19 results on '"Yang, S.-D."'
Search Results
2. Zero mean curvature surfaces in Lorentz-Minkowski 3-space which change type across a light-like line
- Author
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FUJIMORI, S., KIM, Y. W., KOH, S.-E., ROSSMAN, W., SHIN, H., UMEHARA, M., YAMADA, K., and YANG, S.-D.
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Mathematics - Differential Geometry ,53A10 (Primary) 53B30 (Secondary) ,Differential Geometry (math.DG) ,35M10 ,FOS: Mathematics ,53A10 ,53B30 - Abstract
It is well-known that space-like maximal surfaces and time-like minimal surfaces in Lorentz-Minkowski 3-space R^3_1 have singularities in general. They are both characterized as zero mean curvature surfaces. We are interested in the case where the singular set consists of a light-like line, since this case has not been analyzed before. As a continuation of a previous work by the authors, we give the first example of a family of such surfaces which change type across the light-like line. As a corollary, we also obtain a family of zero mean curvature hypersurfaces in R^{n+1}_1 that change type across an (n-1)-dimensional light-like plane., 10 pages, 1 figure; Version 3: Sections 2 and 3 in Version 2 are removed, since they are not directly related to our main theorem in the revision
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- 2015
3. Search for $XYZ$ states in $\Upsilon(1S)$ inclusive decays
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Belle Collaboration, Shen, C. P., Yuan, C. Z., Ban, Y., Aihara, H., Asner, D. M., Badhrees, I., Bakich, A. M., Barberio, E., Behera, P., Bhardwaj, V., Bhuyan, B., Biswal, J., Bondar, A., Bonvicini, G., Bozek, A., Bračko, M., Browder, T. E., Červenkov, D., Chekelian, V., Chen, A., Chilikin, K., Chistov, R., Cho, K., Chobanova, V., Choi, S. -K., Choi, Y., Cinabro, D., Dalseno, J., Danilov, M., Dash, N., Di Carlo, S., Doležal, Z., Drásal, Z., Dutta, D., Eidelman, S., Farhat, H., Fast, J. E., Ferber, T., Fulsom, B. G., Gaur, V., Gabyshev, N., Garmash, A., Goldenzweig, P., Haba, J., Hayasaka, K., Hayashii, H., Hou, W. -S., Iijima, T., Inguglia, G., Ishikawa, A., Itoh, R., Jacobs, W. W., Jeon, H. B., Joo, K. K., Julius, T., Kang, K. H., Kim, D. Y., Kim, J. B., Kim, K. T., Kim, S. H., Kim, Y. J., Kinoshita, K., Kodyš, P., Korpar, S., Kotchetkov, D., Križan, P., Krokovny, P., Kuhr, T., Kuzmin, A., Kwon, Y. -J., Lange, J. S., Li, C. H., Li, H., Li, L., Li, Y., Gioi, L. Li, Libby, J., Liventsev, D., Luo, T., Masuda, M., Matsuda, T., Matvienko, D., Moll, A., Moon, H. K., Mussa, R., Nakao, M., Nanut, T., Nath, K. J., Natkaniec, Z., Nayak, M., Negishi, K., Nishida, S., Ogawa, S., Okuno, S., Olsen, S. L., Pakhlov, P., Pakhlova, G., Pal, B., Pestotnik, R., Petrič, M., Piilonen, L. E., Pulvermacher, C., Ritter, M., Rostomyan, A., Sakai, Y., Sandilya, S., Santelj, L., Sanuki, T., Savinov, V., Schlüter, T., Schneider, O., Schnell, G., Schwanda, C., Seino, Y., Senyo, K., Seon, O., Seong, I. S., Sevior, M. E., Shibata, T. -A., Shiu, J. -G., Simon, F., Sokolov, A., Solovieva, E., Starič, M., Sumiyoshi, T., Takizawa, M., Tanida, K., Tenchini, F., Trabelsi, K., Uchida, M., Uglov, T., Unno, Y., Uno, S., Varner, G., Vinokurova, A., Vorobyev, V., Wang, C. H., Wang, M. -Z., Wang, P., Wang, X. L., Watanabe, M., Watanabe, Y., Williams, K. M., Won, E., Yamaoka, J., Yang, S. D., Yashchenko, S., Yook, Y., Yusa, Y., Zhang, Z. P., Zhilich, V., Zhukova, V., Zhulanov, V., and Zupanc, A.
