Separated Response Functions in Exclusive, Forward \pi^{\pm} Electroproduction on Deuterium
Background: Measurements of forward exclusive meson production at different squared four-momenta of the exchanged virtual photon, Q^2, and at different four-momentum transfer, t, can be used to probe QCD's transition from meson-nucleon degrees of freedom at long distances to quark-gluon degrees...
Ausführliche Beschreibung
Autor*in: |
Huber, G. M [verfasserIn] |
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Format: |
Artikel |
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Sprache: |
Englisch |
Erschienen: |
2014 |
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Systematik: |
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Übergeordnetes Werk: |
Enthalten in: Physical review / C - Woodbury, NY : Inst., 1970, (2014) |
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Übergeordnetes Werk: |
year:2014 |
Links: |
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DOI / URN: |
10.1103/PhysRevC.91.015202 |
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Katalog-ID: |
OLC1966212046 |
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520 | |a Background: Measurements of forward exclusive meson production at different squared four-momenta of the exchanged virtual photon, Q^2, and at different four-momentum transfer, t, can be used to probe QCD's transition from meson-nucleon degrees of freedom at long distances to quark-gluon degrees of freedom at short scales. Ratios of separated response functions in \pi^- and \pi^+ electroproduction are particularly informative. The ratio for transverse photons may allow this transition to be more easily observed, while the ratio for longitudinal photons provides a crucial verification of the assumed pole dominance, needed for reliable extraction of the pion form factor from electroproduction data. Method: Data were acquired with 2.6-5.2 GeV electron beams and the HMS+SOS spectrometers in Jefferson Lab Hall C, at central Q^2 values of 0.6, 1.0, 1.6 GeV^2 at W=1.95 GeV, and Q^2=2.45 GeV^2 at W=2.22 GeV. There was significant coverage in \phi and \epsilon, which allowed separation of \sigma_{L,T,LT,TT}. Results: \sigma_L shows a clear signature of the pion pole, with a sharp rise at small -t. In contrast, \sigma_T is much flatter versus t. The longitudinal/transverse ratios evolve with Q^2 and t, and at the highest Q^2=2.45 GeV^2 show a slight enhancement for \pi^- production compared to \pi^+. The \pi^-/\pi^+ ratio for transverse photons exhibits only a small Q^2-dependence, following a nearly universal curve with t, with a steep transition to a value of about 0.25, consistent with s-channel quark knockout. The \sigma_{TT}/\sigma_T ratio also drops rapidly with Q^2, qualitatively consistent with s-channel helicity conservation. The \pi^-/\pi^+ ratio for longitudinal photons indicates a small isoscalar contamination at W=1.95 GeV, consistent with what was observed in our earlier determination of the pion form factor at these kinematics. | ||
650 | 4 | |a Nuclear Experiment | |
700 | 1 | |a Blok, H. P |4 oth | |
700 | 1 | |a Butuceanu, C |4 oth | |
700 | 1 | |a Gaskell, D |4 oth | |
700 | 1 | |a Horn, T |4 oth | |
700 | 1 | |a Mack, D. J |4 oth | |
700 | 1 | |a Abbott, D |4 oth | |
700 | 1 | |a Aniol, K |4 oth | |
700 | 1 | |a Anklin, H |4 oth | |
700 | 1 | |a Armstrong, C |4 oth | |
700 | 1 | |a Arrington, J |4 oth | |
700 | 1 | |a Assamagan, K |4 oth | |
700 | 1 | |a Avery, S |4 oth | |
700 | 1 | |a Baker, O. K |4 oth | |
700 | 1 | |a Barrett, B |4 oth | |
700 | 1 | |a Beise, E. J |4 oth | |
700 | 1 | |a Bochna, C |4 oth | |
700 | 1 | |a Boeglin, W |4 oth | |
700 | 1 | |a Brash, E. J |4 oth | |
700 | 1 | |a Breuer, H |4 oth | |
700 | 1 | |a Chang, C. C |4 oth | |
700 | 1 | |a Chant, N |4 oth | |
700 | 1 | |a Christy, M. E |4 oth | |
700 | 1 | |a Dunne, J |4 oth | |
700 | 1 | |a Eden, T |4 oth | |
700 | 1 | |a Ent, R |4 oth | |
700 | 1 | |a Fenker, H |4 oth | |
700 | 1 | |a Gibson, E. F |4 oth | |
700 | 1 | |a Gilman, R |4 oth | |
700 | 1 | |a Gustafsson, K |4 oth | |
700 | 1 | |a Hinton, W |4 oth | |
700 | 1 | |a Holt, R. J |4 oth | |
700 | 1 | |a Jackson, H |4 oth | |
700 | 1 | |a Jin, S |4 oth | |
700 | 1 | |a Jones, M. K |4 oth | |
700 | 1 | |a Keppel, C. E |4 oth | |
700 | 1 | |a Kim, P. H |4 oth | |
700 | 1 | |a Kim, W |4 oth | |
700 | 1 | |a King, P. M |4 oth | |
700 | 1 | |a Klein, A |4 oth | |
700 | 1 | |a Koltenuk, D |4 oth | |
700 | 1 | |a Kovaltchouk, V |4 oth | |
700 | 1 | |a Liang, M |4 oth | |
700 | 1 | |a Liu, J |4 oth | |
700 | 1 | |a Lolos, G. J |4 oth | |
700 | 1 | |a Lung, A |4 oth | |
700 | 1 | |a Margaziotis, D. J |4 oth | |
700 | 1 | |a Markowitz, P |4 oth | |
700 | 1 | |a Matsumura, A |4 oth | |
700 | 1 | |a McKee, D |4 oth | |
700 | 1 | |a Meekins, D |4 oth | |
700 | 1 | |a Mitchell, J |4 oth | |
700 | 1 | |a Miyoshi, T |4 oth | |
700 | 1 | |a Mkrtchyan, H |4 oth | |
700 | 1 | |a Mueller, B |4 oth | |
700 | 1 | |a Niculescu, G |4 oth | |
700 | 1 | |a Niculescu, I |4 oth | |
700 | 1 | |a Okayasu, Y |4 oth | |
700 | 1 | |a Pentchev, L |4 oth | |
700 | 1 | |a Perdrisat, C |4 oth | |
700 | 1 | |a Pitz, D |4 oth | |
700 | 1 | |a Potterveld, D |4 oth | |
