Related papers: Deep exclusive charged $\pi$ electroproduction abo…

Neutral pion electroproduction in $p(e,e'\pi^0)p$ above $\sqrt{s}>2$ GeV

Electroproduction of neutral pions in exclusive reaction $p(e,e'\pi^0)p$ is studied above the resonance region, $\sqrt{s}>2$ GeV. The reaction amplitude is described by exchanges of vector $\omega(782)$, $\rho(770)$ and axial-vector…

Nuclear Theory · Physics 2011-05-11 Murat M. Kaskulov

Deep exclusive electroproduction of $\pi^+$ at HERMES

Deeply virtual electroproduction of pion in exclusive reaction $p(e,e'\pi^+)n$ is studied using a two-component model which includes soft hadronic and hard partonic reaction mechanisms. The results are compared with the experimental data…

High Energy Physics - Phenomenology · Physics 2009-09-11 Murat M. Kaskulov , Ulrich Mosel

Exclusive pion electroproduction off nucleons and nuclei

We present our results for the exclusive electroproduction of pions off nucleons and nuclei at high values of $Q^2$. In electroproduction of nuclei $A(e,e'\pi)$ we consider the Color Transparency (CT) effect recently observed at JLAB. It is…

Nuclear Theory · Physics 2011-03-09 Murat M. Kaskulov , Ulrich Mosel

Beam spin asymmetry in deeply virtual $\pi$ production

An interpretation of the beam spin azimuthal asymmetries measured at JLAB in deep exclusive electroproduction of charged and neutral pions is presented. The model combines a Regge pole approach with the effect of nucleon resonances. The…

High Energy Physics - Phenomenology · Physics 2015-05-27 Murat M. Kaskulov , Ulrich Mosel

Deep exclusive electroproduction of $\pi^0$ at high $Q^2$ in the quark valence regime

We report measurements of the exclusive neutral pion electroproduction cross section off protons at large values of $x_B$ (0.36, 0.48 and 0.60) and $Q^2$ (3.1 to 8.4 GeV$^2$) obtained from Jefferson Lab Hall A experiment E12-06-014. The…

High Energy Physics - Experiment · Physics 2021-10-26 The Jefferson Lab Hall A Collaboration , M. Dlamini , B. Karki , S. F. Ali , P-J. Lin , F. Georges , H-S Ko , N. Israel , M. N. H. Rashad , A. Stefanko , D. Adikaram , Z. Ahmed , H. Albataineh , B. Aljawrneh , K. Allada , S. Allison , S. Alsalmi , D. Androic , K. Aniol , J. Annand , H. Atac , T. Averett , C. Ayerbe Gayoso , X. Bai , J. Bane , S. Barcus , K. Bartlett , V. Bellini , R. Beminiwattha , J. Bericic , D. Biswas , E. Brash , D. Bulumulla , J. Campbell , A. Camsonne , M. Carmignotto , J. Castellano , C. Chen , J-P. Chen , T. Chetry , M. E. Christy , E. Cisbani , B. Clary , E. Cohen , N. Compton , J. C. Cornejo , S. Covrig Dusa , B. Crowe , S. Danagoulian , T. Danley , F. De Persio , W. Deconinck , M. Defurne , C. Desnault , D. Di , M. Duer , B. Duran , R. Ent , C. Fanelli , G. Franklin , E. Fuchey , C. Gal , D. Gaskell , T. Gautam , O. Glamazdin , K. Gnanvo , V. M. Gray , C. Gu , T. Hague , G. Hamad , D. Hamilton , K. Hamilton , O. Hansen , F. Hauenstein , W. Henry , D. W. Higinbotham , T. Holmstrom , T. Horn , Y. Huang , G. M. Huber , C. Hyde , H. Ibrahim , C-M. Jen , K. Jin , M. Jones , A. Kabir , C. Keppel , V. Khachatryan , P. M. King , S. Li , W. Li , J. Liu , H. Liu , A. Liyanage , J. Magee , S. Malace , J. Mammei , P. Markowitz , E. McClellan , F. Meddi , D. Meekins , K. Mesik , R. Michaels , A. Mkrtchyan , R. Montgomery , C. Munoz Camacho , L. S. Myers , P. Nadel-Turonski , S. J. Nazeer , V. Nelyubin , D. Nguyen , N. Nuruzzaman , M. Nycz , O. F. Obretch , L. Ou , C. Palatchi , B. Pandey , S. Park , K. Park , C. Peng , R. Pomatsalyuk , E. Pooser , A. J. R. Puckett , V. Punjabi , B. Quinn , S. Rahman , P. E. Reimer , J. Roche , I. Sapkota , A. Sarty , B. Sawatzky , N. H. Saylor , B. Schmookler , M. H. Shabestari , A. Shahinyan , S. Sirca , G. R. Smith , S. Sooriyaarachchilage , N. Sparveris , R. Spies , T. Su , A. Subedi , V. Sulkosky , A. Sun , L. Thorne , Y. Tian , N. Ton , F. Tortorici , R. Trotta , G. M. Urciuoli , E. Voutier , B. Waidyawansa , Y. Wang , B. Wojtsekhowski , S. Wood , X. Yan , L. Ye , Z. Ye , C. Yero , J. Zhang , Y. Zhao , P. Zhu