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J/psi(3100) ,molecule [meson] ,+psi%283685%29%22">Upsilon(9460) --> psi(3685) ,charmonium ,exotic [meson] ,branching ratio [Upsilon(9460)] ,BELLE ,annihilation [electron positron] ,tetraquark ,tracks ,hybrid [meson] ,decay modes ,High Energy Physics - Experiment ,High Energy Physics - Phenomenology ,KEK-B ,colliding beams [electron positron] ,+J%2Fpsi%283100%29+anything%22">Upsilon(9460) --> J/psi(3100) anything ,High Energy Physics::Experiment ,ddc:530 ,psi(3685) ,upper limit ,experimental results - Abstract
The branching fractions of the $\Upsilon(1S)$ inclusive decays into final states with a $J/\psi$ or a $\psi(2S)$ are measured with improved precision to be $\BR(\Upsilon(1S)\to J/\psi + {\rm anything})=(5.25\pm 0.13(\mathrm{stat.})\pm 0.25(\mathrm{syst.}))\times 10^{-4}$ and $\BR(\Upsilon(1S)\to \psi(2S) + {\rm anything})=(1.23\pm 0.17(\mathrm{stat.})\pm 0.11(\mathrm{syst.}))\times 10^{-4}$. The first search for $\Upsilon(1S)$ decays into $XYZ$ states that decay into a $J/\psi$ or a $\psi(2S)$ plus one or two charged tracks yields no significant signals for $XYZ$ states in any of the examined decay modes, and upper limits on their production rates in $\Upsilon(1S)$ inclusive decays are determined., Comment: 10 pages, 7 figures, 3 tables
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- 2016
- Full Text
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4. Search for $XYZ$ states in $��(1S)$ inclusive decays
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Belle Collaboration, Shen, C. P., Yuan, C. Z., Ban, Y., Aihara, H., Asner, D. M., Badhrees, I., Bakich, A. M., Barberio, E., Behera, P., Bhardwaj, V., Bhuyan, B., Biswal, J., Bondar, A., Bonvicini, G., Bozek, A., Bra��ko, M., Browder, T. E., ��ervenkov, D., Chekelian, V., Chen, A., Chilikin, K., Chistov, R., Cho, K., Chobanova, V., Choi, S. -K., Choi, Y., Cinabro, D., Dalseno, J., Danilov, M., Dash, N., Di Carlo, S., Dole��al, Z., Dr��sal, Z., Dutta, D., Eidelman, S., Farhat, H., Fast, J. E., Ferber, T., Fulsom, B. G., Gaur, V., Gabyshev, N., Garmash, A., Goldenzweig, P., Haba, J., Hayasaka, K., Hayashii, H., Hou, W. -S., Iijima, T., Inguglia, G., Ishikawa, A., Itoh, R., Jacobs, W. W., Jeon, H. B., Joo, K. K., Julius, T., Kang, K. H., Kim, D. Y., Kim, J. B., Kim, K. T., Kim, S. H., Kim, Y. J., Kinoshita, K., Kody��, P., Korpar, S., Kotchetkov, D., Kri��an, P., Krokovny, P., Kuhr, T., Kuzmin, A., Kwon, Y. -J., Lange, J. S., Li, C. H., Li, H., Li, L., Li, Y., Gioi, L. Li, Libby, J., Liventsev, D., Luo, T., Masuda, M., Matsuda, T., Matvienko, D., Moll, A., Moon, H. K., Mussa, R., Nakao, M., Nanut, T., Nath, K. J., Natkaniec, Z., Nayak, M., Negishi, K., Nishida, S., Ogawa, S., Okuno, S., Olsen, S. L., Pakhlov, P., Pakhlova, G., Pal, B., Pestotnik, R., Petri��, M., Piilonen, L. E., Pulvermacher, C., Ritter, M., Rostomyan, A., Sakai, Y., Sandilya, S., Santelj, L., Sanuki, T., Savinov, V., Schl��ter, T., Schneider, O., Schnell, G., Schwanda, C., Seino, Y., Senyo, K., Seon, O., Seong, I. S., Sevior, M. E., Shibata, T. -A., Shiu, J. -G., Simon, F., Sokolov, A., Solovieva, E., Stari��, M., Sumiyoshi, T., Takizawa, M., Tanida, K., Tenchini, F., Trabelsi, K., Uchida, M., Uglov, T., Unno, Y., Uno, S., Varner, G., Vinokurova, A., Vorobyev, V., Wang, C. H., Wang, M. -Z., Wang, P., Wang, X. L., Watanabe, M., Watanabe, Y., Williams, K. M., Won, E., Yamaoka, J., Yang, S. D., Yashchenko, S., Yook, Y., Yusa, Y., Zhang, Z. P., Zhilich, V., Zhukova, V., Zhulanov, V., and Zupanc, A.
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High Energy Physics - Experiment (hep-ex) ,High Energy Physics - Phenomenology (hep-ph) ,FOS: Physical sciences ,High Energy Physics::Experiment - Abstract
The branching fractions of the $��(1S)$ inclusive decays into final states with a $J/��$ or a $��(2S)$ are measured with improved precision to be $\BR(��(1S)\to J/��+ {\rm anything})=(5.25\pm 0.13(\mathrm{stat.})\pm 0.25(\mathrm{syst.}))\times 10^{-4}$ and $\BR(��(1S)\to ��(2S) + {\rm anything})=(1.23\pm 0.17(\mathrm{stat.})\pm 0.11(\mathrm{syst.}))\times 10^{-4}$. The first search for $��(1S)$ decays into $XYZ$ states that decay into a $J/��$ or a $��(2S)$ plus one or two charged tracks yields no significant signals for $XYZ$ states in any of the examined decay modes, and upper limits on their production rates in $��(1S)$ inclusive decays are determined., 10 pages, 7 figures, 3 tables
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- 2016
- Full Text
- View/download PDF
5. Evidence of $\Upsilon(1S) \to J/\psi+\chi_{c1}$ and search for double-charmonium production in $\Upsilon(1S)$ and $\Upsilon(2S)$ decays
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Yang, S. D., Shen, C. P., Aushev, T., Piilonen, L. E., Ribežl, E., Ritter, Marti, Rostomyan, Armine, Sakai, Y., Sandilya, S., Santelj, L., Sanuki, T., Schneider, O., Schnell, Gunar, Ayad, R., Schwanda, C., Semmler, D., Senyo, K., Shebalin, V., Shibata, T. -A., Shiu, J. -G., Shwartz, B., Sibidanov, A., Simon, Frank, Sohn, Y. -S., Bakich, A. M., Sokolov, A., Staric, Marko, Steder, Michael, Sumiyoshi, T., Tamponi, U., Tanida, K., Tatishvili, G., Teramoto, Y., Uchida, M., Uehara, S., Bansal, V., Uglov, T., Unno, Y., Uno, S., Urquijo, P., Usov, Y., Vahsen, S. E., Van Hulse, C., Vanhoefer, P., Varner, G., Vinokurova, A., Behera, P., Vorobyev, V., Vossen, A., Wagner, M. N., Wang, C. H., Wang, M. -Z., Wang, P., Wang, X. L., Watanabe, M., Watanabe, Y., Won, E., Bhuyan, B., Yamaoka, J., Yashchenko, Sergey, Yook, Y., Yuan, C. Z., Zhang, Z. P., Zhilich, V., Zhulanov, V., Belle Collaboration, Bobrov, Andrey, Bozek, A., Bračko, M., Browder, T. E., Ban, Y., Červenkov, D., Chekelian, Vladimir, Chen, A., Cheon, B. G., Chilikin, K., Chistov, R., Cho, K., Chobanova, V., Choi, S. -K., Choi, Y., Abdesselam, A., Cinabro, D., Dalseno, J., Danilov, Michael, Dingfelder, J., Doležal, Z., Drásal, Z., Drutskoy, Alexey, Dutta, Koushik, Eidelman, S., Farhat, H., Adachi, I., Fast, J. E., Ferber, Torben, Gaur, V., Gabyshev, N., Ganguly, S., Garmash, A., Gillard, R., Goh, Y. M., Golob, B., Haba, J., Aihara, H., Hara, T., Hayashii, H., He, X. H., Hou, W. -S., Huschle, M., Iijima, T., Inami, K., Ishikawa, A., Itoh, Ryosuke, Jaegle, I., Said, S. Al, Joffe, D., Joo, K. K., Julius, T., Kawasaki, T., Kim, D. Y., Kim, Hyun-Jeong, Kim, J. B., Kim, Joo-Hee, Kim, K. T., Kinoshita, K., Arinstein, K., Ko, B. R., Kodys, Peter, Korpar, Samo, Krizan, Peter, Krokovny, P., Kuzmin, Alexei, Kwon, Y. -J., Lange, Jens Sören, Li, Jie, Li, Yongjin, Asner, D. M., Gioi, L. Li, Libby, J., Liventsev, D., Lukin, P., Miyabayashi, K., Miyata, H., Moll, A., Mussa, R., Nakano, E., Nakao, Mikihiko, Aulchenko, V., Nanut, T., Nisar, N. K., Nishida, S., Okuno, S., Ostrowicz, Waclaw, Park, C. W., Park, H., Pedlar, T. K., Pestotnik, Rok, and Petrič, M.
