100 results on '"W. Yuan"'
Search Results
2. 121P ATM germline mutations in lethal prostate cancer
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R.M. Grochot, S. Carreira, S. Miranda, I. Figueiredo, C. Bertan, J. Rekowski, W. Yuan, A. Ferreira, R. Riisnaes, A. Neeb, B. Gurel, M.D.L.D. Fenor de la Maza, J. Carmichael, D. Westaby, C. Guo, A. Sharp, and J.S. de Bono
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Oncology ,Hematology - Published
- 2022
3. Composition-dependent mechanical property changes in Au-ion-irradiated borosilicate glasses
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W. Yuan, Limin Zhang, B.T. Zhang, Y. Zhao, Binghuang Duan, Y.D. Guan, Tieshan Wang, Li-Chuan Chen, Peng Lv, and X.Y. Zhang
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Nuclear and High Energy Physics ,Materials science ,Borosilicate glass ,Analytical chemistry ,Modulus ,Young's modulus ,Nanoindentation ,Ion ,symbols.namesake ,Nuclear Energy and Engineering ,symbols ,General Materials Science ,Composition (visual arts) ,Irradiation ,Ternary operation - Abstract
The mechanical property changes in three kinds of ternary borosilicate glasses (named NBS glasses) induced by 8.0-MeV Au3+ were studied by nanoindentation measurements. For these borosilicate glasses, the molar ratio R = [Na2O]/[B2O3] is varied (1.34, 0.75, and 0.40 for NBS1, NBS2, and NBS3, respectively), while their molar ratio K = [SiO2]/[B2O3] is fixed at 4.04. The nanoindentation results indicate that both the hardness and reduced Young modulus were decreased after irradiation. No obvious difference in both hardness and modulus variations of these three NBS glasses was observed. Based on the main structures of their pristine samples, the reedmergnerite groups containing Si-O-BIV may be the structural origin of Au-ion-irradiated mechanical property changes in the homogeneous glasses with R > 0.5. However, the modification of the silica network and phase separation may dominate the mechanical property changes for glasses with R ≤ 0.5. The ion- and electron-irradiation-induced mechanical property changes of these NBS glasses were also compared in this study. The extended incubation dose and the slower decreasing rate can be observed in electron-irradiation-induced hardness and modulus variations, which may be caused by the different mechanisms between both irradiation scenarios.
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- 2019
4. The effects of temperature and Ce-dopant concentration on the synthesis of zirconolite glass-ceramic
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Limin Zhang, B.H. Duan, Zhehao Chen, Yedong Guan, Bingtao Zhang, Tieshan Wang, W. Yuan, Duofei Zhang, Peng Lv, Liang Chen, and Chenglong Pan
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010302 applied physics ,Zirconolite ,Glass-ceramic ,Materials science ,Dopant ,Scanning electron microscope ,Process Chemistry and Technology ,Nucleation ,02 engineering and technology ,Thermal treatment ,021001 nanoscience & nanotechnology ,01 natural sciences ,Surfaces, Coatings and Films ,Electronic, Optical and Magnetic Materials ,law.invention ,Chemical engineering ,law ,0103 physical sciences ,Materials Chemistry ,Ceramics and Composites ,Particle size ,Crystallization ,0210 nano-technology - Abstract
Zirconolite based glass-ceramic has been deemed as a promising waste form for high-level waste (HLW). In this study, the zirconolite (nominally CaZrTi2O7) glass-ceramic based on a SiO2-B2O3-Na2O-CaO-ZrO2-TiO2-Al2O3 system was sought to be synthesized by two-step thermal treatment. The temperature effects such as nucleation temperature and cooling rate were studied. The influence of the Ce-dopant concentration on crystallization behavior was also investigated. For characterization, powder X-ray diffraction (XRD), thermogravimetry-differential scanning calorimeter (TG-DSC) and scanning electron microscopy (SEM) were applied. Our results illustrate that homogeneous zirconolite with the particle size of 1.8 μm can be the target phase when the glass matrix underwent a rapid cooling process and the nucleation temperature was controlled at around 860 °C. Besides, the results also indicate that the distribution of the zirconolite along with its lattice parameters change regularly as the increase of CeO2 concentration. A larger crystal size of zirconolite phase and some trace amounts of precipitated phases are observed when the CeO2 concentration exceed 3 wt%. This work emphasizes the synthesis of zirconolite glass-ceramic in a SiO2-B2O3-Na2O-CaO-ZrO2-TiO2-Al2O3 system, which is expected to provide basic technical data for underground disposal of HLW.
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- 2019
5. Measurement of the e+e−→Σ0Σ¯0 cross sections at center-of-mass energies from 2.3864 to 3.0200 GeV
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M. Ablikim, M.N. Achasov, P. Adlarson, S. Ahmed, M. Albrecht, A. Amoroso, Q. An, Y. Bai, O. Bakina, R. Baldini Ferroli, I. Balossino, Y. Ban, K. Begzsuren, J.V. Bennett, N. Berger, M. Bertani, D. Bettoni, F. Bianchi, J. Biernat, J. Bloms, A. Bortone, I. Boyko, R.A. Briere, H. Cai, X. Cai, A. Calcaterra, G.F. Cao, N. Cao, S.A. Cetin, J.F. Chang, W.L. Chang, G. Chelkov, D.Y. Chen, G. Chen, H.S. Chen, M.L. Chen, S.J. Chen, X.R. Chen, Y.B. Chen, W. Cheng, G. Cibinetto, F. Cossio, X.F. Cui, H.L. Dai, J.P. Dai, X.C. Dai, A. Dbeyssi, R.B. de Boer, D. Dedovich, Z.Y. Deng, A. Denig, I. Denysenko, M. Destefanis, F. De Mori, Y. Ding, C. Dong, J. Dong, L.Y. Dong, M.Y. Dong, S.X. Du, J. Fang, S.S. Fang, Y. Fang, R. Farinelli, L. Fava, F. Feldbauer, G. Felici, C.Q. Feng, M. Fritsch, C.D. Fu, Y. Fu, X.L. Gao, Y. Gao, Y.G. Gao, I. Garzia, E.M. Gersabeck, A. Gilman, K. Goetzen, L. Gong, W.X. Gong, W. Gradl, M. Greco, L.M. Gu, M.H. Gu, S. Gu, Y.T. Gu, C.Y. Guan, A.Q. Guo, L.B. Guo, R.P. Guo, Y.P. Guo, A. Guskov, S. Han, T.T. Han, T.Z. Han, X.Q. Hao, F.A. Harris, K.L. He, F.H. Heinsius, T. Held, Y.K. Heng, M. Himmelreich, T. Holtmann, Y.R. Hou, Z.L. Hou, H.M. Hu, J.F. Hu, T. Hu, Y. Hu, G.S. Huang, L.Q. Huang, X.T. Huang, Z. Huang, N. Huesken, T. Hussain, W. Ikegami Andersson, W. Imoehl, M. Irshad, S. Jaeger, S. Janchiv, Q. Ji, Q.P. Ji, X.B. Ji, X.L. Ji, H.B. Jiang, X.S. Jiang, X.Y. Jiang, J.B. Jiao, Z. Jiao, S. Jin, Y. Jin, T. Johansson, N. Kalantar-Nayestanaki, X.S. Kang, R. Kappert, M. Kavatsyuk, B.C. Ke, I.K. Keshk, A. Khoukaz, P. Kiese, R. Kiuchi, R. Kliemt, L. Koch, O.B. Kolcu, B. Kopf, M. Kuemmel, M. Kuessner, A. Kupsc, M.G. Kurth, W. Kühn, J.J. Lane, J.S. Lange, P. Larin, L. Lavezzi, H. Leithoff, M. Lellmann, T. Lenz, C. Li, C.H. Li, Cheng Li, D.M. Li, F. Li, G. Li, H.B. Li, H.J. Li, J.L. Li, J.Q. Li, Ke Li, L.K. Li, Lei Li, P.L. Li, P.R. Li, S.Y. Li, W.D. Li, W.G. Li, X.H. Li, X.L. Li, Z.B. Li, Z.Y. Li, H. Liang, Y.F. Liang, Y.T. Liang, L.Z. Liao, J. Libby, C.X. Lin, B. Liu, B.J. Liu, C.X. Liu, D. Liu, D.Y. Liu, F.H. Liu, Fang Liu, Feng Liu, H.B. Liu, H.M. Liu, Huanhuan Liu, Huihui Liu, J.B. Liu, J.Y. Liu, K. Liu, K.Y. Liu, Ke Liu, L. Liu, Q. Liu, S.B. Liu, Shuai Liu, T. Liu, X. Liu, Y.B. Liu, Z.A. Liu, Z.Q. Liu, Y.F. Long, X.C. Lou, F.X. Lu, H.J. Lu, J.D. Lu, J.G. Lu, X.L. Lu, Y. Lu, Y.P. Lu, C.L. Luo, M.X. Luo, P.W. Luo, T. Luo, X.L. Luo, S. Lusso, X.R. Lyu, F.C. Ma, H.L. Ma, L.L. Ma, M.M. Ma, Q.M. Ma, R.Q. Ma, R.T. Ma, X.N. Ma, X.X. Ma, X.Y. Ma, Y.M. Ma, F.E. Maas, M. Maggiora, S. Maldaner, S. Malde, Q.A. Malik, A. Mangoni, Y.J. Mao, Z.P. Mao, S. Marcello, Z.X. Meng, J.G. Messchendorp, G. Mezzadri, T.J. Min, R.E. Mitchell, X.H. Mo, Y.J. Mo, N.Yu. Muchnoi, H. Muramatsu, S. Nakhoul, Y. Nefedov, F. Nerling, I.B. Nikolaev, Z. Ning, S. Nisar, S.L. Olsen, Q. Ouyang, S. Pacetti, X. Pan, Y. Pan, A. Pathak, P. Patteri, M. Pelizaeus, H.P. Peng, K. Peters, J. Pettersson, J.L. Ping, R.G. Ping, A. Pitka, R. Poling, V. Prasad, H. Qi, H.R. Qi, M. Qi, T.Y. Qi, S. Qian, W.-B. Qian, Z. Qian, C.F. Qiao, L.Q. Qin, X.P. Qin, X.S. Qin, Z.H. Qin, J.F. Qiu, S.Q. Qu, K.H. Rashid, K. Ravindran, C.F. Redmer, A. Rivetti, V. Rodin, M. Rolo, G. Rong, Ch. Rosner, M. Rump, A. Sarantsev, M. Savrié, Y. Schelhaas, C. Schnier, K. Schoenning, D.C. Shan, W. Shan, X.Y. Shan, M. Shao, C.P. Shen, P.X. Shen, X.Y. Shen, H.C. Shi, R.S. Shi, X. Shi, X.D. Shi, J.J. Song, Q.Q. Song, W.M. Song, Y.X. Song, S. Sosio, S. Spataro, F.F. Sui, G.X. Sun, J.F. Sun, L. Sun, S.S. Sun, T. Sun, W.Y. Sun, Y.J. Sun, Y.K. Sun, Y.Z. Sun, Z.T. Sun, Y.H. Tan, Y.X. Tan, C.J. Tang, G.Y. Tang, J. Tang, V. Thoren, B. Tsednee, I. Uman, B. Wang, B.L. Wang, C.W. Wang, D.Y. Wang, H.P. Wang, K. Wang, L.L. Wang, M. Wang, M.Z. Wang, Meng Wang, W.H. Wang, W.P. Wang, X. Wang, X.F. Wang, X.L. Wang, Y. Wang, Y.D. Wang, Y.F. Wang, Y.Q. Wang, Z. Wang, Z.Y. Wang, Ziyi Wang, Zongyuan Wang, T. Weber, D.H. Wei, P. Weidenkaff, F. Weidner, S.P. Wen, D.J. White, U. Wiedner, G. Wilkinson, M. Wolke, L. Wollenberg, J.F. Wu, L.H. Wu, L.J. Wu, X. Wu, Z. Wu, L. Xia, H. Xiao, S.Y. Xiao, Y.J. Xiao, Z.J. Xiao, X.H. Xie, Y.G. Xie, Y.H. Xie, T.Y. Xing, X.A. Xiong, G.F. Xu, J.J. Xu, Q.J. Xu, W. Xu, X.P. Xu, L. Yan, W.B. Yan, W.C. Yan, Xu Yan, H.J. Yang, H.X. Yang, L. Yang, R.X. Yang, S.L. Yang, Y.H. Yang, Y.X. Yang, Yifan Yang, Zhi Yang, M. Ye, M.H. Ye, J.H. Yin, Z.Y. You, B.X. Yu, C.X. Yu, G. Yu, J.S. Yu, T. Yu, C.Z. Yuan, W. Yuan, X.Q. Yuan, Y. Yuan, Z.Y. Yuan, C.X. Yue, A. Yuncu, A.A. Zafar, Y. Zeng, B.X. Zhang, Guangyi Zhang, H.H. Zhang, H.Y. Zhang, J.L. Zhang, J.Q. Zhang, J.W. Zhang, J.Y. Zhang, J.Z. Zhang, Jianyu Zhang, Jiawei Zhang, L. Zhang, Lei Zhang, S. Zhang, S.F. Zhang, T.J. Zhang, X.Y. Zhang, Y. Zhang, Y.H. Zhang, Y.T. Zhang, Yan Zhang, Yao Zhang, Yi Zhang, Z.H. Zhang, Z.Y. Zhang, G. Zhao, J. Zhao, J.Y. Zhao, J.Z. Zhao, Lei Zhao, Ling Zhao, M.G. Zhao, Q. Zhao, S.J. Zhao, Y.B. Zhao, Y.X. Zhao, Z.G. Zhao, A. Zhemchugov, B. Zheng, J.P. Zheng, Y. Zheng, Y.H. Zheng, B. Zhong, C. Zhong, L.P. Zhou, Q. Zhou, X. Zhou, X.K. Zhou, X.R. Zhou, A.N. Zhu, J. Zhu, K. Zhu, K.J. Zhu, S.H. Zhu, W.J. Zhu, X.L. Zhu, Y.C. Zhu, Z.A. Zhu, B.S. Zou, and J.H. Zou
