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2013 [化學學系暨研究所] 學位論文 , Y. Kitahama, Y. Chen, B. Zhao, Y. Ozaki J. Phys. Chem. Lett. 2012, 3, 3204.
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2010-10 [機械與機電工程學系暨研究所] 期刊論文 Journal of Micromechanics and Microengineering 20(11), 115033(7pages) ) c ∂y y=0 0 ∂x x=0 p(x,t) − P(t) = 1 − x . (14) pmax − P(t) a
(w is the thickness along z-direction, not shown here
CC Hung; SM Yang; SE Tsai
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2018-03-13 [航空太空工程學系暨研究所] 期刊論文 Advances in Mechanical Engineering 10(3), p.1-8 + 1 z x domain. The electric fueld E~i, the immittance Z~ej, and P~ = B (k , k ) eg0(yd) ð6Þ the current density
Wei, Te-Yu; Yeh, Ping-Hung; Lu, Shih-Yuan; Wang, Zhong-Lin
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2009 [物理學系暨研究所] 期刊論文 Journal of the American Chemical Society 131(48), pp.17690–17695 ) Kuang, Q.; Lao, C.; Wang, Z. L.; Xie, Z.; Zheng, L. J. Am. Chem. Soc. 2007, 129, 6070.
(6) Shen, G.; Chen, P. C.; Ryu, K.; Zhou, C. J. Mater
Christine Amsler; Yi Yi Chen; Peter Schimdt; Hung Jen Wang
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2020-08-19 [經濟學系暨研究所] 期刊論文 Empirical Economics 60, p.53–363 (. A p-dimensional random variable Z is distributed as CSNp,q(μ,, D,,) if
its density is f (z) Cp(z/ μ,)q(D(z − μ)/ ,).Herep and q are the
p-variate
張桓碩; Chang, Huan-Shuo
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2014 [化學學系暨研究所] 學位論文 . Kim, D. Lee, J. Power Sources. 90 (2000) 139.
23. X. Guan, H. Zhou, Z. Liu, Y. Wang, J. Zhang, Mater. Res. Bull. 43 (2008) 1046.
24. X. Guan, H. Zhou
Yu, Shu-hui; Lin, Chien-chih; Cheng, Hung-wen
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2012-03 [財務金融學系暨研究所] 期刊論文 Journal of Time Series Analysis 33(2), pp.276-286 þ a1B þþapBpÞð1 BÞyt ¼ et;
where p 1, B is thePbackshift operator and 1 + a1z + + apzp 6¼ 0 for all |z| 1, Lemma 1 of Ing et al. (2010) implies
蔡慧駿; Tsay, Huoy-shyi
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2006-11 [機械與機電工程學系暨研究所] 期刊論文 Journal of the Acoustical Society of America 120(5), pp.2686-2693 from the initially un-deformed position.
Hence, the initial conditions for the foam are ui=0, Ui=0,
u.i=0, and U. i=0 i=x,y,z at t=0. ui and Ui i=x,y
Liu, Kuan-Liang; Hsu, Jyh-Ping; Tseng, Shiojenn
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2013-07 [應用數學與數據科學學系] 期刊論文 Langmuir 29(30), pp.9598-9603 ,z), Cj(r,z), v(r,z), and p(r,z)be
the electric potential, the molar concentration of ionic species j,
the fluid velocity, and the pressure
Chang, P. C.; Chen, S. H.; Lie, T.; Liu, Y. C.
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2011-05 [資訊工程學系暨研究所] 期刊論文 International Journal of Innovative Computing, Information and Control 7(5A), p.2323-2344 Chang, P. C. Chen, S. H. Lie, T. Liu, Y. C. A Genetic Algorithm Enhanced by Dominance Properties for Single Machine Scheduling Problems with Setup
Tong, Tinghao; Lee, Ming-Hsien; Zhang*, Jun
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2019-12-03 [物理學系暨研究所] 期刊論文 The Journal of Physical Chemistry C 123(51), p.31167-31174 (49) Ok, K. M.; Halasyamani, P. S.; Casanova, D.; Llunell, M.;
Structure of BaTiS3. Z. Naturforsch., B 1980, 35, 775. Alemany, P
郭芳綺; Kuo, Fang-chi
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2010 [國際企業學系暨研究所] 學位論文 ,” Harvard Business Review, Vol. 38 (July-August), p. p. 24-47.
Li, Z. G. and R. P. Dant (1997), “Dimension of Product Quality and Country-of-Origin
吳忠武; Wu, Jong-wuu
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2001-01-01 [統計學系暨研究所] 期刊論文 Statistical Papers 42(1), pp.123-133 )
and probability mass ( or densaty) function ( p.m.f. (or p.d.f.)) f(z). Let
Y,=max{Xx,X2,... ,X,}, for n > 1. We say Xj is an upper record value
Shieh, Chung-tsun
,
2004-04 [應用數學與數據科學學系] 期刊論文 Inverse Problems 20(2), pp.589-600 , (1.1)
can be viewed as a discretization of the one-dimensional Schro¨dinger equation
y(x) +[λ − p(x)]y(x) = 0
Chou, Chung-Pin; Lee, T. K.; Ho, Chang-ming
,
2006-09 [物理學系暨研究所] 期刊論文 Physical Review B (Condensed Matter and Materials Physics) 74(9), 092503(4pages) -RVB state on finite square lattices. With
SW, particularly, Z- for removing an electron defined in k
Eq. 1 below, calculated, we
