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Electronic and Excitonic Structures of Inorganic–Organic Perovskite-Type Quantum-Well Crystal (C<sub>4</sub>H<sub>9</sub>NH<sub>3</sub>)<sub>2</sub>PbBr<sub>4</sub>

Ken’ichiro TanakaDepartment of Materials Science, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, JapanTakayuki TakahashiDepartment of Materials Science, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, JapanTakashi KondoDepartment of Materials Science, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, JapanKenichi UmedaDepartment of Physics, Sophia University, 7-1 Kioi-cho, Chiyoda-ku, Tokyo 102-8554, JapanKazuhiro EmaDepartment of Physics, Sophia University, 7-1 Kioi-cho, Chiyoda-ku, Tokyo 102-8554, JapanT. UmebayashiDepartment of Quantum Engineering and Systems Science, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, JapanKeisuke AsaiDepartment of Quantum Engineering and Systems Science, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, JapanK. UchidaInstitute for Solid State Physics, The University of Tokyo, Kashiwanoha, Kashiwa, Chiba 277-8581, JapanNoboru MiuraInstitute for Solid State Physics, The University of Tokyo, Kashiwanoha, Kashiwa, Chiba 277-8581, Japan
2005en
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Annotatsiya

The electronic and excitonic structures of an inorganic–organic perovskite-type quantum-well crystal (C 4 H 9 NH 3 ) 2 PbBr 4 have been investigated by optical absorption, photoluminescence, electroabsorption, two-photon absorption, and magnetoabsorption spectroscopies. Excitons in (C 4 H 9 NH 3 ) 2 PbBr 4 are of the Wannier-type, and n s ( n ≥2) excitons form an ideal two-dimensional Wannier exciton system. The binding energy, longitudinal–transverse splitting energy, and exchange energy of 1s excitons have been determined to be 480, 70 and 31 meV, respectively. These high values originate from both a strong two-dimensional confinement and the image charge effect. These values are larger than those in (C 6 H 13 NH 3 ) 2 PbI 4 , owing to the smaller dielectric constant of the well layer in (C 4 H 9 NH 3 ) 2 PbBr 4 than that in (C 6 H 13 NH 3 ) 2 PbI 4 . The seemingly unusual electric-field dependence of excitons resonance is also reasonably understood by taking the image charge effect into account.

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