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Nuclear and High Energy Physics - Published
- 2022
6. China’s participation in the international RRT for Ic measurement of superconducting cables organized by IEC/TC90
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J. Li, Y. Shi, G.M. Zhang, L.W. Jing, J.X. Zheng, C.L. Liu, W. Yuan, Y.S. Wang, M. Song, Y.J. Xia, X.H. Zong, Y.W. Han, D.N. Zheng, X.J. Zhou, T. Matsushita, and G. Nishijima
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- 2022
7. POS-427 LEFLUNOMIDE PLUS LOW-DOSE PREDNISONE IN PATIENTS WITH PROGRESSIVE IgA NEPHROPATHY: A MULTICENTER, PROSPECTIVE, RANDOMIZED, OPEN-LABELLED AND CONTROLLED TRIAL
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Z. ZHANG, Z. Ni, Z. Yu, F. Lu, C. Mei, X. Ding, W. Yuan, W. Zhang, G. Jiang, M. Sun, L. He, Y. Deng, H. Pang, and J. Qian
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Nephrology - Published
- 2022
8. Variation of hardness and modulus of sodium borosilicate glass irradiated with different ions
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Tianhe Wang, B.H. Duan, Xin Zhang, H.B. Peng, M.L. Sun, M. Guan, Fengfei Liu, Xin Du, and W. Yuan
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010302 applied physics ,Nuclear and High Energy Physics ,Chemical resistance ,Materials science ,Borosilicate glass ,Sodium ,Modulus ,chemistry.chemical_element ,02 engineering and technology ,021001 nanoscience & nanotechnology ,01 natural sciences ,Ion ,Viscosity ,chemistry ,0103 physical sciences ,Vitrification ,Irradiation ,Composite material ,0210 nano-technology ,Instrumentation - Abstract
Borosilicate glass with characteristics of high thermal, mechanical and chemical resistance has plenty of applications. As one of the candidates who are possible to vitrify high level radioactive waste, the borosilicate glass has been studied extensively. The borosilicate glass was added with sodium to increase electrical conductivity and decrease viscosity. The tolerance of sodium borosilicate glass on irradiation is important to vitrification. In this work, the sodium borosilicate glass samples were irradiated with different ions. The dependence of hardness and modulus on irradiation dose was studied. A semi-empirical formulation was proposed. Possible reasons for the change of modulus and hardness were discussed.
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- 2018
9. Comparison of hardness variation of ion irradiated borosilicate glasses with different projected ranges
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B.H. Duan, H.B. Peng, Tianhe Wang, Bingtao Zhang, Xin Du, W. Yuan, Xin Zhang, M.L. Sun, and Fengfei Liu
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010302 applied physics ,Nuclear and High Energy Physics ,Range (particle radiation) ,Materials science ,Borosilicate glass ,Analytical chemistry ,Extrapolation ,02 engineering and technology ,Radiation ,Nanoindentation ,021001 nanoscience & nanotechnology ,01 natural sciences ,Ion ,0103 physical sciences ,Vitrification ,Irradiation ,0210 nano-technology ,Instrumentation - Abstract
Borosilicate glass has potential application for vitrification of high-level radioactive waste, which attracts extensive interest in studying its radiation durability. In this study, sodium borosilicate glass samples were irradiated with 4 MeV Kr 17+ ion, 5 MeV Xe 26+ ion and 0.3 MeV P + ion, respectively. The hardness of irradiated borosilicate glass samples was measured with nanoindentation in continuous stiffness mode and quasi continuous stiffness mode, separately. Extrapolation method, mean value method, squared extrapolation method and selected point method are used to obtain hardness of irradiated glass and a comparison among these four methods is conducted. The extrapolation method is suggested to analyze the hardness of ion irradiated glass. With increasing irradiation dose, the values of hardness for samples irradiated with Kr, Xe and P ions dropped and then saturated at 0.02 dpa. Besides, both the maximum variations and decay constants for three kinds of ions with different energies are similar indicates the similarity behind the hardness variation in glasses after irradiation. Furthermore, the hardness variation of low energy P ion irradiated samples whose range is much smaller than those of high energy Kr and Xe ions, has the same trend as that of Kr and Xe ions. It suggested that electronic energy loss did not play a significant role in hardness decrease for irradiation of low energy ions.
- Published
- 2018
10. Measurement of the inclusive branching fraction for ψ(3686)→KS0+anything
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M. Ablikim, M.N. Achasov, P. Adlarson, S. Ahmed, M. Albrecht, R. Aliberti, A. Amoroso, Q. An, X.H. Bai, Y. Bai, O. Bakina, R. Baldini Ferroli, I. Balossino, Y. Ban, K. Begzsuren, J.V. Bennett, N. Berger, M. Bertani, D. Bettoni, F. Bianchi, J. Biernat, J. Bloms, A. Bortone, I. Boyko, R.A. Briere, H. Cai, X. Cai, A. Calcaterra, G.F. Cao, N. Cao, S.A. Cetin, J.F. Chang, W.L. Chang, G. Chelkov, D.Y. Chen, G. Chen, H.S. Chen, M.L. Chen, S.J. Chen, X.R. Chen, Y.B. Chen, Z.J. Chen, W.S. Cheng, G. Cibinetto, F. Cossio, X.F. Cui, H.L. Dai, X.C. Dai, A. Dbeyssi, R.E. de Boer, D. Dedovich, Z.Y. Deng, A. Denig, I. Denysenko, M. Destefanis, F. De Mori, Y. Ding, C. Dong, J. Dong, L.Y. Dong, M.Y. Dong, S.X. Du, J. Fang, S.S. Fang, Y. Fang, R. Farinelli, L. Fava, F. Feldbauer, G. Felici, C.Q. Feng, M. Fritsch, C.D. Fu, Y. Fu, X.L. Gao, Y. Gao, Y.G. Gao, I. Garzia, E.M. Gersabeck, A. Gilman, K. Goetzen, L. Gong, W.X. Gong, W. Gradl, M. Greco, L.M. Gu, M.H. Gu, S. Gu, Y.T. Gu, C.Y. Guan, A.Q. Guo, L.B. Guo, R.P. Guo, Y.P. Guo, A. Guskov, S. Han, T.T. Han, T.Z. Han, X.Q. Hao, F.A. Harris, K.L. He, F.H. Heinsius, C.H. Heinz, T. Held, Y.K. Heng, M. Himmelreich, T. Holtmann, Y.R. Hou, Z.L. Hou, H.M. Hu, J.F. Hu, T. Hu, Y. Hu, G.S. Huang, L.Q. Huang, X.T. Huang, Y.P. Huang, Z. Huang, T. Hussain, N. Hüsken, W. Ikegami Andersson, W. Imoehl, M. Irshad, S. Jaeger, S. Janchiv, Q. Ji, Q.P. Ji, X.B. Ji, X.L. Ji, H.B. Jiang, X.S. Jiang, J.B. Jiao, Z. Jiao, S. Jin, Y. Jin, T. Johansson, N. Kalantar-Nayestanaki, X.S. Kang, R. Kappert, M. Kavatsyuk, B.C. Ke, I.K. Keshk, A. Khoukaz, P. Kiese, R. Kiuchi, R. Kliemt, L. Koch, O.B. Kolcu, B. Kopf, M. Kuemmel, M. Kuessner, A. Kupsc, M.G. Kurth, W. Kühn, J.J. Lane, J.S. Lange, P. Larin, A. Lavania, L. Lavezzi, H. Leithoff, M. Lellmann, T. Lenz, C. Li, C.H. Li, Cheng Li, D.M. Li, F. Li, G. Li, H. Li, H.B. Li, H.J. Li, J.L. Li, J.Q. Li, Ke Li, L.K. Li, Lei Li, P.L. Li, P.R. Li, S.Y. Li, W.D. Li, W.G. Li, X.H. Li, X.L. Li, Z.Y. Li, H. Liang, Y.F. Liang, Y.T. Liang, G.R. Liao, L.Z. Liao, J. Libby, C.X. Lin, B. Liu, B.J. Liu, C.X. Liu, D. Liu, D.Y. Liu, F.H. Liu, Fang Liu, Feng Liu, H.B. Liu, H.M. Liu, Huanhuan Liu, Huihui Liu, J.B. Liu, J.Y. Liu, K. Liu, K.Y. Liu, L. Liu, Q. Liu, S.B. Liu, Shuai Liu, T. Liu, W.M. Liu, X. Liu, Y.B. Liu, Z.A. Liu, Z.Q. Liu, X.C. Lou, F.X. Lu, H.J. Lu, J.D. Lu, J.G. Lu, X.L. Lu, Y. Lu, Y.P. Lu, C.L. Luo, M.X. Luo, P.W. Luo, T. Luo, X.L. Luo, S. Lusso, X.R. Lyu, F.C. Ma, H.L. Ma, L.L. Ma, M.M. Ma, Q.M. Ma, R.Q. Ma, R.T. Ma, X.N. Ma, X.X. Ma, X.Y. Ma, Y.M. Ma, F.E. Maas, M. Maggiora, S. Maldaner, S. Malde, Q.A. Malik, A. Mangoni, Y.J. Mao, Z.P. Mao, S. Marcello, Z.X. Meng, J.G. Messchendorp, G. Mezzadri, T.J. Min, R.E. Mitchell, X.H. Mo, N.Yu. Muchnoi, H. Muramatsu, S. Nakhoul, Y. Nefedov, F. Nerling, I.B. Nikolaev, Z. Ning, S. Nisar, S.L. Olsen, Q. Ouyang, S. Pacetti, X. Pan, Y. Pan, A. Pathak, P. Patteri, M. Pelizaeus, H.P. Peng, K. Peters, J. Pettersson, J.L. Ping, R.G. Ping, A. Pitka, R. Poling, V. Prasad, H. Qi, H.R. Qi, M. Qi, T.Y. Qi, S. Qian, W.B. Qian, Z. Qian, C.F. Qiao, L.Q. Qin, X.S. Qin, Z.H. Qin, J.F. Qiu, S.Q. Qu, K.H. Rashid, K. Ravindran, C.F. Redmer, A. Rivetti, V. Rodin, M. Rolo, G. Rong, Ch. Rosner, M. Rump, A. Sarantsev, Y. Schelhaas, C. Schnier, K. Schoenning, M. Scodeggio, D.C. Shan, W. Shan, X.Y. Shan, M. Shao, C.P. Shen, P.X. Shen, X.Y. Shen, H.C. Shi, R.S. Shi, X. Shi, X.D. Shi, J.J. Song, Q.Q. Song, W.M. Song, Y.X. Song, S. Sosio, S. Spataro, F.F. Sui, G.X. Sun, J.F. Sun, L. Sun, S.S. Sun, T. Sun, W.Y. Sun, X. Sun, Y.J. Sun, Y.K. Sun, Y.Z. Sun, Z.T. Sun, Y.H. Tan, Y.X. Tan, C.J. Tang, G.Y. Tang, J. Tang, J.X. Teng, V. Thoren, I. Uman, B. Wang, B.L. Wang, C.W. Wang, D.Y. Wang, H.P. Wang, K. Wang, L.L. Wang, M. Wang, M.Z. Wang, Meng Wang, W.H. Wang, W.P. Wang, X. Wang, X.F. Wang, X.L. Wang, Y. Wang, Y.D. Wang, Y.F. Wang, Y.Q. Wang, Z. Wang, Z.Y. Wang, Ziyi Wang, Zongyuan Wang, D.H. Wei, P. Weidenkaff, F. Weidner, S.P. Wen, D.J. White, U. Wiedner, G. Wilkinson, M. Wolke, L. Wollenberg, J.F. Wu, L.H. Wu, L.J. Wu, X. Wu, Z. Wu, L. Xia, H. Xiao, S.Y. Xiao, Y.J. Xiao, Z.J. Xiao, X.H. Xie, Y.G. Xie, Y.H. Xie, T.Y. Xing, X.A. Xiong, G.F. Xu, J.J. Xu, Q.J. Xu, W. Xu, X.P. Xu, Y.C. Xu, F. Yan, L. Yan, W.B. Yan, W.C. Yan, Xu Yan, H.J. Yang, H.X. Yang, L. Yang, R.X. Yang, S.L. Yang, Y.H. Yang, Y.X. Yang, Yifan Yang, Zhi Yang, M. Ye, M.H. Ye, J.H. Yin, Z.Y. You, B.X. Yu, C.X. Yu, G. Yu, J.S. Yu, T. Yu, C.Z. Yuan, W. Yuan, X.Q. Yuan, Y. Yuan, Z.Y. Yuan, C.X. Yue, A.A. Zafar, Y. Zeng, B.X. Zhang, Guangyi Zhang, H. Zhang, H.H. Zhang, H.Y. Zhang, J.L. Zhang, J.Q. Zhang, J.W. Zhang, J.Y. Zhang, J.Z. Zhang, Jianyu Zhang, Jiawei Zhang, Lei Zhang, S. Zhang, S.F. Zhang, T.J. Zhang, X.Y. Zhang, Y. Zhang, Y.H. Zhang, Y.T. Zhang, Yan Zhang, Yao Zhang, Yi Zhang, Z.Y. Zhang, G. Zhao, J. Zhao, J.Y. Zhao, J.Z. Zhao, Lei Zhao, Ling Zhao, M.G. Zhao, Q. Zhao, S.J. Zhao, Y.B. Zhao, Y.X. Zhao, Z.G. Zhao, A. Zhemchugov, B. Zheng, J.P. Zheng, Y.H. Zheng, B. Zhong, C. Zhong, L.P. Zhou, Q. Zhou, X. Zhou, X.K. Zhou, X.R. Zhou, A.N. Zhu, J. Zhu, K. Zhu, K.J. Zhu, S.H. Zhu, W.J. Zhu, Y.C. Zhu, Z.A. Zhu, B.S. Zou, and J.H. Zou
