416,388 research outputs found

    Case comment: R (Wang Yam) v Central Criminal Court

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    In R (Wang Yam) v Central Criminal Court the Supreme Court has held that the domestic courts enjoy an inherent jurisdiction to make orders which have the effect of preventing an applicant to the Court of Human Rights from putting material before that court. This analysis considers the decision in the context of the growth of ā€˜secret trialsā€™ in the domestic criminal system, arguing that the Supreme Courtā€™s decision may merely postpone a dispute between the UK and the Strasbourg Court on the implications of this growth in secrecy for the UKā€™s compliance with the Convention

    Structural and optical properties of MOCVD AllnN epilayers

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    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

    Direct determination of the ambipolar diffusion length in strained InxGa1āˆ’xAs/InP quantum wells by cathodoluminescence

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    The ambipolar diffusion length is measured in strained InxGa1āˆ’xAs/InP quantum wells for several mole fractions in the interval 0.3<x<0.8 by cathodoluminescence. The ambipolar diffusion length is found to have a significantly higher value in the lower indium mole fraction samples corresponding to tensile-strained wells. This longer diffusion length for the tensile samples is consistent with results of carrier lifetime experiments by M. C. Wang, K. Kash, C. E. Zah, R. Bhat, and S. L. Chuang [Appl. Phys. Lett. 62, 166 (1993)]

    New necessary conditions for (negative) Latin square type partial difference sets in abelian groups

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    Partial difference sets (for short, PDSs) with parameters (n2n^2, r(nāˆ’Ļµ)r(n-\epsilon), Ļµn+r2āˆ’3Ļµr\epsilon n+r^2-3\epsilon r, r2āˆ’Ļµrr^2-\epsilon r) are called Latin square type (respectively negative Latin square type) PDSs if Ļµ=1\epsilon=1 (respectively Ļµ=āˆ’1\epsilon=-1). In this paper, we will give restrictions on the parameter rr of a (negative) Latin square type partial difference set in an abelian group of non-prime power order. As far as we know no previous general restrictions on rr were known. Our restrictions are particularly useful when aa is much larger than bb. As an application, we show that if there exists an abelian negative Latin square type PDS with parameter set (9p4s,r(3p2s+1),āˆ’3p2s+r2+3r,r2+r)(9p^{4s}, r(3p^{2s}+1),-3p^{2s}+r^2+3r,r^2+r), 1ā‰¤rā‰¤3p2sāˆ’121 \le r \le \frac{3p^{2s}-1}{2}, pā‰”1(mod4)p\equiv 1 \pmod 4 a prime number and ss is an odd positive integer, then there are at most three possible values for rr. For two of these three rr values, J. Polhill gave constructions in 2009

    On Fugledeā€™s conjecture and the existence of universal spectra

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    Recent methods developed by, Too [18], Kolountzakis and Matolcsi [7] have led to counterexamples to Fugelde's Spectral Set Conjecture in both directions. Namely, in R(5) Tao produced a spectral set which is not a tile, while Kolountzakis and Matolcsi showed all example of a nonspectral tile. In search of lower dimensional nonspectral tiles we were led to investigate the Universal Spectrum Conjecture (USC) of Lagarias and Wang [14]. In particular, we prove here that the USC and the "tile --> spectral " direction of Fuglede's conjecture are equivalent in any dimensions. Also, we show by an example that the sufficient condition of Lagarias and Szabo [13] for the existence of universal spectra is not necessary. This fact causes considerable difficulties in producing lower dimensional examples of tiles which have no spectra. We overcome these difficulties by invoking some ideas of Revesz and Farkas [2], and obtain nonspectral tiles in R(3)
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