Automated Author ProfileOsipenko, M.
Osipenko, M.
Current S-Index
Sum of Dataset Indices for all datasets
Average Dataset Index per Dataset
Average Dataset Index per dataset
Total Datasets
Total datasets for this author
Average FAIR Score
Average FAIR Score per dataset
Total Citations
Total citations to the author's datasets
Total Mentions
Total mentions of the author's datasets
S-Index Interpretation
The S-Index (Sharing Index) is a comprehensive metric that represents the cumulative impact of all your datasets. It is calculated as the sum of Dataset Index scores across all your claimed datasets.
What it means:
- A higher S-index indicates greater overall impact of your datasets relative to typical datasets in their fields of research
- The S-Index grows as you add more datasets or as existing datasets gain more citations and mentions
- It provides a single number to track your research data impact over time
Current S-Index: 3.9 (sum of 10 datasets Dataset Index scores)
More information here.
S-Index Over Time
Cumulative Citations Over Time
Cumulative Mentions Over Time
Datasets
Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (1) covers the proton data for the W range from 1.1300 to 1.6300 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (2) covers the proton data for the W range from 1.6500 to 1.1300 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (3) covers the deuteron data for the W range from 1.0850 to 1.3450 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (4) covers the deuteron data for the W range from 1.3550 to 1.6350 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (5) covers the deuteron data for the W range from 1.6450 to 2.0650 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (6) covers the deuteron data for the W range from 2.0750 to 2.7950 GeV.
Authors
- Dharmawardane, K.V. ;
- Kuhn, S.E. ;
- Bosted, Peter E. ;
- Prok, Y. ;
- Adams, G. ;
- Ambrozewicz, P. ;
- Anghinolfi, M. ;
- Asryan, G. ;
- Avakian, H. ;
- Baghdasaryan, Hovhannes ;
- Baillie, N. ;
- Ball, J.P. ;
- Baltzell, N.A. ;
- Barrow, S. ;
- Batourine, V. ;
- Battaglieri, M. ;
- Beard, K. ;
- Bedlinskiy, Ivan ;
- Bektasoglu, M. ;
- Bellis, M. ;
- Benmouna, N. ;
- Biselli, Angela S. ;
- Bonner, B.E. ;
- Bouchigny, S. ;
- Boiarinov, S. ;
- Bradford, R. ;
- Branford, D. ;
- Brooks, W.K. ;
- Bultmann, S. ;
- Burkert, V.D. ;
- Butuceanu, C. ;
- Calarco, J.R. ;
- Careccia, S.L. ;
- Carman, D.S. ;
- Carnahan, B. ;
- Cazes, A. ;
- Chen, S. ;
- Cole, P.L. ;
- Collins, P. ;
- Coltharp, P. ;
- Cords, D. ;
- Corvisiero, P. ;
- Crabb, D. ;
- Crannell, H. ;
- Crede, V. ;
- Cummings, J.P. ;
- De Masi, R. ;
- DeVita, R. ;
- De Sanctis, E. ;
- Degtyarenko, P.V. ;
- Denizli, H. ;
- Dennis, L. ;
- Deur, A. ;
- Djalali, C. ;
- Dodge, G.E. ;
- Donnelly, J. ;
- Doughty, D. ;
- Dragovitsch, P. ;
- Dugger, M. ;
- Dytman, S. ;
- Dzyubak, O.P. ;
- Egiyan, H. ;
- Egiyan, K.S. ;
- Elouadrhiri, L. ;
- Eugenio, P. ;
- Fatemi, R. ;
- Fedotov, G. ;
- Feuerbach, R.J. ;
- Forest, T.A. ;
- Funsten, H. ;
- Garc Con, M. ;
- Gavalian, G. ;
- Gilfoyle, G.P. ;
- Giovanetti, K.L. ;
- Girod, F.X. ;
- Goetz, J.T. ;
- Golovatch, E. ;
- Gonenc, A. ;
- Gothe, R.W. ;
- Griffioen, K.A. ;
- Guidal, M. ;
- Guillo, M. ;
- Guler, Nevzat ;
- Guo, L. ;
- Gyurjyan, V. ;
- Hadjidakis, C. ;
- Hafidi, K. ;
- Hakobyan, R.S. ;
- Hardie, J. ;
- Heddle, D. ;
- Hersman, F.W. ;
- Hicks, K. ;
- Hleiqawi, I. ;
- Holtrop, M. ;
- Huertas, M. ;
- Hyde, Charles Earl ;
- Ilieva, Y. ;
- Ireland, D.G. ;
- Ishkhanov, B.S. ;
- Isupov, E.L. ;
- Ito, M.M. ;
- Jenkins, David A. ;
- Jo, H.S. ;
- Joo, K. ;
- Juengst, H.G. ;
- Keith, C. ;
- Kellie, J.D. ;
- Khandaker, M. ;
- Kim, K.Y. ;
- Kim, K. ;
- Kim, W. ;
- Klein, A. ;
- Klein, F.J. ;
- Klusman, M. ;
- Kossov, M. ;
- Kramer, L.H. ;
- Kubarovsky, V. ;
- Kuhn, Joachim ;
- Kuleshov, S.V. ;
- Lachniet, J. ;
- Laget, J.M. ;
- Langheinrich, J. ;
- Lawrence, D. ;
- Lima, A.C.S. ;
- Livingston, K. ;
- Lu, H. ;
- Lukashin, K. ;
- MacCormick, M. ;
- Manak, J.J. ;
- Markov, N. ;
- McAleer, S. ;
- McKinnon, B. ;
- McNabb, J.W.C. ;
- Mecking, B.A. ;
- Mestayer, M.D. ;
- Meyer, C.A. ;
- Mibe, T. ;
- Mikhailov, K. ;
- Minehart, R. ;
- Mirazita, M. ;
- Miskimen, R. ;
- Mokeev, V. ;
- Morand, L. ;
- Morrow, S.A. ;
- Moteabbed, M. ;
- Mueller, J. ;
- Mutchler, G.S. ;
- Nadel-Turonski, P. ;
- Napolitano, J. ;
- Nasseripour, R. ;
- Niccolai, S. ;
- Niculescu, G. ;
- Niculescu, I. ;
- Niczyporuk, B.B. ;
- Niroula, M.R. ;
- Niyazov, R.A. ;
- Nozar, M. ;
- O'Rielly, G.V. ;
- Osipenko, M. ;
- Ostrovidov, A.I. ;
- Park, K. ;
- Pasyuk, E. ;
- Paterson, C. ;
- Philips, S.A. ;
- Pierce, J. ;
- Pivnyuk, N. ;
- Pocanic, D. ;
- Pogorelko, O. ;
- Polli, E. ;
- Pozdniakov, S. ;
- Preedom, B.M. ;
- Price, J.W. ;
- Protopopescu, D. ;
- Qin, L.M. ;
- Raue, B.A. ;
- Riccardi, G. ;
- Ricco, G. ;
- Ripani, M. ;
- Ritchie, B.G. ;
- Ronchetti, F. ;
- Rosner, G. ;
- Rossi, P. ;
- Rowntree, D. ;
- Rubin, P.D. ;
- Sabatie, F. ;
- Salgado, C. ;
- Santoro, J.P. ;
- Sapunenko, V. ;
- Schumacher, R.A. ;
- Serov, V.S. ;
- Sharabian, Y.G. ;
- Shaw, J. ;
- Shvedunov, N.V. ;
- Skabelin, A.V. ;
- Smith, E.S. ;
- Smith, L.C. ;
- Sober, D.I. ;
- Stavinsky, A. ;
- Stepanyan, S.S. ;
- Stepanyan, S. ;
- Stokes, B.E. ;
- Stoler, P. ;
- Strakovsky, I.I. ;
- Strauch, S. ;
- Suleiman, R. ;
- Taiuti, M. ;
- Taylor, S. ;
- Tedeschi, D.J. ;
- Thoma, U. ;
- Thompson, R. ;
- Tkabladze, A. ;
- Tkachenko, S. ;
- Todor, L. ;
- Tur, C. ;
- Ungaro, M. ;
- Vineyard, M.F. ;
- Vlassov, A.V. ;
- Weinstein, L.B. ;
- Weygand, D.P. ;
- Williams, M. ;
- Wolin, E. ;
- Wood, M.H. ;
- Yegneswaran, A. ;
- Yun, J. ;
- Zana, L. ;
- Zhang, J. ;
- Zhao, B. ;
- Zhao, Z.
Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (1) contains the structure function data for Q2 = 0.30 and 0.40 GeV2.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (2) contains the structure function data for Q2 = 0.50 and 0.60 GeV2.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (3) covers the absolute cross sections in the W region 1.110 to 1.150 GeV.. Numerical values supplied by H Egiyan.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (4) covers the absolute cross sections in the W region 1.170 to 1.210 GeV.. Numerical values supplied by H Egiyan.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (5) covers the absolute cross sections in the W region 1.230 to 1.270 GeV.. Numerical values supplied by H Egiyan.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (6) covers the absolute cross sections in the W region 1.290 to 1.330 GeV.. Numerical values supplied by H Egiyan.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (7) covers the absolute cross sections in the W region 1.350 to 1.390 GeV.. Numerical values supplied by H Egiyan.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (8) covers the absolute cross sections in the W region 1.410 to 1.450 GeV.. Numerical values supplied by H Egiyan.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (9) covers the absolute cross sections in the W region 1.470 to 1.510 GeV.. Numerical values supplied by H Egiyan.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (10) covers the absolute cross sections in the W region 1.530 to1.570 GeV.. Numerical values supplied by H Egiyan.