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Physics ,Nuclear and High Energy Physics ,Annihilation ,010308 nuclear & particles physics ,Branching fraction ,Continuum (design consultancy) ,01 natural sciences ,Measure (mathematics) ,law.invention ,Nuclear physics ,law ,0103 physical sciences ,010306 general physics ,Collider ,Beam energy - Abstract
Using 5.9 pb−1 of e + e − annihilation data collected at center-of-mass energies from 3.640 to 3.701 GeV with the BESIII detector at the BEPCII Collider, we measure the observed cross sections of e + e − → K S 0 X (where X = anything ). From a fit to these observed cross sections with the sum of continuum and ψ ( 3686 ) and J / ψ Breit-Wigner functions and considering initial state radiation and the BEPCII beam energy spread, we obtain for the first time the product of ψ ( 3686 ) leptonic width and inclusive decay branching fraction Γ ψ ( 3686 ) e e B ( ψ ( 3686 ) → K S 0 X ) = ( 373.8 ± 6.7 ± 20.0 ) eV, and assuming Γ ψ ( 3686 ) e e is ( 2.33 ± 0.04 ) keV from PDG value, we measure B ( ψ ( 3686 ) → K S 0 X ) = ( 16.04 ± 0.29 ± 0.90 ) % , where the first uncertainty is statistical and the second is systematic.
- Published
- 2021
11. Will river erosion below the Three Gorges Dam stop in the middle Yangtze?
- Author
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Brian Finlayson, Zhijun Dai, Taoyuan Wei, Shilun Yang, Xijun Lai, Zhongyuan Chen, W. Yuan, Shu Gao, Maotian Li, and D. Yin
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Hydrology ,geography ,geography.geographical_feature_category ,010504 meteorology & atmospheric sciences ,0208 environmental biotechnology ,Sediment ,02 engineering and technology ,01 natural sciences ,020801 environmental engineering ,Water resources ,River mouth ,Erosion ,Carrying capacity ,Environmental impact assessment ,Sediment transport ,Geology ,Channel (geography) ,0105 earth and related environmental sciences ,Water Science and Technology - Abstract
The environmental impact of the Three Gorges Dam has been a subject of vigorous academic, political and social debate since its inception. This includes the key issue of post-dam river channel erosion, which was predicted by the feasibility study to extend to the river mouth. In this paper we examine the geomorphic response of the channel of the middle Yangtze for 660 km downstream of the dam. Using data on channel characteristics, bed material and sediment transport, we show that in the decade following the dam closure, pre-dam seasonal erosion has been replaced by year-round erosion, a pattern most marked at the upstream end of the study area. The sediment carrying capacity of the river channel has been largely reduced below the dam. The locus of bed scour has moved progressively downstream, ceasing as the bed material became too coarse to be transported (e.g. D50: 0.29 mm pre-dam coarsened to 20 mm below the dam by 2008). About 400 km below the dam there is a reduction in channel slope that changes the sediment carrying capacity from 0.25 kg m−3 to only about 0.05 kg m−3, which is insufficient to move bed sediment. The new long-term hydro-morphological equilibrium that will be established in this section of the middle Yangtze will prevent the further incision downstream initiated by the Three Gorges Dam. The results suggest that the full extent of adverse environmental impact predicted by the pre-dam studies will not eventuate.
- Published
- 2017
12. Potential effect on the interaction of highly charged ion with graphene
- Author
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H.B. Peng, Lanxi Wang, Hao Chen, Tieshan Wang, Fengfei Liu, W. Yuan, Duofei Zhang, Xin Du, Di Yang, and M.L. Sun
- Subjects
Nuclear and High Energy Physics ,Materials science ,Graphene ,Highly charged ion ,02 engineering and technology ,021001 nanoscience & nanotechnology ,01 natural sciences ,Charged particle ,law.invention ,Ion ,symbols.namesake ,law ,Chemical physics ,0103 physical sciences ,Physics::Atomic and Molecular Clusters ,symbols ,Atomic physics ,010306 general physics ,0210 nano-technology ,Spectroscopy ,Bilayer graphene ,Raman spectroscopy ,Instrumentation ,Graphene nanoribbons - Abstract
Graphene is two dimensional materials which is composited by carbon atoms in honeycomb like lattice. Because of its wonderful characteristics, graphene was studied extensively. In this study, the interaction of highly charged ions (HCI) with the graphene was studied via Raman spectroscopy. The difference of Raman spectra of graphene impacted by HCIs with different charge states was presented. The intensity ratio of D peak to G peak varied with the square root of fluence was displayed. A model that was fitted with experimental results was proposed. According to the model, the potential effect that the size of damaged region grew with potential energy of HCI was proposed for the interaction of HCI with graphene.
- Published
- 2017
13. Variation of hardness and modulus of borosilicate glass irradiated with Kr ions
- Author
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M.L. Sun, B.H. Duan, Dongyan Yang, Tianhe Wang, H.B. Peng, Liang Chen, Xin Du, and W. Yuan
- Subjects
010302 applied physics ,Nuclear and High Energy Physics ,Materials science ,Borosilicate glass ,Modulus ,02 engineering and technology ,Radiation ,021001 nanoscience & nanotechnology ,01 natural sciences ,Durability ,Ion ,0103 physical sciences ,Vitrification ,Nanoindenter ,Irradiation ,Composite material ,0210 nano-technology ,Instrumentation - Abstract
Borosilicate glass has potential application for vitrification of high-level waste, which attracts extensive interest in studying their radiation durability. The NBS1 and NBS2 glasses were irradiated with 4 MeV Kr ions. The hardness and modulus of irradiated glasses were measured with a MTS G200 Nanoindenter device. With the increase of the irradiation, both the values of hardness and the modulus dropped and then saturated. The trend was consistent with previous studies, but the decay constants for the hardness of NBS1 and NBS2 were less than those in previous studies.
- Published
- 2017
14. Nanoscale imaging of alteration layers of corroded international simple glass particles using ToF-SIMS
- Author
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W. Yuan, James J. Neeway, Yanyan Zhang, Jiandong Zhang, Joseph V. Ryan, Tieshan Wang, and Zihua Zhu
- Subjects
010302 applied physics ,Nuclear and High Energy Physics ,SIMPLE (dark matter experiment) ,Materials science ,Mineralogy ,chemistry.chemical_element ,02 engineering and technology ,Lateral resolution ,021001 nanoscience & nanotechnology ,01 natural sciences ,Secondary ion mass spectrometry ,chemistry ,0103 physical sciences ,Glass corrosion ,Particle ,Composite material ,0210 nano-technology ,Instrumentation ,Nanoscopic scale ,Carbon - Abstract
Glass particles with dimensions typically ranging from tens to hundreds of microns are often used in glass corrosion research in order to accelerate testing. Two-dimensional and three-dimensional nanoscale imaging techniques are badly needed to characterize the alteration layers at the surfaces of these corroded glass particles. Time-of-flight secondary ion mass spectrometry (ToF-SIMS) can provide a lateral resolution as low as ∼100 nm, and, compared to other imaging techniques, is sensitive to elements lighter than carbon. In this work, we used ToF-SIMS to characterize the alteration layers of corroded international simple glass (ISG) particles. At most particle surfaces, inhomogeneous or no alteration layers were observed, indicating that the thickness of the alterations layers may be too thin to be observable by ToF-SIMS imaging. Relatively thick (e.g., 1–10 µm) alteration layers were inhomogeneously distributed at a small portion of surfaces. More interestingly, some large-size (tens of microns) glass particles were fully altered. Above observations suggest that weak attachment and the defects on ISG particle surfaces play an important role in ISG glass corrosion.