Exclusive $\bm{\pi^{0}p}$ electroproduction off protons in the resonance region at photon virtualities 0.4~GeV$\bm{^{2}}$ $\bm{\leq~ Q^{2} \leq~1}$~GeV$\bm{^{2}}$

The exclusive electroproduction process $ep \rightarrow e'p'\pi^{0}$ was measured in the range of photon virtualities $Q^{2} = 0.4 - 1.0$~GeV$^{2}$ and the invariant mass range of the $p\pi^{0}$ system of $W = 1.1 - 1.8$~GeV. These…

Nuclear Experiment · Physics 2020-01-29 N. Markov , K. Joo , V. D. Burkert , V. I. Mokeev , L. C. Smith , M. Ungaro , S. Adhikari , M. J. ~Amaryan , G. Angelini , H. ~Atac , H. ~Avakian , C. Ayerbe Gayoso , N. A. ~Baltzell , L. Barion , M. ~Battaglieri , I. ~Bedlinskiy , I. ~Bedlinskiy , F. Benmokhtar , A. S. ~Biselli , F. ~Bossù , S. ~Boiarinov , W. J. ~Briscoe , W. K. ~Brooks , D. S. ~Carman , J. C. ~Carvajal , A. ~Celentano , P. ~Chatagnon , T. Chetry , P. L. ~Cole , M. ~Contalbrigo , V. ~Crede , G. Ciullo , A. ~D'Angelo , N. ~Dashyan , R. ~De~Vita , E. ~De~Sanctis , M. Defurne , A. ~Deur , S. Diehl , C. ~Djalali , R. ~Dupre , M. ~Ehrhart , A. ~El~Alaoui , L. ~El~Fassi , P. ~Eugenio , C. ~Evans , A. ~Filippi , Y. ~Ghandilyan , F. X. ~Girod , E. ~Golovatch , R. W. ~Gothe , K. A. ~Griffioen , M. ~Guidal , K. ~Hafidi , H. ~Hakobyan , M. ~Hattawy , T. B. ~Hayward , K. ~Hicks , M. ~Holtrop , Y. ~Ilieva , D. G. ~Ireland , B. S. ~Ishkhanov , E. L. ~Isupov , D. ~Jenkins , H. S. ~Jo , D. ~Keller , M. ~Khachatryan , A. ~Khanal , M. ~Khandaker , A. ~Kim , C. W. ~Kim , W. ~Kim , F. J. ~Klein , V. ~Kubarovsky , L. Lanza , M. ~Leali , K. ~Livingston , I . J . D. ~MacGregor , D. ~Marchand , V. ~Mascagna , B. ~McKinnon , T. ~Mineeva , M. ~Mirazita , P. ~Nadel-Turonski , S. ~Nanda , S. ~Niccolai , G. ~Niculescu , M. ~Osipenko , M. ~Paolone , L. L. ~Pappalardo , R. ~Paremuzyan , K. ~Park , E. ~Pasyuk , W. ~Phelps , O. ~Pogorelko , J. W. ~Price , Y. ~Prok , D. ~Protopopescu , M. ~Ripani , D. Riser , A. ~Rizzo , J. ~Rowley , F. ~Sabatié , C. ~Salgado , R. A. ~Schumacher , Y. G. ~Sharabian , U. ~Shrestha , D. ~Sokhan , O. ~Soto , N. ~Sparveris , S. ~Stepanyan , P. ~Stoler , I. I. ~Strakovsky , S. ~Strauch , M. ~Taiuti , J. A. ~Tan , N. ~Tyler , L. ~Venturelli , H. ~Voskanyan , E. ~Voutier , R. Wang , X. ~Wei , M. H. ~Wood , N. ~Zachariou