700 | 1 | |a Punjabi, V |4 oth | |
700 | 1 | |a Qin, L. M |4 oth | |
700 | 1 | |a Reimer, P. E |4 oth | |
700 | 1 | |a Reinhold, J |4 oth | |
700 | 1 | |a Roche, J |4 oth | |
700 | 1 | |a Roos, P. G |4 oth | |
700 | 1 | |a Sarty, A |4 oth | |
700 | 1 | |a Shin, I. K |4 oth | |
700 | 1 | |a Smith, G. R |4 oth | |
700 | 1 | |a Stepanyan, S |4 oth | |
700 | 1 | |a Tang, L. G |4 oth | |
700 | 1 | |a Tadevosyan, V |4 oth | |
700 | 1 | |a Tvaskis, V |4 oth | |
700 | 1 | |a van der Meer, R. L. J |4 oth | |
700 | 1 | |a Vansyoc, K |4 oth | |
700 | 1 | |a Van Westrum, D |4 oth | |
700 | 1 | |a Vidakovic, S |4 oth | |
700 | 1 | |a Volmer, J |4 oth | |
700 | 1 | |a Vulcan, W |4 oth | |
700 | 1 | |a Warren, G |4 oth | |
700 | 1 | |a Wood, S. A |4 oth | |
700 | 1 | |a Xu, C |4 oth | |
700 | 1 | |a Yan, C |4 oth | |
700 | 1 | |a Zhao, W. -X |4 oth | |
700 | 1 | |a Zheng, X |4 oth | |
700 | 1 | |a Zihlmann, B |4 oth | |
700 | 1 | |a Collaboration, The Jefferson Lab Fpi |4 oth | |
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10.1103/PhysRevC.91.015202 doi PQ20160617 (DE-627)OLC1966212046 (DE-599)GBVOLC1966212046 (PRQ)a733-70b082594eaff6beee1d0a03a55de5ae779bb9495e483c92691e3fd53a918b6e0 (KEY)0054933920140000000000000000separatedresponsefunctionsinexclusiveforwardpipmel DE-627 ger DE-627 rakwb eng 530 DNB UA 6500. AVZ rvk Huber, G. M verfasserin aut Separated Response Functions in Exclusive, Forward \pi^{\pm} Electroproduction on Deuterium 2014 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Background: Measurements of forward exclusive meson production at different squared four-momenta of the exchanged virtual photon, Q^2, and at different four-momentum transfer, t, can be used to probe QCD's transition from meson-nucleon degrees of freedom at long distances to quark-gluon degrees of freedom at short scales. Ratios of separated response functions in \pi^- and \pi^+ electroproduction are particularly informative. The ratio for transverse photons may allow this transition to be more easily observed, while the ratio for longitudinal photons provides a crucial verification of the assumed pole dominance, needed for reliable extraction of the pion form factor from electroproduction data. Method: Data were acquired with 2.6-5.2 GeV electron beams and the HMS+SOS spectrometers in Jefferson Lab Hall C, at central Q^2 values of 0.6, 1.0, 1.6 GeV^2 at W=1.95 GeV, and Q^2=2.45 GeV^2 at W=2.22 GeV. There was significant coverage in \phi and \epsilon, which allowed separation of \sigma_{L,T,LT,TT}. Results: \sigma_L shows a clear signature of the pion pole, with a sharp rise at small -t. In contrast, \sigma_T is much flatter versus t. The longitudinal/transverse ratios evolve with Q^2 and t, and at the highest Q^2=2.45 GeV^2 show a slight enhancement for \pi^- production compared to \pi^+. The \pi^-/\pi^+ ratio for transverse photons exhibits only a small Q^2-dependence, following a nearly universal curve with t, with a steep transition to a value of about 0.25, consistent with s-channel quark knockout. The \sigma_{TT}/\sigma_T ratio also drops rapidly with Q^2, qualitatively consistent with s-channel helicity conservation. The \pi^-/\pi^+ ratio for longitudinal photons indicates a small isoscalar contamination at W=1.95 GeV, consistent with what was observed in our earlier determination of the pion form factor at these kinematics. Nuclear Experiment Blok, H. P oth Butuceanu, C oth Gaskell, D oth Horn, T oth Mack, D. J oth Abbott, D oth Aniol, K oth Anklin, H oth Armstrong, C oth Arrington, J oth Assamagan, K oth Avery, S oth Baker, O. K oth Barrett, B oth Beise, E. J oth Bochna, C oth Boeglin, W oth Brash, E. J oth Breuer, H oth Chang, C. C oth Chant, N oth Christy, M. E oth Dunne, J oth Eden, T oth Ent, R oth Fenker, H oth Gibson, E. F oth Gilman, R oth Gustafsson, K oth Hinton, W oth Holt, R. J oth Jackson, H oth Jin, S oth Jones, M. K oth Keppel, C. E oth Kim, P. H oth Kim, W oth King, P. M oth Klein, A oth Koltenuk, D oth Kovaltchouk, V oth Liang, M oth Liu, J oth Lolos, G. J oth Lung, A oth Margaziotis, D. J oth Markowitz, P oth Matsumura, A oth McKee, D oth Meekins, D oth Mitchell, J oth Miyoshi, T oth Mkrtchyan, H oth Mueller, B oth Niculescu, G oth Niculescu, I oth Okayasu, Y oth Pentchev, L oth Perdrisat, C oth Pitz, D oth Potterveld, D oth Punjabi, V oth Qin, L. M oth Reimer, P. E oth Reinhold, J oth Roche, J oth Roos, P. G oth Sarty, A oth Shin, I. K oth Smith, G. R oth Stepanyan, S oth Tang, L. G oth Tadevosyan, V oth Tvaskis, V oth van der Meer, R. L. J oth Vansyoc, K oth Van Westrum, D oth Vidakovic, S oth Volmer, J oth Vulcan, W oth Warren, G oth Wood, S. A oth Xu, C oth Yan, C oth Zhao, W. -X oth Zheng, X oth Zihlmann, B oth Collaboration, The Jefferson Lab Fpi oth Enthalten in Physical review / C Woodbury, NY : Inst., 1970 (2014) (DE-627)129508659 (DE-600)209771-0 (DE-576)01491493X 2469-9985 nnns year:2014 http://dx.doi.org/10.1103/PhysRevC.91.015202 Volltext http://arxiv.org/abs/1412.5140 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY SSG-OPC-AST GBV_ILN_21 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 UA 6500. AR 2014 |
spelling |