- Published
- 2017
15. Corrigendum to 'Measurement of the e+e− → π+π− cross section between 600 and 900 MeV using initial state radiation' [Phys. Lett. B 753 (2016) 629–638]
- Author
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M. Ablikim, M.N. Achasov, P. Adlarson, S. Ahmed, M. Albrecht, R. Aliberti, A. Amoroso, Q. An, X.H. Bai, Y. Bai, O. Bakina, R. Baldini Ferroli, I. Balossino, Y. Ban, K. Begzsuren, N. Berger, M. Bertani, D. Bettoni, F. Bianchi, J. Biernat, J. Bloms, A. Bortone, I. Boyko, R.A. Briere, H. Cai, X. Cai, A. Calcaterra, G.F. Cao, N. Cao, S.A. Cetin, J.F. Chang, W.L. Chang, G. Chelkov, D.Y. Chen, G. Chen, H.S. Chen, M.L. Chen, S.J. Chen, X.R. Chen, Y.B. Chen, Z.J. Chen, W.S. Cheng, G. Cibinetto, F. Cossio, X.F. Cui, H.L. Dai, X.C. Dai, A. Dbeyssi, R.E. de Boer, D. Dedovich, Z.Y. Deng, A. Denig, I. Denysenko, M. Destefanis, F. De Mori, Y. Ding, C. Dong, J. Dong, L.Y. Dong, M.Y. Dong, X. Dong, S.X. Du, J. Fang, S.S. Fang, Y. Fang, R. Farinelli, L. Fava, F. Feldbauer, G. Felici, C.Q. Feng, M. Fritsch, C.D. Fu, Y. Gao, Y.G. Gao, I. Garzia, E.M. Gersabeck, A. Gilman, K. Goetzen, L. Gong, W.X. Gong, W. Gradl, M. Greco, L.M. Gu, M.H. Gu, S. Gu, Y.T. Gu, C.Y. Guan, A.Q. Guo, L.B. Guo, R.P. Guo, Y.P. Guo, A. Guskov, T.T. Han, X.Q. Hao, F.A. Harris, K.L. He, F.H. Heinsius, C.H. Heinz, T. Held, Y.K. Heng, C. Herold, M. Himmelreich, T. Holtmann, Y.R. Hou, Z.L. Hou, H.M. Hu, J.F. Hu, T. Hu, Y. Hu, G.S. Huang, L.Q. Huang, X.T. Huang, Y.P. Huang, Z. Huang, N. Huesken, T. Hussain, W. Ikegami Andersson, W. Imoehl, M. Irshad, S. Jaeger, S. Janchiv, Q. Ji, Q.P. Ji, X.B. Ji, X.L. Ji, H.B. Jiang, X.S. Jiang, J.B. Jiao, Z. Jiao, S. Jin, Y. Jin, T. Johansson, N. Kalantar-Nayestanaki, X.S. Kang, R. Kappert, M. Kavatsyuk, B.C. Ke, I.K. Keshk, A. Khoukaz, P. Kiese, R. Kiuchi, R. Kliemt, L. Koch, O.B. Kolcu, B. Kopf, M. Kuemmel, M. Kuessner, A. Kupsc, M.G. Kurth, W. Kühn, J.J. Lane, J.S. Lange, P. Larin, A. Lavania, L. Lavezzi, Z.H. Lei, H. Leithoff, M. Lellmann, T. Lenz, C. Li, C.H. Li, Cheng Li, D.M. Li, F. Li, G. Li, H. Li, H.B. Li, H.J. Li, J.L. Li, J.Q. Li, Ke Li, L.K. Li, Lei Li, P.L. Li, P.R. Li, S.Y. Li, W.D. Li, W.G. Li, X.H. Li, X.L. Li, Z.Y. Li, H. Liang, Y.F. Liang, Y.T. Liang, G.R. Liao, L.Z. Liao, J. Libby, C.X. Lin, B.J. Liu, C.X. Liu, D. Liu, F.H. Liu, Fang Liu, Feng Liu, H.B. Liu, H.M. Liu, Huanhuan Liu, Huihui Liu, J.B. Liu, J.Y. Liu, K. Liu, K.Y. Liu, Ke Liu, L. Liu, M.H. Liu, Q. Liu, S.B. Liu, Shuai Liu, T. Liu, W.M. Liu, X. Liu, Y.B. Liu, Z.A. Liu, Z.Q. Liu, X.C. Lou, F.X. Lu, H.J. Lu, J.D. Lu, J.G. Lu, X.L. Lu, Y. Lu, Y.P. Lu, C.L. Luo, M.X. Luo, P.W. Luo, T. Luo, X.L. Luo, S. Lusso, X.R. Lyu, F.C. Ma, H.L. Ma, L.L. Ma, M.M. Ma, Q.M. Ma, R.Q. Ma, R.T. Ma, X.X. Ma, X.Y. Ma, F.E. Maas, M. Maggiora, S. Maldaner, S. Malde, Q.A. Malik, A. Mangoni, Y.J. Mao, Z.P. Mao, S. Marcello, Z.X. Meng, J.G. Messchendorp, G. Mezzadri, T.J. Min, R.E. Mitchell, X.H. Mo, Y.J. Mo, N.Yu. Muchnoi, H. Muramatsu, S. Nakhoul, Y. Nefedov, F. Nerling, I.B. Nikolaev, Z. Ning, S. Nisar, S.L. Olsen, Q. Ouyang, S. Pacetti, X. Pan, Y. Pan, A. Pathak, P. Patteri, M. Pelizaeus, H.P. Peng, K. Peters, J. Pettersson, J.L. Ping, R.G. Ping, A. Pitka, R. Poling, V. Prasad, H. Qi, H.R. Qi, K.H. Qi, M. Qi, T.Y. Qi, S. Qian, W.-B. Qian, Z. Qian, C.F. Qiao, L.Q. Qin, X.S. Qin, Z.H. Qin, J.F. Qiu, S.Q. Qu, K. Ravindran, C.F. Redmer, A. Rivetti, V. Rodin, M. Rolo, G. Rong, Ch. Rosner, M. Rump, H.S. Sang, A. Sarantsev, Y. Schelhaas, C. Schnier, K. Schoenning, M. Scodeggio, D.C. Shan, W. Shan, X.Y. Shan, M. Shao, C.P. Shen, P.X. Shen, X.Y. Shen, H.C. Shi, R.S. Shi, X. Shi, X.D. Shi, J.J. Song, W.M. Song, Y.X. Song, S. Sosio, S. Spataro, K.X. Su, F.F. Sui, G.X. Sun, H.K. Sun, J.F. Sun, L. Sun, S.S. Sun, T. Sun, W.Y. Sun, X. Sun, Y.J. Sun, Y.K. Sun, Y.Z. Sun, Z.T. Sun, Y.H. Tan, Y.X. Tan, C.J. Tang, G.Y. Tang, J. Tang, J.X. Teng, V. Thoren, I. Uman, B. Wang, C.W. Wang, D.Y. Wang, H.P. Wang, K. Wang, L.L. Wang, M. Wang, M.Z. Wang, Meng Wang, W.H. Wang, W.P. Wang, X. Wang, X.F. Wang, X.L. Wang, Y. Wang, Y.D. Wang, Y.F. Wang, Y.Q. Wang, Z. Wang, Z.Y. Wang, Ziyi Wang, Zongyuan Wang, D.H. Wei, P. Weidenkaff, F. Weidner, S.P. Wen, D.J. White, U. Wiedner, G. Wilkinson, M. Wolke, L. Wollenberg, J.F. Wu, L.H. Wu, L.J. Wu, X. Wu, Z. Wu, L. Xia, H. Xiao, S.Y. Xiao, Z.J. Xiao, X.H. Xie, Y.G. Xie, Y.H. Xie, T.Y. Xing, G.F. Xu, J.J. Xu, Q.J. Xu, W. Xu, X.P. Xu, Y.C. Xu, F. Yan, L. Yan, W.B. Yan, W.C. Yan, Xu Yan, H.J. Yang, H.X. Yang, L. Yang, S.L. Yang, Y.H. Yang, Y.X. Yang, Yifan Yang, Zhi Yang, M. Ye, M.H. Ye, J.H. Yin, Z.Y. You, B.X. Yu, C.X. Yu, G. Yu, J.S. Yu, T. Yu, C.Z. Yuan, L. Yuan, W. Yuan, X.Q. Yuan, Y. Yuan, Z.Y. Yuan, C.X. Yue, A. Yuncu, A.A. Zafar, Y. Zeng, B.X. Zhang, Guangyi Zhang, H. Zhang, H.H. Zhang, H.Y. Zhang, J.J. Zhang, J.L. Zhang, J.Q. Zhang, J.W. Zhang, J.Y. Zhang, J.Z. Zhang, Jianyu Zhang, Jiawei Zhang, Lei Zhang, S. Zhang, S.F. Zhang, Shulei Zhang, X.D. Zhang, X.Y. Zhang, Y. Zhang, Y.H. Zhang, Y.T. Zhang, Yan Zhang, Yao Zhang, Yi Zhang, Z.H. Zhang, Z.Y. Zhang, G. Zhao, J. Zhao, J.Y. Zhao, J.Z. Zhao, Lei Zhao, Ling Zhao, M.G. Zhao, Q. Zhao, S.J. Zhao, Y.B. Zhao, Y.X. Zhao, Z.G. Zhao, A. Zhemchugov, B. Zheng, J.P. Zheng, Y. Zheng, Y.H. Zheng, B. Zhong, C. Zhong, L.P. Zhou, Q. Zhou, X. Zhou, X.K. Zhou, X.R. Zhou, A.N. Zhu, J. Zhu, K. Zhu, K.J. Zhu, S.H. Zhu, T.J. Zhu, W.J. Zhu, Y.C. Zhu, Z.A. Zhu, B.S. Zou, and J.H. Zou
- Subjects
Nuclear and High Energy Physics ,010308 nuclear & particles physics ,Covariance matrix ,BESIII ,Hadronic cross section ,01 natural sciences ,Pion form factor ,lcsh:QC1-999 ,NO ,0103 physical sciences ,Initial state radiation ,010306 general physics ,Muon anomaly ,lcsh:Physics - Abstract
In Ref. [1] the BESIII collaboration published a cross section measurement of the process e+e−→π+π− in the energy range between 600 and 900 MeV. In this corrigendum, we report a corrected evaluation of the statistical errors in terms of a fully propagated covariance matrix. The correction also yields a reduced statistical uncertainty for the hadronic vacuum polarization contribution to the anomalous magnetic moment of the muon, which now reads as aμππ,LO(600−900MeV)=(368.2±1.5stat±3.3syst)×10−10. The central values of the cross section measurement and of aμππ,LO, as well as the systematic uncertainties remain unchanged.
- Published
- 2021
16. Morphological study of borosilicate glass surface irradiated by heavy ions
- Author
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Dexing Yang, Tieshan Wang, W. Yuan, H.B. Peng, X. Du, Junqiu Zhang, G.F. Zhang, Zihua Zhu, Lei Chen, and B.H. Duan
- Subjects
Materials science ,genetic structures ,Analytical chemistry ,02 engineering and technology ,Radiation ,01 natural sciences ,Ion ,law.invention ,Optical microscope ,law ,0103 physical sciences ,Materials Chemistry ,Irradiation ,010302 applied physics ,Borosilicate glass ,Surfaces and Interfaces ,General Chemistry ,021001 nanoscience & nanotechnology ,Condensed Matter Physics ,Radiation effect ,Surfaces, Coatings and Films ,Secondary ion mass spectrometry ,Transmission electron microscopy ,sense organs ,0210 nano-technology ,human activities - Abstract
Borosilicate glass is a candidate material for radiation waste formation and other optical applications in various fields. To understand the radiation effect of borosilicate glass, heavy ion (Ar q + , Kr q + and Xe q + ) irradiations were used to simulate the alpha and recoiled nuclei irradiations in this study. The surface morphology of glass has been compared to ion irradiation doses and ion energies. The surface topography evolution of irradiated samples is characterized by optical microscopy, atomic force microscopy (AFM), transmission electron microscopy (TEM) and secondary ion mass spectrometry (SIMS). Micro-bumps are observed on the sample surface after irradiation with 5 MeV Xe q + over 5 × 10 13 ions·cm − 2 . The size and density of the bumps increases with increasing irradiation dose. At a low dose, bumps are on the nanometer (nm) scale and rather rare. While the dose is higher than 9 × 10 15 ions·cm − 2 , the size of bumps is on the scale of a few microns, and the density is saturated. However, the height of the bumps increases from a few nm to over 150 nm with further irradiation. The distribution of micro-bumps is nearly homogeneous. The bumps are condensed and swell up, and there is no crystallized structure according to the TEM diffraction pattern. Element migration and concentrations are observed with SIMS imaging. The arrayed micro-bumps are a new finding, and they might be used to change the surface properties. Bump formation is caused by phase separation, and volume swelling is induced by ion irradiation.
