1989
DOI: 10.1088/0953-8984/1/40/024
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Two-dimensional magnetopolaron coupling to both homopolar and longitudinal optic phonons in the layer compound InSe

Abstract: We have studied cyclotron resonance of the two-dimensional electron gas (2DEG) found in the layered semiconductor InSe at magnetic fields up to 30 T. The results show the first direct observation of resonant polaron coupling to a homopolar optic phonon, coupling via a deformation potential. We have also observed a large increase in the cyclotron effective mass as the LO phonon energy is approached, indicating the strongest polaron effects yet seen in any 2D system (a = 0.3).

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Cited by 11 publications
(6 citation statements)
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“…The A 2 (LO) and E 2 (LO) modes at 198 and 207 cm −1 , forbidden by selection rules, 26 show strong intensities due to resonance with the exciton energy of InSe. 27,28 Matching well with our theoretical phonon calculations in Figure 1b, two single-phonon modes of A 1 1 and A 1 2 modes are observed in the Raman spectrum. Their phonon vibrations are attributed to the out-of-plane vibration of the In and Se atoms in two different configurations.…”
Section: ■ Results and Discussionsupporting
confidence: 88%
See 1 more Smart Citation
“…The A 2 (LO) and E 2 (LO) modes at 198 and 207 cm −1 , forbidden by selection rules, 26 show strong intensities due to resonance with the exciton energy of InSe. 27,28 Matching well with our theoretical phonon calculations in Figure 1b, two single-phonon modes of A 1 1 and A 1 2 modes are observed in the Raman spectrum. Their phonon vibrations are attributed to the out-of-plane vibration of the In and Se atoms in two different configurations.…”
Section: ■ Results and Discussionsupporting
confidence: 88%
“…As seen in Figure b, the room-temperature unpolarized Raman spectra excited by linearly polarized 514 nm laser shows five Raman peaks at 114, 177, 198, 207, and 225 cm –1 , which can be assigned to the 3R-InSe Raman modes of A 1 1 , E 1 , A 2 (LO), E 2 (LO), and A 1 2 , respectively. , The schematic representations of atom displacements in these phonons modes are displayed in Figure S3. The A 2 (LO) and E 2 (LO) modes at 198 and 207 cm –1 , forbidden by selection rules, show strong intensities due to resonance with the exciton energy of InSe. , Matching well with our theoretical phonon calculations in Figure b, two single-phonon modes of A 1 1 and A 1 2 modes are observed in the Raman spectrum. Their phonon vibrations are attributed to the out-of-plane vibration of the In and Se atoms in two different configurations.…”
Section: Resultssupporting
confidence: 87%
“…The presence of 2D electrons in InSe and the role that they play in transport properties has been widely investigated [27]- [32]. The origin of 2D electrons in InSe is extrinsic.…”
Section: D Electronsmentioning
confidence: 99%
“…The 2D states are electric subbands that have been atributed to quantum size effects in thin layers limited by stacking fault related barriers [13]. Other authors have proposed a model in which 2D electronic subbands in InSe are created by a high concentration of donor impurities bound to a stacking fault, like in δ-doping systems [32]. This model is inconsistent with the low areal concentration and high 2D electron mobility in InSe at low temperature.…”
Section: D Electronsmentioning
confidence: 99%
“…Consequently, it was considered [2] that in n-type material, during the growth of the crystal, the shallow donor impurities are accumulated at the defect planes leading to the formation of several sheets with a low individual estimated electron density (of order 1 × 10 11 cm −2 ). Subsequent cyclotron studies [3,4] have confirmed the proposed electron gas model. An improvement [5] of this model was done by considering a quasi-twodimensional (Q2D) behaviour of the electron gas.…”
Section: Introductionmentioning
confidence: 66%