10.1103/PhysRevC.91.015202 doi PQ20160617 (DE-627)OLC1966212046 (DE-599)GBVOLC1966212046 (PRQ)a733-70b082594eaff6beee1d0a03a55de5ae779bb9495e483c92691e3fd53a918b6e0 (KEY)0054933920140000000000000000separatedresponsefunctionsinexclusiveforwardpipmel DE-627 ger DE-627 rakwb eng 530 DNB UA 6500. AVZ rvk Huber, G. M verfasserin aut Separated Response Functions in Exclusive, Forward \pi^{\pm} Electroproduction on Deuterium 2014 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Background: Measurements of forward exclusive meson production at different squared four-momenta of the exchanged virtual photon, Q^2, and at different four-momentum transfer, t, can be used to probe QCD's transition from meson-nucleon degrees of freedom at long distances to quark-gluon degrees of freedom at short scales. Ratios of separated response functions in \pi^- and \pi^+ electroproduction are particularly informative. The ratio for transverse photons may allow this transition to be more easily observed, while the ratio for longitudinal photons provides a crucial verification of the assumed pole dominance, needed for reliable extraction of the pion form factor from electroproduction data. Method: Data were acquired with 2.6-5.2 GeV electron beams and the HMS+SOS spectrometers in Jefferson Lab Hall C, at central Q^2 values of 0.6, 1.0, 1.6 GeV^2 at W=1.95 GeV, and Q^2=2.45 GeV^2 at W=2.22 GeV. There was significant coverage in \phi and \epsilon, which allowed separation of \sigma_{L,T,LT,TT}. Results: \sigma_L shows a clear signature of the pion pole, with a sharp rise at small -t. In contrast, \sigma_T is much flatter versus t. The longitudinal/transverse ratios evolve with Q^2 and t, and at the highest Q^2=2.45 GeV^2 show a slight enhancement for \pi^- production compared to \pi^+. The \pi^-/\pi^+ ratio for transverse photons exhibits only a small Q^2-dependence, following a nearly universal curve with t, with a steep transition to a value of about 0.25, consistent with s-channel quark knockout. The \sigma_{TT}/\sigma_T ratio also drops rapidly with Q^2, qualitatively consistent with s-channel helicity conservation. The \pi^-/\pi^+ ratio for longitudinal photons indicates a small isoscalar contamination at W=1.95 GeV, consistent with what was observed in our earlier determination of the pion form factor at these kinematics. Nuclear Experiment Blok, H. P oth Butuceanu, C oth Gaskell, D oth Horn, T oth Mack, D. J oth Abbott, D oth Aniol, K oth Anklin, H oth Armstrong, C oth Arrington, J oth Assamagan, K oth Avery, S oth Baker, O. K oth Barrett, B oth Beise, E. J oth Bochna, C oth Boeglin, W oth Brash, E. J oth Breuer, H oth Chang, C. C oth Chant, N oth Christy, M. E oth Dunne, J oth Eden, T oth Ent, R oth Fenker, H oth Gibson, E. F oth Gilman, R oth Gustafsson, K oth Hinton, W oth Holt, R. J oth Jackson, H oth Jin, S oth Jones, M. K oth Keppel, C. E oth Kim, P. H oth Kim, W oth King, P. M oth Klein, A oth Koltenuk, D oth Kovaltchouk, V oth Liang, M oth Liu, J oth Lolos, G. J oth Lung, A oth Margaziotis, D. J oth Markowitz, P oth Matsumura, A oth McKee, D oth Meekins, D oth Mitchell, J oth Miyoshi, T oth Mkrtchyan, H oth Mueller, B oth Niculescu, G oth Niculescu, I oth Okayasu, Y oth Pentchev, L oth Perdrisat, C oth Pitz, D oth Potterveld, D oth Punjabi, V oth Qin, L. M oth Reimer, P. E oth Reinhold, J oth Roche, J oth Roos, P. G oth Sarty, A oth Shin, I. K oth Smith, G. R oth Stepanyan, S oth Tang, L. G oth Tadevosyan, V oth Tvaskis, V oth van der Meer, R. L. J oth Vansyoc, K oth Van Westrum, D oth Vidakovic, S oth Volmer, J oth Vulcan, W oth Warren, G oth Wood, S. A oth Xu, C oth Yan, C oth Zhao, W. -X oth Zheng, X oth Zihlmann, B oth Collaboration, The Jefferson Lab Fpi oth Enthalten in Physical review / C Woodbury, NY : Inst., 1970 (2014) (DE-627)129508659 (DE-600)209771-0 (DE-576)01491493X 2469-9985 nnns year:2014 http://dx.doi.org/10.1103/PhysRevC.91.015202 Volltext http://arxiv.org/abs/1412.5140 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY SSG-OPC-AST GBV_ILN_21 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 UA 6500. AR 2014 |
allfields_unstemmed |
10.1103/PhysRevC.91.015202 doi PQ20160617 (DE-627)OLC1966212046 (DE-599)GBVOLC1966212046 (PRQ)a733-70b082594eaff6beee1d0a03a55de5ae779bb9495e483c92691e3fd53a918b6e0 (KEY)0054933920140000000000000000separatedresponsefunctionsinexclusiveforwardpipmel DE-627 ger DE-627 rakwb eng 530 DNB UA 6500. AVZ rvk Huber, G. M verfasserin aut Separated Response Functions in Exclusive, Forward \pi^{\pm} Electroproduction on Deuterium 2014 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Background: Measurements of forward exclusive meson production at different squared four-momenta of the exchanged virtual photon, Q^2, and at different four-momentum transfer, t, can be used to probe QCD's transition from meson-nucleon degrees of freedom at long distances to quark-gluon degrees of freedom at short scales. Ratios of separated response functions in \pi^- and \pi^+ electroproduction are particularly informative. The ratio for transverse photons may allow this transition to be more easily observed, while the ratio for longitudinal photons provides a crucial verification of the assumed pole dominance, needed for reliable extraction of the pion form factor from electroproduction data. Method: Data were acquired with 