      <author>Nyberg, J.</author>
      <author>Pietralla, N.</author>
      <author>Pietri, S.</author>
      <author>Podolyák, Zs.</author>
      <author>Ponomarev, V. Yu.</author>
      <author>Pullia, A.</author>
      <author>Quintana, B.</author>
      <author>Rainovski, G.</author>
      <author>Ralet, D.</author>
      <author>Recchia, F.</author>
      <author>Reese, M.</author>
      <author>Regan, P.</author>
      <author>Reiter, P.</author>
      <author>Riboldi, S.</author>
      <author>Rudolph, D.</author>
      <author>Salsac, M. D.</author>
      <author>Sanchis, E.</author>
      <author>Sarmiento, L. G.</author>
      <author>Schaffner, H.</author>
      <author>Simpson, J.</author>
      <author>Stezowski, O.</author>
      <author>Valiente-Dobón, J. J.</author>
      <author>Wollersheim, H. J.</author>
    </authors>
    <subsidiary-authors>
      <author>KSP</author>
      <author>SFS</author>
      <author>DTL</author>
      <author>EEL</author>
    </subsidiary-authors>
  </contributors>
  <titles>
    <title>Low-lying electric dipole ${\gamma}$-continuum for the unstable $^{62,64}Fe$ nuclei: Strength evolution with neutron number</title>
    <secondary-title>Physics letters / B</secondary-title>
  </titles>
  <periodical>
    <full-title>Physics letters / B</full-title>
  </periodical>
  <publisher>North-Holland Publ.</publisher>
  <pub-location>Amsterdam</pub-location>
  <isbn>0370-2693</isbn>
  <electronic-resource-num>10.1016/j.physletb.2020.135951</electronic-resource-num>
  <language>English</language>
  <pages>135951</pages>
  <number/>
  <volume>811</volume>
  <abstract>The γ -ray emission from the nuclei $^{62,64}$Fe following Coulomb excitation at bombarding energy of 400-440 AMeV was measured with special focus on E 1 transitions in the energy region 4-8 MeV. The unstable neutron-rich nuclei $^{62,64}$Fe were produced at the FAIR-GSI laboratories and selected with the FRS spectrometer. The γ decay was detected with AGATA. From the measured γ -ray spectra the summed E 1 strength is extracted and compared to microscopic quasi-particle phonon model calculations. The trend of the E 1 strength with increasing neutron number is found to be fairly well reproduced with calculations that assume a rather complex structure of the 1$^−$ states (three-phonon states) inducing a strong fragmentation of the E 1 nuclear response below the neutron binding energy.</abstract>
  <notes>
    <note>This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/). Funded by SCOAP3 ; </note>
  </notes>
  <label>PUB:(DE-HGF)16, ; 0, ; </label>
  <keywords>
    <keyword>64 Fe</keyword>
    <keyword>62 Fe</keyword>
    <keyword>Nuclear structure</keyword>
    <keyword>Dipole excitation around neutron threshold</keyword>
    <keyword>64Fe</keyword>
    <keyword>62Fe</keyword>
  </keywords>
  <accession-num>WOS:000612225400080</accession-num>
  <work-type>Journal Article</work-type>
  <dates>
    <pub-dates>
      <year>2020</year>
    </pub-dates>
  </dates>
  <accession-num>GSI-2021-00581</accession-num>
  <year>2020</year>
  <urls>
    <related-urls>
      <url>https://repository.gsi.de/record/237998</url>
      <url>https://doi.org/10.1016/j.physletb.2020.135951</url>
      <url>&lt;Go to ISI&gt;://WOS:000612225400080</url>
    </related-urls>
  </urls>
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