{"department":[{"_id":"293"}],"volume":58,"author":[{"orcid":"0000-0001-8864-2072","full_name":"Meier, Torsten","last_name":"Meier","first_name":"Torsten","id":"344"},{"first_name":"K.","full_name":"Bott, K.","last_name":"Bott"},{"full_name":"Hader, J.","last_name":"Hader","first_name":"J."},{"first_name":"D.","full_name":"Brinkmann, D.","last_name":"Brinkmann"},{"full_name":"Koch, S.W.","last_name":"Koch","first_name":"S.W."},{"last_name":"Thomas","full_name":"Thomas, P.","first_name":"P."}],"main_file_link":[{"url":"https://journals.aps.org/prb/abstract/10.1103/PhysRevB.58.15911"}],"doi":"10.1103/PhysRevB.58.15911","date_created":"2023-04-02T20:58:52Z","publication_status":"published","abstract":[{"text":"In his Comment on our work Glutsch raises, on the basis of a calculation for a dimerized three-dimensional superlattice, four points: (1) odd-parity excitons do not contribute to optical absorption, (2) there are no forbidden single-particle transitions, (3) there is a coupling of the e1-hh2 exciton (called ¯X in Ref. 1) to the underlying e1-hh1 continuum that leads to a Fano resonance, and (4) the extension of the exciton wave function is infinite in an all space directions rather than having a small extension. In this Reply these four points are addressed and it is shown that our previous conclusions remain valid.","lang":"eng"}],"extern":"1","title":"Reply to Comment on \"Odd-parity excitons in semiconductor superlattices\"","date_updated":"2023-04-02T20:58:56Z","intvolume":"        58","issue":"23","article_number":"15911","citation":{"short":"T. Meier, K. Bott, J. Hader, D. Brinkmann, S.W. Koch, P. Thomas, Physical Review B 58 (1998).","ama":"Meier T, Bott K, Hader J, Brinkmann D, Koch SW, Thomas P. Reply to Comment on “Odd-parity excitons in semiconductor superlattices.” <i>Physical Review B</i>. 1998;58(23). doi:<a href=\"https://doi.org/10.1103/PhysRevB.58.15911\">10.1103/PhysRevB.58.15911</a>","ieee":"T. Meier, K. Bott, J. Hader, D. Brinkmann, S. W. Koch, and P. Thomas, “Reply to Comment on ‘Odd-parity excitons in semiconductor superlattices,’” <i>Physical Review B</i>, vol. 58, no. 23, Art. no. 15911, 1998, doi: <a href=\"https://doi.org/10.1103/PhysRevB.58.15911\">10.1103/PhysRevB.58.15911</a>.","bibtex":"@article{Meier_Bott_Hader_Brinkmann_Koch_Thomas_1998, title={Reply to Comment on “Odd-parity excitons in semiconductor superlattices”}, volume={58}, DOI={<a href=\"https://doi.org/10.1103/PhysRevB.58.15911\">10.1103/PhysRevB.58.15911</a>}, number={2315911}, journal={Physical Review B}, publisher={American Physical Society}, author={Meier, Torsten and Bott, K. and Hader, J. and Brinkmann, D. and Koch, S.W. and Thomas, P.}, year={1998} }","chicago":"Meier, Torsten, K. Bott, J. Hader, D. Brinkmann, S.W. Koch, and P. Thomas. “Reply to Comment on ‘Odd-Parity Excitons in Semiconductor Superlattices.’” <i>Physical Review B</i> 58, no. 23 (1998). <a href=\"https://doi.org/10.1103/PhysRevB.58.15911\">https://doi.org/10.1103/PhysRevB.58.15911</a>.","mla":"Meier, Torsten, et al. “Reply to Comment on ‘Odd-Parity Excitons in Semiconductor Superlattices.’” <i>Physical Review B</i>, vol. 58, no. 23, 15911, American Physical Society, 1998, doi:<a href=\"https://doi.org/10.1103/PhysRevB.58.15911\">10.1103/PhysRevB.58.15911</a>.","apa":"Meier, T., Bott, K., Hader, J., Brinkmann, D., Koch, S. W., &#38; Thomas, P. (1998). Reply to Comment on “Odd-parity excitons in semiconductor superlattices.” <i>Physical Review B</i>, <i>58</i>(23), Article 15911. <a href=\"https://doi.org/10.1103/PhysRevB.58.15911\">https://doi.org/10.1103/PhysRevB.58.15911</a>"},"publisher":"American Physical Society","type":"journal_article","year":"1998","user_id":"49063","_id":"43343","status":"public","publication":"Physical Review B","language":[{"iso":"eng"}]}