- Published
- 2016
17. Evolutions of molecular oxygen formation and sodium migration in Xe ion irradiated borosilicate glasses
- Author
-
Peng Lv, Xing Du, Liang Chen, Jiandong Zhang, Shuai Nan, Tieshan Wang, Duofei F. Zhang, Zihua Zhu, and W. Yuan
- Subjects
Materials science ,Sodium ,Population ,Analytical chemistry ,chemistry.chemical_element ,02 engineering and technology ,01 natural sciences ,Fluence ,Ion ,symbols.namesake ,0103 physical sciences ,Materials Chemistry ,Irradiation ,education ,Penetration depth ,010302 applied physics ,education.field_of_study ,Borosilicate glass ,Radiochemistry ,021001 nanoscience & nanotechnology ,Condensed Matter Physics ,Electronic, Optical and Magnetic Materials ,chemistry ,Ceramics and Composites ,symbols ,0210 nano-technology ,Raman spectroscopy - Abstract
The modifications of a commercial borosilicate glass induced by Xe ion irradiation have been studied by Raman spectroscopy and ToF-SIMS depth profiling. A decrease in the average Si–O–Si angle, an increase in the population of three-membered rings and an increase of the glass polymerization are evidenced. The molecular oxygen appears in the irradiated glasses after the irradiation fluence reaches approximately 10 15 ions/cm 2 . The O 2 concentration decreases with the depth of irradiated glass at the ion fluence of 2 × 10 16 ions/cm 2 . A sodium depleted layer at the surface and a depleted zone at around the penetration depth of 5 MeV Xe ions are observed. The thickness of the sodium depleted layer increases with the irradiation fluence. Moreover, comparing with previous results after electron and Ar ion irradiation, it can be concluded that the nuclear energy deposition can partially inhibit the formation of molecular oxygen and increase the threshold value of electron energy deposition for the molecular oxygen formation.
- Published
- 2016
18. Effect of irradiation on hardness of borosilicate glass
- Author
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H.B. Peng, M.L. Sun, K.J. Yang, H. S. Chen, Tianhe Wang, B.H. Duan, Liang Chen, W. Yuan, and D. Yang
- Subjects
010302 applied physics ,Materials science ,Borosilicate glass ,Analytical chemistry ,02 engineering and technology ,Nanoindentation ,021001 nanoscience & nanotechnology ,Condensed Matter Physics ,01 natural sciences ,Radiation effect ,Electronic, Optical and Magnetic Materials ,Ion ,0103 physical sciences ,Atom ,Materials Chemistry ,Ceramics and Composites ,Irradiation ,0210 nano-technology ,Nuclear chemistry - Abstract
Borosilicate glass samples were irradiated by Xe and Kr ions with different fluences. The nanoindentation hardness of samples was measured. For samples irradiated by Xe and Kr ions, the hardness variation dropped with the irradiation dose in displacement per atom. The experimental results are consistent with those of other studies. A rough model was proposed to explain the results of this study and those of others.
- Published
- 2016
19. Study of modifications in the mechanical properties of sodium aluminoborosilicate glass induced by heavy ions and electrons
- Author
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Tieshan Wang, S. Nan, Duofei Zhang, Xin Du, Peng Lv, Liang Chen, W. Yuan, and H.B. Peng
- Subjects
010302 applied physics ,Nuclear and High Energy Physics ,Materials science ,Radiochemistry ,Analytical chemistry ,Young's modulus ,02 engineering and technology ,021001 nanoscience & nanotechnology ,Alkali metal ,01 natural sciences ,Electron spectroscopy ,law.invention ,Ion ,symbols.namesake ,law ,0103 physical sciences ,symbols ,Electron beam processing ,Irradiation ,0210 nano-technology ,Raman spectroscopy ,Electron paramagnetic resonance ,Instrumentation - Abstract
Radiation effects on the mechanical properties of sodium aluminoborosilicate glass induced by 4 MeV Kr, 5 MeV Xe ions and 1.2 MeV electrons have been investigated by nano-indentation measurements. Raman and electron paramagnetic resonance (EPR) spectroscopies were used to characterize the microstructure evolution of electron irradiated samples. The nano-indentation results indicated that the mean hardness was reduced by 12.8%, and the mean reduced Young modulus was increased by 3.5% after heavy ion irradiation. Both the hardness and reduced Young modulus variations reached stabilization when the nuclear deposited energy was around 3 x 10(21) keV(nucl)/cm(3). Although decreases of hardness (about 6.6%) and reduced Young modulus (about 3.1%) were also observed when the deposited electronic energy reached approximately 1.5 x 10(22) keV(elec)/cm(3) after electron irradiation, the results still emphasized that the nuclear energy deposition is the major factor for the evolution in the hardness and modulus of the sodium aluminoborosilicate glass under ion irradiation, rather than a synergy process of the electronic and nuclear energy depositions. (C) 2016 Elsevier B.V. All rights reserved.
- Published
- 2016
20. Radiation-induced Vaginal Injury After Treatment for Cervical Cancer
- Author
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Lunxu Liu, K.S. Zhang, Fan Shi, Jin Su, J. Wang, L. Wei, W. Yuan, R.H. Wang, Yongyan Wang, Tao Wang, B.G. Liu, Zhihua Liu, L. Dai, W. Xue, C. Gao, Yexiong Li, Jun Ma, and H. Yuan
- Subjects
Cervical cancer ,Cancer Research ,medicine.medical_specialty ,Radiation ,business.industry ,Vaginal injury ,Urology ,Radiation induced ,medicine.disease ,Oncology ,medicine ,Radiology, Nuclear Medicine and imaging ,business ,After treatment - Published
- 2020
21. Baseline Score Of Coronary Artery Calcification Is An Optimal Factor To Predict Cac Progression
- Author
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W. Yuan, Mathew Budoff, D. Zhao, Dong Li, S. Mao, and Y. Gao
- Subjects
medicine.medical_specialty ,business.industry ,Internal medicine ,Coronary artery calcification ,medicine ,Cardiology ,Radiology, Nuclear Medicine and imaging ,Cardiology and Cardiovascular Medicine ,Baseline (configuration management) ,business - Published
- 2020
22. Loss of the Epigenetic Mark 5-hmC in Psoriasis: Implications for Epidermal Stem Cell Dysregulation
- Author
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Catherine A. Lee, Matthew R. Ramsey, Shuyun Xu, Xunwei Wu, Anna Mandinova, Christine W. Yuan, Yvon Woappi, Tingjian Zu, Markus H. Frank, Michael J. Wells, Feng Li, George F. Murphy, Natasha Y. Frank, Christine G. Lian, and Phammela Abarzua
- Subjects
Epigenomics ,Keratinocytes ,0301 basic medicine ,Primary Cell Culture ,Down-Regulation ,Dermatology ,Biology ,Biochemistry ,Article ,Dioxygenases ,Epigenesis, Genetic ,Mixed Function Oxygenases ,Mice ,03 medical and health sciences ,chemistry.chemical_compound ,0302 clinical medicine ,Proto-Oncogene Proteins ,medicine ,Animals ,Humans ,Psoriasis ,Epigenetics ,Molecular Biology ,Tissue homeostasis ,5-Hydroxymethylcytosine ,Stem Cells ,Wnt signaling pathway ,Sequence Analysis, DNA ,Cell Biology ,DNA Methylation ,Nestin ,Ascorbic acid ,Cell biology ,DNA-Binding Proteins ,Histone Code ,Disease Models, Animal ,030104 developmental biology ,medicine.anatomical_structure ,chemistry ,030220 oncology & carcinogenesis ,5-Methylcytosine ,Female ,Stem cell ,Keratinocyte - Abstract
Epigenetic regulation has a profound influence on stem cell fate during normal development in maintenance of physiologic tissue homeostasis. Here we report diminished ten-eleven translocation (TET) methylcytosine dioxygenase expression and loss of the DNA hydroxymethylation mark 5-hydroxymethylcytosine (5-hmC) in keratinocyte stem cells and transit amplifying cells in human psoriasis and in imiquimod-induced murine psoriasis. Loss of 5-hmC was associated with dysregulated keratinocyte stem cell kinetics, resulting in accumulation of nestin and FABP5-expressing transit amplifying cells to produce classic psoriatic epidermal architecture. Moreover, 5-hmC loss was accompanied by diminished TET1 and TET2 mRNA expression. Genome-wide mapping of epidermal 5-hmC in murine psoriasis revealed loci-specific loss of 5-hmC in genes regulating stem cell homeostasis, including MBD1, RTN1, STRN4, PRKD2, AKT1, and MAPKAP2, as well as those associated with RAR and Wnt/β-catenin signaling pathways. In vitro restoration of TET expression by ascorbic acid was accomplished in cultured human keratinocyte stem cells to show similar Ca++-induced differentiation, resulting in increased 5-hmC levels and reduced nestin expression. To our knowledge, an epigenetic deficiency in psoriasis with relevance to stem cell dysregulation has not been previously reported. This observation raises the possibility that epigenetic modifiers that impact on the TET–5-hmC pathway may be a relevant approach of heretofore unappreciated therapeutic utility.
- Published
- 2020
23. REM sleep behavior disorder causes symptom fluctuations in parkinson's disease
- Author
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Y.-L. Liu, Jing Li, W. Yuan, Chun-Feng Liu, Yun Shen, and Kang-Ping Xiong
- Subjects
medicine.medical_specialty ,Parkinson's disease ,business.industry ,medicine ,General Medicine ,medicine.disease ,Psychiatry ,business ,REM sleep behavior disorder - Published
- 2019
24. Surface modification of Li(Li0.17Ni0.2Co0.05Mn0.58)O2 with CeO2 as cathode material for Li-ion batteries
- Author
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Guobang Li, W. Yuan, Qian Liu, Huan Zhang, and Xu-Zhen Gao
- Subjects
Materials science ,General Chemical Engineering ,Inorganic chemistry ,Oxide ,chemistry.chemical_element ,Nanoparticle ,Cathode ,law.invention ,chemistry.chemical_compound ,chemistry ,law ,Electrochemistry ,Surface modification ,Lithium ,Thermal stability ,Surface charge ,Faraday efficiency - Abstract
Li-rich layered oxides are of great importance as cathode materials for advanced lithium ion batteries. In this work, Li-rich layered Li(Li 0.17 Ni 0.2 Co 0.05 Mn 0.58 )O 2 oxide is synthesized by a spray-drying method, and modified subsequently with CeO 2 nanoparticles. It is demonstrated that the surface of the Li(Li 0.17 Ni 0.2 Co 0.05 Mn 0.58 )O 2 oxide is modified with CeO 2 nanocrystallites, which exist as isolated nano-particles or a thick CeO 2 layer with increasing CeO 2 content. After the surface modification with CeO 2 nanoparticles, Li(Li 0.17 Ni 0.2 Co 0.05 Mn 0.58 )O 2 oxide presents lower surface charge transfer resistance, larger discharge capacity and higher initial coulombic efficiency. In particular, the modified sample with 1 wt % CeO 2 shows the optimized cycle stability and high-rate discharge capability. In addition, the thermal stability of the cathode at delithiated state is improved to a certain extent by the surface modification with CeO 2 nanoparticles, which is attributed to that the oxygen generated from the initial charge can be absorbed and stored in CeO 2 nanoparticles on the surface of Li(Li 0.17 Ni 0.2 Co 0.05 Mn 0.58 )O 2 .
- Published
- 2014
25. LEFT VENTRICULAR STRAIN BY CARDIAC MRI IN END-STAGE RENAL DISEASE PATIENTS AFTER KIDNEY TRANSPLANTATION
- Author
-
I. Gong, B. Al-Amro, G. Prasad, P. Connelly, D. Deva, H. Leong-Poi, M. Nash, W. Yuan, L. Gunaratnam, R. Wald, S. Kim, C. Lok, K. Connelly, and A. Yan
- Subjects
medicine.medical_specialty ,business.industry ,Internal medicine ,medicine ,Cardiology ,Cardiology and Cardiovascular Medicine ,business ,medicine.disease ,Left ventricular strain ,Kidney transplantation ,End stage renal disease - Published
- 2018
26. OR68: Effects of a Micronutrient Pack on Micronutrient Status, Homocysteine Level, Oxidative Stress Biomarkers and Functions in Institutional Older Adults: A Multicenter Randomized, Double-Blind, Placebo-Controlled Study
- Author
-
Yundai Chen, Ying Lu, N. Lin, H. Xie, J. Sun, H. Jin, C. Wu, W. Yuan, Y. Yang, X. Li, Q. Ren, and H. Li
- Subjects
medicine.medical_specialty ,Nutrition and Dietetics ,Homocysteine ,business.industry ,Placebo-controlled study ,Critical Care and Intensive Care Medicine ,Micronutrient ,medicine.disease_cause ,Double blind ,chemistry.chemical_compound ,chemistry ,Internal medicine ,Medicine ,business ,Oxidative stress - Published
- 2019
27. Raman spectra and nano-indentation of Ar-irradiated borosilicate glass
- Author
-
K.J. Yang, F. Tian, Liang Chen, Lei Zhang, W. Yuan, H.B. Peng, Tieshan Wang, and G.F. Zhang
- Subjects
Nuclear and High Energy Physics ,Materials science ,Borosilicate glass ,Analytical chemistry ,Mineralogy ,Nanoindentation ,symbols.namesake ,Molecular geometry ,Polymerization ,symbols ,Molecule ,Irradiation ,Raman spectroscopy ,Instrumentation - Abstract
The structural evolutions of a commercial borosilicate glass induced by 2 MeV Ar irradiation have been studied by Raman spectroscopy, and the modification of the mechanical properties has been investigated with nano-indentation tests. The main peaks at approximately 480 cm−1 in the Raman spectra were found to be shifted toward higher wave numbers after irradiation, which means a decrease of the Si–O–Si bond angle. A weak band, which is called a D2 “defect” peak, appears in the Raman spectra of irradiated glasses. A higher concentration of O2 molecules is found in the irradiated glasses; however, the polymerization of the irradiated glass network has not been changed compared with the pristine glass. The mean hardness of the glasses is decreased up to 17% after irradiation, and the variation of the hardness saturates after the deposited nuclear energy reaches approximately 5.5 × 1020 keVnucl cm−3.
