Enhancement of the Strained Si Forbidden Doublet Transverse Optical Phonon Raman Band for Quantitative Stress Measurement

2012 ◽  
Vol 51 ◽  
pp. 078002
Author(s):  
Vladimir Poborchii ◽  
Tetsuya Tada ◽  
Toshihiko Kanayama
2013 ◽  
Vol 103 (17) ◽  
pp. 171905
Author(s):  
J. S. Kim ◽  
H. C. Ryu ◽  
S. H. Kim ◽  
H. Kim ◽  
H. Rho ◽  
...  

2010 ◽  
Vol 97 (4) ◽  
pp. 041915 ◽  
Author(s):  
Vladimir Poborchii ◽  
Tetsuya Tada ◽  
Toshihiko Kanayama

2014 ◽  
Vol 996 ◽  
pp. 380-385 ◽  
Author(s):  
Theo J. Rickert ◽  
James J. Thomas ◽  
Lasse Suominen

Shot-Peening is used to generate surface-near compressive residual stresses in final shape parts, usually to improve their fatigue properties. The success of the process can be checked in different ways. XRD and Hole-Drilling determine quantitative stress depth profiles in specific locations. Barkhausen noise measurements evaluate a near-surface zone in real-time and can cover large areas quickly. It is a fully nondestructive method. This study compares ESPI Hole-Drilling, which is a very fast technique, and XRD, which is very precise but slower, to Barkhausen Noise results for the case of three steel rings shot-peened with different intensities.


2020 ◽  
Vol 20 (7) ◽  
pp. 4358-4363
Author(s):  
Jeung Hun Park ◽  
Richard S. Kim ◽  
Se-Jeong Park ◽  
Gye-Choon Park ◽  
Choong-Heui Chung

We report the relation between the catalyst patterning conditions and the intensity of the 1st order Raman active modes in Au-catalyzed GaAs nanowire bundles. We fabricated e-beam lithographically Au-patterned GaAs(111)B substrates by varying the patterning conditions (e-beam dose rate, dot-size and interdot-spacings), and grew GaAs nanowires via vapor–liquid–solid process using a solid-source molecular beam epitaxy. To understand the effects of the substrate preparation conditions and resulting morphologies on the optical characteristics of 1st order transverse optical and longitudinal optical phonon modes of GaAs, we characterized the nanowire bundles using complementary μ-Raman spectroscopy and scanning electron microscopy as a function of the e-beam dose rate (145–595 μC/cm2), inter-dot spacing (100 and 150 nm) and pattern size (100 and 150 nm). Ensembles of single crystalline GaAs nanowires covered with different Au-thickness exhibit a downshift and asymmetric broadening of the 1st order transverse optical and longitudinal optical phonon peaks relative to GaAs bulk modes. We also showed that the sensitivity of a downshift and broadening of Raman spectra are directly related to morphological and surface coverage variations in as-grown nanowires. We observed clear increases of the transverse optical and longitudinal optical intensity as well as the relatively higher peak shift and broadening of Raman spectra from the 100 nm patterning in response to the dose rate change. Strong dependence of Raman spectra of the nanowire bundles on the e-beam dose rate changes are attributed to the variations in spatial density, size, shape and random growth orientation of the wires. We have shown that the identification of the changes in GaAs longitudinal optical and Arsenic anti-site peaks is good indicators to characterize the quality of as-grown GaAs nanowires. Our finding confirms the utilization of Raman spectroscopy as a powerful tool for characterizing chemical, structural, and morphological information of as-grown nanowires within the supporting substrate.


Nano Letters ◽  
2014 ◽  
Vol 14 (7) ◽  
pp. 3793-3798 ◽  
Author(s):  
Maria Vanessa Balois ◽  
Norihiko Hayazawa ◽  
Alvarado Tarun ◽  
Satoshi Kawata ◽  
Manfred Reiche ◽  
...  

Nano Letters ◽  
2011 ◽  
Vol 11 (11) ◽  
pp. 4780-4788 ◽  
Author(s):  
Alvarado Tarun ◽  
Norihiko Hayazawa ◽  
Hidekazu Ishitobi ◽  
Satoshi Kawata ◽  
Manfred Reiche ◽  
...  

2020 ◽  
Vol 30 (1) ◽  
pp. 79
Author(s):  
Vuong Van Cuong ◽  
Dinh Ba Khuong ◽  
Dao Van Lap

We demonstrate that a two-colour three-pulsenonlinear spectroscopy can be used to study the dynamics of excited carriers inSi quantum dot structures embedded in SiN. Decays of the transverse optical phonon population and the transverse acoustic phonon population are measured and discussed. A simple theoretical modelis also used to support interpretation of our experimental observations.


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