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10.52 GeV-cms ,+J%2Fpsi%283100%29+chi%2Fc1%283510%29%22">Upsilon(9460) --> J/psi(3100) chi/c1(3510) ,factorization [quantum chromodynamics] ,High Energy Physics::Phenomenology ,nonrelativistic [quantum chromodynamics] ,BELLE ,annihilation [electron positron] ,branching ratio: upper limit [Upsilon(9460)] ,X(3940) ,High Energy Physics - Experiment ,branching ratio: upper limit [Upsilon(10020)] ,High Energy Physics - Phenomenology ,KEK-B ,hadronic decay [upsilon mesons] ,High Energy Physics::Experiment ,branching ratio: measured [Upsilon(9460)] ,experimental results - Abstract
Using data samples of $102\times10^6$ $\Upsilon(1S)$ and $158\times10^6$ $\Upsilon(2S)$ events collected with the Belle detector, a first experimental search has been made for double-charmonium production in the exclusive decays $\Upsilon(1S,2S)\rightarrow J/\psi(\psi')+X$, where $X=\eta_c$, $\chi_{cJ} (J=~0,~1,~2)$, $\eta_c(2S)$, $X(3940)$, and $X(4160)$. No significant signal is observed in the spectra of the mass recoiling against the reconstructed $J/\psi$ or $\psi'$ except for the evidence of $\chi_{c1}$ production with a significance of $4.6\sigma$ for $\Upsilon(1S)\rightarrow J/\psi+\chi_{c1}$. The measured branching fraction $\BR(\Upsilon(1S)\rightarrow J/\psi+\chi_{c1})$ is $(3.90\pm1.21(\rm stat.)\pm0.23 (\rm syst.))\times10^{-6}$. The $90\%$ confidence level upper limits on the branching fractions of the other modes having a significance of less than $3\sigma$ are determined. These results are consistent with theoretical calculations using the nonrelativistic QCD factorization approach., Comment: 12 pages, 4 figures, 1 table. The fit range was extended to include X(4160) signal according to referee's suggestions. Other results unchanged. Paper was accepted for publication as a regular article in Physical Review D
- Published
- 2014
6. Evidence of $\mathrm{\Upsilon }\left(1S\right)\to J/\psi +{\chi }_{c1}$ and search for double-charmonium production in $\mathrm{\Upsilon }\left(1S\right)$ and $\mathrm{\Upsilon }\left(2S\right)$ decays
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Yang, S. D., Shen, C. P., Ayad, R., Shibata, T. -A., Shiu, J. -G., Shwartz, B., Sibidanov, A., Sohn, Y. -S., Sokolov, A., Staric, Marko, Steder, Michael, Sumiyoshi, T., Tamponi, U., Bakich, A. M., Tanida, K., Tatishvili, G., Teramoto, Y., Uchida, M., Uehara, S., Uglov, T., Unno, Y., Uno, S., Urquijo, P., Usov, Y., Bansal, V., Vahsen, S. E., Van Hulse, C., Vanhoefer, P., Varner, G., Vinokurova, A., Vorobyev, V., Vossen, A., Wagner, M. N., Wang, C. H., Wang, M. -Z., Behera, P., Wang, P., Wang, X. L., Watanabe, M., Watanabe, Y., Won, E., Yamaoka, J., Yashchenko, Sergey, Yook, Y., Yuan, C. Z., Zhang, Z. P., Bhuyan, B., Zhilich, V., Zhulanov, V., Belle Collaboration, Al Said, S., Bobrov, A., Danilov, M., Drutskoy, A., Dutta, K., Gaur, V., Hayasaka, K., Bozek, A., Kim, H. J., Kim, J. H., Kuzmin, A., Li, J., Li, Y., Li Gioi, L., Ritter, M., Schnell, G., Simon, F., Bračko, M., Browder, T. E., Červenkov, D., Chekelian, Vladimir, Ban, Y., Chen, A., Cheon, B. G., Chilikin, K., Chistov, R., Cho, K., Chobanova, V., Choi, S. -K., Choi, Y., Cinabro, D., Dalseno, J., Abdesselam, A., Dingfelder, J., Doležal, Z., Drásal, Z., Eidelman, S., Farhat, H., Fast, J. E., Ferber, Torben, Gabyshev, N., Ganguly, S., Garmash, A., Adachi, I., Gillard, R., Goh, Y. M., Golob, B., Haba, J., Hara, T., Hayashii, H., He, X. H., Hou, W. -S., Huschle, M., Iijima, T., Aihara, H., Inami, K., Ishikawa, A., Itoh, Ryosuke, Jaegle, I., Joffe, D., Joo, K. K., Julius, T., Kawasaki, T., Kim, D. Y., Kim, J. B., Arinstein, K., Kim, K. T., Kinoshita, K., Ko, B. R., Kodys, Peter, Korpar, Samo, Krizan, Peter, Krokovny, P., Kwon, Y. -J., Lange, Jens Sören, Libby, J., Asner, D. M., Liventsev, D., Lukin, P., Miyabayashi, K., Miyata, H., Moll, A., Mussa, R., Nakano, E., Nakao, Mikihiko, Nanut, T., Nisar, N. K., Aulchenko, V., Nishida, S., Okuno, S., Ostrowicz, Waclaw, Park, C. W., Park, H., Pedlar, T. K., Pestotnik, Rok, Petrič, M., Piilonen, L. E., Ribežl, E., Aushev, T., Rostomyan, Armine, Sakai, Y., Sandilya, S., Santelj, L., Sanuki, T., Schneider, O., Schwanda, C., Semmler, D., Senyo, K., and Shebalin, V.