Authors
- Egiyan, H. ;
- Aznauryan, I.G. ;
- Burkert, V.D. ;
- Griffioen, K.A. ;
- Joo, K. ;
- Minehart, R. ;
- Smith, L.C. ;
- Adams, G. ;
- Ambrozewicz, P. ;
- Anciant, E. ;
- Anghinolfi, M. ;
- Asavapibhop, B. ;
- Audit, G. ;
- Auger, T. ;
- Avakian, H. ;
- Baghdasaryan, Hovhannes ;
- Ball, J.P. ;
- Baltzel, N. ;
- Barrow, S. ;
- Battaglieri, M. ;
- Beard, K. ;
- Bektasoglu, M. ;
- Bellis, M. ;
- Benmouna, N. ;
- Bianchi, N. ;
- Biselli, Angela S. ;
- Boiarinov, S. ;
- Bonner, B.E. ;
- Bouchigny, S. ;
- Bradford, R. ;
- Branford, D. ;
- Briscoe, W.J. ;
- Brooks, W.K. ;
- Butuceanu, C. ;
- Calarco, J.R. ;
- Careccia, S.L. ;
- Carman, D.S. ;
- Carnahan, B. ;
- Cetina, C. ;
- Chen, S. ;
- Cole, P.L. ;
- Coleman, A. ;
- Cords, D. ;
- Corvisiero, P. ;
- Crabb, D. ;
- Crannell, H. ;
- Cummings, J.P. ;
- DeSanctis, E. ;
- DeVita, R. ;
- Degtyarenko, P.V. ;
- Denizli, H. ;
- Dennis, L. ;
- Dharmawardane, K.V. ;
- Djalali, C. ;
- Dodge, G.E. ;
- Donnely, J. ;
- Doughty, D. ;
- Dragovitsch, P. ;
- Dugger, M. ;
- Dytman, S. ;
- Dzyubak, O.P. ;
- Eckhause, M. ;
- Egiyan, K.S. ;
- Elouadrhiri, L. ;
- Empl, A. ;
- Eugenio, P. ;
- Fatemi, R. ;
- Fedotov, G. ;
- Feldman, G. ;
- Feuerbach, R.J. ;
- Forest, T.A. ;
- Funsten, H. ;
- Gaff, S.J. ;
- Gai, M. ;
- Gavalian, G. ;
- Gilad, S. ;
- Gilfoyle, G.P. ;
- Giovanetti, K.L. ;
- Girard, P. ;
- Goetz, G.T. ;
- Gordon, C.I.O. ;
- Gothe, R. ;
- Guidal, M. ;
- Guillo, M. ;
- Guler, Nevzat ;
- Guo, L. ;
- Gyurjyan, V. ;
- Hadjidakis, C. ;
- Hakobyan, R.S. ;
- Hardie, J. ;
- Heddle, D. ;
- Hersman, F.W. ;
- Hicks, K. ;
- Hicks, R.S. ;
- Hleiqawi, I. ;
- Holtrop, M. ;
- Hu, J. ;
- Hyde, Charles Earl ;
- Ilieva, Y. ;
- Ireland, D.G. ;
- Ishkhanov, B. ;
- Ito, M.M. ;
- Jenkins, David A. ;
- Juengst, Henry G. ;
- Kelley, J.H. ;
- Kellie, J.D. ;
- Khandaker, M. ;
- Kim, D.H. ;
- Kim, K.Y. ;
- Kim, K. ;
- Kim, M.S. ;
- Kim, W. ;
- Klein, A. ;
- Klein, F.J. ;
- Klimenko, A.V. ;
- Klusman, M. ;
- Kossov, M. ;
- Kramer, L.H. ;
- Kuang, Y. ;
- Kubarovsky, V. ;
- Kuhn, S.E. ;
- Kuhn, Joachim ;
- Lachniet, J. ;
- Laget, J.M. ;
- Langheinrich, J. ;
- Lawrence, D. ;
- Livingston, K. ;
- Longhi, A. ;
- Lukashin, K. ;
- Manak, J.J. ;
- Marchand, C. ;
- McAleer, S. ;
- McKinnon, B. ;
- McNabb, J.W.C. ;
- Mecking, B.A. ;
- Mehrabyan, S. ;
- Melone, J.J. ;
- Mestayer, M.D. ;
- Meyer, C.A. ;
- Mikhailov, K. ;
- Mirazita, M. ;
- Miskimen, R. ;
- Mokeev, V. ;
- Morand, L. ;
- Morrow, S.A. ;
- Muccifora, V. ;
- Mueller, J. ;
- Murphy, L.Y. ;
- Mutchler, G.S. ;
- Napolitano, J. ;
- Nasseripour, R. ;
- Nelson, S.O. ;
- Niccolai, S. ;
- Niculescu, G. ;
- Niculescu, I. ;
- Niczyporuk, B.B. ;
- Niyazov, R.A. ;
- Nozar, M. ;
- O'Rielly, G.V. ;
- Osipenko, M. ;
- Park, K. ;
- Pasyuk, E. ;
- Peterson, G. ;
- Philips, S.A. ;
- Pivnyuk, N. ;
- Pocanic, D. ;
- Pogorelko, O. ;
- Polli, E. ;
- Pozdniakov, S. ;
- Preedom, B.M. ;
- Price, J.W. ;
- Prok, Y. ;
- Protopopescu, D. ;
- Qin, L.M. ;
- Raue, B.A. ;
- Riccardi, G. ;
- Ricco, G. ;
- Ripani, M. ;
- Ritchie, B.G. ;
- Ronchetti, F. ;
- Rosner, G. ;
- Rossi, P. ;
- Rowntree, D. ;
- Rubin, P.D. ;
- Sabatie, F. ;
- Sabourov, K. ;
- Salgado, C. ;
- Santoro, J.P. ;
- Sapunenko, V. ;
- Sargsyan, M. ;
- Schumacher, R.A. ;
- Serov, V.S. ;
- Shafi, A. ;
- Sharabian, Y.G. ;
- Shaw, J. ;
- Simionatto, S. ;
- Skabelin, A.V. ;
- Smith, E.S. ;
- Sober, D.I. ;
- Spraker, M. ;
- Stavinsky, A. ;
- Stepanyan, S. ;
- Stoler, P. ;
- Strakovsky, I.I. ;
- Strauch, S. ;
- Taiuti, M. ;
- Taylor, S. ;
- Tedeschi, D.J. ;
- Thoma, U. ;
- Thompson, R. ;
- Tkabladze, A. ;
- Todor, L. ;
- Tur, C. ;
- Ungaro, M. ;
- Vineyard, M.F. ;
- Vlassov, A.V. ;
- Wang, K. ;
- Weinstein, L.B. ;
- Weller, H. ;
- Weygand, D.P. ;
- Whisnant, C.S. ;
- Wolin, E. ;
- Wood, M.H. ;
- Yegneswaran, A. ;
- Yun, J. ;
- Zhang, J. ;
- Zhao, J. ;
- Zhou, Z.
Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (1) contains the structure function data for Q2 = 0.30 and 0.40 GeV2.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (2) contains the structure function data for Q2 = 0.50 and 0.60 GeV2.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (3) covers the absolute cross sections in the W region 1.110 to 1.150 GeV.. Numerical values supplied by H Egiyan.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (4) covers the absolute cross sections in the W region 1.170 to 1.210 GeV.. Numerical values supplied by H Egiyan.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (5) covers the absolute cross sections in the W region 1.230 to 1.270 GeV.. Numerical values supplied by H Egiyan.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (6) covers the absolute cross sections in the W region 1.290 to 1.330 GeV.. Numerical values supplied by H Egiyan.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (7) covers the absolute cross sections in the W region 1.350 to 1.390 GeV.. Numerical values supplied by H Egiyan.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (8) covers the absolute cross sections in the W region 1.410 to 1.450 GeV.. Numerical values supplied by H Egiyan.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (9) covers the absolute cross sections in the W region 1.470 to 1.510 GeV.. Numerical values supplied by H Egiyan.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (10) covers the absolute cross sections in the W region 1.530 to1.570 GeV.. Numerical values supplied by H Egiyan.