2.6-5.2 GeV electron beams and the HMS+SOS spectrometers in Jefferson Lab Hall C, at central Q^2 values of 0.6, 1.0, 1.6 GeV^2 at W=1.95 GeV, and Q^2=2.45 GeV^2 at W=2.22 GeV. There was significant coverage in \phi and \epsilon, which allowed separation of \sigma_{L,T,LT,TT}. Results: \sigma_L shows a clear signature of the pion pole, with a sharp rise at small -t. In contrast, \sigma_T is much flatter versus t. The longitudinal/transverse ratios evolve with Q^2 and t, and at the highest Q^2=2.45 GeV^2 show a slight enhancement for \pi^- production compared to \pi^+. The \pi^-/\pi^+ ratio for transverse photons exhibits only a small Q^2-dependence, following a nearly universal curve with t, with a steep transition to a value of about 0.25, consistent with s-channel quark knockout. The \sigma_{TT}/\sigma_T ratio also drops rapidly with Q^2, qualitatively consistent with s-channel helicity conservation. The \pi^-/\pi^+ ratio for longitudinal photons indicates a small isoscalar contamination at W=1.95 GeV, consistent with what was observed in our earlier determination of the pion form factor at these kinematics. Nuclear Experiment Blok, H. P oth Butuceanu, C oth Gaskell, D oth Horn, T oth Mack, D. J oth Abbott, D oth Aniol, K oth Anklin, H oth Armstrong, C oth Arrington, J oth Assamagan, K oth Avery, S oth Baker, O. K oth Barrett, B oth Beise, E. J oth Bochna, C oth Boeglin, W oth Brash, E. J oth Breuer, H oth Chang, C. C oth Chant, N oth Christy, M. E oth Dunne, J oth Eden, T oth Ent, R oth Fenker, H oth Gibson, E. F oth Gilman, R oth Gustafsson, K oth Hinton, W oth Holt, R. J oth Jackson, H oth Jin, S oth Jones, M. K oth Keppel, C. E oth Kim, P. H oth Kim, W oth King, P. M oth Klein, A oth Koltenuk, D oth Kovaltchouk, V oth Liang, M oth Liu, J oth Lolos, G. J oth Lung, A oth Margaziotis, D. J oth Markowitz, P oth Matsumura, A oth McKee, D oth Meekins, D oth Mitchell, J oth Miyoshi, T oth Mkrtchyan, H oth Mueller, B oth Niculescu, G oth Niculescu, I oth Okayasu, Y oth Pentchev, L oth Perdrisat, C oth Pitz, D oth Potterveld, D oth Punjabi, V oth Qin, L. M oth Reimer, P. E oth Reinhold, J oth Roche, J oth Roos, P. G oth Sarty, A oth Shin, I. K oth Smith, G. R oth Stepanyan, S oth Tang, L. G oth Tadevosyan, V oth Tvaskis, V oth van der Meer, R. L. J oth Vansyoc, K oth Van Westrum, D oth Vidakovic, S oth Volmer, J oth Vulcan, W oth Warren, G oth Wood, S. A oth Xu, C oth Yan, C oth Zhao, W. -X oth Zheng, X oth Zihlmann, B oth Collaboration, The Jefferson Lab Fpi oth Enthalten in Physical review / C Woodbury, NY : Inst., 1970 (2014) (DE-627)129508659 (DE-600)209771-0 (DE-576)01491493X 2469-9985 nnns year:2014 http://dx.doi.org/10.1103/PhysRevC.91.015202 Volltext http://arxiv.org/abs/1412.5140 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY SSG-OPC-AST GBV_ILN_21 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 UA 6500. AR 2014 |
allfieldsGer |
10.1103/PhysRevC.91.015202 doi PQ20160617 (DE-627)OLC1966212046 (DE-599)GBVOLC1966212046 (PRQ)a733-70b082594eaff6beee1d0a03a55de5ae779bb9495e483c92691e3fd53a918b6e0 (KEY)0054933920140000000000000000separatedresponsefunctionsinexclusiveforwardpipmel DE-627 ger DE-627 rakwb eng 530 DNB UA 6500. AVZ rvk Huber, G. M verfasserin aut Separated Response Functions in Exclusive, Forward \pi^{\pm} Electroproduction on Deuterium 2014 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Background: Measurements of forward exclusive meson production at different squared four-momenta of the exchanged virtual photon, Q^2, and at different four-momentum transfer, t, can be used to probe QCD's transition from meson-nucleon degrees of freedom at long distances to quark-gluon degrees of freedom at short scales. Ratios of separated response functions in \pi^- and \pi^+ electroproduction are particularly informative. The ratio for transverse photons may allow this transition to be more easily observed, while the ratio for longitudinal photons provides a crucial verification of the assumed pole dominance, needed for reliable extraction of the pion form factor from electroproduction data. Method: Data were acquired with 2.6-5.2 GeV electron beams and the HMS+SOS spectrometers in Jefferson Lab Hall C, at central Q^2 values of 0.6, 1.0, 1.6 GeV^2 at W=1.95 GeV, and Q^2=2.45 GeV^2 at W=2.22 GeV. There was significant coverage in \phi and \epsilon, which allowed separation of \sigma_{L,T,LT,TT}. Results: \sigma_L shows a clear signature of the pion pole, with a sharp rise at small -t. In contrast, \sigma_T is much flatter versus t. The longitudinal/transverse ratios evolve with Q^2 and t, and at the highest Q^2=2.45 GeV^2 show a slight enhancement for \pi^- production compared to \pi^+. The \pi^-/\pi^+ ratio for transverse photons exhibits only a small Q^2-dependence, following a nearly universal curve with t, with a steep transition to a value of about 0.25, consistent with s-channel quark knockout. The \sigma_{TT}/\sigma_T ratio also drops rapidly with Q^2, qualitatively consistent with s-channel helicity conservation. The \pi^-/\pi^+ ratio for longitudinal photons indicates a small isoscalar contamination at W=1.95 GeV, consistent with what was observed in our earlier determination of the pion form factor at these