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10.52 GeV-cms ,+J%2Fpsi%283100%29+chi%2Fc1%283510%29%22">Upsilon(9460) --> J/psi(3100) chi/c1(3510) ,factorization [quantum chromodynamics] ,nonrelativistic [quantum chromodynamics] ,BELLE ,annihilation [electron positron] ,branching ratio: upper limit [Upsilon(9460)] ,X(3940) ,branching ratio: upper limit [Upsilon(10020)] ,KEK-B ,hadronic decay [upsilon mesons] ,High Energy Physics::Experiment ,ddc:530 ,branching ratio: measured [Upsilon(9460)] ,experimental results - Abstract
Using data samples of $102×{10}^{6}$ $\mathrm{\Upsilon }\left(1S\right)$ and $158×{10}^{6}$ $\mathrm{\Upsilon }\left(2S\right)$ events collected with the Belle detector, a first experimental search has been made for double-charmonium production in the exclusive decays $\mathrm{\Upsilon }\left(1S,2S\right)\to J/\psi \left({\psi }^{\prime }\right)+X$, where $X={\eta }_{c}$, ${\chi }_{cJ}\left(J=0,1,2\right)$, ${\eta }_{c}\left(2S\right)$, $X\left(3940\right)$, and $X\left(4160\right)$. No significant signal is observed in the spectra of the mass recoiling against the reconstructed $J/\psi $ or ${\psi }^{\prime }$ except for the evidence of ${\chi }_{c1}$ production with a significance of $4.6\sigma $ for $\mathrm{\Upsilon }\left(1S\right)\to J/\psi +{\chi }_{c1}$. The measured branching fraction $\mathcal{B}\left(\mathrm{\Upsilon }\left(1S\right)\to J/\psi +{\chi }_{c1}\right)$ is $\left[3.90±1.21\left(\text{stat}\right)±0.23\left(\text{syst}\right)\right]×{10}^{-6}$. The 90% C.L. upper limits on the branching fractions of the other modes having a significance of less than $3\sigma $ are determined. These results are consistent with theoretical calculations using the nonrelativistic QCD factorization approach.
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- 2014
- Full Text
- View/download PDF
7. Evidence of $��(1S) \to J/��+��_{c1}$ and search for double-charmonium production in $��(1S)$ and $��(2S)$ decays
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Belle Collaboration, Yang, S. D., Shen, C. P., Ban, Y., Abdesselam, A., Adachi, I., Aihara, H., Said, S. Al, Arinstein, K., Asner, D. M., Aulchenko, V., Aushev, T., Ayad, R., Bakich, A. M., Bansal, V., Behera, P., Bhuyan, B., Bobrov, A., Bozek, A., Bra��ko, M., Browder, T. E., ��ervenkov, D., Chekelian, V., Chen, A., Cheon, B. G., Chilikin, K., Chistov, R., Cho, K., Chobanova, V., Choi, S. -K., Choi, Y., Cinabro, D., Dalseno, J., Danilov, M., Dingfelder, J., Dole��al, Z., Dr��sal, Z., Drutskoy, A., Dutta, K., Eidelman, S., Farhat, H., Fast, J. E., Ferber, T., Gaur, V., Gabyshev, N., Ganguly, S., Garmash, A., Gillard, R., Goh, Y. M., Golob, B., Haba, J., Hara, T., Hayashii, H., He, X. H., Hou, W. -S., Huschle, M., Iijima, T., Inami, K., Ishikawa, A., Itoh, R., Jaegle, I., Joffe, D., Joo, K. K., Julius, T., Kawasaki, T., Kim, D. Y., Kim, H. J., Kim, J. B., Kim, J. H., Kim, K. T., Kinoshita, K., Ko, B. R., Kody��, P., Korpar, S., Kri��an, P., Krokovny, P., Kuzmin, A., Kwon, Y. -J., Lange, J. S., Li, J., Li, Y., Gioi, L. Li, Libby, J., Liventsev, D., Lukin, P., Miyabayashi, K., Miyata, H., Moll, A., Mussa, R., Nakano, E., Nakao, M., Nanut, T., Nisar, N. K., Nishida, S., Okuno, S., Ostrowicz, W., Park, C. W., Park, H., Pedlar, T. K., Pestotnik, R., Petri��, M., Piilonen, L. E., Ribe��l, E., Ritter, M., Rostomyan, A., Sakai, Y., Sandilya, S., Santelj, L., Sanuki, T., Schneider, O., Schnell, G., Schwanda, C., Semmler, D., Senyo, K., Shebalin, V., Shibata, T. -A., Shiu, J. -G., Shwartz, B., Sibidanov, A., Simon, F., Sohn, Y. -S., Sokolov, A., Stari��, M., Steder, M., Sumiyoshi, T., Tamponi, U., Tanida, K., Tatishvili, G., Teramoto, Y., Uchida, M., Uehara, S., Uglov, T., Unno, Y., Uno, S., Urquijo, P., Usov, Y., Vahsen, S. E., Van Hulse, C., Vanhoefer, P., Varner, G., Vinokurova, A., Vorobyev, V., Vossen, A., Wagner, M. N., Wang, C. H., Wang, M. -Z., Wang, P., Wang, X. L., Watanabe, M., Watanabe, Y., Won, E., Yamaoka, J., Yashchenko, S., Yook, Y., Yuan, C. Z., Zhang, Z. P., Zhilich, V., and Zhulanov, V.