Authors
- Egiyan, H. ;
- Aznauryan, I.G. ;
- Burkert, V.D. ;
- Griffioen, K.A. ;
- Joo, K. ;
- Minehart, R. ;
- Smith, L.C. ;
- Adams, G. ;
- Ambrozewicz, P. ;
- Anciant, E. ;
- Anghinolfi, M. ;
- Asavapibhop, B. ;
- Audit, G. ;
- Auger, T. ;
- Avakian, H. ;
- Baghdasaryan, Hovhannes ;
- Ball, J.P. ;
- Baltzel, N. ;
- Barrow, S. ;
- Battaglieri, M. ;
- Beard, K. ;
- Bektasoglu, M. ;
- Bellis, M. ;
- Benmouna, N. ;
- Bianchi, N. ;
- Biselli, Angela S. ;
- Boiarinov, S. ;
- Bonner, B.E. ;
- Bouchigny, S. ;
- Bradford, R. ;
- Branford, D. ;
- Briscoe, W.J. ;
- Brooks, W.K. ;
- Butuceanu, C. ;
- Calarco, J.R. ;
- Careccia, S.L. ;
- Carman, D.S. ;
- Carnahan, B. ;
- Cetina, C. ;
- Chen, S. ;
- Cole, P.L. ;
- Coleman, A. ;
- Cords, D. ;
- Corvisiero, P. ;
- Crabb, D. ;
- Crannell, H. ;
- Cummings, J.P. ;
- DeSanctis, E. ;
- DeVita, R. ;
- Degtyarenko, P.V. ;
- Denizli, H. ;
- Dennis, L. ;
- Dharmawardane, K.V. ;
- Djalali, C. ;
- Dodge, G.E. ;
- Donnely, J. ;
- Doughty, D. ;
- Dragovitsch, P. ;
- Dugger, M. ;
- Dytman, S. ;
- Dzyubak, O.P. ;
- Eckhause, M. ;
- Egiyan, K.S. ;
- Elouadrhiri, L. ;
- Empl, A. ;
- Eugenio, P. ;
- Fatemi, R. ;
- Fedotov, G. ;
- Feldman, G. ;
- Feuerbach, R.J. ;
- Forest, T.A. ;
- Funsten, H. ;
- Gaff, S.J. ;
- Gai, M. ;
- Gavalian, G. ;
- Gilad, S. ;
- Gilfoyle, G.P. ;
- Giovanetti, K.L. ;
- Girard, P. ;
- Goetz, G.T. ;
- Gordon, C.I.O. ;
- Gothe, R. ;
- Guidal, M. ;
- Guillo, M. ;
- Guler, Nevzat ;
- Guo, L. ;
- Gyurjyan, V. ;
- Hadjidakis, C. ;
- Hakobyan, R.S. ;
- Hardie, J. ;
- Heddle, D. ;
- Hersman, F.W. ;
- Hicks, K. ;
- Hicks, R.S. ;
- Hleiqawi, I. ;
- Holtrop, M. ;
- Hu, J. ;
- Hyde, Charles Earl ;
- Ilieva, Y. ;
- Ireland, D.G. ;
- Ishkhanov, B. ;
- Ito, M.M. ;
- Jenkins, David A. ;
- Juengst, Henry G. ;
- Kelley, J.H. ;
- Kellie, J.D. ;
- Khandaker, M. ;
- Kim, D.H. ;
- Kim, K.Y. ;
- Kim, K. ;
- Kim, M.S. ;
- Kim, W. ;
- Klein, A. ;
- Klein, F.J. ;
- Klimenko, A.V. ;
- Klusman, M. ;
- Kossov, M. ;
- Kramer, L.H. ;
- Kuang, Y. ;
- Kubarovsky, V. ;
- Kuhn, S.E. ;
- Kuhn, Joachim ;
- Lachniet, J. ;
- Laget, J.M. ;
- Langheinrich, J. ;
- Lawrence, D. ;
- Livingston, K. ;
- Longhi, A. ;
- Lukashin, K. ;
- Manak, J.J. ;
- Marchand, C. ;
- McAleer, S. ;
- McKinnon, B. ;
- McNabb, J.W.C. ;
- Mecking, B.A. ;
- Mehrabyan, S. ;
- Melone, J.J. ;
- Mestayer, M.D. ;
- Meyer, C.A. ;
- Mikhailov, K. ;
- Mirazita, M. ;
- Miskimen, R. ;
- Mokeev, V. ;
- Morand, L. ;
- Morrow, S.A. ;
- Muccifora, V. ;
- Mueller, J. ;
- Murphy, L.Y. ;
- Mutchler, G.S. ;
- Napolitano, J. ;
- Nasseripour, R. ;
- Nelson, S.O. ;
- Niccolai, S. ;
- Niculescu, G. ;
- Niculescu, I. ;
- Niczyporuk, B.B. ;
- Niyazov, R.A. ;
- Nozar, M. ;
- O'Rielly, G.V. ;
- Osipenko, M. ;
- Park, K. ;
- Pasyuk, E. ;
- Peterson, G. ;
- Philips, S.A. ;
- Pivnyuk, N. ;
- Pocanic, D. ;
- Pogorelko, O. ;
- Polli, E. ;
- Pozdniakov, S. ;
- Preedom, B.M. ;
- Price, J.W. ;
- Prok, Y. ;
- Protopopescu, D. ;
- Qin, L.M. ;
- Raue, B.A. ;
- Riccardi, G. ;
- Ricco, G. ;
- Ripani, M. ;
- Ritchie, B.G. ;
- Ronchetti, F. ;
- Rosner, G. ;
- Rossi, P. ;
- Rowntree, D. ;
- Rubin, P.D. ;
- Sabatie, F. ;
- Sabourov, K. ;
- Salgado, C. ;
- Santoro, J.P. ;
- Sapunenko, V. ;
- Sargsyan, M. ;
- Schumacher, R.A. ;
- Serov, V.S. ;
- Shafi, A. ;
- Sharabian, Y.G. ;
- Shaw, J. ;
- Simionatto, S. ;
- Skabelin, A.V. ;
- Smith, E.S. ;
- Sober, D.I. ;
- Spraker, M. ;
- Stavinsky, A. ;
- Stepanyan, S. ;
- Stoler, P. ;
- Strakovsky, I.I. ;
- Strauch, S. ;
- Taiuti, M. ;
- Taylor, S. ;
- Tedeschi, D.J. ;
- Thoma, U. ;
- Thompson, R. ;
- Tkabladze, A. ;
- Todor, L. ;
- Tur, C. ;
- Ungaro, M. ;
- Vineyard, M.F. ;
- Vlassov, A.V. ;
- Wang, K. ;
- Weinstein, L.B. ;
- Weller, H. ;
- Weygand, D.P. ;
- Whisnant, C.S. ;
- Wolin, E. ;
- Wood, M.H. ;
- Yegneswaran, A. ;
- Yun, J. ;
- Zhang, J. ;
- Zhao, J. ;
- Zhou, Z.
Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (1) covers the proton data for the W range from 1.1300 to 1.6300 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (2) covers the proton data for the W range from 1.6500 to 1.1300 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (3) covers the deuteron data for the W range from 1.0850 to 1.3450 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (4) covers the deuteron data for the W range from 1.3550 to 1.6350 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (5) covers the deuteron data for the W range from 1.6450 to 2.0650 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (6) covers the deuteron data for the W range from 2.0750 to 2.7950 GeV.
Authors
- Dharmawardane, K.V. ;
- Kuhn, S.E. ;
- Bosted, Peter E. ;
- Prok, Y. ;
- Adams, G. ;
- Ambrozewicz, P. ;
- Anghinolfi, M. ;
- Asryan, G. ;
- Avakian, H. ;
- Baghdasaryan, Hovhannes ;
- Baillie, N. ;
- Ball, J.P. ;
- Baltzell, N.A. ;
- Barrow, S. ;
- Batourine, V. ;
- Battaglieri, M. ;
- Beard, K. ;
- Bedlinskiy, Ivan ;
- Bektasoglu, M. ;
- Bellis, M. ;
- Benmouna, N. ;
- Biselli, Angela S. ;
- Bonner, B.E. ;
- Bouchigny, S. ;
- Boiarinov, S. ;
- Bradford, R. ;
- Branford, D. ;
- Brooks, W.K. ;
- Bultmann, S. ;
- Burkert, V.D. ;
- Butuceanu, C. ;
- Calarco, J.R. ;
- Careccia, S.L. ;
- Carman, D.S. ;
- Carnahan, B. ;
- Cazes, A. ;
- Chen, S. ;
- Cole, P.L. ;
- Collins, P. ;
- Coltharp, P. ;
- Cords, D. ;
- Corvisiero, P. ;
- Crabb, D. ;
- Crannell, H. ;
- Crede, V. ;
- Cummings, J.P. ;
- De Masi, R. ;
- DeVita, R. ;
- De Sanctis, E. ;
- Degtyarenko, P.V. ;
- Denizli, H. ;
- Dennis, L. ;
- Deur, A. ;
- Djalali, C. ;
- Dodge, G.E. ;
- Donnelly, J. ;
- Doughty, D. ;
- Dragovitsch, P. ;
- Dugger, M. ;
- Dytman, S. ;
- Dzyubak, O.P. ;
- Egiyan, H. ;
- Egiyan, K.S. ;
- Elouadrhiri, L. ;
- Eugenio, P. ;
- Fatemi, R. ;
- Fedotov, G. ;
- Feuerbach, R.J. ;
- Forest, T.A. ;
- Funsten, H. ;
- Garc Con, M. ;
- Gavalian, G. ;
- Gilfoyle, G.P. ;
- Giovanetti, K.L. ;
- Girod, F.X. ;
- Goetz, J.T. ;
- Golovatch, E. ;
- Gonenc, A. ;
- Gothe, R.W. ;
- Griffioen, K.A. ;
- Guidal, M. ;
- Guillo, M. ;
- Guler, Nevzat ;
- Guo, L. ;
- Gyurjyan, V. ;
- Hadjidakis, C. ;
- Hafidi, K. ;
- Hakobyan, R.S. ;
- Hardie, J. ;
- Heddle, D. ;
- Hersman, F.W. ;
- Hicks, K. ;
- Hleiqawi, I. ;
- Holtrop, M. ;
- Huertas, M. ;
- Hyde, Charles Earl ;
- Ilieva, Y. ;
- Ireland, D.G. ;
- Ishkhanov, B.S. ;
- Isupov, E.L. ;
- Ito, M.M. ;
- Jenkins, David A. ;
- Jo, H.S. ;
- Joo, K. ;
- Juengst, H.G. ;
- Keith, C. ;
- Kellie, J.D. ;
- Khandaker, M. ;
- Kim, K.Y. ;
- Kim, K. ;
- Kim, W. ;
- Klein, A. ;
- Klein, F.J. ;
- Klusman, M. ;
- Kossov, M. ;
- Kramer, L.H. ;
- Kubarovsky, V. ;
- Kuhn, Joachim ;
- Kuleshov, S.V. ;
- Lachniet, J. ;
- Laget, J.M. ;
- Langheinrich, J. ;
- Lawrence, D. ;
- Lima, A.C.S. ;
- Livingston, K. ;
- Lu, H. ;
- Lukashin, K. ;
- MacCormick, M. ;
- Manak, J.J. ;
- Markov, N. ;
- McAleer, S. ;
- McKinnon, B. ;
- McNabb, J.W.C. ;
- Mecking, B.A. ;
- Mestayer, M.D. ;
- Meyer, C.A. ;
- Mibe, T. ;
- Mikhailov, K. ;
- Minehart, R. ;
- Mirazita, M. ;
- Miskimen, R. ;
- Mokeev, V. ;
- Morand, L. ;
- Morrow, S.A. ;
- Moteabbed, M. ;
- Mueller, J. ;
- Mutchler, G.S. ;
- Nadel-Turonski, P. ;