Pion and proton form factors in the Regge description of electroproduction $p(e,e'\pi^+)n$

Electroproduction of $\pi^+$ above the resonance region is analyzed in the Regge model for $\pi+\rho$ exchanges. Importance of the roles of pion and proton form factors in the process is discussed in comparison with existing models of…

Nuclear Theory · Physics 2015-12-01 Tae Keun Choi , Kook Jin Kong , Byung Geel Yu

Hard exclusive pion electroproduction at backward angles with CLAS

We report on the first measurement of cross sections for exclusive deeply virtual pion electroproduction off the proton, $e p \to e^\prime n \pi^+$, above the resonance region at backward pion center-of-mass angles. The…

Nuclear Experiment · Physics 2018-03-16 K. Park , M. Guidal , R. W. Gothe , B. Pire , K. Semenov-Tian-Shansky , J. -M. Laget

Resonance-Parton Duality in $(e,e'\pi)$ off Nucleons

Regge-pole based descriptions of pion-electroproduction on nucleons have given a very good description of the longitudinal components of the cross sections. However, these very same models grossly underestimate the transverse components. A…

Nuclear Theory · Physics 2015-06-03 Murat Kaskulov , Ulrich Mosel

Deep exclusive $\pi^+$ electroproduction off the proton at CLAS

The exclusive electroproduction of $\pi^+$ above the resonance region was studied using the $\rm{CEBAF}$ Large Acceptance Spectrometer ($\rm{CLAS}$) at Jefferson Laboratory by scattering a 6 GeV continuous electron beam off a hydrogen…

Nuclear Experiment · Physics 2013-01-29 K. Park , M. Guidal , R. W. Gothe , J. M. Laget , M. Garçon , K. P. Adhikari , M. Aghasyan , M. J. Amaryan , M. Anghinolfi , H. Avakian , H. Baghdasaryan , J. Ball , N. A. Baltzell , M. Battaglieri , I. Bedlinsky , R. P. Bennett , A. S. Biselli , C. Bookwalter , S. Boiarinov , W. J. Briscoe , W. K. Brooks , V. D. Burkert , D. S. Carman , A. Celentano , S. Chandavar , G. Charles , M. Contalbrigo , V. Crede , A. D'Angelo , A. Daniel , N. Dashyan , R. De Vita , E. De Sanctis , A. Deur , C. Djalali , G. E. Dodge , D. Doughty , R. Dupre , H. Egiyan , A. El Alaoui , L. El Fassi , A. Fradi , P. Eugenio , G. Fedotov , S. Fegan , J. A. Fleming , T. A. Forest , N. Gevorgyan , G. P. Gilfoyle , K. L. Giovanetti , F. X. Girod , W. Gohn , E. Golovatch , L. Graham , K. A. Griffioen , B. Guegan , L. Guo , K. Hafidi , H. Hakobyan , C. Hanretty , D. Heddle , K. Hicks , D. Ho , M. Holtrop , Y. Ilieva , D. G. Ireland , B. S. Ishkhanov , D. Jenkins , H. S. Jo , D. Keller , M. Khandaker , P. Khetarpal , A. Kim , W. Kim , F. J. Klein , S. Koirala , A. Kubarovsky , V. Kubarovsky , S. E. Kuhn , S. V. Kuleshov , K. Livingston , H. Y. Lu , I. J. D. MacGregor , Y. Mao , N. Markov , D. Martinez , M. Mayer , B. McKinnon , C. A. Meyer , T. Mineeva , M. Mirazita , V. Mokeev , H. Moutarde , E. Munevar , C. Munoz Camacho , P. Nadel-Turonski , C. S. Nepali , S. Niccolai , G. Niculescu , I. Niculescu , M. Osipenko , A. I. Ostrovidov , L. L. Pappalardo , R. Paremuzyan , S. Park , E. Pasyuk , S. Anefalos Pereira , E. Phelps , S. Pisano , O. Pogorelko , S. Pozdniakov , J. W. Price , S. Procureur , D. Protopopescu , A. J. R. Puckett , B. A. Raue , G. Ricco , D. Rimal , M. Ripani , G. Rosner , P. Rossi , F. Sabatie , M. S. Saini , C. Salgado , D. Schott , R. A. Schumacher , E. Seder , H. Seraydaryan , Y. G. Sharabian , E. S. Smith , G. D. Smith , D. I. Sober , D. Sokhan , S. S. Stepanyan , P. Stoler , I. I. Strakovsky , S. Strauch , M. Taiuti , W. Tang , C. E. Taylor , Ye Tian , S. Tkachenko , A. Trivedi , M. Ungaro , B . Vernarsky , H. Voskanyan , E. Voutier , N. K. Walford , D. P. Watts , L. B. Weinstein , D. P. Weygand , M. H. Wood , N. Zachariou , J. Zhang , Z. W. Zhao , I. Zonta