- Published
- 2013
28. Study of irradiation damage in borosilicate glass induced by He ions and electrons
- Author
-
Lei Zhang, C.X. Li, Kehu Yang, H.B. Peng, W. Yuan, Tieshan Wang, Guixu Zhang, F. Tian, and Liang Chen
- Subjects
Nuclear and High Energy Physics ,Materials science ,Borosilicate glass ,Analytical chemistry ,Silicate ,Ion ,chemistry.chemical_compound ,symbols.namesake ,chemistry ,Polymerization ,symbols ,Radiation damage ,Irradiation ,Raman spectroscopy ,Instrumentation ,Deposition (chemistry) ,Nuclear chemistry - Abstract
Radiation effects on borosilicate glass induced by 0.5 MeV He ions and 1.2 MeV electrons have been investigated by nano-indentation and Raman measurements. The nano-indentation results indicated that the average hardness of the He-irradiated glasses were reduced by 14% with the nuclear energy deposition, and kept constant after the nuclear energy deposition exceeding 5 × 1020 keV/cm3. By the Raman measurements, the polymerization of the silicate network was found to be enhanced by the electronic energy deposition in the electron-irradiated glasses. It is concluded that the nuclear energy deposition is the major factor for the evolution in the plastic response of the borosilicate glass, while the electronic energy deposition influences the change of silicate network and migration of alkaline, which causes sight change of the mechanical properties.
- Published
- 2013
29. Formation of monolayer graphene on a basal HOPG surface irradiated with Xe ions
- Author
-
W. Yuan, K.J. Yang, Tianhe Wang, Xia Lu, Qiang Wang, H.B. Peng, Rui Cheng, and Yongtao Zhao
- Subjects
Nuclear and High Energy Physics ,Materials science ,Graphene ,Highly charged ion ,Analytical chemistry ,Ion source ,Electron cyclotron resonance ,law.invention ,Ion ,symbols.namesake ,Highly oriented pyrolytic graphite ,law ,symbols ,Irradiation ,Raman spectroscopy ,Instrumentation - Abstract
Highly charged Xe q + ( q = 5, 21, 26) ions with kinetic energy of 450 keV were extracted from electron cyclotron resonance ion source. Highly oriented pyrolytic graphite (HOPG) basal surfaces were impacted by the Xe q + ions. The samples were analyzed with Raman spectroscopy. There appeared a tiny peak in Raman spectrum at position of 2643 cm −1 for the impact of Xe 5+ ion, which suggested the monolayer graphene was formed on the HOPG surface. The intensity of the peak depended on the charge state of incident ions.
- Published
- 2013
30. Exosomal miRNAs derived from umbilical mesenchymal stem cells inhibit hepatitis C virus infection
- Author
-
H. Liu, X. Qian, P. Zhao, C. Xu, Yan Wang, W. Yuan, Z. Qi, and S. Fang
- Subjects
Hepatitis ,Hepatology ,business.industry ,Hepatitis C virus ,microRNA ,Mesenchymal stem cell ,Medicine ,Exosomal mirnas ,business ,medicine.disease ,medicine.disease_cause ,Virology ,Virus - Published
- 2017
31. Long-Term Outcome of Sensorineural and Conductive Hearing Loss Following Intensity Modulated Radiation Therapy in Nasopharyngeal Carcinoma
- Author
-
G. Yang, Y. Zhu, Jiyao Li, S.Z. Wang, Wei Wang, Y. Gong, X. Huang, L. Zou, H. Ding, W. Zhu, Hui Zhang, and W. Yuan
- Subjects
Cancer Research ,medicine.medical_specialty ,Radiation ,business.industry ,Intensity-modulated radiation therapy ,medicine.disease ,Conductive hearing loss ,Term (time) ,Oncology ,Nasopharyngeal carcinoma ,medicine ,Radiology, Nuclear Medicine and imaging ,Radiology ,business - Published
- 2018
32. Aerodynamics of laminar separation flutter at a transitional Reynolds number
- Author
-
Dominique Poirel and W. Yuan
- Subjects
Airfoil ,Mechanical Engineering ,Reynolds number ,Laminar flow ,Mechanics ,NACA airfoil ,Physics::Fluid Dynamics ,symbols.namesake ,Flow separation ,Classical mechanics ,symbols ,Flutter ,Pitching moment ,Aerodynamic center ,Mathematics - Abstract
Experimental observations of self-sustained pitch oscillations of a NACA 0012 airfoil at transitional Reynolds numbers were recently reported. The aeroelastic limit cycle oscillations, herein labelled as laminar separation flutter, occur in the range 5.0×104≤Rec≤1.3×105. They are well behaved, have a small amplitude and oscillate about θ=0°. It has been speculated that laminar separation leading to the formation of a laminar separation bubble, occurring at these Reynolds numbers, plays an essential role in these oscillations. This paper focuses on the Rec=7.7×104 case, with the elastic axis located at 18.6% chord. Considering that the experimental rig acts as a dynamic balance, the aerodynamic moment is derived and is empirically modelled as a generalized Duffing–van-der-Pol nonlinearity. As expected, it behaves nonlinearly with pitch displacement and rate. It also indicates a dynamically unstable equilibrium point, i.e. negative aerodynamic damping. In addition, large eddy simulations of the flow around the airfoil undergoing prescribed simple harmonic motion, using the same amplitude and frequency as the aeroelastic oscillations, are performed. The comparison between the experiment and simulations is conclusive. Both approaches show that the work done by the airflow on the airfoil is positive and both have the same magnitude. The large eddy simulation (LES) computations indicate that at θ=0°, the pitching motion induces a lag in the separation point on both surfaces of the airfoil resulting in negative pitching moment when pitching down, and positive moment when pitching up, thus feeding the LCO.
- Published
- 2010
33. Decreased ratio of Tregs to Th17 cells exacerbates disease progression of autoimmune hepatitis
- Author
-
W. Yuan, Qin Ning, Yinkun Liu, D. Huang, Peng Wang, and W. Yan
- Subjects
Hepatology ,business.industry ,Disease progression ,Immunology ,Medicine ,Autoimmune hepatitis ,business ,medicine.disease - Published
- 2018
34. Morphological and cytological studies of diploid and colchicine-induced tetraploid lines of crape myrtle (Lagerstroemia indica L.)
- Author
-
Yao-Mei Ye, Xianfeng Shi, J. Tong, G.R. Li, and W. Yuan
- Subjects
Epidermis (botany) ,biology ,fungi ,food and beverages ,Horticulture ,Lagerstroemia indica ,biology.organism_classification ,medicine.disease_cause ,Plant morphology ,Pollen ,Ornamental plant ,Botany ,medicine ,Cultivar ,Ploidy ,Lythraceae - Abstract
The tips of cotyledon-stage seedlings of three crape myrtle cultivars (“Zi Wei”, “Hong Wei” and “Yin Wei”) were treated with colchicine. Various concentrations of colchicine and different treatment durations were tested. Seedlings of “Zi Wei” treated with 0.5% colchicine for 72 h and seedlings of “Yin Wei” treated with colchicine (0.2% for 96 h, 0.5% for 48 h and 0.8% for 72 h) demonstrated high rates of mutation; “Hong Wei” showed a slightly lower rate. The highest rate of morphological variation was 54.17% and this was achieved when tips were treated with 0.5% colchicine for 72 h. Putative tetraploid plants were identified with morphological and cytological variations, such as larger and thicker leaves, darker green coloration, larger stomata, lower density of stomata across the lower leaf epidermis and increased numbers of chloroplasts per stomata guard cell. Flow cytometric analysis demonstrated that the nuclear DNA content of 15 of these putative tetraploids (of which 7 were “Zi Wei”, 5 were “Yin Wei”, and 3 were “Hong Wei”) was indeed doubled relative to that of control diploid plants. The chromosome number of the tetraploid plants was 2 n = 4 x = 96, while that of the control diploid plants was 2 n = 2 x = 48. Ornamental characteristics were also enhanced in the tetraploid plants, with increased diameter of the individual flowers and greater basal length of the petals and claws. Pollen diameter and the size of capsules and seeds were also significantly greater than those of diploid plants.
- Published
- 2010
35. Rap1b is critical for glycoprotein VI-mediated but not ADP receptor-mediated α2β1 activation
- Author
-
W. Yuan, Mark K. Larson, Zhengyan Wang, J. Liu, Stephen P. Holly, Gilbert C. White, Leslie V. Parise, and M. Chrzanowska-Wodnicka
- Subjects
Blood Platelets ,Mice, Knockout ,Receptors, Purinergic P2 ,Integrin ,Platelet Membrane Glycoproteins ,Hematology ,Biology ,Platelet membrane glycoprotein ,Article ,Collagen receptor ,Cell biology ,Mice ,Platelet Adhesiveness ,rap GTP-Binding Proteins ,Platelet adhesiveness ,biology.protein ,Animals ,Platelet ,Collagen ,Platelet activation ,Integrin alpha2beta1 ,Signal transduction ,GPVI ,Cell Shape ,Signal Transduction - Abstract
The platelet alpha2beta1 integrin functions as both an adhesion and signaling receptor upon exposure to collagen. Recent studies have indicated that alpha2beta1 function can be activated via inside-out signaling, similar to the prototypical platelet integrin alphaIIbbeta3. However, signaling molecules that regulate alpha2beta1 activation in platelets are not well defined. A strong candidate molecule is the small GTPase Rap1b, the dominant platelet isoform of Rap1, which regulates alphaIIbbeta3 activation.We hypothesized that Rap1b positively regulates alpha2beta1 during agonist-induced platelet activation.To test whether Rap1b activates alpha2beta1 downstream of glycoprotein (GP)VI or other platelet receptors, we stimulated platelets purified from Rap1b-/- or wild-type mice with diverse agonists and measured alpha2beta1 activation using fluorescein isothiocyanate-labeled monomeric collagen. We also examined the role of Rap1b in outside-in signaling pathways by analyzing adhesion and spreading of Rap1b-/- or wild-type platelets on monomeric, immobilized collagen. Finally, we monitored the activation status of related Rap GTPases to detect changes in signaling pathways potentially associated with Rap1b-mediated events.Rap1b-/- platelets displayed comparable ADP-induced or thrombin-induced alpha2beta1 activation as wild-type platelets, but reduced convulxin-dependent alpha2beta1 activation. Rap1b-/- platelets exhibited increased spreading on immobilized collagen but similar adhesion to immobilized collagen compared to wild-type platelets. Rap1b-/- platelets also showed Rap1a and Rap2 activation upon agonist stimulation, possibly revealing functional compensation among Rap family members.Rap1b is required for maximal GPVI-induced but not ADP-induced activation of alpha2beta1 in murine platelets.
