scholarly journals Accessing the Conduction Band Dispersion in CH3NH3PbI3 Single Crystals

Author(s):  
Jinpeng Yang ◽  
Haruki Sato ◽  
Hibiki Orio ◽  
Xianjie Liu ◽  
Mats Fahlman ◽  
...  
2002 ◽  
Vol 13 (2-4) ◽  
pp. 1078-1081 ◽  
Author(s):  
C. Skierbiszewski ◽  
S.P. Łepkowski ◽  
P. Perlin ◽  
T. Suski ◽  
W. Jantsch ◽  
...  

2015 ◽  
Vol 49 (5) ◽  
pp. 574-578 ◽  
Author(s):  
S. V. Luniov ◽  
O. V. Burban ◽  
P. F. Nazarchuk

1985 ◽  
Vol 63 (11) ◽  
pp. 1405-1408 ◽  
Author(s):  
Y. Frongillo ◽  
M. Aubin ◽  
S. Jandl

We have measured the Seebeck coefficient of quasi-two-dimensional single crystals of SnSe2, SnS0.1Se1.9, and SnS0.3Se1.7, grown by the Bridgman technique, and SnSe2, grown by iodine transport, over a large temperature range varying from 15 (4.2 for SnSe2) to 300 K. To assist in the interpretation of these results, the Hall coefficient and resistivity were measured on SnSe2 and SnS0.1Se1.9 Bridgman samples. All these measurements were done in a plane perpendicular to the c axis. It was found that, as the temperature decreases, the absolute value of the Seebeck coefficient decreases slightly before a surprisingly large increase at the lowest temperatures. We interpret these results as the manifestation of two conduction mechanisms: electrons in the conduction band and hopping of electrons between impurities.


2017 ◽  
Vol 19 (7) ◽  
pp. 5361-5365 ◽  
Author(s):  
Congcong Wang ◽  
Benjamin R. Ecker ◽  
Haotong Wei ◽  
Jinsong Huang ◽  
Jian-Qiao Meng ◽  
...  

The ARPES study of perovskite single crystals revealed the band structure along theΓXandΓMdirections.


2019 ◽  
Vol 13 (1) ◽  
pp. 011009 ◽  
Author(s):  
Jin-Peng Yang ◽  
Si-Xian Ren ◽  
Takuma Yamaguchi ◽  
Matthias Meissner ◽  
Li-wen Cheng ◽  
...  

2004 ◽  
Vol 114 ◽  
pp. 335-337 ◽  
Author(s):  
R. B. Morgunov ◽  
A. A. Baskakov ◽  
L. R. Dunin-Barkovskiy ◽  
S. S. Khasanov ◽  
R. P. Shibaeva ◽  
...  

1992 ◽  
Vol 46 (23) ◽  
pp. 15602-15605 ◽  
Author(s):  
J.-M. Themlin ◽  
S. Bouzidi ◽  
F. Coletti ◽  
J.-M. Debever ◽  
G. Gensterblum ◽  
...  

Author(s):  
V. A. Tedzhetov ◽  
A. V. Podkopaev ◽  
A. A. Sysoev

The development of high energy physics and medicine has raised the necessity of heavy stintillating materials with a large total gamma quantum absorption cross-section, high quantum output and fast response. Cerium doped lutetium silicate Lu2SiO5 : Ce3+ (LSO) has high density, large effective atomic number and high conversion efficiency. In this work we have reported optical absorption spectroscopy and photoluminescence data for LSO single crystals grown using the modified Musatov method. The absorption spectra show the fundamental intrinsic absorption edge of Lu2SiO5 at ~200 nm and four extrinsic absorption bands of Ce3+ activator near 250—375 nm. The band gap is 6.19 to 6.29 eV depending on optical beam direction. We have confirmed that the extrinsic absorption bands correspond to optical transitions in Ce3+ activator ions localized in two crystallographically non-equivalent CeI and CeII positions. We have estimated that oscillator force for the optical transitions in Ce3+ ions. The photoluminescence spectra excited by 3.49 eV photon energy UV laser contain three bands: ~2.96 eV, ~3.13 eV (CeI) and ~2.70 eV (CeII). The energy structure of electron traps in LSO has been studied with thermally stimulated luminescence, the crystals being exposed to UV with different spectral and energy parameters. All the experimental thermally stimulated luminescence curves contain at least two peaks at 345 and 400 K with a 4 : 1 intensity ratio attributable to electron traps at 0.92—0.96 and1.12—1.18 eV. LSO exposure to high pressure mercury lamp radiation having the highest energy has for the first time showed the presence of traps at 0.88 eV. A model of the energy structure of LSO has been developed. The luminescence mechanism in the material is more complex than purely intracenter one. We show that high excitation energies may lead to ionization by the mechanism hva + Ce3+ = Ce4+ + e-. We have assumed that the storage of excitation energy involves not only Ce3+ activator but also the conduction band as well as trap states localized near the conduction band.


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