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High Energy Physics - Experiment (hep-ex) ,High Energy Physics - Phenomenology (hep-ph) ,FOS: Physical sciences ,High Energy Physics::Experiment - Abstract
Using data samples of $102\times10^6$ $��(1S)$ and $158\times10^6$ $��(2S)$ events collected with the Belle detector, a first experimental search has been made for double-charmonium production in the exclusive decays $��(1S,2S)\rightarrow J/��(��')+X$, where $X=��_c$, $��_{cJ} (J=~0,~1,~2)$, $��_c(2S)$, $X(3940)$, and $X(4160)$. No significant signal is observed in the spectra of the mass recoiling against the reconstructed $J/��$ or $��'$ except for the evidence of $��_{c1}$ production with a significance of $4.6��$ for $��(1S)\rightarrow J/��+��_{c1}$. The measured branching fraction $\BR(��(1S)\rightarrow J/��+��_{c1})$ is $(3.90\pm1.21(\rm stat.)\pm0.23 (\rm syst.))\times10^{-6}$. The $90\%$ confidence level upper limits on the branching fractions of the other modes having a significance of less than $3��$ are determined. These results are consistent with theoretical calculations using the nonrelativistic QCD factorization approach., 12 pages, 4 figures, 1 table. The fit range was extended to include X(4160) signal according to referee's suggestions. Other results unchanged. Paper was accepted for publication as a regular article in Physical Review D
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- 2014
- Full Text
- View/download PDF
8. Prevalence of hematoma after anterior cervical spine surgery: A meta-analysis
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Liu, F. -Y, Huo, L. -S, Song, Y. -L, Yang, D. -L, Zhang, L. -J, Yang, S. -D, Wang, H., and Wenyuan Ding
9. Ultrasensitive second-harmonic generation frequency-resolved optical gating using an fiber-pigtailed aperiodically poled lithium niobate waveguide at 1.55μm
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Houxun Miao, Weiner, A. M., Yang, S. -D, Langrock, C., Roussev, R. V., and Fejer, M. M.
10. Observation of psi prime decays to rho(770) pi and rho(2150) pi
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Ablikim, M., Bai, J. Z., Ban, Y., Bian, J. G., Cai, X., Chang-Zheng Yuan, Chen, H. F., Chen, H. S., Chen, H. X., Chen, J. C., Chen, Jin, Chen, Jun, Chen, M. L., Chen, Y. B., Chi, S. P., Chu, Y. P., Cui, X. Z., Dai, H. L., Dai, Y. S., Deng, Z. Y., Dong, L. Y., Du, S. X., Du, Z. Z., Fang, J., Fang, S. S., Fu, C. D., Fu, H. Y., Gao, C. S., Gao, Y. N., Gong, M. Y., Gong, W. X., Gu, S. D., Guo, Y. N., Guo, Y. Q., Guo, Z. J., Harris, F. A., He, K. L., He, M., He, X., Heng, Y. K., Hu, H. M., Hu, T., Huang, G. S., Huang, L., Huang, X. P., Ji, X. B., Jia, Q. Y., Jiang, C. H., Jiang, X. S., Jin, D. P., Jin, S., Jin, Y., Lai, Y. F., Li, F., Li, G., Li, H. B., Li, H. H., Li, J., Li, J. C., Li, Q. J., Li, R. B., Li, R. Y., Li, S. M., Li, W. G., Li, X. L., Li, X. Q., Li, X. S., Liang, Y. F., Liao, H. B., Liu, C. X., Liu, F., Liu, Fang, Liu, H. M., Liu, J. B., Liu, J. P., Liu, R. G., Liu, Z. A., Liu, Z. X., Lu, F., Lu, G. R., Lu, J. G., Luo, C. L., Luo, X. L., Ma, F. C., Ma, J. M., Ma, L. L., Ma, Q. M., Ma, X. Y., Mao, Z. P., Mo, X. H., Nie, J., Nie, Z. D., Olsen, S. L., Peng, H. P., Qi, N. D., Qian, C. D., Qin, H., Qiu, J. F., Ren, Z. Y., Rong, G., Shan, L. Y., Shang, L., Shen, D. L., Shen, X. Y., Sheng, H. Y., Shi, F., Shi, X., Sun, H. S., Sun, S. S., Sun, Y. Z., Sun, Z. J., Tang, X., Tao, N., Tian, Y. R., Tong, G. L., Varner, Gary Sim, Wang, D. Y., Wang, J. Z., Wang, K., Wang, L., Wang, L. S., Wang, M., Wang, P., Wang, P. L., Wang, S. Z., Wang, W. F., Wang, Y. F., Wang, Zhe, Wang, Z., Wang, Zheng, Wang, Z. Y., Wei, C. L., Wei, D. H., Wu, N., Wu, Y. M., Xia, X. M., Xie, X. X., Xin, B., Xu, G. F., Xu, H., Xu, Y., Xue, S. T., Yan, M. L., Yang, F., Yang, H. X., Yang, J., Yang, S. D., Yang, Y. X., Ye, M., Ye, M. H., Ye, Y. X., Yi, L. H., Yi, Z. Y., Yu, C. S., Yu, G. W., Yuan, C. Z., Yuan, J. M., Yuan, Y., Yue, Q., Zang, S. L., Zeng, Yu, Zeng, Y., Zhang, B. X., Zhang, B. Y., Zhang, C. C., Zhang, D. H., Zhang, H. Y., Zhang, J., Zhang, J. Y., Zhang, J. W., Zhang, L. S., Zhang, Q. J., Zhang, S. Q., Zhang, X. M., Zhang, X. Y., Zhang, Y. J., Zhang, Y. Y., Zhang, Yi-Yun, Zhang, Z. P., Zhang, Z. Q., Zhao, D. X., Zhao, J. B., Zhao, J. W., Zhao, M. G., Zhao, P. P., Zhao, W. R., Zhao, X. J., Zhao, Y. B., Zhao, Z. G., Zheng, H. Q., Zheng, J. P., Zheng, L. S., Zheng, Z. P., Zhong, X. C., Zhou, B. Q., Zhou, G. M., Zhou, L., Zhou, N. F., Zhu, K. J., Zhu, Q. M., Zhu, Y. C., Zhu, Y. S., Zhu, Ying-Chun, Zhu, Z. A., and Zhuang, B. A.