- Napolitano, J. ;
- Nasseripour, R. ;
- Niccolai, S. ;
- Niculescu, G. ;
- Niculescu, I. ;
- Niczyporuk, B.B. ;
- Niroula, M.R. ;
- Niyazov, R.A. ;
- Nozar, M. ;
- O'Rielly, G.V. ;
- Osipenko, M. ;
- Ostrovidov, A.I. ;
- Park, K. ;
- Pasyuk, E. ;
- Paterson, C. ;
- Philips, S.A. ;
- Pierce, J. ;
- Pivnyuk, N. ;
- Pocanic, D. ;
- Pogorelko, O. ;
- Polli, E. ;
- Pozdniakov, S. ;
- Preedom, B.M. ;
- Price, J.W. ;
- Protopopescu, D. ;
- Qin, L.M. ;
- Raue, B.A. ;
- Riccardi, G. ;
- Ricco, G. ;
- Ripani, M. ;
- Ritchie, B.G. ;
- Ronchetti, F. ;
- Rosner, G. ;
- Rossi, P. ;
- Rowntree, D. ;
- Rubin, P.D. ;
- Sabatie, F. ;
- Salgado, C. ;
- Santoro, J.P. ;
- Sapunenko, V. ;
- Schumacher, R.A. ;
- Serov, V.S. ;
- Sharabian, Y.G. ;
- Shaw, J. ;
- Shvedunov, N.V. ;
- Skabelin, A.V. ;
- Smith, E.S. ;
- Smith, L.C. ;
- Sober, D.I. ;
- Stavinsky, A. ;
- Stepanyan, S.S. ;
- Stepanyan, S. ;
- Stokes, B.E. ;
- Stoler, P. ;
- Strakovsky, I.I. ;
- Strauch, S. ;
- Suleiman, R. ;
- Taiuti, M. ;
- Taylor, S. ;
- Tedeschi, D.J. ;
- Thoma, U. ;
- Thompson, R. ;
- Tkabladze, A. ;
- Tkachenko, S. ;
- Todor, L. ;
- Tur, C. ;
- Ungaro, M. ;
- Vineyard, M.F. ;
- Vlassov, A.V. ;
- Weinstein, L.B. ;
- Weygand, D.P. ;
- Williams, M. ;
- Wolin, E. ;
- Wood, M.H. ;
- Yegneswaran, A. ;
- Yun, J. ;
- Zana, L. ;
- Zhang, J. ;
- Zhao, B. ;
- Zhao, Z.
Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (1) contains the structure function data for Q2 = 0.30 and 0.40 GeV2.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (2) contains the structure function data for Q2 = 0.50 and 0.60 GeV2.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (3) covers the absolute cross sections in the W region 1.110 to 1.150 GeV.. Numerical values supplied by H Egiyan.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (4) covers the absolute cross sections in the W region 1.170 to 1.210 GeV.. Numerical values supplied by H Egiyan.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (5) covers the absolute cross sections in the W region 1.230 to 1.270 GeV.. Numerical values supplied by H Egiyan.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (6) covers the absolute cross sections in the W region 1.290 to 1.330 GeV.. Numerical values supplied by H Egiyan.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (7) covers the absolute cross sections in the W region 1.350 to 1.390 GeV.. Numerical values supplied by H Egiyan.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (8) covers the absolute cross sections in the W region 1.410 to 1.450 GeV.. Numerical values supplied by H Egiyan.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (9) covers the absolute cross sections in the W region 1.470 to 1.510 GeV.. Numerical values supplied by H Egiyan.Jefferson Lab - CEBAF. Measurement of the absolute cross sections and combinations of longitudinal and transverse structure functions in the electroproduction reaction E- P --& gt; E- PI+ N in the first and second nucleon resonance regions. The experiment uses an incident electron beam of energy 1.5 GeV and covers theQ2 range 0.25 to 0.65 GeV2.. This part (10) covers the absolute cross sections in the W region 1.530 to1.570 GeV.. Numerical values supplied by H Egiyan.
Authors
- Egiyan, H. ;
- Aznauryan, I.G. ;
- Burkert, V.D. ;
- Griffioen, K.A. ;
- Joo, K. ;
- Minehart, R. ;
- Smith, L.C. ;
- Adams, G. ;
- Ambrozewicz, P. ;
- Anciant, E. ;
- Anghinolfi, M. ;
- Asavapibhop, B. ;
- Audit, G. ;
- Auger, T. ;
- Avakian, H. ;
- Baghdasaryan, Hovhannes ;
- Ball, J.P. ;
- Baltzel, N. ;
- Barrow, S. ;
- Battaglieri, M. ;
- Beard, K. ;
- Bektasoglu, M. ;
- Bellis, M. ;
- Benmouna, N. ;
- Bianchi, N. ;
- Biselli, Angela S. ;
- Boiarinov, S. ;
- Bonner, B.E. ;
- Bouchigny, S. ;
- Bradford, R. ;
- Branford, D. ;
- Briscoe, W.J. ;
- Brooks, W.K. ;
- Butuceanu, C. ;
- Calarco, J.R. ;
- Careccia, S.L. ;
- Carman, D.S. ;
- Carnahan, B. ;
- Cetina, C. ;
- Chen, S. ;
- Cole, P.L. ;
- Coleman, A. ;
- Cords, D. ;
- Corvisiero, P. ;
- Crabb, D. ;
- Crannell, H. ;
- Cummings, J.P. ;
- DeSanctis, E. ;
- DeVita, R. ;
- Degtyarenko, P.V. ;
- Denizli, H. ;
- Dennis, L. ;
- Dharmawardane, K.V. ;
- Djalali, C. ;
- Dodge, G.E. ;
- Donnely, J. ;
- Doughty, D. ;
- Dragovitsch, P. ;
- Dugger, M. ;
- Dytman, S. ;
- Dzyubak, O.P. ;
- Eckhause, M. ;
- Egiyan, K.S. ;
- Elouadrhiri, L. ;
- Empl, A. ;
- Eugenio, P. ;
- Fatemi, R. ;
- Fedotov, G. ;
- Feldman, G. ;
- Feuerbach, R.J. ;
- Forest, T.A. ;
- Funsten, H. ;
- Gaff, S.J. ;
- Gai, M. ;
- Gavalian, G. ;
- Gilad, S. ;
- Gilfoyle, G.P. ;
- Giovanetti, K.L. ;
- Girard, P. ;
- Goetz, G.T. ;
- Gordon, C.I.O. ;
- Gothe, R. ;
- Guidal, M. ;
- Guillo, M. ;
- Guler, Nevzat ;
- Guo, L. ;
- Gyurjyan, V. ;
- Hadjidakis, C. ;
- Hakobyan, R.S. ;
- Hardie, J. ;
- Heddle, D. ;
- Hersman, F.W. ;
- Hicks, K. ;
- Hicks, R.S. ;
- Hleiqawi, I. ;
- Holtrop, M. ;
- Hu, J. ;
- Hyde, Charles Earl ;
- Ilieva, Y. ;
- Ireland, D.G. ;
- Ishkhanov, B. ;
- Ito, M.M. ;
- Jenkins, David A. ;
- Juengst, Henry G. ;
- Kelley, J.H. ;
- Kellie, J.D. ;
- Khandaker, M. ;
- Kim, D.H. ;
- Kim, K.Y. ;
- Kim, K. ;
- Kim, M.S. ;
- Kim, W. ;
- Klein, A. ;
- Klein, F.J. ;
- Klimenko, A.V. ;
- Klusman, M. ;
- Kossov, M. ;
- Kramer, L.H. ;
- Kuang, Y. ;
- Kubarovsky, V. ;
- Kuhn, S.E. ;
- Kuhn, Joachim ;
- Lachniet, J. ;
- Laget, J.M. ;
- Langheinrich, J. ;
- Lawrence, D. ;
- Livingston, K. ;
- Longhi, A. ;
- Lukashin, K. ;
- Manak, J.J. ;
- Marchand, C. ;
- McAleer, S. ;
- McKinnon, B. ;
- McNabb, J.W.C. ;
- Mecking, B.A. ;
- Mehrabyan, S. ;
- Melone, J.J. ;
- Mestayer, M.D. ;
- Meyer, C.A. ;
- Mikhailov, K. ;
- Mirazita, M. ;
- Miskimen, R. ;
- Mokeev, V. ;
- Morand, L. ;
- Morrow, S.A. ;
- Muccifora, V. ;
- Mueller, J. ;
- Murphy, L.Y. ;
- Mutchler, G.S. ;
- Napolitano, J. ;
- Nasseripour, R. ;
- Nelson, S.O. ;
- Niccolai, S. ;
- Niculescu, G. ;
- Niculescu, I. ;
- Niczyporuk, B.B. ;
- Niyazov, R.A. ;
- Nozar, M. ;
- O'Rielly, G.V. ;
- Osipenko, M. ;
- Park, K. ;
- Pasyuk, E. ;
- Peterson, G. ;
- Philips, S.A. ;
- Pivnyuk, N. ;
- Pocanic, D. ;
- Pogorelko, O. ;
- Polli, E. ;
- Pozdniakov, S. ;
- Preedom, B.M. ;
- Price, J.W. ;
- Prok, Y. ;
- Protopopescu, D. ;
- Qin, L.M. ;
- Raue, B.A. ;
- Riccardi, G. ;
- Ricco, G. ;
- Ripani, M. ;
- Ritchie, B.G. ;
- Ronchetti, F. ;
- Rosner, G. ;
- Rossi, P. ;
- Rowntree, D. ;
- Rubin, P.D. ;
- Sabatie, F. ;
- Sabourov, K. ;
- Salgado, C. ;
- Santoro, J.P. ;
- Sapunenko, V. ;
- Sargsyan, M. ;
- Schumacher, R.A. ;
- Serov, V.S. ;
- Shafi, A. ;
- Sharabian, Y.G. ;
- Shaw, J. ;
- Simionatto, S. ;
- Skabelin, A.V. ;
- Smith, E.S. ;
- Sober, D.I. ;
- Spraker, M. ;
- Stavinsky, A. ;
- Stepanyan, S. ;
- Stoler, P. ;
- Strakovsky, I.I. ;
- Strauch, S. ;
- Taiuti, M. ;
- Taylor, S. ;
- Tedeschi, D.J. ;
- Thoma, U. ;
- Thompson, R. ;
- Tkabladze, A. ;
- Todor, L. ;
- Tur, C. ;
- Ungaro, M. ;
- Vineyard, M.F. ;
- Vlassov, A.V. ;
- Wang, K. ;
- Weinstein, L.B. ;
- Weller, H. ;
- Weygand, D.P. ;
- Whisnant, C.S. ;
- Wolin, E. ;
- Wood, M.H. ;
- Yegneswaran, A. ;
- Yun, J. ;
- Zhang, J. ;
- Zhao, J. ;
- Zhou, Z.
Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (1) covers the proton data for the W range from 1.1300 to 1.6300 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (2) covers the proton data for the W range from 1.6500 to 1.1300 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (3) covers the deuteron data for the W range from 1.0850 to 1.3450 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (4) covers the deuteron data for the W range from 1.3550 to 1.6350 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (5) covers the deuteron data for the W range from 1.6450 to 2.0650 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (6) covers the deuteron data for the W range from 2.0750 to 2.7950 GeV.
Authors
- Dharmawardane, K.V. ;
- Kuhn, S.E. ;
- Bosted, Peter E. ;
- Prok, Y. ;
- Adams, G. ;
- Ambrozewicz, P. ;
- Anghinolfi, M. ;
- Asryan, G. ;
- Avakian, H. ;
- Baghdasaryan, Hovhannes ;
- Baillie, N. ;
- Ball, J.P. ;
- Baltzell, N.A. ;
- Barrow, S. ;
- Batourine, V. ;
- Battaglieri, M. ;
- Beard, K. ;
- Bedlinskiy, Ivan ;
- Bektasoglu, M. ;
- Bellis, M. ;
- Benmouna, N. ;
- Biselli, Angela S. ;
- Bonner, B.E. ;
- Bouchigny, S. ;
- Boiarinov, S. ;
- Bradford, R. ;
- Branford, D. ;
- Brooks, W.K. ;
- Bultmann, S. ;
- Burkert, V.D. ;
- Butuceanu, C. ;
- Calarco, J.R. ;
- Careccia, S.L. ;
- Carman, D.S. ;
- Carnahan, B. ;
- Cazes, A. ;
- Chen, S. ;
- Cole, P.L. ;
- Collins, P. ;
- Coltharp, P. ;
- Cords, D. ;
- Corvisiero, P. ;
- Crabb, D. ;
- Crannell, H. ;
- Crede, V. ;
- Cummings, J.P. ;
- De Masi, R. ;
- DeVita, R. ;
- De Sanctis, E. ;
- Degtyarenko, P.V. ;
- Denizli, H. ;
- Dennis, L. ;
- Deur, A. ;
- Djalali, C. ;
- Dodge, G.E. ;
- Donnelly, J. ;
- Doughty, D. ;
- Dragovitsch, P. ;
- Dugger, M. ;
- Dytman, S. ;
- Dzyubak, O.P. ;
- Egiyan, H. ;
- Egiyan, K.S. ;
- Elouadrhiri, L. ;
- Eugenio, P. ;
- Fatemi, R. ;
- Fedotov, G. ;
- Feuerbach, R.J. ;
- Forest, T.A. ;
- Funsten, H. ;
- Garc Con, M. ;
- Gavalian, G. ;
- Gilfoyle, G.P. ;
- Giovanetti, K.L. ;
- Girod, F.X. ;
- Goetz, J.T. ;
- Golovatch, E. ;
- Gonenc, A. ;
- Gothe, R.W. ;
- Griffioen, K.A. ;
- Guidal, M. ;
- Guillo, M. ;
- Guler, Nevzat ;
- Guo, L. ;
- Gyurjyan, V. ;
- Hadjidakis, C. ;
- Hafidi, K. ;
- Hakobyan, R.S. ;
- Hardie, J. ;
- Heddle, D. ;
- Hersman, F.W. ;
- Hicks, K. ;
- Hleiqawi, I. ;
- Holtrop, M. ;
- Huertas, M. ;
- Hyde, Charles Earl ;
- Ilieva, Y. ;
- Ireland, D.G. ;
- Ishkhanov, B.S. ;
- Isupov, E.L. ;
- Ito, M.M. ;
- Jenkins, David A. ;
- Jo, H.S. ;
- Joo, K. ;
- Juengst, H.G. ;
- Keith, C. ;
- Kellie, J.D. ;
- Khandaker, M. ;
- Kim, K.Y. ;
- Kim, K. ;
- Kim, W. ;
- Klein, A. ;
- Klein, F.J. ;
- Klusman, M. ;
- Kossov, M. ;
- Kramer, L.H. ;
- Kubarovsky, V. ;
- Kuhn, Joachim ;
- Kuleshov, S.V. ;
- Lachniet, J. ;
- Laget, J.M. ;
- Langheinrich, J. ;
- Lawrence, D. ;
- Lima, A.C.S. ;
- Livingston, K. ;
- Lu, H. ;
- Lukashin, K. ;
- MacCormick, M. ;
- Manak, J.J. ;
- Markov, N. ;
- McAleer, S. ;
- McKinnon, B. ;
- McNabb, J.W.C. ;
- Mecking, B.A. ;
- Mestayer, M.D. ;
- Meyer, C.A. ;
- Mibe, T. ;
- Mikhailov, K. ;
- Minehart, R. ;
- Mirazita, M. ;
- Miskimen, R. ;
- Mokeev, V. ;
- Morand, L. ;
- Morrow, S.A. ;
- Moteabbed, M. ;
- Mueller, J. ;
- Mutchler, G.S. ;
- Nadel-Turonski, P. ;
- Napolitano, J. ;
- Nasseripour, R. ;
- Niccolai, S. ;
- Niculescu, G. ;
- Niculescu, I. ;
- Niczyporuk, B.B. ;
- Niroula, M.R. ;
- Niyazov, R.A. ;
- Nozar, M. ;
- O'Rielly, G.V. ;
- Osipenko, M. ;
- Ostrovidov, A.I. ;
- Park, K. ;
- Pasyuk, E. ;
- Paterson, C. ;
- Philips, S.A. ;
- Pierce, J. ;
- Pivnyuk, N. ;
- Pocanic, D. ;
- Pogorelko, O. ;
- Polli, E. ;
- Pozdniakov, S. ;
- Preedom, B.M. ;
- Price, J.W. ;
- Protopopescu, D. ;
- Qin, L.M. ;
- Raue, B.A. ;
- Riccardi, G. ;
- Ricco, G. ;
- Ripani, M. ;
- Ritchie, B.G. ;
- Ronchetti, F. ;
- Rosner, G. ;
- Rossi, P. ;
- Rowntree, D. ;
- Rubin, P.D. ;
- Sabatie, F. ;
- Salgado, C. ;
- Santoro, J.P. ;
- Sapunenko, V. ;
- Schumacher, R.A. ;
- Serov, V.S. ;
- Sharabian, Y.G. ;
- Shaw, J. ;
- Shvedunov, N.V. ;
- Skabelin, A.V. ;
- Smith, E.S. ;
- Smith, L.C. ;
- Sober, D.I. ;
- Stavinsky, A. ;
- Stepanyan, S.S. ;
- Stepanyan, S. ;
- Stokes, B.E. ;
- Stoler, P. ;
- Strakovsky, I.I. ;
- Strauch, S. ;
- Suleiman, R. ;
- Taiuti, M. ;
- Taylor, S. ;
- Tedeschi, D.J. ;
- Thoma, U. ;
- Thompson, R. ;
- Tkabladze, A. ;
- Tkachenko, S. ;
- Todor, L. ;
- Tur, C. ;
- Ungaro, M. ;
- Vineyard, M.F. ;
- Vlassov, A.V. ;
- Weinstein, L.B. ;
- Weygand, D.P. ;
- Williams, M. ;
- Wolin, E. ;
- Wood, M.H. ;
- Yegneswaran, A. ;
- Yun, J. ;
- Zana, L. ;
- Zhang, J. ;
- Zhao, B. ;
- Zhao, Z.
Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (1) covers the proton data for the W range from 1.1300 to 1.6300 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (2) covers the proton data for the W range from 1.6500 to 1.1300 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (3) covers the deuteron data for the W range from 1.0850 to 1.3450 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (4) covers the deuteron data for the W range from 1.3550 to 1.6350 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (5) covers the deuteron data for the W range from 1.6450 to 2.0650 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (6) covers the deuteron data for the W range from 2.0750 to 2.7950 GeV.
