234,599 research outputs found
Structural and optical properties of MOCVD AllnN epilayers
7] M.-Y. Ryu, C.Q. Chen, E. Kuokstis, J.W. Yang, G. Simin, M. Asif Khan, Appl. Phys. Lett. 80 (2002) 3730. [8] D. Xu, Y. Wang, H. Yang, L. Zheng, J. Li, L. Duan, R. Wu, Sci. China (a) 42 (1999) 517. [9] H. Hirayama, A. Kinoshita, A. Hirata, Y. Aoyagi, Phys. Stat. Sol. (a) 188 (2001) 83. [10] Y. Chen, T. Takeuchi, H. Amano, I. Akasaki, N. Yamada, Y. Kaneko, S.Y. Wang, Appl. Phys. Lett. 72 (1998) 710. [11] Ig-Hyeon Kim, Hyeong-Soo Park, Yong-Jo Park, Taeil Kim, Appl. Phys. Lett. 73 (1998) 1634. [12] K. Watanabe, J.R. Yang, S.Y. Huang, K. Inoke, J.T. Hsu, R.C. Tu, T. Yamazaki, N. Nakanishi, M. Shiojiri, Appl. Phys. Lett. 82 (2003) 718
Wang Bi\u27s Annotation on Laozi\u27s Place in China and Japan: Focusing on Ogyu Sorai
Wang Bi\u27s Annotation on Laozi 『老子』王弼注 is considered one of the representative notes on Laozi. In Chinahowever, it was not until 1781 when this book was included in Sikuquanshu 『四庫全書』 that the study of Wang Bi\u27s note became popular. In Japan, while Wang Bi\u27s note was introduced before the 5th century, it received rare recognition until Okada Touin\u27s Laozi Daodejing Annotated by Wang Bi 岡田東贇 『老子道徳経王弼注』 published in 1734. However, further research reveals that Ogyu Sorai 荻生徂徠 had pointed out in Keishishiyohran 『経子史要覧』 that, in reading Laozi from the view of classical rhetoric 古文辞学 Wang Bi\u27s annotation should be referred to. Keishishiyohran was based on Sorai\u27s dictation before 1728, and it was earlier than both Okada Touin\u27s Laozi Annotated by Wang Bi (1734) and Sikuquanshu (1781). Therefore< judging from evidences currently available, it seems fair to conclude that Sorai was the pioneer who introduced Wang Bi\u27s annotation into the field of Laozi studies
Two dimensional foam rheology with viscous drag
We formulate and apply a continuum model that incorporates elasticity, yield
stress, plasticity and viscous drag. It is motivated by the two-dimensional
foam rheology experiments of Debregeas et al. [G. Debregeas, H. Tabuteau, and
J.-M. di Meglio, Phys. Rev. Lett. 87, 178305 (2001)] and Wang et al [Y. Wang,
K. Krishan, and M. Dennin, Phys. Rev. E 73, 031401 (2006)], and is successful
in exhibiting their principal features an exponentially decaying velocity
profile and strain localisation. Transient effects are also identified.Comment: accepted version (to appear in PRL). Some parts of the paper have
been rewritten (mainly introduction and final discussion
Heartbeat Optical Coherence Tomography
__Abstract__
Coronary artery disease (CAD) is a manifestation of atherosclerosis, a systemic inflammatory disease of
the arteries that causes the formation of plaques in the artery walls. Different plaques may give rise to
different symptoms: a gradual narrowing (stenosis) of the vessel by growth of a fibrous or calcific plaque
will cause chest pain (due to cardiac ischemia) upon exertion, a condition called stable CAD. Sudden
onset of chest pain, or chest pain at rest, is a symptom of unstable CAD or acute coronary syndrome
(ACS), which is associated with thrombus formation on plaques, mostly due to rupture of a lipid-core
lesion. The most severe form of this disease may lead to a myocardial infarction or heart attack
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