11. Evidence of gamma(1S) -> J/Psi +chi(c1) and search for double-charmonium production in gamma(1S) and gamma(2S) decays
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Yang, S. D., Shen, C. P., Ban, Y., Abdesselam, A., Adachi, I., Aihara, H., Al Said, S., Arinstein, K., Asner, D. M., Aulchenko, V., Aushev, T., Ayad, R., Bakich, A. M., Bansal, V., Behera, P., Bhuyan, B., Bobrov, A., Bozek, A., Bracko, M., Browder, T. E., Cervenkov, D., Chekelian, V., Chen, A., Cheon, B. G., Chilikin, K., Chistov, R., Cho, K., Chobanova, V., Choi, S. -K., Choi, Y., Cinabro, D., Dalseno, J., Danilov, M., Dingfelder, J., Dolezal, Z., Drasal, Z., Drutskoy, A., Dutta, K., Eidelman, S., Farhat, H., Fast, J. E., Ferber, T., Gaur, V., Gabyshev, N., Ganguly, S., Garmash, A., Gillard, R., Goh, Y. M., Golob, B., Haba, J., Hara, T., Hayasaka, K., Hayashii, H., He, X. H., Hou, W. -S., Huschle, M., Iijima, T., Inami, K., Ishikawa, A., Itoh, R., Jaegle, I., Joffe, D., Joo, K. K., Julius, T., Kawasaki, T., Kim, D. Y., Kim, H. J., Kim, J. B., Kim, J. H., Kim, K. T., Kinoshita, K., Ko, B. R., Kodys, P., Korpar, S., Krizan, P., Krokovny, P., Kuzmin, A., Kwon, Y. -J., Lange, J. S., Li, J., Li, Y., Gioi, L. Li, Libby, J., Liventsev, D., Lukin, P., Miyabayashi, K., Miyata, H., Moll, A., Mussa, R., Nakano, E., Nakao, M., Nanut, T., Nisar, N. K., Nishida, S., Okuno, S., Ostrowicz, W., Park, C. W., Park, H., Pedlar, T. K., Pestotnik, R., Petric, M., Piilonen, L. E., Ribezl, E., Ritter, M., Rostomyan, A., Sakai, Y., Sandilya, S., Santelj, L., Sanuki, T., Schneider, O., Schnell, G., Schwanda, C., Semmler, D., Senyo, K., Shebalin, V., Shibata, T. -A., Shiu, J. -G., Shwartz, B., Sibidanov, A., Simon, F., Sohn, Y. -S., Sokolov, A., Staric, M., Steder, M., Sumiyoshi, T., Tamponi, U., Tanida, K., Tatishvili, G., Teramoto, Y., Uchida, M., Uehara, S., Uglov, T., Unno, Y., Uno, S., Urquijo, P., Usov, Y., Vahsen, S. E., Van Hulse, C., Vanhoefer, P., Varner, G., Vinokurova, A., Vorobyev, V., Vossen, A., Wagner, M. N., Wang, C. H., Wang, M. -Z., Wang, P., Wang, X. L., Watanabe, M., Watanabe, Y., Won, E., Yamaoka, J., Yashchenko, S., Yook, Y., Yuan, C. Z., Zhang, Z. P., Zhilich, V., Zhulanov, V., and Belle Collaboration
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High Energy Physics::Experiment - Abstract
Using data samples of 102 x 10(6) gamma(1S) and 158 x 10(6) gamma(2S) events collected with the Belle detector, a first experimental search has been made for double-charmonium production in the exclusive decays gamma(1S, 2S) --> J/psi(psi') + X, where X = eta(c).chi(cJ) (J = 0, 1, 2), eta(c)(2S), X(3940), and X(4160). No significant signal is observed in the spectra of the mass recoiling against the reconstructed J/psi or psi' except for the evidence of chi(c1) production with a significance of 4.6 sigma for gamma(1S) -> J/psi + chi(c1). The measured branching fraction B(gamma(1S) -> J/psi + chi(c1)) is [3.90 +/- 1.21 (stat) +/- 0.23(syst) x 10(-6). The 90% C.L. upper limits on the branching fractions of the other modes having a significance of less than 3 sigma are determined. These results are consistent with theoretical calculations using the nonrelativistic QCD factorization approach.
