Spatially Resolved Doping Concentration and Nonradiative Lifetime Profiles in Single Si-Doped InP Nanowires Using Photoluminescence Mapping

Nano Letters ◽  
2015 ◽  
Vol 15 (5) ◽  
pp. 3017-3023 ◽  
Author(s):  
Fan Wang ◽  
Qian Gao ◽  
Kun Peng ◽  
Zhe Li ◽  
Ziyuan Li ◽  
...  
1990 ◽  
Vol 41-42 ◽  
pp. 480-486 ◽  
Author(s):  
S. Goto ◽  
H. Kakibayashi ◽  
M. Kawata ◽  
T. Usagawa

2002 ◽  
Vol 09 (02) ◽  
pp. 693-698 ◽  
Author(s):  
N. TAKAHASHI ◽  
T. ZHANG ◽  
M. SPANGENBERG ◽  
D. GREIG ◽  
T.-H. SHEN ◽  
...  

Thin epitaxial Fe films were grown on singular and vicinal GaAs(001) substrates, and their magnetic and electronic structures were investigated by synchrotron-based spin-resolved and spin-integrated photoelectron spectroscopy with different Fe thickness. There were two types of substrates: one was a Si-doped n-type GaAs(001) surface with doping concentration of 2 × 1018 cm -3 (singular substrate), and the other was orientated by 3° toward the (111)A direction (vicinal substrate). Spin polarization of the secondary electron peak at different growth stages of Fe coverage for the singular substrate sample and the vicinal one were measured. In the case of singular substrates, there was a dependence of their initial surface reconstruction, which is associated with complex domain structure, while no such the dependence was observed in the case of vicinal substrates. The result from the vicinal sample suggests the geometrical influence of the initial surface stoichiometry of the substrate.


1997 ◽  
Vol 482 ◽  
Author(s):  
I. D. Goepfert ◽  
E. F. Schubert ◽  
J. M. Redwing

AbstractWe investigate the optical properties of n-type Gallium Nitride (GaN) with concentrations ranging from 5×1016 to 7×1018 cm−3. The near-band edge ultraviolet (UV) transition increases monotonically with the doping concentration. The photoluminescence linewidth of the near-bandgap optical transition increases from 47 to 78 meV as the doping concentration is increased. The broadening is modeled by taking into account potential fluctuations caused by the random distribution of donor impurities. Excellent agreement is found between experimental and theoretical results. We also investigate the origin of the yellow luminescence in GaN. At low excitation densities the experimental ratio of the UV-to-yellow photoluminescence does not change significantly as the doping concentration is increased by two orders of magnitude. Analysis of the luminescence in terms of a theoretical model indicates that the yellow luminescence is due to compensating impurities or defects.


2013 ◽  
Vol 1558 ◽  
Author(s):  
Baozhu Wang ◽  
Bahadir Kucukgok ◽  
Qinyue He ◽  
Andrew G. Melton ◽  
Jacob Leach ◽  
...  

ABSTRACTIn this study, thermoelectric properties of bulk and epitaxy GaN with various doping concentration are investigated. Seebeck coefficients decreased with the increase of carrier concentration for both bulk and epitaxial GaN samples, and the Seebeck coefficients of epitaxial GaN samples are found to be larger than that of bulk GaN samples in the similar carrier density due to the higher dislocation scattering. For epitaxial samples, a high power factor of 4.72 × 10-4 W/m-K2 is observed. The power factors of the bulk GaN samples are in the range of from 0.315× 10-4W/m-K2 to 0.354× 10-4W/m-K2 due to the low Seebeck coefficients.


2000 ◽  
Vol 639 ◽  
Author(s):  
Mee-Yi Ryu ◽  
Young Jun Yu ◽  
Phil Won Yu ◽  
Eun-joo Shin ◽  
Eunsoon Oh ◽  
...  

ABSTRACTA systematic study of photoluminescence (PL) and time-resolved PL spectra from In0.15Ga0.85N/In0.015Ga0.985N quantum wells (QWs) with different Si doping concentration in the barriers has been carried out. As the Si doping concentration increases, the PL emission intensity was increased and the PL peak energy was blueshifted. The energy separation between the spontaneous emission (SPE) and stimulated emission (SE) peaks decrease with increasing Si doping concentration. We also observed that the slow decay time τ2 in the QWs decreases with increasing Si doping concentration, from ∼ 130 ns for [Si] = 2 × 1018 cm−3 to ∼ 30 ns for [Si] = 1 × 1019 cm−3. The PL emission peak shifts to lower energies with delay time after a pulsed excitation and this shift decreases with increasing Si doping concentration. The increased recombination rate, the decrease of peak shift with delay time, and the reduced separation between the SPE and SE peaks with increasing Si doping concentration are attributed to the screening of piezoelectric field by carriers originated from Si doped barriers.


1997 ◽  
Vol 28 (8-10) ◽  
pp. 985-992 ◽  
Author(s):  
J. Gerster ◽  
J.M. Schneider ◽  
C. Ehret ◽  
W. Limmer ◽  
R. Sauer ◽  
...  

Nanomaterials ◽  
2020 ◽  
Vol 10 (8) ◽  
pp. 1576 ◽  
Author(s):  
Umberto Celano ◽  
Andres Gomez ◽  
Paola Piedimonte ◽  
Sabine Neumayer ◽  
Liam Collins ◽  
...  

The ability to develop ferroelectric materials using binary oxides is critical to enable novel low-power, high-density non-volatile memory and fast switching logic. The discovery of ferroelectricity in hafnia-based thin films, has focused the hopes of the community on this class of materials to overcome the existing problems of perovskite-based integrated ferroelectrics. However, both the control of ferroelectricity in doped-HfO2 and the direct characterization at the nanoscale of ferroelectric phenomena, are increasingly difficult to achieve. The main limitations are imposed by the inherent intertwining of ferroelectric and dielectric properties, the role of strain, interfaces and electric field-mediated phase, and polarization changes. In this work, using Si-doped HfO2 as a material system, we performed a correlative study with four scanning probe techniques for the local sensing of intrinsic ferroelectricity on the oxide surface. Putting each technique in perspective, we demonstrated that different origins of spatially resolved contrast can be obtained, thus highlighting possible crosstalk not originated by a genuine ferroelectric response. By leveraging the strength of each method, we showed how intrinsic processes in ultrathin dielectrics, i.e., electronic leakage, existence and generation of energy states, charge trapping (de-trapping) phenomena, and electrochemical effects, can influence the sensed response. We then proceeded to initiate hysteresis loops by means of tip-induced spectroscopic cycling (i.e., “wake-up”), thus observing the onset of oxide degradation processes associated with this step. Finally, direct piezoelectric effects were studied using the high pressure resulting from the probe’s confinement, noticing the absence of a net time-invariant piezo-generated charge. Our results are critical in providing a general framework of interpretation for multiple nanoscale processes impacting ferroelectricity in doped-hafnia and strategies for sensing it.


1992 ◽  
Vol 7 (1A) ◽  
pp. A294-A299 ◽  
Author(s):  
J L Weyher ◽  
P J van der Wel ◽  
C Frigeri
Keyword(s):  
Lec Gaas ◽  

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