Trion Binding Energy Variation on Photoluminescence Excitation Energy and Power during Direct to Indirect Bandgap Crossover in Monolayer and Few-Layer MoS2

Author(s):  
Sergii Golovynskyi ◽  
Oleksandr I. Datsenko ◽  
Dan Dong ◽  
Yan Lin ◽  
Iqra Irfan ◽  
...  
2016 ◽  
Vol 30 (06) ◽  
pp. 1650021 ◽  
Author(s):  
Yonglei Jia ◽  
Junlin Liu

The exciton effects in 1-nm-wide armchair graphene nanoribbons (AGNRs) under the uniaxial strain were studied within the nonorthogonal tight-binding (TB) model, supplemented by the long-range Coulomb interactions. The obtained results show that both the excitation energy and exciton binding energy are modulated by the uniaxial strain. The variation of these energies depends on the ribbon family. In addition, the results show that the variation of the exciton binding energy is much weaker than the variation of excitation energy. Our results provide new guidance for the design of optomechanical systems based on graphene nanoribbons.


1995 ◽  
Vol 417 ◽  
Author(s):  
F. A. J. M. Driessen ◽  
H. M. Cheong ◽  
A. Mascarehas

AbstractEfficient, low-temperature luminescence at energies far above that of the exciting cw-laser is reported at junctions of GaAs-GaInP2 and GaAs-AlxGa1−x.InP2. The signal originates from the high-band gap layers and disappears only if the excitation energy is tuned below the GaAs band gap, as monitored by up-converted photoluminescence excitation spectroscopy. This shows that the non-linear process is induced by the generation of electrons and holes in the GaAs. Furthermore, it is found that the up-conversion is only observed if the (A1)GaInP2 layers are CuPtB long-range ordered. The reason for this is the inherent presence of metastable states in these ordered alloys. It is argued that cold Auger processes cause the nonlinear effect at these type I interfaces.


1995 ◽  
Vol 51 (6) ◽  
pp. 2942-2951 ◽  
Author(s):  
D. R. Chakrabarty ◽  
V. M. Datar ◽  
Suresh Kumar ◽  
E. T. Mirgule ◽  
H. H. Oza ◽  
...  

1984 ◽  
Vol 29 (8) ◽  
pp. 4772-4774 ◽  
Author(s):  
B. Etienne ◽  
N. V. Tien ◽  
R. E. Nahory ◽  
J. C. Dewinter ◽  
M. Voos ◽  
...  

2000 ◽  
Vol 609 ◽  
Author(s):  
Leandro R. Tessler ◽  
Cínthia Piamonteze ◽  
Ana Carola Iniguez ◽  
Abner de Siervo ◽  
Richard Landers ◽  
...  

ABSTRACTOne very important problem concerning erbium-doped silicon is the electronic structure of the Er3+ impurities. In particular, it is still not clear if the 4f levels can be treated as frozen core levels or their overlap with s and p states of their neighbors must be considered explicitly. For crystalline Si, the 4f levels have been supposed to be anywhere between 20 eV below the valence band and within the energy gap. In this paper we report on the first ultraviolet photoemission spectroscopy (UPS) measurements on Er-doped a-Si:H. Samples of a-Si:H<Er> with different Er contents (up to 1 at. % Er) were prepared by co-sputtering from a Si target partially covered with metallic Er platelets. In order to enhance the Er states relative to the Si and H states, the excitation energy was tuned between 40 and 140 eV with a synchrotron light source. At 140 eV excitation energy the cross-section of the Er 4f and 5p states is more than an order of magnitude higher than the cross section of the Si 3s or 3p states. As the Er concentration increases, a shoulder and then a peak appears at 10.0±0.5 eV binding energy. The intensity and width of this peak is well correlated with the Er concentration, and with the Er 5p and 5p½ levels at 26 and 32 eV binding energy, respectively. We attribute the peak at 10.0±0.5 eV binding energy to the Er 4f level. These are the only occupied states that can be related to the presence of Er, indicating that these levels are not valence states and consequently can be treated as frozen core levels.


1996 ◽  
Vol 53 (4) ◽  
pp. 2022-2022 ◽  
Author(s):  
D. R. Chakrabarty ◽  
V. M. Datar ◽  
Suresh Kumar ◽  
E. T. Mirgule ◽  
H. H. Oza ◽  
...  

1992 ◽  
Vol 283 ◽  
Author(s):  
Edward B. Stokes ◽  
Peter D. Persans

ABSTRACTWe present photoluminescence excitation spectra for glasses doped with CdSxSe(1-x). The peak of the emission spectrum is blue shifted toward the bandgap as excitation energy flux is increased. Total photoluminescence emission intensity is observed to be significantly enhanced and blue shifted by exciting with photon energies greater than ∼4 eV. A simple model of the nanoparticle band structure is presented to account for the observed spectra.


2014 ◽  
Vol 118 (31) ◽  
pp. 18059-18063 ◽  
Author(s):  
Said Kazaoui ◽  
Steffan Cook ◽  
Nicolas Izard ◽  
Yoichi Murakami ◽  
Shigeo Maruyama ◽  
...  

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