12. Bone fracture and the interaction between bisphosphonates and proton pump inhibitors: A meta-analysis
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Yang, S. -D, Chen, Q., Wei, H. -K, Feng Zhang, Yang, D. -L, Shen, Y., and Ding, W. -Y
13. Evidence of kappa particle in J / psi ---> anti-K*(892)0 K+ pi
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Bai, J. Z., Ban, Y., Bian, J. G., Cai, X., Chang, J. F., Chen, H. F., Chen, H. S., Chen, Jie, Chen, J. C., Chen, Y. B., Chi, S. P., Chu, Y. P., Cui, X. Z., Dai, Y. S., Dai, Y. M., Dong, L. Y., Du, S. X., Du, Z. Z., Fang, J., Fang, S. S., Fu, C. D., Fu, H. Y., Fu, L. P., Gao, C. S., Gao, M. L., Gao, Y. N., Gong, M. Y., Gong, W. X., Gu, S. D., Guo, Y. N., Guo, Y. Q., Guo, Z. J., Han, S. W., He, J., He, K. L., He, M., He, X., Heng, Y. K., Hong, T., Hu, H. M., Hu, T., Huang, G. S., Huang, L., Huang, X. P., Ji, X. B., Jiang, C. H., Jiang, X. S., Jin, D. P., Jin, S., Jin, Y., Ke, Z. J., Lai, Y. F., Li, F., Li, G., Li, H. H., Li, J., Li, J. C., Li, K., Li, Q. J., Li, R. B., Li, R. Y., Li, W., Li, W. G., Li, X. Q., Li, X. S., Liu, C. F., Liu, C. X., Liu, Fang, Liu, F., Liu, H. M., Liu, J. B., Liu, J. P., Liu, R. G., Liu, Y., Liu, Z. A., Liu, Z. X., Lu, G. R., Lu, F., Lu, H. J., Lu, J. G., Lu, Z. J., Luo, X. L., Ma, E. C., Ma, F. C., Ma, J. M., Mao, Z. P., Meng, X. C., Mo, X. H., Nie, J., Nie, Z. D., Peng, H. P., Qi, N. D., Qian, C. D., Qiu, J. F., Rong, G., Ruan, T. N., Shen, D. L., Shen, H., Shen, X. Y., Sheng, H. Y., Shi, F., Song, L. W., Sun, H. S., Sun, S. S., Sun, Y. Z., Sun, Z. J., Tang, S. Q., Tang, X., Tian, D., Tian, Y. R., Tong, G. L., Wang, J., Wang, J. Z., Wang, L., Wang, L. S., Wang, M., Meng Wang, Wang, P., Wang, P. L., Wang, W. F., Wang, Y. F., Wang, Zhe, Wang, Z., Wang, Zheng, Wang, Z. Y., Wei, C. L., Wu, N., Xia, X. M., Xie, X. X., Xu, G. F., Xu, Y., Xue, S. T., Yan, M. L., Yan, W. B., Yang, G. A., Yang, H. X., Yang, J., Yang, S. D., Ye, M. H., Ye, Y. X., Ying, J., Yu, C. S., Yu, G. W., Yuan, J. M., Yuan, Y., Yue, Q., Zang, S. L., Zeng, Y., Zhang, B. X., Zhang, B. Y., Zhang, C. C., Zhang, D. H., Zhang, H. Y., Zhang, J., Zhang, J. M., Zhang, J. W., Zhang, L. S., Zhang, Q. J., Zhang, S. Q., Zhang, X. Y., Zhang, Yi-Yun, Zhang, Y. J., Zhang, Y. Y., Zhang, Z. P., Zhao, D. X., Zhao, Jia-Wei, Zhao, J. W., Zhao, P. P., Zhao, W. R., Zhao, Y. B., Zhao, Z. G., Zheng, H. Q., Zheng, J. P., Zheng, L. S., Zheng, Z. P., Zhong, X. C., Zhou, B. Q., Zhou, G. M., Zhou, L., Zhou, N. F., Zhu, K. J., Zhu, Q. M., Zhu, Ying-Chun, Zhu, Y. C., Zhu, Y. S., Zhu, Z. A., Zhuang, B. A., and Zou, B. S.
14. Impaired D2 dopamine receptor function in mice lacking type 5 adenylyl cyclase
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Lee, K. -W, Hong, J. -H, Choi, I. Y., Che, Y., Lee, J. -K, Yang, S. -D, Song, C. -W, Kang, H. S., Lee, J. -H, Noh, J. S., Shin, H. -S, and Pyung-Lim Han
15. Observation of a near-threshold enhancement in the pp̄ mass spectrum from radiative J/ψ → γpp̄ decays
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Bai, J. Z., Ban, Y., Bian, J. G., Cai, X., Chang, J. F., Chen, H. F., Chen, H. S., Chen, J., Chen, J. C., Chen, Y. B., Chi, S. P., Chu, Y. P., Cui, X. Z., Dai, Y. M., Dai, Y. S., Dong, L. Y., Du, S. X., Du, Z. Z., Dunwoodie, W., Fang, J., Fang, S. S., Fu, C. D., Fu, H. Y., Fu, L. P., Gao, C. S., Gao, M. L., Gao, Y. N., Gong, M. Y., Gong, W. X., Gu, S. D., Guo, Y. N., Guo, Y. Q., Guo, Z. J., Han, S. W., Harris, F. A., He, J., He, K. L., He, M., He, X., Heng, Y. K., Hong, T., Hu, H. M., Hu, T., Huang, G. S., Huang, L., Huang, X. P., Joseph Izen, Ji, X. B., Jiang, C. H., Jiang, X. S., Jin, D. P., Jin, S., Jin, Y., Jones, B. D., Ke, Z. J., Kong, D., Lai, Y. F., Li, F., Li, G., Li, H. H., Li, J., Li, J. C., Li, K., Li, Q. J., Li, R. B., Li, R. Y., Li, W., Li, W. G., Li, X. Q., Li, X. S., Liu, C. F., Liu, C. X., Liu, F., Liu, H. M., Liu, J. B., Liu, J. P., Liu, R. G., Liu, Y., Liu, Z. A., Liu, Z. X., Lou, X. C., Lu, G. R., Lu, F., Lu, H. J., Lu, J. G., Lu, Z. J., Luo, X. L., Ma, E. C., Ma, F. C., Ma, J. M., Malchow, R., Mao, Z. P., Meng, X. C., Mo, X. H., Nie, J., Nie, Z. D., Olsen, S. L., Paluselli, D., Peng, H. P., Qi, N. D., Qian, C. D., Qiu, J. F., Rong, G., Shen, D. L., Shen, H., Shen, X. Y., Sheng, H. Y., Shi, F., Song, L. W., Sun, H. S., Sun, S. S., Sun, Y. Z., Sun, Z. J., Tang, S. Q., Tang, X., Tian, D., Tian, Y. R., Toki, W., Tong, G. L., Varner, G. S., Wang, J., Wang, J. Z., Wang, L., Wang, L. S., Wang, M., Wang, P., Wang, P. L., Wang, W. F., Wang, Y. F., Wang, Z., Wang, Z. Y., Wei, C. L., Wu, N., Xia, X. M., Xie, X. X., Xu, G. F., Xu, Y., Xue, S. T., Yan, M. L., Yan, W. B., Yang, G. A., Yang, H. X., Yang, J., Yang, S. D., Ye, M. H., Ye, Y. X., Ying, J., Yu, C. S., Yu, G. W., Yuan, C. Z., Yuan, J. M., Yuan, Y., Yue, Q., Zang, S. L., Zeng, Y., Zhang, B. X., Zhang, B. Y., Zhang, C. C., Zhang, D. H., Zhang, H. Y., Zhang, J., Zhang, J. M., Zhang, J. W., Zhang, L. S., Zhang, Q. J., Zhang, S. Q., Zhang, X. Y., Zhang, Y. J., Zhang, Y., Zhang, Y. Y., Zhang, Z. P., Zhao, D. X., Zhao, J., Zhao, J. W., Zhao, P. P., Zhao, W. R., Zhao, Y. B., Zhao, Z. G., Zheng, J. P., Zheng, L. S., Zheng, Z. P., Zhong, X. C., Zhou, B. Q., Zhou, G. M., Zhou, L., Zhou, N. F., Zhu, K. J., Zhu, Q. M., Zhu, Y., Zhu, Y. C., Zhu, Y. S., Zhu, Z. A., Zhuang, B. A., and Zou, B. S.