Authors
- Dharmawardane, K.V. ;
- Kuhn, S.E. ;
- Bosted, Peter E. ;
- Prok, Y. ;
- Adams, G. ;
- Ambrozewicz, P. ;
- Anghinolfi, M. ;
- Asryan, G. ;
- Avakian, H. ;
- Baghdasaryan, Hovhannes ;
- Baillie, N. ;
- Ball, J.P. ;
- Baltzell, N.A. ;
- Barrow, S. ;
- Batourine, V. ;
- Battaglieri, M. ;
- Beard, K. ;
- Bedlinskiy, Ivan ;
- Bektasoglu, M. ;
- Bellis, M. ;
- Benmouna, N. ;
- Biselli, Angela S. ;
- Bonner, B.E. ;
- Bouchigny, S. ;
- Boiarinov, S. ;
- Bradford, R. ;
- Branford, D. ;
- Brooks, W.K. ;
- Bultmann, S. ;
- Burkert, V.D. ;
- Butuceanu, C. ;
- Calarco, J.R. ;
- Careccia, S.L. ;
- Carman, D.S. ;
- Carnahan, B. ;
- Cazes, A. ;
- Chen, S. ;
- Cole, P.L. ;
- Collins, P. ;
- Coltharp, P. ;
- Cords, D. ;
- Corvisiero, P. ;
- Crabb, D. ;
- Crannell, H. ;
- Crede, V. ;
- Cummings, J.P. ;
- De Masi, R. ;
- DeVita, R. ;
- De Sanctis, E. ;
- Degtyarenko, P.V. ;
- Denizli, H. ;
- Dennis, L. ;
- Deur, A. ;
- Djalali, C. ;
- Dodge, G.E. ;
- Donnelly, J. ;
- Doughty, D. ;
- Dragovitsch, P. ;
- Dugger, M. ;
- Dytman, S. ;
- Dzyubak, O.P. ;
- Egiyan, H. ;
- Egiyan, K.S. ;
- Elouadrhiri, L. ;
- Eugenio, P. ;
- Fatemi, R. ;
- Fedotov, G. ;
- Feuerbach, R.J. ;
- Forest, T.A. ;
- Funsten, H. ;
- Garc Con, M. ;
- Gavalian, G. ;
- Gilfoyle, G.P. ;
- Giovanetti, K.L. ;
- Girod, F.X. ;
- Goetz, J.T. ;
- Golovatch, E. ;
- Gonenc, A. ;
- Gothe, R.W. ;
- Griffioen, K.A. ;
- Guidal, M. ;
- Guillo, M. ;
- Guler, Nevzat ;
- Guo, L. ;
- Gyurjyan, V. ;
- Hadjidakis, C. ;
- Hafidi, K. ;
- Hakobyan, R.S. ;
- Hardie, J. ;
- Heddle, D. ;
- Hersman, F.W. ;
- Hicks, K. ;
- Hleiqawi, I. ;
- Holtrop, M. ;
- Huertas, M. ;
- Hyde, Charles Earl ;
- Ilieva, Y. ;
- Ireland, D.G. ;
- Ishkhanov, B.S. ;
- Isupov, E.L. ;
- Ito, M.M. ;
- Jenkins, David A. ;
- Jo, H.S. ;
- Joo, K. ;
- Juengst, H.G. ;
- Keith, C. ;
- Kellie, J.D. ;
- Khandaker, M. ;
- Kim, K.Y. ;
- Kim, K. ;
- Kim, W. ;
- Klein, A. ;
- Klein, F.J. ;
- Klusman, M. ;
- Kossov, M. ;
- Kramer, L.H. ;
- Kubarovsky, V. ;
- Kuhn, Joachim ;
- Kuleshov, S.V. ;
- Lachniet, J. ;
- Laget, J.M. ;
- Langheinrich, J. ;
- Lawrence, D. ;
- Lima, A.C.S. ;
- Livingston, K. ;
- Lu, H. ;
- Lukashin, K. ;
- MacCormick, M. ;
- Manak, J.J. ;
- Markov, N. ;
- McAleer, S. ;
- McKinnon, B. ;
- McNabb, J.W.C. ;
- Mecking, B.A. ;
- Mestayer, M.D. ;
- Meyer, C.A. ;
- Mibe, T. ;
- Mikhailov, K. ;
- Minehart, R. ;
- Mirazita, M. ;
- Miskimen, R. ;
- Mokeev, V. ;
- Morand, L. ;
- Morrow, S.A. ;
- Moteabbed, M. ;
- Mueller, J. ;
- Mutchler, G.S. ;
- Nadel-Turonski, P. ;
- Napolitano, J. ;
- Nasseripour, R. ;
- Niccolai, S. ;
- Niculescu, G. ;
- Niculescu, I. ;
- Niczyporuk, B.B. ;
- Niroula, M.R. ;
- Niyazov, R.A. ;
- Nozar, M. ;
- O'Rielly, G.V. ;
- Osipenko, M. ;
- Ostrovidov, A.I. ;
- Park, K. ;
- Pasyuk, E. ;
- Paterson, C. ;
- Philips, S.A. ;
- Pierce, J. ;
- Pivnyuk, N. ;
- Pocanic, D. ;
- Pogorelko, O. ;
- Polli, E. ;
- Pozdniakov, S. ;
- Preedom, B.M. ;
- Price, J.W. ;
- Protopopescu, D. ;
- Qin, L.M. ;
- Raue, B.A. ;
- Riccardi, G. ;
- Ricco, G. ;
- Ripani, M. ;
- Ritchie, B.G. ;
- Ronchetti, F. ;
- Rosner, G. ;
- Rossi, P. ;
- Rowntree, D. ;
- Rubin, P.D. ;
- Sabatie, F. ;
- Salgado, C. ;
- Santoro, J.P. ;
- Sapunenko, V. ;
- Schumacher, R.A. ;
- Serov, V.S. ;
- Sharabian, Y.G. ;
- Shaw, J. ;
- Shvedunov, N.V. ;
- Skabelin, A.V. ;
- Smith, E.S. ;
- Smith, L.C. ;
- Sober, D.I. ;
- Stavinsky, A. ;
- Stepanyan, S.S. ;
- Stepanyan, S. ;
- Stokes, B.E. ;
- Stoler, P. ;
- Strakovsky, I.I. ;
- Strauch, S. ;
- Suleiman, R. ;
- Taiuti, M. ;
- Taylor, S. ;
- Tedeschi, D.J. ;
- Thoma, U. ;
- Thompson, R. ;
- Tkabladze, A. ;
- Tkachenko, S. ;
- Todor, L. ;
- Tur, C. ;
- Ungaro, M. ;
- Vineyard, M.F. ;
- Vlassov, A.V. ;
- Weinstein, L.B. ;
- Weygand, D.P. ;
- Williams, M. ;
- Wolin, E. ;
- Wood, M.H. ;
- Yegneswaran, A. ;
- Yun, J. ;
- Zana, L. ;
- Zhang, J. ;
- Zhao, B. ;
- Zhao, Z.
Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (1) covers the proton data for the W range from 1.1300 to 1.6300 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (2) covers the proton data for the W range from 1.6500 to 1.1300 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (3) covers the deuteron data for the W range from 1.0850 to 1.3450 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (4) covers the deuteron data for the W range from 1.3550 to 1.6350 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (5) covers the deuteron data for the W range from 1.6450 to 2.0650 GeV.Jefferson Lab.-CEBAF. Measurement of the virtual photon asymmetry A1 and the spin structure function G1 in E- P and E- DEUT interactions using longitudinally polarized NH3 and ND3 targets with a longitudinally polarized electron beam of energy 1.6 and 5.7 GeV. The data cover the resonance and DIS regions with Q2 from 0.05 to 5.0 GeV2 and final state invariant mass W up to about 3 GeV.. The data here have been provided by K.V.Dharmawardane and S.E.Kuhn from the CLAS database.. This part (6) covers the deuteron data for the W range from 2.0750 to 2.7950 GeV.