Probing hard/soft factorization via beam-spin asymmetry in exclusive pion electroproduction from the proton

Deep exclusive meson production (DEMP) reactions, such as $p(\vec{e},e'\pi^+)n$, provide opportunities to study the three-dimensional structure of the nucleon through differential cross section and beam- and target-spin asymmetry…

Nuclear Experiment · Physics 2026-02-20 Alicia C. Postuma , Garth M. Huber , D. J. Gaskell , N. Heinrich , T. Horn , M. Junaid , S. J. D. Kay , V. Kumar , P. Markowitz , J. Roche , R. Trotta , A. Usman , B. -G. Yu , T. K. Choi , K. -J. Kong , S. Ali , R. Ambrose , D. Androic , W. Armstrong , A. Bandari , V. Berdnikov , H. Bhatt , D. Bhetuwal , D. Biswas , M. Boer , P. Bosted , E. Brash , A. Camsonne , J. P. Chen , J. Chen , M. Chen , M. E. Christy , S. Covrig , M. M. Dalton , W. Deconinck , M. Diefenthaler , B. Duran , D. Dutta , M. Elaasar , R. Ent , H. Fenker , E. Fuchey , D. Hamilton , J. -O. Hansen , F. Hauenstein , S. Jia , M. K. Jones , S. Joosten , M. L. Kabir , A. Karki , C. Keppel , E. Kinney , N. Lashley-Colthirst , W. B. Li , D. Mack , S. Malace , M. McCaughan , Z. E. Meziani , R. Michaels , R. Montgomery , M. Muhoza , C. Munoz Camacho , G. Niculescu , I. Niculescu , Z. Papandreou , S. Park , E. Pooser , M. Rehfuss , B. Sawatzky , G. R. Smith , H. Szumila-Vance , A. Teymurazyan , H. Voskanyan , B. Wojtsekhowski , S. A. Wood , Z. Ye , C. Yero , J. Zhang , X. Zheng

First measurement of hard exclusive $\pi^- \Delta^{++}$ electroproduction beam-spin asymmetries off the proton

The polarized cross section ratio $\sigma_{LT'}/\sigma_{0}$ from hard exclusive $\pi^{-} \Delta^{++}$ electroproduction off an unpolarized hydrogen target has been extracted based on beam-spin asymmetry measurements using a 10.2 GeV / 10.6…