16. Risk assessment of lower-limb deep vein thrombosis in patients with lumbar spondylolisthesis: A retrospective study
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Liu, S., Yang, S. -D, Yang, D. -L, and Wenyuan Ding
17. Search for XYZ states in Upsilon(1S) inclusive decays
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Shen, C. P., Yuan, C. Z., Ban, Y., Aihara, H., Asner, D. M., Badhrees, I., Bakich, A. M., Barberio, E., Behera, P., Bhardwaj, V., Bhuyan, B., Biswal, J., Bondar, A., Bonvicini, G., Bozek, A., Bracko, M., Browder, T. E., Cervenkov, D., Chekelian, V., Chen, A., Cheon, B. G., Chilikin, K., Chistov, R., Cho, K., Chobanova, V., Choi, S. -K., Choi, Y., Cinabro, D., Dalseno, J., Danilov, M., Dash, N., Di Carlo, S., Dolezal, Z., Drasal, Z., Dutta, D., Eidelman, S., Farhat, H., Fast, J. E., Ferber, T., Fulsom, B. G., Gaur, V., Gabyshev, N., Garmash, A., Goldenzweig, P., Haba, J., Hayasaka, K., Hayashii, H., Hou, W. -S., Iijima, T., Inguglia, G., Ishikawa, A., Itoh, R., Jacobs, W. W., Jeon, H. B., Joo, K. K., Julius, T., Kang, K. H., Kim, D. Y., Kim, J. B., Kim, K. T., Kim, S. H., Kim, Y. J., Kinoshita, K., Kodys, P., Korpar, S., Kotchetkov, D., Krizan, P., Krokovny, P., Kuhr, T., Kuzmin, A., Kwon, Y. -J., Lange, J. S., Li, C. H., Li, H., Li, L., Li, Y., Gioi, L. Li, Libby, J., Liventsev, D., Luo, T., Masuda, M., Matsuda, T., Matvienko, D., Moll, A., Moon, H. K., Mussa, R., Nakao, M., Nanut, T., Nath, K. J., Natkaniec, Z., Nayak, M., Negishi, K., Nishida, S., Ogawa, S., Okuno, S., Olsen, S. L., Pakhlov, P., Pakhlova, G., Pal, B., Pestotnik, R., Petric, M., Piilonen, L. E., Pulvermacher, C., Ritter, M., Rostomyan, A., Sakai, Y., Sandilya, S., Santelj, L., Sanuki, T., Savinov, V., Schlueter, T., Schneider, O., Schnell, G., Schwanda, C., Seino, Y., Senyo, K., Seon, O., Seong, I. S., Sevior, M. E., Shibata, T. -A., Shiu, J. -G., Simon, F., Sokolov, A., Solovieva, E., Staric, M., Sumiyoshi, T., Takizawa, M., Tanida, K., Tenchini, F., Trabelsi, K., Uchida, M., Uglov, T., Unno, Y., Uno, S., Varner, G., Vinokurova, A., Vorobyev, V., Wang, C. H., Wang, M. -Z., Wang, P., Wang, X. L., Watanabe, M., Watanabe, Y., Williams, K. M., Won, E., Yamaoka, J., Yang, S. D., Yashchenko, S., Yook, Y., Yusa, Y., Zhang, Z. P., Zhilich, V., Zhukova, V., Zhulanov, V., Zupanc, A., and Belle Collaboration
- Subjects
High Energy Physics::Experiment - Abstract
The branching fractions of the Upsilon(1S) inclusive decays into final states with a J/psi or psi(2S) are measured with improved precision to be B Upsilon(1S) -> J/psi + anything = (5.25 +/- 0.13(stat) +/- 0.25(syst) x 10(-4) and B Upsilon(1S) -> psi(2S) + anything = (1.23 +/- 0.17(stat) +/- 0.11(syst)) x 10(-4). The first search for Upsilon(1S) decays into XYZ states that decay into a J/psi or a psi(2S) plus one or two charged tracks yields no significant signals for XYZ states in any of the examined decay modes, and upper limits on their production rates in Upsilon(1S) inclusive decays are determined.
18. Correlative analyses of isolated upper lumbar disc herniation and adjacent wedge-shaped vertebrae
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Xu, J. -X, Yang, S. -D, Wang, B. -L, Yang, D. -L, Wenyuan Ding, and Shen, Y.
19. Levofloxacin increases apoptosis of rat annulus fibrosus cells via the mechanism of upregulating MMP-2 and MMP-13
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Wei, H. -K, Yang, S. -D, Bai, Z. -L, Zhang, X., Yang, D. -L, and Wenyuan Ding
Catalog
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