- Published
- 2009
36. A liquid–gas phase mixed-reactant fuel cell with a RuSeW cathode electrocatalyst
- Author
-
W. Yuan, H. Cheng, and Keith Scott
- Subjects
Renewable Energy, Sustainability and the Environment ,Formic acid ,Inorganic chemistry ,Energy Engineering and Power Technology ,Direct-ethanol fuel cell ,Electrocatalyst ,Cathode ,law.invention ,Catalysis ,chemistry.chemical_compound ,chemistry ,law ,Methanol ,Electrical and Electronic Engineering ,Physical and Theoretical Chemistry ,Hydrogen peroxide ,Power density - Abstract
Some data in mixed-reactant fuel cells (MRFC) at Newcastle using formic acid, methanol and ethanol are reported. The importance of using a fuel-tolerant selective cathode catalyst has been identified. The influence of fuel and oxidant conditions and feeding patterns has been evaluated. The cell performance using air, oxygen and hydrogen peroxide is reported. The highest peak power density of 16 mW cm −2 was obtained with formic acid. The MRFC gave power densities approximately half those of a conventional, un-mixed-reactant fuel cell.
- Published
- 2008
37. The effect of restored microbiotic crusts on erosion of soil from a desert area in China
- Author
-
W. Yuan, L. Han, Zhuo Dong, Ze Zhang, and Anzhou Zhao
- Subjects
Hydrology ,Ecology ,Crust ,Wind speed ,Chine ,Wind profile power law ,Saltation (geology) ,Soil water ,Aeolian processes ,Geomorphology ,Ecology, Evolution, Behavior and Systematics ,Geology ,Earth-Surface Processes ,Wind tunnel - Abstract
Samples of microbiotic crusts were collected along the northern part of the Zhongwei–Gantang section of the Baotou-Lanzhou railway, which lies at the southeastern fringe of China's Tengger Desert. We collected intact crust samples, let them recover for 1 year, then created five levels of disturbance: no disturbance (intact crusts), light disturbance (disturbance of 10% and 20% of the total area), moderate disturbance (40% disturbance), and severe disturbance (80% disturbance). We used these samples to simulate the effect of microbiotic crusts on wind erosion. Wind tunnel experiments let us determine the wind velocity required for the initiation of saltation, the threshold velocity (u*), the aerodynamic roughness length (z0), and the wind profile above sand surfaces covered by microbiotic crusts. The wind velocity for the initiation of saltation with an intact microbiotic crust was about 19 m s−1, which is greater than the value of 13.08 m s−1 for shifting sands. z0 was between 0.03 and 0.13 cm, which was larger than the value of 0.0288 for shifting sands, and reached its maximum (0.13 cm) at the 40% disturbance level, and u* was between 0.15 and 1.21 m s−1. The relationships between u*, free-stream wind velocity (u), and z0 followed the equations u*=a+bu and z0=0.01563(1+u*)3.49341. The wind profile above the surface was divided into three sections, with the greatest changes in wind speed occurring below a height of 0.1 m.
- Published
- 2008
38. A study of the effect of nanostructured surface layers on the fatigue behaviors of a C-2000 superalloy
- Author
-
Juan C. Villegas, Peter K. Liaw, D.E. Fielden, J.W. Tian, Dwaine L. Klarstrom, Leon L. Shaw, and W. Yuan
- Subjects
Materials science ,Scanning electron microscope ,Mechanical Engineering ,Metallurgy ,Work hardening ,Condensed Matter Physics ,Fatigue limit ,Superalloy ,Compressive strength ,Mechanics of Materials ,Residual stress ,Hardening (metallurgy) ,General Materials Science ,Surface layer - Abstract
Fatigue behaviors of a Ni-based C-2000 superalloy subjected to the surface nanocrystallization and hardening (SNH) process were investigated. The influence of the SNH processing condition on the fatigue properties of the material was analyzed. The near-surface structures of the SNH-treated specimens were characterized by means of the scanning-electron microscopy, X-ray diffraction, and transmission-electron microscopy. It is shown that the SNH is an effective method to render the material with the features, such as a nanostructured and work-hardened surface layer as well as compressive residual stresses, which can pronouncedly improve the fatigue strength of the material. However, excessive treatments deteriorate the fatigue properties, and the surface contaminations are considered to be the main reason.
- Published
- 2007
39. Evaluation of carbon-supported ruthenium-selenium-tungsten catalysts for direct methanol fuel cells
- Author
-
H. Cheng, JB Lakeman, W. Yuan, D.J. Browning, and Keith Scott
- Subjects
inorganic chemicals ,Waste management ,Renewable Energy, Sustainability and the Environment ,Decarbonylation ,Inorganic chemistry ,Energy Engineering and Power Technology ,chemistry.chemical_element ,Tungsten ,equipment and supplies ,Direct-ethanol fuel cell ,Catalysis ,Ruthenium ,chemistry.chemical_compound ,chemistry ,Methanol ,Electrical and Electronic Engineering ,Physical and Theoretical Chemistry ,Methanol fuel ,Carbon - Abstract
The use of ruthenium-selenium-tungsten catalysts as methanol tolerant cathodes for direct methanol fuel cells is reported. The novel catalysts were produced by decarbonylation of ruthenium and tungsten carbonyls in the presence of selenium and carbon powders. The produced materials were characterised in both half cells and fuel cells. The addition of tungsten led to better oxygen reduction performance, giving current densities up to 30% greater and cell power densities up to 25% greater than those obtained with ruthenium-selenium alone. There is only a minor loss in methanol tolerance in the presence of tungsten. The improvement in performance is a consequence of the beneficial influence of tungsten on the structure and properties of catalysts. The effects of fuel cell operating conditions are also reported. The new catalysts were compared to Pt.
- Published
- 2007
40. The catalytic activity and methanol tolerance of transition metal modified-ruthenium–selenium catalysts
- Author
-
D.J. Browning, JB Lakeman, H Cheng, Keith Scott, and W. Yuan
- Subjects
Process Chemistry and Technology ,Industrial catalysts ,Inorganic chemistry ,chemistry.chemical_element ,Tungsten ,Catalysis ,Nanomaterial-based catalyst ,Ruthenium ,Rhodium ,chemistry.chemical_compound ,chemistry ,Transition metal ,Methanol ,General Environmental Science - Abstract
The activity of ruthenium-based catalysts towards oxygen reduction was enhanced by addition of tungsten, molybdenum and rhodium. The catalysts were produced by decarbonylation of the ruthenium and transition metal carbonyls in the presence of selenium (sulphur) and carbon powders. The produced materials were characterised by scanning electron microscopy and energy dispersive spectroscopy as well as by electrochemical evaluations in both half cells and direct methanol fuel cells. All transition metal-modified catalysts exhibited better performance than those of ruthenium–selenium (sulphur) alone, but the tungsten modification seemed the best approach. The RuSe0.20W0.29 catalyst delivered the maximum power density of up to 40 mW cm−2. The improvement is a consequence of the enhanced activity towards oxygen reduction with a minor loss in methanol tolerance as well as a stabilising effect of tungsten on catalysts. The new catalysts were compared to Pt and to sulphur-containing catalysts.
- Published
- 2007
41. Fabrication and evaluation of Pt–Fe alloys as methanol tolerant cathode materials for direct methanol fuel cells
- Author
-
Keith Scott, W. Yuan, and H. Cheng
- Subjects
Fabrication ,Renewable Energy, Sustainability and the Environment ,Scanning electron microscope ,Analytical chemistry ,Energy Engineering and Power Technology ,Cathode ,Catalysis ,law.invention ,chemistry.chemical_compound ,Direct methanol fuel cell ,chemistry ,Chemical engineering ,law ,Methanol ,Electrical and Electronic Engineering ,Physical and Theoretical Chemistry ,Methanol fuel ,Power density - Abstract
Carbon-supported platinum–iron catalysts were prepared and characterised by means of scanning electron microscopy, energy-dispersive X-ray and X-ray diffraction techniques. The catalysts were tested for oxygen reduction in half-cells and in direct methanol fuel cells using voltammetric and steady-state polarisation measurements. Methanol oxidation was partially suppressed and higher net oxygen reduction currents were achieved at the PtFe/C cathodes, compared to the Pt alone. An increase in power density of up to 20–30% was achieved by using the PtFe/C rather than the Pt/C cathodes.
- Published
- 2006
42. Increased glycophorin A somatic cell variant frequency in arsenic-exposed patients of Guizhou, China
- Author
-
M.L. Cheng, W. Yuan, H. Xiao, N. Fang, M.L. Zhao, L.M. Liu, Y.S. Zhou, D.X. Chen, H.H. Xu, Q.B. Wa, L. Jiang, H. Du, Jie Liu, X.J. Zhang, and Michael P. Waalkes
- Subjects
Adult ,Male ,China ,medicine.medical_specialty ,Pathology ,Erythrocytes ,Skin Neoplasms ,Population ,chemistry.chemical_element ,Biology ,Toxicology ,medicine.disease_cause ,Arsenic ,Flow cytometry ,Gene Frequency ,Internal medicine ,medicine ,Humans ,Glycophorin ,Glycophorins ,education ,Allele frequency ,Alleles ,education.field_of_study ,integumentary system ,Arsenic toxicity ,medicine.diagnostic_test ,Environmental Exposure ,General Medicine ,Middle Aged ,Flow Cytometry ,Immunohistochemistry ,Coal ,Endocrinology ,chemistry ,Mutation ,biology.protein ,Female ,Biomarkers ,Genotoxicity - Abstract
Exposure to arsenic through domestic burning arsenic-containing coal causes various tumors in a population of Guizhou, China. The glycophorin A (GPA) assay is a human mutation assay detecting somatic variation in erythrocytes expressing the MN blood type, and was used to assess genotoxicity of arsenic-exposed patients. Peripheral blood was collected from 18 adult healthy subjects and 40 arsenic-exposed patients in heparin-treated tubes. Erythrocytes were isolated, fixed in formalin and immuno-labeled with fluorescent antibodies against GPA, followed by flow cytometry analysis. Arsenic exposure increased the variant frequency (expressed as the number of variant red cells per 10(6) erythrocytes): NN, 3.7 in healthy subjects versus 21.2 in arsenic-exposed patients; N phi, 12.6 versus 33.1; MM, 13.1 versus 110; and M phi, 5.2 versus 20.3. The total GPA variant frequency was increased about five-fold (34.7 in healthy subjects versus 185 in arsenosis patients). Furthermore, the variant frequency was significantly higher in skin tumor-bearing patients: NN, 19.4 in arsenic-exposed non-tumor patients versus 31.5 in tumor-bearing patients; N phi, 29.5 versus 54.5; MM, 102 versus 159; M phi, 15.9 versus 45.1. Total GPA variant frequency in arsenic-exposed patients bearing skin tumors was significantly increased compared to patients without skin tumors (167 versus 290). The relationship between arsenic exposure history and GPA variant frequency was less evident. These data demonstrate that arsenic exposure is associated with mutations at the GPA locus, an effect exaggerated in patients bearing arsenic-induced skin tumors. The variant frequency of GPA could be a useful biomarker for arsenic exposure and arsenic carcinogenesis.
- Published
- 2006
43. The influence of a new fabrication procedure on the catalytic activity of ruthenium–selenium catalysts
- Author
-
W. Yuan, H. Cheng, and Keith Scott
- Subjects
inorganic chemicals ,Scanning electron microscope ,General Chemical Engineering ,Inorganic chemistry ,Energy-dispersive X-ray spectroscopy ,chemistry.chemical_element ,Electrocatalyst ,Catalysis ,Ruthenium ,chemistry.chemical_compound ,Direct methanol fuel cell ,Crystallinity ,chemistry ,Electrochemistry ,Methanol - Abstract
A new procedure has been introduced to enhance catalytic activity of ruthenium–selenium electro-catalysts for oxygen reduction, in which materials are treated under hydrogen atmosphere at elevated temperatures. The characterisation using scanning electron microscopy, energy dispersive spectroscopy or energy dispersive X-ray spectroscopy exhibited that the treatment at 400 °C made catalysts denser while their porous nature remained, led to a good degree of crystallinity and an optimum Se:Ru ratio. The half cell test confirms feasibility of the new procedure; the catalyst treated at 400 °C gave the highest reduction current (55.9 mA cm −2 at −0.4 V) and a low methanol oxidation effect coefficient (3.8%). The direct methanol fuel cell with the RuSe 400 °C cathode catalyst (2 mg RuSe cm −2 ) generated a power density of 33.8 mW cm −2 using 2 M methanol and 2 bar oxygen at 90 °C. The new procedure produced the catalysts with low decay rates. The best sample was compared to the Pt and to the reported ruthenium–selenium catalyst. Possible reasons for the observations are discussed.
