Probing charge transfer states at organic and hybrid internal interfaces by photothermal deflection spectroscopy

2019 ◽  
Vol 31 (12) ◽  
pp. 124001 ◽  
Author(s):  
David Becker-Koch ◽  
Boris Rivkin ◽  
Fabian Paulus ◽  
Hengyang Xiang ◽  
Yifan Dong ◽  
...  
2015 ◽  
Vol 137 (16) ◽  
pp. 5256-5259 ◽  
Author(s):  
Ester Buchaca-Domingo ◽  
Koen Vandewal ◽  
Zhuping Fei ◽  
Scott E. Watkins ◽  
Fiona H. Scholes ◽  
...  

2012 ◽  
Vol 2012 ◽  
pp. 1-5 ◽  
Author(s):  
S. Ktifa ◽  
M. Ghrib ◽  
F. Saadallah ◽  
H. Ezzaouia ◽  
N. Yacoubi

We have studied the optical properties of nanocrystalline silicon (nc-Si) film deposited by plasma enhancement chemical vapor deposition (PECVD) on porous aluminum structure using, respectively, the Photothermal Deflection Spectroscopy (PDS) and Photoluminescence (PL). The aim of this work is to investigate the influence of anodisation current on the optical properties of the porous aluminum silicon layers (PASL). The morphology characterization studied by atomic force microscopy (AFM) technique has shown that the grain size of (nc-Si) increases with the anodisation current. However, a band gap shift of the energy gap was observed.


2008 ◽  
Vol 103 (9) ◽  
pp. 094906 ◽  
Author(s):  
Adam R. Krause ◽  
Charles Van Neste ◽  
Larry Senesac ◽  
Thomas Thundat ◽  
Eric Finot

1991 ◽  
pp. 269-272
Author(s):  
J. Serra ◽  
J. Andreu ◽  
G. Sardin ◽  
C. Roch ◽  
J.M. Asensi ◽  
...  

1992 ◽  
Vol 283 ◽  
Author(s):  
S. Q. Gu ◽  
J. M. Viner ◽  
P. C. Taylor ◽  
M. J. Williams ◽  
W. A. Turner ◽  
...  

ABSTRACTPhotoluminescence (PL) has been investigated in hydrogenated microcrystalline silicon (μc-Si:H) samples as a function of boron doping for films prepared by remote plasma enhanced chemical vapor deposition. When the dark conductivity a is below about 10-5 S/cm, the PL spectra exhibit a shape which is close to that of the so-called band tail PL in undoped hydrogenated amorphous silicon (a-Si:H) at 77 K. When a increases, the PL intensity decreases at 77 K. For samples with a on the order of 10-3 S/cm, the PL spectra show only a narrow, low energy PL band which peaks around 0.8–0.9 eV. In these samples, the PL at higher energy is essentially not observable. This trend is similar to that which occurs in doped a-Si:H. However, for higher doping levels (σ ∼ 1 S/cm) the PL in μc-Si:H, although very weak, exhibits a broad band which contains intensity at higher energies. The absorption spectra in these samples, as measured by photothermal deflection spectroscopy (PDS), show the same relationships with the corresponding PL spectra as do the PDS spectra in doped a-Si:H.


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