kinematics. Nuclear Experiment Blok, H. P oth Butuceanu, C oth Gaskell, D oth Horn, T oth Mack, D. J oth Abbott, D oth Aniol, K oth Anklin, H oth Armstrong, C oth Arrington, J oth Assamagan, K oth Avery, S oth Baker, O. K oth Barrett, B oth Beise, E. J oth Bochna, C oth Boeglin, W oth Brash, E. J oth Breuer, H oth Chang, C. C oth Chant, N oth Christy, M. E oth Dunne, J oth Eden, T oth Ent, R oth Fenker, H oth Gibson, E. F oth Gilman, R oth Gustafsson, K oth Hinton, W oth Holt, R. J oth Jackson, H oth Jin, S oth Jones, M. K oth Keppel, C. E oth Kim, P. H oth Kim, W oth King, P. M oth Klein, A oth Koltenuk, D oth Kovaltchouk, V oth Liang, M oth Liu, J oth Lolos, G. J oth Lung, A oth Margaziotis, D. J oth Markowitz, P oth Matsumura, A oth McKee, D oth Meekins, D oth Mitchell, J oth Miyoshi, T oth Mkrtchyan, H oth Mueller, B oth Niculescu, G oth Niculescu, I oth Okayasu, Y oth Pentchev, L oth Perdrisat, C oth Pitz, D oth Potterveld, D oth Punjabi, V oth Qin, L. M oth Reimer, P. E oth Reinhold, J oth Roche, J oth Roos, P. G oth Sarty, A oth Shin, I. K oth Smith, G. R oth Stepanyan, S oth Tang, L. G oth Tadevosyan, V oth Tvaskis, V oth van der Meer, R. L. J oth Vansyoc, K oth Van Westrum, D oth Vidakovic, S oth Volmer, J oth Vulcan, W oth Warren, G oth Wood, S. A oth Xu, C oth Yan, C oth Zhao, W. -X oth Zheng, X oth Zihlmann, B oth Collaboration, The Jefferson Lab Fpi oth Enthalten in Physical review / C Woodbury, NY : Inst., 1970 (2014) (DE-627)129508659 (DE-600)209771-0 (DE-576)01491493X 2469-9985 nnns year:2014 http://dx.doi.org/10.1103/PhysRevC.91.015202 Volltext http://arxiv.org/abs/1412.5140 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY SSG-OPC-AST GBV_ILN_21 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 UA 6500. AR 2014 |
allfieldsSound |
10.1103/PhysRevC.91.015202 doi PQ20160617 (DE-627)OLC1966212046 (DE-599)GBVOLC1966212046 (PRQ)a733-70b082594eaff6beee1d0a03a55de5ae779bb9495e483c92691e3fd53a918b6e0 (KEY)0054933920140000000000000000separatedresponsefunctionsinexclusiveforwardpipmel DE-627 ger DE-627 rakwb eng 530 DNB UA 6500. AVZ rvk Huber, G. M verfasserin aut Separated Response Functions in Exclusive, Forward \pi^{\pm} Electroproduction on Deuterium 2014 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Background: Measurements of forward exclusive meson production at different squared four-momenta of the exchanged virtual photon, Q^2, and at different four-momentum transfer, t, can be used to probe QCD's transition from meson-nucleon degrees of freedom at long distances to quark-gluon degrees of freedom at short scales. Ratios of separated response functions in \pi^- and \pi^+ electroproduction are particularly informative. The ratio for transverse photons may allow this transition to be more easily observed, while the ratio for longitudinal photons provides a crucial verification of the assumed pole dominance, needed for reliable extraction of the pion form factor from electroproduction data. Method: Data were acquired with 2.6-5.2 GeV electron beams and the HMS+SOS spectrometers in Jefferson Lab Hall C, at central Q^2 values of 0.6, 1.0, 1.6 GeV^2 at W=1.95 GeV, and Q^2=2.45 GeV^2 at W=2.22 GeV. There was significant coverage in \phi and \epsilon, which allowed separation of \sigma_{L,T,LT,TT}. Results: \sigma_L shows a clear signature of the pion pole, with a sharp rise at small -t. In contrast, \sigma_T is much flatter versus t. The longitudinal/transverse ratios evolve with Q^2 and t, and at the highest Q^2=2.45 GeV^2 show a slight enhancement for \pi^- production compared to \pi^+. The \pi^-/\pi^+ ratio for transverse photons exhibits only a small Q^2-dependence, following a nearly universal curve with t, with a steep transition to a value of about 0.25, consistent with s-channel quark knockout. The \sigma_{TT}/\sigma_T ratio also drops rapidly with Q^2, qualitatively consistent with s-channel helicity conservation. The \pi^-/\pi^+ ratio for longitudinal photons indicates a small isoscalar contamination at W=1.95 GeV, consistent with what was observed in our earlier determination of the pion form factor at these kinematics. Nuclear Experiment Blok, H. P oth Butuceanu, C oth Gaskell, D oth Horn, T oth Mack, D. J oth Abbott, D oth Aniol, K oth Anklin, H oth Armstrong, C oth Arrington, J oth Assamagan, K oth Avery, S oth Baker, O. K oth Barrett, B oth Beise, E. J oth Bochna, C oth Boeglin, W oth Brash, E. J oth Breuer, H oth Chang, C. C oth Chant, N oth Christy, M. E oth Dunne, J oth Eden, T oth Ent, R oth Fenker, H oth Gibson, E. F oth Gilman, R oth Gustafsson, K oth Hinton, W oth Holt, R. J oth Jackson, H oth Jin, S oth Jones, M. K oth Keppel, C. E oth Kim, P. H oth Kim, W oth King, P. M oth Klein, A oth Koltenuk, D oth Kovaltchouk, V oth Liang, M oth Liu, J oth Lolos, G. J oth Lung, A oth Margaziotis, D. J oth Markowitz, P oth Matsumura, A oth McKee, D oth Meekins, D oth Mitchell, J oth Miyoshi, T oth Mkrtchyan, H oth Mueller, B oth Niculescu, G oth Niculescu, I oth Okayasu, Y oth Pentchev, L oth Perdrisat, C oth Pitz, D oth Potterveld, D oth Punjabi, V oth Qin, L. M oth Reimer, P. E oth Reinhold, J oth Roche, J oth Roos, P. G oth Sarty, A oth Shin, I. K oth Smith, G. R oth Stepanyan, S oth Tang, L. G oth Tadevosyan, V oth Tvaskis, V oth van der Meer, R. L. J oth Vansyoc, K oth Van Westrum, D oth Vidakovic, S oth Volmer, J oth Vulcan, W oth Warren, G oth Wood, S. A oth Xu, C oth Yan, C oth Zhao, W. -X oth Zheng, X oth Zihlmann, B oth Collaboration, The Jefferson Lab Fpi oth Enthalten in Physical review / C Woodbury, NY : Inst., 1970 (2014) (DE-627)129508659 (DE-600)209771-0 (DE-576)01491493X 2469-9985 nnns year:2014 http://dx.doi.org/10.1103/PhysRevC.91.015202 Volltext http://arxiv.org/abs/1412.5140 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY SSG-OPC-AST GBV_ILN_21 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 UA 6500. AR 2014 |