- Published
- 2006
44. A systematic search of highly variable X-ray sources with the XMM-Newton serendipitous survey
- Author
-
Stefanie Komossa, M. G. Watson, J. P. Osborne, and W. Yuan
- Subjects
Physics ,Atmospheric Science ,Supermassive black hole ,Committee on Space Research ,Astrophysics::High Energy Astrophysical Phenomena ,Aerospace Engineering ,Astronomy ,Astronomy and Astrophysics ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Astrophysics ,Galaxy ,Accretion (astrophysics) ,Black hole ,Geophysics ,Amplitude ,Space and Planetary Science ,ROSAT ,General Earth and Planetary Sciences ,Gamma-ray burst ,Astrophysics::Galaxy Astrophysics - Abstract
We describe an ongoing programme to search for X-ray sources with long-term, large amplitude X-ray variability. The method is to compare the X-ray sources from the XMM-Newton Serendipitous Survey with those from the previous ROSAT pointed observations and the ROSAT All-sky Survey. The work is largely motivated by the recent discovery of a new type of X-ray flares characterised by enormous amplitude flux variability and associated with normal galaxies [Komossa, S., Ludwig Biermann Award lecture: X-ray evidence for supermassive black holes at the centers of nearby, non-active galaxies. Rev. Mod. Astron. 15, 27, 2002]. Other objects of interest are black hole accretion systems, such as X-ray binaries and AGN, GRB afterglows, extremes of stellar flares, and other objects undergoing extremely violent physical processes. In this paper, we describe the programme and present some preliminary results. (c) 2005 COSPAR. Published by Elsevier Ltd. All rights reserved.
- Published
- 2006
45. Thermomechanical postbuckling of composite laminated plates by the spline finite strip method
- Author
-
D.J. Dawe, W. Yuan, and Y. Ge
- Subjects
Materials science ,business.industry ,Finite strip method ,B-spline ,Composite number ,Structural engineering ,Spline (mathematics) ,Buckling ,Plate theory ,Ceramics and Composites ,Boundary value problem ,Composite material ,business ,Temperature load ,Civil and Structural Engineering - Abstract
The thermomechanical postbuckling behaviour of composite laminated plates is studied with the aid of the B-spline finite strip method under the combination of temperature load and applied uniaxial mechanical stress. To account for through-thickness shear deformation effects, the thermal-elastic, first-order shear deformation (Reissner–Mindlin) plate theory is used in this paper. General boundary conditions and laminate lay-ups can be accommodated in the newly developed finite strip approach. A range of applications is described and the results generated by the finite strip procedure are compared with the results of previous studies. The spline finite strip method is shown to be versatile and accurate with good convergence qualities.
- Published
- 2005
46. Fatigue behavior of Zr–Ti–Ni–Cu–Be bulk-metallic glasses
- Author
-
C.T. Liu, Raymond A. Buchanan, William H. Peter, B. Yang, A. Peker, Michael L. Benson, Gongyao Wang, Lu Huang, M. Freels, W. Yuan, Charlie R. Brooks, and Peter K. Liaw
- Subjects
Materials science ,Amorphous metal ,Morphology (linguistics) ,business.industry ,Mechanical Engineering ,Alloy ,Metallurgy ,Metals and Alloys ,Fatigue testing ,General Chemistry ,engineering.material ,Edge (geometry) ,Casting ,Mechanics of Materials ,Nondestructive testing ,Materials Chemistry ,engineering ,Fracture (geology) ,Composite material ,business - Abstract
The high-cycle fatigue (HCF) behavior of the Zr 41.2 Ti 13.8 Cu 12.5 Ni 10 Be 22.5 (in at.%) bulk-metallic glass (BMG) was studied. Two batches of samples that are from different lots (Batches 59 and 94) are employed in present experiments. The HCF experiments were conducted, using an electrohydraulic machine at a frequency of 10 Hz with a R ratio of 0.1 in air at room temperature and under tension-tension loading, where R = σ min. / σ max. . ( σ min. and σ max. are the applied minimum and maximum stresses, respectively). A high-speed and high-sensitivity thermographic-infrared (IR) imaging system was employed for the nondestructive evaluation of temperature evolutions during fatigue testing. No distinct sparking phenomenon was observed at the final fracture moment for this alloy. The fatigue lifetime of Batch 59 is longer than that of Batch 94 at high stress levels (maximum stresses >864 MPa). Moreover, the fatigue-endurance limit of Batch 59 (703 MPa) is somewhat greater than that of Batch 94 (615 MPa). The vein pattern and liquid droplets were observed in the apparent-melting region along the edge of the fractured surfaces. The fracture morphology suggests that fatigue cracks initiated from casting defects, such as porosities and inclusions, which have an important effect on the fatigue behavior of BMGs.
- Published
- 2005
47. Progress toward a new measurement of the parity violating asymmetry in n→+p→d+γ
- Author
-
V. R. Pomeroy, W. M. Snow, M. Leuschner, D. R. Rich, E. I. Sharapov, J. D. Bowman, S. I. Penttilä, V. W. Yuan, and W. S. Wilburn
- Subjects
Physics ,Nuclear and High Energy Physics ,media_common.quotation_subject ,Detector ,Gamma ray ,Parity (physics) ,Signal ,Asymmetry ,Magnetic field ,Nuclear physics ,Neutron capture ,Sensitivity (control systems) ,Nuclear Experiment ,Instrumentation ,media_common - Abstract
We outline the motivation and conceptual design for a new experiment aimed at a 10-fold improvement in the accuracy of the parity-violating asymmetry A_gamma in the angular distribution of 2.2 MeV gamma rays from the n+p-->d+gamma reaction. This observable is primarily sensitive to the weak pion-nucleon coupling H_pi^1. A proof-of-principle experiment using unpolarized low-energy neutron capture on polyethylene and an array of 12 CsI detectors operated in current mode has been performed. Results of this test experiment including the current mode signal, electronic noise and detector sensitivity to magnetic fields are reported., Comment: 19 pages, 9 eps figures, uses RevTeX and epsfig, submitted to NIM
- Published
- 2003
48. Development of sustainability indicators by communities in China: a case study of Chongming County, Shanghai
- Author
-
Simon M. Hutchinson, Philip James, C. Shi, W. Yuan, and K. Hodgson
- Subjects
Adult ,China ,Conservation of Natural Resources ,Fossil Fuels ,Economic growth ,Consensus ,Environmental Engineering ,Adolescent ,Best practice ,Management, Monitoring, Policy and Law ,Humans ,Social Change ,Public engagement ,Child ,Students ,Waste Management and Disposal ,Environmental planning ,Sustainable development ,Health Priorities ,Social change ,Community Participation ,General Medicine ,Benchmarking ,Faculty ,Geography ,Social Conditions ,Public participation ,Sustainability ,Environment Design - Abstract
Public participation as a means of identifying sustainability indicators for Chongming County, Shanghai, China was evaluated by an international group drawing on established best practice. An initial 'long list' of 86 sustainability indicators, based on previous indicator systems developed in China, was identified. This 'long list' was reduced via consultations with local academics and local-government officers from Shanghai City and Chongming County to a 'short list' of 17 indicators. This short-list was subjected to further community consultation involving 159 local-government officers, teachers, students (aged 12-14 years), farmers and workers. Data from the consultations indicated differences in the understanding of sustainable development among the different sectors. By combining the data from the different sectors it was possible to identify a consensus around 4 core and 7 additional indicators. These are proposed as indicators which could be used to steer local activities directed towards sustainable development. The list of indicators produced by the people of Chongming Island was compared to local indicator systems in Europe. In comparison with European lists the Chongming list was found to have a greater emphasis on economic development but a similar level of concern for environmental matters. This study has special significance as it reports on the implementation of a process involving local resident participation in the process of sustainable development in China.
- Published
- 2003
49. Parity-violating gamma-ray asymmetry in the neutron-proton capture
- Author
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S. I. Pentilla, K. Morimoto, Timothy Chupp, Michael Gericke, M. B. Leuschner, F. W. Hersmann, Yasuhiro Masuda, W. D. Ramsay, G. L. Jones, S. Ishimoto, S. J. Freedman, S. Muto, S. W. Wilburn, Gregory S. Mitchell, R. D. Carlini, S. A. Page, H. Nann, E. I. Sharapov, T. R. Gentile, J. D. Bowman, Y. W. Yuan, T. Ino, T. B. Smith, T. Case, K. P. Coulter, W. M. Snow, and G. L. Greene
- Subjects
Coupling constant ,Physics ,Nuclear and High Energy Physics ,Particle physics ,media_common.quotation_subject ,Nuclear Theory ,Radiative capture ,Gamma ray ,Parity (physics) ,Asymmetry ,Nuclear physics ,Neutron ,Nuclear Experiment ,media_common - Abstract
An experiment to measure γ-ray asymmetry A γ with a high precision in neutron-proton radiative capture is under construction at LANSCE. The experiment will determine the weak pion-nucleon coupling constant H π 1 ,, 30% of its predicted value.
- Published
- 2003
50. Association between protease-specific proteolytic cleavage of brevican and synaptic loss in the dentate gyrus of kainate-treated rats
- Author
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Paul E. Gottschall, John D. Sandy, Russell T. Matthews, and W Yuan
- Subjects
Male ,Disintegrins ,Neurotoxins ,Nerve Tissue Proteins ,Kainate receptor ,Biology ,Antibodies ,Gene Expression Regulation, Enzymologic ,Substrate Specificity ,Rats, Sprague-Dawley ,ADAMTS1 Protein ,Excitatory Amino Acid Agonists ,Neuropil ,medicine ,Animals ,Lectican ,Lectins, C-Type ,RNA, Messenger ,Brevican ,Kainic Acid ,General Neuroscience ,Dentate gyrus ,ADAMTS ,Perineuronal net ,Metalloendopeptidases ,Denervation ,Peptide Fragments ,Rats ,Cell biology ,ADAM Proteins ,ADAMTS4 ,medicine.anatomical_structure ,Chondroitin Sulfate Proteoglycans ,Biochemistry ,Dentate Gyrus ,Synapses ,ADAMTS4 Protein ,Procollagen N-Endopeptidase - Abstract
Proteolytic fragments generated by ADAMTS ( a d isintegrin a nd m etalloprotease with t hrombo s pondin motifs)-mediated cleavage of the aggregating chondroitin sulfate proteoglycan, brevican, have been identified, but not localized in the CNS. The purpose of this study, using kainate-induced CNS lesion, was to examine the spatial and quantitative relationship between ADAMTS1 and 4 mRNA expression and ADAMTS-mediated cleavage of brevican (as determined by the abundance of the neo-epitope QEAVESE at the C-terminal of the cleaved brevican G1 domain). In untreated rats, in situ hybridization and reverse transcriptase polymerase chain reaction indicated that ADAMTS4 expression was higher than ADAMTS1 and was localized to hippocampus, temporal lobe and other areas of cortex, striatum and hypothalamus. ADAMTS4 mRNA expression in these regions correlated with the presence of the QEAVESE neo-epitope, which was concentrated in perineuronal nets and in neuropil. In rats that seized after kainate, there was a dramatic elevation in ADAMTS1 and ADAMTS4 transcript that correlated and co-localized with a robust elevation in an extractable, 55-kDa fragment of brevican in temporal lobe and hippocampus. This fragment consisted, at least in part, of the ADAMTS-cleaved epitope G1-QEAVESE. The kainate-induced elevation in this ADAMTS-cleaved fragment was localized to amygdaloid and thalamic nuclei, hippocampus, caudate–putamen, cingulate cortex, and the outer molecular layer of the dentate gyrus where it was accompanied by a robust elevation in ADAMTS1 and 4 mRNA and a 28% decline in synaptic density 5 days after kainate. Thus, complexes of extracellular matrix proteins that exist in perineuronal nets and in the neuropil are cleaved by specific matrix-degrading proteases at early time points during excitotoxic neurodegeneration. The observed ADAMTS-induced cleavage of brevican in the dentate outer molecular layer is closely associated with diminished synaptic density, and may, therefore, contribute to synaptic loss and/or reorganization in this region.
- Published
- 2002
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