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991.
Structural insight into chain-length control and product specificity of pentaketide chromone synthase from Aloe arborescens 总被引:1,自引:0,他引:1
The crystal structures of a wild-type and a mutant PCS, a novel plant type III polyketide synthase from a medicinal plant, Aloe arborescens, were solved at 1.6 A resolution. The crystal structures revealed that the pentaketide-producing wild-type and the octaketide-producing M207G mutant shared almost the same overall folding, and that the large-to-small substitution dramatically increases the volume of the polyketide-elongation tunnel by opening a gate to two hidden pockets behind the active site of the enzyme. The chemically inert active site residue 207 thus controls the number of condensations of malonyl-CoA, solely depending on the steric bulk of the side chain. These findings not only provided insight into the polyketide formation reaction, but they also suggested strategies for the engineered biosynthesis of polyketides. 相似文献
992.
Hirasawa Y Tanaka T Kobayashi J Kawahara N Goda Y Morita H 《Chemical & pharmaceutical bulletin》2008,56(10):1473-1476
A novel C(19)N-type Lycopodium alkaloid, malycorin A (1) consisting of a serratinane skeleton with 2-propanol unit has been isolated from the club moss Lycopodium phlegmaria, together with two new C(16)N-type alkaloids, malycorins B (2) and C (3), and the structures and relative stereochemistry were elucidated on the basis of spectroscopic data. 相似文献
993.
994.
Yuko Ikeda Pranee Phinyocheep Sumet Kittipoom Jareerat Ruancharoen Yota Kokubo Yuichi Morita Kensuke Hijikata Shinzo Kohjiya 《先进技术聚合物》2008,19(11):1608-1615
Mechanical properties of partially hydrogenated natural rubber (HNR) vulcanizates were evaluated regarding their chemical structure and crystallizable nature of HNR, and are reported here, to the best of our knowledge, for the first time. HNRs of three levels of hydrogenation (20.6, 29.0, and 40.6 mol%) were successfully prepared by the chemical modification of natural rubber (NR) latex using N2H4 and H2O2 as reagents, in a sufficient amount for preparing sulfur‐crosslinked samples to be subjected to mechanical and structural measurements. The three HNR vulcanizates were found to be crystallizable upon stretching; it is noted that even 40.6 mol% hydrogenation did not prevent HNR vulcanizates from crystallization upon stretching, while their onset strain of crystallization was higher than that of NR vulcanizate. The hysteresis loss and residual strain up to a stretching ratio of 2 for the HNR vulcanizates tended to become larger with the increase in the degree of the hydrogenation. Tensile and dynamic mechanical properties of 20.6 mol% hydrogenated HNR vulcanizate were comparable to those of NR vulcanizate. From differential scanning calorimetry and temperature dispersion of dynamic modulus or loss, the glass transition temperatures of HNR vulcanizates were found to be almost the same as that of NR vulcanizate, which is also notable. The thermal stability of HNR vulcanizates was better than that of NR vulcanizate. Thus, this chemical modification seems to give a promising NR derivative whose properties can be equivalent or even better than the mother polymer. Copyright © 2008 John Wiley & Sons, Ltd. 相似文献
995.
M. Huang H. Haba M. Murakami M. Asai D. Kaji J. Kanaya Y. Kasamatsu H. Kikunaga Y. Kikutani Y. Komori H. Kudo Y. Kudou K. Morimoto K. Morita K. Nakamura K. Ozeki R. Sakai A. Shinohara T. Sumita K. Tanaka A. Toyoshima K. Tsukada Y. Wakabayashi A. Yoneda 《Journal of Radioanalytical and Nuclear Chemistry》2015,304(2):845-849
996.
Y. Okumura H. Kase K. Morita 《The European Physical Journal C - Particles and Fields》2001,20(1):185-191
The standard model is reconstructed in a generalized differential geometry (GDG) based on the idea of a real structure as
proposed by Coquereaux et al. and Connes. The GDG considered in this article is a kind of non-commutative geometry (NCG) on
the discrete space that successfully reproduces the Higgs mechanism of the spontaneously broken gauge theory. Here, a GDG
is a direct generalization of the differential geometry on an ordinary continuous manifold to the product space of this manifold
with a discrete manifold. In a GDG, a one-form basis on the discrete space is incorporated in addition to the one-form basis on Minkowski space, rather than as in Connes's original work. Although the Lagrangians obtained in this way are the same as those obtained in our previous
formulation of GDG, the basic formalism becomes very simply and clear.
Received: 31 January 2000 / Revised version: 28 July 2000 / Published online: 25 April 2001 相似文献
997.
Y. Moriwaki N. Morita 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》1999,5(1):53-57
Emission and absorption spectra of Mg atoms implanted in liquid helium have been observed in the ultraviolet region. We have presented a model of exciplex formation of Mg-He10 and found that this model is more suitable for understanding the dynamics in the 3s3p 1P? 3s2 1S3s3p^{\:1}P\rightarrow 3s^{2\:1}S transition than the bubble model. 相似文献
998.
Y. Kuramitsu Y. Sakawa T. Morita C.D. Gregory J.N. Waugh M. Koenig N. Woolsey H. Takabe 《High Energy Density Physics》2013,9(1):222-225
Long time evolution of collisionless shocks in laser-produced plasmas is discussed. By irradiating a double plane target a high Mach number collisionless shock has been observed in laser produced counterstreaming plasmas [Kuramitsu et al., Phys. Rev. Lett., 106, 175002 (2011)]. While in early time we observe the shock in front of one plane, which is irradiated with the laser, we observe another shock in front of the other plane in much later time than the first shock formation. These two shocks coexist and collide or merge with each other as time passes. This means that the upstream plasmas for the first and second shocks have to be provided from the second and first shock sides, respectively, i.e., both the first and second shock have to be collisionless. There are two major candidates to account for the long time evolution of the collisionless shocks. One is that the secondary plasmas at the planes can be continuously created by the plasmas from the other planes. Another is that the actual shock thickness is much thiner than the detection limit, as indicated by numerical simulations. 相似文献
999.
1000.
Yuko Ikeda Atsushi Katoh Junichi Shimanuki Shinzo Kohjiya 《Macromolecular rapid communications》2004,25(12):1186-1190
Summary: Three dimensional (3D) nanostructures of particulate silicas in natural rubber (NR) were observed for the first time by use of 3D transmission electron microscopy (3D‐TEM) combined with electron tomography. The method enabled us to visualize and evaluate structural characteristics in 3D space, such as the size and the volume of in situ silica generated in the NR matrix by the sol‐gel reaction of tetraethoxysilane, at nanometer scale resolution.