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Huber, G. M @@aut@@ Blok, H. P @@oth@@ Butuceanu, C @@oth@@ Gaskell, D @@oth@@ Horn, T @@oth@@ Mack, D. J @@oth@@ Abbott, D @@oth@@ Aniol, K @@oth@@ Anklin, H @@oth@@ Armstrong, C @@oth@@ Arrington, J @@oth@@ Assamagan, K @@oth@@ Avery, S @@oth@@ Baker, O. K @@oth@@ Barrett, B @@oth@@ Beise, E. J @@oth@@ Bochna, C @@oth@@ Boeglin, W @@oth@@ Brash, E. J @@oth@@ Breuer, H @@oth@@ Chang, C. C @@oth@@ Chant, N @@oth@@ Christy, M. E @@oth@@ Dunne, J @@oth@@ Eden, T @@oth@@ Ent, R @@oth@@ Fenker, H @@oth@@ Gibson, E. F @@oth@@ Gilman, R @@oth@@ Gustafsson, K @@oth@@ Hinton, W @@oth@@ Holt, R. J @@oth@@ Jackson, H @@oth@@ Jin, S @@oth@@ Jones, M. K @@oth@@ Keppel, C. E @@oth@@ Kim, P. H @@oth@@ Kim, W @@oth@@ King, P. M @@oth@@ Klein, A @@oth@@ Koltenuk, D @@oth@@ Kovaltchouk, V @@oth@@ Liang, M @@oth@@ Liu, J @@oth@@ Lolos, G. J @@oth@@ Lung, A @@oth@@ Margaziotis, D. J @@oth@@ Markowitz, P @@oth@@ Matsumura, A @@oth@@ McKee, D @@oth@@ Meekins, D @@oth@@ Mitchell, J @@oth@@ Miyoshi, T @@oth@@ Mkrtchyan, H @@oth@@ Mueller, B @@oth@@ Niculescu, G @@oth@@ Niculescu, I @@oth@@ Okayasu, Y @@oth@@ Pentchev, L @@oth@@ Perdrisat, C @@oth@@ Pitz, D @@oth@@ Potterveld, D @@oth@@ Punjabi, V @@oth@@ Qin, L. M @@oth@@ Reimer, P. E @@oth@@ Reinhold, J @@oth@@ Roche, J @@oth@@ Roos, P. G @@oth@@ Sarty, A @@oth@@ Shin, I. K @@oth@@ Smith, G. R @@oth@@ Stepanyan, S @@oth@@ Tang, L. G @@oth@@ Tadevosyan, V @@oth@@ Tvaskis, V @@oth@@ van der Meer, R. L. J @@oth@@ Vansyoc, K @@oth@@ Van Westrum, D @@oth@@ Vidakovic, S @@oth@@ Volmer, J @@oth@@ Vulcan, W @@oth@@ Warren, G @@oth@@ Wood, S. A @@oth@@ Xu, C @@oth@@ Yan, C @@oth@@ Zhao, W. -X @@oth@@ Zheng, X @@oth@@ Zihlmann, B @@oth@@ Collaboration, The Jefferson Lab Fpi @@oth@@ |
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2014-01-01T00:00:00Z |
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M</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Separated Response Functions in Exclusive, Forward \pi^{\pm} Electroproduction on Deuterium</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2014</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Background: Measurements of forward exclusive meson production at different squared four-momenta of the exchanged virtual photon, Q^2, and at different four-momentum transfer, t, can be used to probe QCD's transition from meson-nucleon degrees of freedom at long distances to quark-gluon degrees of freedom at short scales. 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Separated Response Functions in Exclusive, Forward \pi^{\pm} Electroproduction on Deuterium |
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Separated Response Functions in Exclusive, Forward \pi^{\pm} Electroproduction on Deuterium |
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separated response functions in exclusive, forward \pi^{\pm} electroproduction on deuterium |
title_auth |
Separated Response Functions in Exclusive, Forward \pi^{\pm} Electroproduction on Deuterium |
abstract |
Background: Measurements of forward exclusive meson production at different squared four-momenta of the exchanged virtual photon, Q^2, and at different four-momentum transfer, t, can be used to probe QCD's transition from meson-nucleon degrees of freedom at long distances to quark-gluon degrees of freedom at short scales. Ratios of separated response functions in \pi^- and \pi^+ electroproduction are particularly informative. The ratio for transverse photons may allow this transition to be more easily observed, while the ratio for longitudinal photons provides a crucial verification of the assumed pole dominance, needed for reliable extraction of the pion form factor from electroproduction data. Method: Data were acquired with 2.6-5.2 GeV electron beams and the HMS+SOS spectrometers in Jefferson Lab Hall C, at central Q^2 values of 0.6, 1.0, 1.6 GeV^2 at W=1.95 GeV, and Q^2=2.45 GeV^2 at W=2.22 GeV. There was significant coverage in \phi and \epsilon, which allowed separation of \sigma_{L,T,LT,TT}. Results: \sigma_L shows a clear signature of the pion pole, with a sharp rise at small -t. In contrast, \sigma_T is much flatter versus t. The longitudinal/transverse ratios evolve with Q^2 and t, and at the highest Q^2=2.45 GeV^2 show a slight enhancement for \pi^- production compared to \pi^+. The \pi^-/\pi^+ ratio for transverse photons exhibits only a small Q^2-dependence, following a nearly universal curve with t, with a steep transition to a value of about 0.25, consistent with s-channel quark knockout. The \sigma_{TT}/\sigma_T ratio also drops rapidly with Q^2, qualitatively consistent with s-channel helicity conservation. The \pi^-/\pi^+ ratio for longitudinal photons indicates a small isoscalar contamination at W=1.95 GeV, consistent with what was observed in our earlier determination of the pion form factor at these kinematics. |