Authors
- Dharmawardane, K.V. ;
- Kuhn, S.E. ;
- Bosted, Peter E. ;
- Prok, Y. ;
- Adams, G. ;
- Ambrozewicz, P. ;
- Anghinolfi, M. ;
- Asryan, G. ;
- Avakian, H. ;
- Baghdasaryan, Hovhannes ;
- Baillie, N. ;
- Ball, J.P. ;
- Baltzell, N.A. ;
- Barrow, S. ;
- Batourine, V. ;
- Battaglieri, M. ;
- Beard, K. ;
- Bedlinskiy, Ivan ;
- Bektasoglu, M. ;
- Bellis, M. ;
- Benmouna, N. ;
- Biselli, Angela S. ;
- Bonner, B.E. ;
- Bouchigny, S. ;
- Boiarinov, S. ;
- Bradford, R. ;
- Branford, D. ;
- Brooks, W.K. ;
- Bultmann, S. ;
- Burkert, V.D. ;
- Butuceanu, C. ;
- Calarco, J.R. ;
- Careccia, S.L. ;
- Carman, D.S. ;
- Carnahan, B. ;
- Cazes, A. ;
- Chen, S. ;
- Cole, P.L. ;
- Collins, P. ;
- Coltharp, P. ;
- Cords, D. ;
- Corvisiero, P. ;
- Crabb, D. ;
- Crannell, H. ;
- Crede, V. ;
- Cummings, J.P. ;
- De Masi, R. ;
- DeVita, R. ;
- De Sanctis, E. ;
- Degtyarenko, P.V. ;
- Denizli, H. ;
- Dennis, L. ;
- Deur, A. ;
- Djalali, C. ;
- Dodge, G.E. ;
- Donnelly, J. ;
- Doughty, D. ;
- Dragovitsch, P. ;
- Dugger, M. ;
- Dytman, S. ;
- Dzyubak, O.P. ;
- Egiyan, H. ;
- Egiyan, K.S. ;
- Elouadrhiri, L. ;
- Eugenio, P. ;
- Fatemi, R. ;
- Fedotov, G. ;
- Feuerbach, R.J. ;
- Forest, T.A. ;
- Funsten, H. ;
- Garc Con, M. ;
- Gavalian, G. ;
- Gilfoyle, G.P. ;
- Giovanetti, K.L. ;
- Girod, F.X. ;
- Goetz, J.T. ;
- Golovatch, E. ;
- Gonenc, A. ;
- Gothe, R.W. ;
- Griffioen, K.A. ;
- Guidal, M. ;
- Guillo, M. ;
- Guler, Nevzat ;
- Guo, L. ;
- Gyurjyan, V. ;
- Hadjidakis, C. ;
- Hafidi, K. ;
- Hakobyan, R.S. ;
- Hardie, J. ;
- Heddle, D. ;
- Hersman, F.W. ;
- Hicks, K. ;
- Hleiqawi, I. ;
- Holtrop, M. ;
- Huertas, M. ;
- Hyde, Charles Earl ;
- Ilieva, Y. ;
- Ireland, D.G. ;
- Ishkhanov, B.S. ;
- Isupov, E.L. ;
- Ito, M.M. ;
- Jenkins, David A. ;
- Jo, H.S. ;
- Joo, K. ;
- Juengst, H.G. ;
- Keith, C. ;
- Kellie, J.D. ;
- Khandaker, M. ;
- Kim, K.Y. ;
- Kim, K. ;
- Kim, W. ;
- Klein, A. ;
- Klein, F.J. ;
- Klusman, M. ;
- Kossov, M. ;
- Kramer, L.H. ;
- Kubarovsky, V. ;
- Kuhn, Joachim ;
- Kuleshov, S.V. ;
- Lachniet, J. ;
- Laget, J.M. ;
- Langheinrich, J. ;
- Lawrence, D. ;
- Lima, A.C.S. ;
- Livingston, K. ;
- Lu, H. ;
- Lukashin, K. ;
- MacCormick, M. ;
- Manak, J.J. ;
- Markov, N. ;
- McAleer, S. ;
- McKinnon, B. ;
- McNabb, J.W.C. ;
- Mecking, B.A. ;
- Mestayer, M.D. ;
- Meyer, C.A. ;
- Mibe, T. ;
- Mikhailov, K. ;
- Minehart, R. ;
- Mirazita, M. ;
- Miskimen, R. ;
- Mokeev, V. ;
- Morand, L. ;
- Morrow, S.A. ;
- Moteabbed, M. ;
- Mueller, J. ;
- Mutchler, G.S. ;
- Nadel-Turonski, P. ;
- Napolitano, J. ;
- Nasseripour, R. ;
- Niccolai, S. ;
- Niculescu, G. ;
- Niculescu, I. ;
- Niczyporuk, B.B. ;
- Niroula, M.R. ;
- Niyazov, R.A. ;
- Nozar, M. ;
- O'Rielly, G.V. ;
- Osipenko, M. ;
- Ostrovidov, A.I. ;
- Park, K. ;
- Pasyuk, E. ;
- Paterson, C. ;
- Philips, S.A. ;
- Pierce, J. ;
- Pivnyuk, N. ;
- Pocanic, D. ;
- Pogorelko, O. ;
- Polli, E. ;
- Pozdniakov, S. ;
- Preedom, B.M. ;
- Price, J.W. ;
- Protopopescu, D. ;
- Qin, L.M. ;
- Raue, B.A. ;
- Riccardi, G. ;
- Ricco, G. ;
- Ripani, M. ;
- Ritchie, B.G. ;
- Ronchetti, F. ;
- Rosner, G. ;
- Rossi, P. ;
- Rowntree, D. ;
- Rubin, P.D. ;
- Sabatie, F. ;
- Salgado, C. ;
- Santoro, J.P. ;
- Sapunenko, V. ;
- Schumacher, R.A. ;
- Serov, V.S. ;
- Sharabian, Y.G. ;
- Shaw, J. ;
- Shvedunov, N.V. ;
- Skabelin, A.V. ;
- Smith, E.S. ;
- Smith, L.C. ;
- Sober, D.I. ;
- Stavinsky, A. ;
- Stepanyan, S.S. ;
- Stepanyan, S. ;
- Stokes, B.E. ;
- Stoler, P. ;
- Strakovsky, I.I. ;
- Strauch, S. ;
- Suleiman, R. ;
- Taiuti, M. ;
- Taylor, S. ;
- Tedeschi, D.J. ;
- Thoma, U. ;
- Thompson, R. ;
- Tkabladze, A. ;
- Tkachenko, S. ;
- Todor, L. ;
- Tur, C. ;
- Ungaro, M. ;
- Vineyard, M.F. ;
- Vlassov, A.V. ;
- Weinstein, L.B. ;
- Weygand, D.P. ;
- Williams, M. ;
- Wolin, E. ;
- Wood, M.H. ;
- Yegneswaran, A. ;
- Yun, J. ;
- Zana, L. ;
- Zhang, J. ;
- Zhao, B. ;
- Zhao, Z.
Jefferson Lab-CEBAF. Measurement of exclusive omega electroproduction off the proton in a large kinematical domain above the nucleon resonance region. The data were collected using a 5.754 GeV electron beam and liquid hydrogen target and has in total an integrated luminsoity of 28.5fb-1 taken over the period Oct 2001 to Jan 2002. Total and differential cross sections (in -T and PHI) are given as well as spin density matrices.. Numerical values supplied by M Garcon.
Authors
- Morand, L. ;
- Dore, D. ;
- Garcon, M. ;
- Guidal, M. ;
- Laget, J.-M. ;
- Morrow, S. ;
- Sabatie, F. ;
- Smith, E. ;
- Adams, G. ;
- Ambrozewicz, P. ;
- Anghinolfi, M. ;
- Asryan, G. ;
- Audit, G. ;
- Avakian, H. ;
- Baghdasaryan, Hovhannes ;
- Ball, J. ;
- Ball, J.P. ;
- Baltzell, N.A. ;
- Barrow, S. ;
- Batourine, V. ;
- Battaglieri, M. ;
- Bektasoglu, M. ;
- Bellis, M. ;
- Benmouna, N. ;
- Berman, B.L. ;
- Biselli, Angela S. ;
- Boiarinov, S. ;
- Bonner, B.E. ;
- Bouchigny, S. ;
- Bradford, R. ;
- Branford, D. ;
- Briscoe, W.J. ;
- Brooks, W.K. ;
- Bultmann, S. ;
- Burkert, V.D. ;
- Butuceanu, C. ;
- Calarco, J.R. ;
- Careccia, S.L. ;
- Carman, D.S. ;
- Cazes, A. ;
- Chen, S. ;
- Cole, P.L. ;
- Cords, D. ;
- Corvisiero, P. ;
- Crabb, D. ;
- Cummings, J.P. ;
- De Sanctis, E. ;
- DeVita, R. ;
- Degtyarenko, P.V. ;
- Denizli, H. ;
- Dennis, L. ;
- Deur, A. ;
- Dharmawardane, K.V. ;
- Dhuga, K.S. ;
- Djalali, C. ;
- Dodge, G.E. ;
- Donnelly, J. ;
- Doughty, D. ;
- Dugger, M. ;
- Dytman, S. ;
- Dzyubak, O.P. ;
- Egiyan, H. ;
- Egiyan, K.S. ;
- Elouadrhiri, L. ;
- Eugenio, P. ;
- Fatemi, R. ;
- Feldman, G. ;
- Fersch, R.G. ;
- Feuerbach, R.J. ;
- Funsten, H. ;
- Gavalian, G. ;
- Gilfoyle, G.P. ;
- Giovanetti, K.L. ;
- Girod, F.-X. ;
- Goetz, J.T. ;
- Gordon, C.I.O. ;
- Gothe, R.W. ;
- Griffioen, K.A. ;
- Guillo, M. ;
- Guler, Nevzat ;
- Guo, L. ;
- Gyurjyan, V. ;
- Hadjidakis, C. ;
- Hakobyan, R.S. ;
- Hardie, J. ;
- Heddle, D. ;
- Hersman, F.W. ;
- Hicks, K. ;
- Hleiqawi, I. ;
- Holtrop, M. ;
- Hyde, Charles Earl ;
- Ilieva, Y. ;
- Ireland, D.G. ;
- Ito, M.M. ;
- Jenkins, David A. ;
- Jo, H.-S. ;
- Joo, K. ;
- Juengst, Henry G. ;
- Kellie, J.D. ;
- Khandaker, M. ;
- Kim, W. ;
- Klein, A. ;
- Klein, F.J. ;
- Klimenko, A.V. ;
- Kossov, M. ;
- Kubarovski, V. ;
- Kramer, L.H. ;
- Kuhn, S.E. ;
- Kuhn, Joachim ;
- Lachniet, J. ;
- Langheinrich, J. ;
- Lawrence, D. ;
- Lee, T. ;
- Li, Ji ;
- Livingston, K. ;
- Marchand, C. ;
- Maximon, L.C. ;
- McAleer, S. ;
- McKinnon, B. ;
- McNabb, J.W.C. ;
- Mecking, B.A. ;
- Mehrabyan, S. ;
- Melone, J.J. ;
- Mestayer, M.D. ;
- Meyer, C.A. ;
- Mikhailov, K. ;
- Minehart, R. ;
- Mirazita, M. ;
- Miskimen, R. ;
- Mokeev, V. ;
- Mueller, J. ;
- Mutchler, G.S. ;
- Napolitano, J. ;
- Nasseripour, R. ;
- Niccolai, S. ;
- Niculescu, G. ;
- Niculescu, I. ;
- Niczyporuk, B.B. ;
- Niyazov, R.A. ;
- Nozar, M. ;
- O'Rielly, G.V. ;
- Osipenko, M. ;
- Ostrovidov, A.I. ;
- Park, K. ;
- Pasyuk, E. ;
- Philips, S.A. ;
- Pivnyuk, N. ;
- Pocanic, D. ;
- Pogorelko, O. ;
- Polli, E. ;
- Popa, I. ;
- Pozdniakov, S. ;
- Preedom, B.M. ;
- Price, J.W. ;
- Prok, Y. ;
- Protopopescu, D. ;
- Raue, B.A. ;
- Riccardi, G. ;
- Ricco, G. ;
- Ripani, M. ;
- Ritchie, B.G. ;
- Ronchetti, F. ;
- Rosner, G. ;
- Rossi, P. ;
- Rubin, P.D. ;
- Salgado, C. ;
- Santoro, J.P. ;
- Sapunenko, V. ;
- Schumacher, R.A. ;
- Serov, V.S. ;
- Sharabian, Y.G. ;
- Shaw, J. ;
- Skabelin, A.V. ;
- Smith, L.C. ;
- Sober, D.I. ;
- Stavinsky, A. ;
- Stepanyan, S. ;
- Stepanyan, S.S. ;
- Stokes, B.E. ;
- Stoler, P. ;
- Strakovsky, I.I. ;
- Strauch, S. ;
- Taiuti, M. ;
- Tedeschi, D.J. ;
- Thoma, U. ;
- Tkabladze, A. ;
- Todor, L. ;
- Tur, C. ;
- Ungaro, M. ;
- Vineyard, M.F. ;
- Vlassov, A.V. ;
- Weinstein, L.B. ;
- Weygand, D.P. ;
- Williams, M. ;
- Wolin, E. ;
- Wood, M.H. ;
- Yegneswaran, A. ;
- Zana, L.
Jefferson Lab-CEBAF. Measurement of the polarized structure function SIG(LTprime) for pion electroproduction at Q**2 of 0.40 and 0.65 GeV.. Data is given for both the (PI0 P) and (PI+ P) channels covering the W region 1.1 to 1.6 GeV. The experiment uses longitudinally polarized electrons at a beam energy of 1.515 GeV.. Numerical values supplied by L.C.Smith.
Authors
- Joo, K. ;
- Smith, L.C. ;
- Aznauryan, I.G. ;
- Burkert, V.D. ;
- Egiyan, H. ;
- Minehart, R. ;
- Adams, G. ;
- Ambrozewicz, P. ;
- Anciant, E. ;
- Anghinolfi, M. ;
- Asavapibhop, B. ;
- Asryan, G. ;
- Audit, G. ;
- Auger, T. ;
- Avakian, H. ;
- Baghdasaryan, Hovhannes ;
- Baillie, N. ;
- Ball, J.P. ;
- Baltzell, N.A. ;
- Barrow, S. ;
- Batourine, V. ;
- Battaglieri, M. ;
- Beard, K. ;
- Bedlinskiy, Ivan ;
- Bektasoglu, M. ;
- Bellis, M. ;
- Benmouna, N. ;
- Berman, B.L. ;
- Bianchi, N. ;
- Biselli, Angela S. ;
- Bonner, B.E. ;
- Bouchigny, S. ;
- Boiarinov, S. ;
- Bradford, R. ;
- Branford, D. ;
- Briscoe, W.J. ;
- Brooks, W.K. ;
- Bueltmann, S. ;
- Butuceanu, C. ;
- Calarco, J.R. ;
- Careccia, S.L. ;
- Carman, D.S. ;
- Carnahan, B. ;
- Cetina, C. ;
- Chen, S. ;
- Cole, P.L. ;
- Coleman, A. ;
- Coltharp, P. ;
- Cords, D. ;
- Corvisiero, P. ;
- Crabb, D. ;
- Cummings, J.P. ;
- De Sanctis, E. ;
- DeVita, R. ;
- Degtyarenko, P.V. ;
- Dennis, L. ;
- Deur, A. ;
- Dharmawardane, K.V. ;
- Dhuga, K.S. ;
- Djalali, C. ;
- Dodge, G.E. ;
- Donnelly, J. ;
- Doughty, D. ;
- Dragovitsch, P. ;
- Dugger, M. ;
- Dytman, S. ;
- Dzyubak, O.P. ;
- Egiyan, K.S. ;
- Elouadrhiri, L. ;
- Empl, A. ;
- Eugenio, P. ;
- Farhi, L. ;
- Fatemi, R. ;
- Fedotov, G. ;
- Feldman, G. ;
- Feuerbach, R.J. ;
- Forest, T.A. ;
- Frolov, V. ;
- Funsten, H. ;
- Gaff, S.J. ;
- Garcon, M. ;
- Gavalian, G. ;
- Gilfoyle, G.P. ;
- Giovanetti, K.L. ;
- Girard, P. ;
- Girod, F.X. ;
- Goetz, J.T. ;
- Gothe, R.W. ;
- Griffioen, K.A. ;
- Guidal, M. ;
- Guillo, M. ;
- Guler, Nevzat ;
- Guo, L. ;
- Gyurjyan, V. ;
- Hakobyan, R.S. ;
- Hardie, J. ;
- Heddle, D. ;
- Hersman, F.W. ;
- Hicks, K. ;
- Hleiqawi, I. ;
- Holtrop, M. ;
- Hu, J. ;
- Hyde, Charles Earl ;
- Ilieva, Y. ;
- Ireland, D.G. ;
- Ishkhanov, B.S. ;
- Ito, M.M. ;
- Jenkins, David A. ;
- Jo, H.S. ;
- Juengst, Henry G. ;
- Kelley, J.H. ;
- Kellie, J.D. ;
- Khandaker, M. ;
- Kim, K.Y. ;
- Kim, K. ;
- Kim, W. ;
- Klein, A. ;
- Klein, F.J. ;
- Klimenko, A.V. ;
- Klusman, M. ;
- Kossov, M. ;
- Kramer, L.H. ;
- Kubarovsky, V. ;
- Kuhn, Joachim ;
- Kuhn, S.E. ;
- Lachniet, J. ;
- Laget, J.M. ;
- Langheinrich, J. ;
- Lawrence, D. ;
- Lee, T. ;
- Livingston, K. ;
- Lukashin, K. ;
- Manak, J.J. ;
- Marchand, C. ;
- Maximon, L.C. ;
- McAleer, S. ;
- McKinnon, B. ;
- McNabb, J.W.C. ;
- Mecking, B.A. ;
- Mestayer, M.D. ;
- Meyer, C.A. ;
- Mikhailov, K. ;
- Mirazita, M. ;
- Miskimen, R. ;
- Mokeev, V. ;
- Morrow, S.A. ;
- Muccifora, V. ;
- Mueller, J. ;
- Mutchler, G.S. ;
- Nadel-Turonski, P. ;
- Napolitano, J. ;
- Nasseripour, R. ;
- Nelson, S.O. ;
- Niccolai, S. ;
- Niculescu, G. ;
- Niculescu, I. ;
- Niczyporuk, B.B. ;
- Niyazov, R.A. ;
- Nozar, M. ;
- O'Rielly, G.V. ;
- Osipenko, M. ;
- Ostrovidov, A.I. ;
- Park, K. ;
- Pasyuk, E. ;
- Peterson, G. ;
- Philips, S.A. ;
- Pierce, J. ;
- Pivnyuk, N. ;
- Pocanic, D. ;
- Pogorelko, O. ;
- Polli, E. ;
- Pozdniakov, S. ;
- Preedom, B.M. ;
- Price, J.W. ;
- Prok, Y. ;
- Protopopescu, D. ;
- Qin, L.M. ;
- Raue, B.A. ;
- Riccardi, G. ;
- Ricco, G. ;
- Ripani, M. ;
- Ritchie, B.G. ;
- Ronchetti, F. ;
- Rosner, G. ;
- Rossi, P. ;
- Rowntree, D. ;
- Rubin, P.D. ;
- Sabatie, F. ;
- Sabourov, K. ;
- Salgado, C. ;
- Santoro, J.P. ;
- Sapunenko, V. ;
- Schumacher, R.A. ;
- Serov, V.S. ;
- Shafi, A. ;
- Sharabian, Y.G. ;
- Shaw, J. ;
- Simionatto, S. ;
- Skabelin, A.V. ;
- Smith, E.S. ;
- Sober, D.I. ;
- Spraker, M. ;
- Stavinsky, A. ;
- Stepanyan, S.S. ;
- Stepanyan, S. ;
- Stokes, B.E. ;
- Stoler, P. ;
- Strakovsky, I.I. ;
- Strauch, S. ;
- Taiuti, M. ;
- Taylor, S. ;
- Tedeschi, D.J. ;
- Thoma, U. ;
- Thompson, R. ;
- Tkabladze, A. ;
- Tur, C. ;
- Ungaro, M. ;
- Vineyard, M.F. ;
- Vlassov, A.V. ;
- Wang, K. ;
- Weinstein, L.B. ;
- Weller, H. ;
- Weygand, D.P. ;
- Williams, M. ;
- Wolin, E. ;
- Wood, M.H. ;
- Yegneswaran, A. ;
- Yun, J. ;
- Zana, L. ;
- Zhang, J.