abstractGer |
Background: Measurements of forward exclusive meson production at different squared four-momenta of the exchanged virtual photon, Q^2, and at different four-momentum transfer, t, can be used to probe QCD's transition from meson-nucleon degrees of freedom at long distances to quark-gluon degrees of freedom at short scales. Ratios of separated response functions in \pi^- and \pi^+ electroproduction are particularly informative. The ratio for transverse photons may allow this transition to be more easily observed, while the ratio for longitudinal photons provides a crucial verification of the assumed pole dominance, needed for reliable extraction of the pion form factor from electroproduction data. Method: Data were acquired with 2.6-5.2 GeV electron beams and the HMS+SOS spectrometers in Jefferson Lab Hall C, at central Q^2 values of 0.6, 1.0, 1.6 GeV^2 at W=1.95 GeV, and Q^2=2.45 GeV^2 at W=2.22 GeV. There was significant coverage in \phi and \epsilon, which allowed separation of \sigma_{L,T,LT,TT}. Results: \sigma_L shows a clear signature of the pion pole, with a sharp rise at small -t. In contrast, \sigma_T is much flatter versus t. The longitudinal/transverse ratios evolve with Q^2 and t, and at the highest Q^2=2.45 GeV^2 show a slight enhancement for \pi^- production compared to \pi^+. The \pi^-/\pi^+ ratio for transverse photons exhibits only a small Q^2-dependence, following a nearly universal curve with t, with a steep transition to a value of about 0.25, consistent with s-channel quark knockout. The \sigma_{TT}/\sigma_T ratio also drops rapidly with Q^2, qualitatively consistent with s-channel helicity conservation. The \pi^-/\pi^+ ratio for longitudinal photons indicates a small isoscalar contamination at W=1.95 GeV, consistent with what was observed in our earlier determination of the pion form factor at these kinematics. |
abstract_unstemmed |
Background: Measurements of forward exclusive meson production at different squared four-momenta of the exchanged virtual photon, Q^2, and at different four-momentum transfer, t, can be used to probe QCD's transition from meson-nucleon degrees of freedom at long distances to quark-gluon degrees of freedom at short scales. Ratios of separated response functions in \pi^- and \pi^+ electroproduction are particularly informative. The ratio for transverse photons may allow this transition to be more easily observed, while the ratio for longitudinal photons provides a crucial verification of the assumed pole dominance, needed for reliable extraction of the pion form factor from electroproduction data. Method: Data were acquired with 2.6-5.2 GeV electron beams and the HMS+SOS spectrometers in Jefferson Lab Hall C, at central Q^2 values of 0.6, 1.0, 1.6 GeV^2 at W=1.95 GeV, and Q^2=2.45 GeV^2 at W=2.22 GeV. There was significant coverage in \phi and \epsilon, which allowed separation of \sigma_{L,T,LT,TT}. Results: \sigma_L shows a clear signature of the pion pole, with a sharp rise at small -t. In contrast, \sigma_T is much flatter versus t. The longitudinal/transverse ratios evolve with Q^2 and t, and at the highest Q^2=2.45 GeV^2 show a slight enhancement for \pi^- production compared to \pi^+. The \pi^-/\pi^+ ratio for transverse photons exhibits only a small Q^2-dependence, following a nearly universal curve with t, with a steep transition to a value of about 0.25, consistent with s-channel quark knockout. The \sigma_{TT}/\sigma_T ratio also drops rapidly with Q^2, qualitatively consistent with s-channel helicity conservation. The \pi^-/\pi^+ ratio for longitudinal photons indicates a small isoscalar contamination at W=1.95 GeV, consistent with what was observed in our earlier determination of the pion form factor at these kinematics. |
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title_short |
Separated Response Functions in Exclusive, Forward \pi^{\pm} Electroproduction on Deuterium |
url |
http://dx.doi.org/10.1103/PhysRevC.91.015202 http://arxiv.org/abs/1412.5140 |
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Blok, H. P Butuceanu, C Gaskell, D Horn, T Mack, D. J Abbott, D Aniol, K Anklin, H Armstrong, C Arrington, J Assamagan, K Avery, S Baker, O. K Barrett, B Beise, E. J Bochna, C Boeglin, W Brash, E. J Breuer, H Chang, C. C Chant, N Christy, M. E Dunne, J Eden, T Ent, R Fenker, H Gibson, E. F Gilman, R Gustafsson, K Hinton, W Holt, R. J Jackson, H Jin, S Jones, M. K Keppel, C. E Kim, P. H Kim, W King, P. M Klein, A Koltenuk, D Kovaltchouk, V Liang, M Liu, J Lolos, G. J Lung, A Margaziotis, D. J Markowitz, P Matsumura, A McKee, D Meekins, D Mitchell, J Miyoshi, T Mkrtchyan, H Mueller, B Niculescu, G Niculescu, I Okayasu, Y Pentchev, L Perdrisat, C Pitz, D Potterveld, D Punjabi, V Qin, L. M Reimer, P. E Reinhold, J Roche, J Roos, P. G Sarty, A Shin, I. K Smith, G. R Stepanyan, S Tang, L. G Tadevosyan, V Tvaskis, V van der Meer, R. L. J Vansyoc, K Van Westrum, D Vidakovic, S Volmer, J Vulcan, W Warren, G Wood, S. A Xu, C Yan, C Zhao, W. -X Zheng, X Zihlmann, B Collaboration, The Jefferson Lab Fpi |
author2Str |
Blok, H. P Butuceanu, C Gaskell, D Horn, T Mack, D. J Abbott, D Aniol, K Anklin, H Armstrong, C Arrington, J Assamagan, K Avery, S Baker, O. K Barrett, B Beise, E. J Bochna, C Boeglin, W Brash, E. J Breuer, H Chang, C. C Chant, N Christy, M. E Dunne, J Eden, T Ent, R Fenker, H Gibson, E. F Gilman, R Gustafsson, K Hinton, W Holt, R. J Jackson, H Jin, S Jones, M. K Keppel, C. E Kim, P. H Kim, W King, P. M Klein, A Koltenuk, D Kovaltchouk, V Liang, M Liu, J Lolos, G. J Lung, A Margaziotis, D. J Markowitz, P Matsumura, A McKee, D Meekins, D Mitchell, J Miyoshi, T Mkrtchyan, H Mueller, B Niculescu, G Niculescu, I Okayasu, Y Pentchev, L Perdrisat, C Pitz, D Potterveld, D Punjabi, V Qin, L. M Reimer, P. E Reinhold, J Roche, J Roos, P. G Sarty, A Shin, I. K Smith, G. R Stepanyan, S Tang, L. G Tadevosyan, V Tvaskis, V van der Meer, R. L. J Vansyoc, K Van Westrum, D Vidakovic, S Volmer, J Vulcan, W Warren, G Wood, S. A Xu, C Yan, C Zhao, W. -X Zheng, X Zihlmann, B Collaboration, The Jefferson Lab Fpi |
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M</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Separated Response Functions in Exclusive, Forward \pi^{\pm} Electroproduction on Deuterium</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2014</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Background: Measurements of forward exclusive meson production at different squared four-momenta of the exchanged virtual photon, Q^2, and at different four-momentum transfer, t, can be used to probe QCD's transition from meson-nucleon degrees of freedom at long distances to quark-gluon degrees of freedom at short scales. Ratios of separated response functions in \pi^- and \pi^+ electroproduction are particularly informative. The ratio for transverse photons may allow this transition to be more easily observed, while the ratio for longitudinal photons provides a crucial verification of the assumed pole dominance, needed for reliable extraction of the pion form factor from electroproduction data. Method: Data were acquired with 2.6-5.2 GeV electron beams and the HMS+SOS spectrometers in Jefferson Lab Hall C, at central Q^2 values of 0.6, 1.0, 1.6 GeV^2 at W=1.95 GeV, and Q^2=2.45 GeV^2 at W=2.22 GeV. There was significant coverage in \phi and \epsilon, which allowed separation of \sigma_{L,T,LT,TT}. Results: \sigma_L shows a clear signature of the pion pole, with a sharp rise at small -t. In contrast, \sigma_T is much flatter versus t. The longitudinal/transverse ratios evolve with Q^2 and t, and at the highest Q^2=2.45 GeV^2 show a slight enhancement for \pi^- production compared to \pi^+. The \pi^-/\pi^+ ratio for transverse photons exhibits only a small Q^2-dependence, following a nearly universal curve with t, with a steep transition to a value of about 0.25, consistent with s-channel quark knockout. The \sigma_{TT}/\sigma_T ratio also drops rapidly with Q^2, qualitatively consistent with s-channel helicity conservation. The \pi^-/\pi^+ ratio for longitudinal photons indicates a small isoscalar contamination at W=1.95 GeV, consistent with what was observed in our earlier determination of the pion form factor at these kinematics.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Nuclear Experiment</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Blok, H. P</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Butuceanu, C</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Gaskell, D</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Horn, T</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Mack, D. J</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Abbott, D</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Aniol, K</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Anklin, H</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Armstrong, C</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Arrington, J</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Assamagan, K</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Avery, S</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Baker, O. K</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Barrett, B</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Beise, E. J</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Bochna, C</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Boeglin, W</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Brash, E. J</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Breuer, H</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Chang, C. C</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Chant, N</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Christy, M. E</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Dunne, J</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Eden, T</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Ent, R</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Fenker, H</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Gibson, E. 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