High Energy Physics - Experiment · Physics 2023-07-26 S. Diehl , N. Trotta , K. Joo , P. Achenbach , Z. Akbar , W. R. Armstrong , H. Atac , H. Avakian , L. Baashen , N. A. Baltzell , L. Barion , M. Bashkanov , M. Battaglieri , I. Bedlinskiy , F. Benmokhtar , A. Bianconi , A. S. Biselli , F. Bossu , K. -T. Brinkmann , W. J. Briscoe , D. Bulumulla , V. Burkert , R. Capobianco , D. S. Carman , J. C. Carvajal , A. Celentano , G. Charles , P. Chatagnon , V. Chesnokov , G. Ciullo , P. L. Cole , M. Contalbrigo , G. Costantini , V. Crede , A. D'Angelo , N. Dashyan , R. De Vita , A. Deur , C. Djalali , R. Dupre , M. Ehrhart , A. El Alaoui , L. El Fassi , L. Elouadrhiri , S. Fegan , A. Filippi , G. Gavalian , D. I. Glazier , A. A. Golubenko , G. Gosta , R. W. Gothe , Y. Gotra , K. Griffioen , K. Hafidi , H. Hakobyan , M. Hattawy , T. B. Hayward , D. Heddle , A. Hobart , M. Holtrop , I. Illari , D. G. Ireland , E. L. Isupov , H. S. Jo , R. Johnston , D. Keller , M. Khachatryan , A. Khanal , A. Kim , W. Kim , V. Klimenko , A. Kripko , V. Kubarovsky , S. E. Kuhn , V. Lagerquist , L. Lanza , M. Leali , S. Lee , P. Lenisa , X. Li , I . J . D. MacGregor , D. Marchand , V. Mascagna , G. Matousek , B. McKinnon , C. McLauchlin , Z. E. Meziani , S. Migliorati , R. G. Milner , T. Mineeva , M. Mirazita , V. Mokeev , P. Moran , C. Munoz Camacho , P. Naidoo , K. Neupane , S. Niccolai , G. Niculescu , M. Osipenko , P. Pandey , M. Paolone , L. L. Pappalardo , R. Paremuzyan , S. J. Paul , W. Phelps , N. Pilleux , M. Pokhrel , J. Poudel , J. W. Price , Y. Prok , A. Radic , B. A. Raue , T. Reed , J. Richards , M. Ripani , J. Ritman , P. Rossi , F. Sabatie , C. Salgado , S. Schadmand , A. Schmidt , Y. G. Sharabian , U. Shrestha , D. Sokhan , N. Sparveris , M. Spreafico , S. Stepanyan , I. Strakovsky , S. Strauch , M. Turisini , R. Tyson , M. Ungaro , S. Vallarino , L. Venturelli , H. Voskanyan , E. Voutier , D. P. Watts , X. Wei , R. Williams , R. Wishart , M. H. Wood , M. Yurov , N. Zachariou , Z. W. Zhao , M. Zurek

Exclusive ${\pi}^0$ electroproduction at $W>2$ GeV with CLAS

Exclusive neutral-pion electroproduction ($ep\to e^\prime p^\prime \pi^0$) was measured at Jefferson Lab with a 5.75-GeV electron beam and the CLAS detector. Differential cross sections $d^4\sigma/dtdQ^2dx_Bd\phi_\pi$ and structure…

Nuclear Experiment · Physics 2019-08-15 I. Bedlinskiy , V. Kubarovsky , S. Niccolai , P. Stoler , K. P. Adhikari , M. D. Anderson , S. Anefalos Pereira , H. Avakian , J. Ball , N. A. Baltzell , M. Battaglieri , V. Batourine , A. S. Biselli , S. Boiarinov , J. Bono , W. J. Briscoe , W. K. Brooks , V. D. Burkert , D. S. Carman , A. Celentano , S. Chandavar , L. Colaneri , P. L. Cole , M. Contalbrigo , O. Cortes , V. Crede , A. D'Angelo , N. Dashyan , R. De Vita , E. De Sanctis , A. Deur , C. Djalali , D. Doughty , R. Dupre , H. Egiyan , A. El Alaoui , L. El Fassi , L. Elouadrhiri , P. Eugenio , G. Fedotov , S. Fegan , J. A. Fleming , T. A. Forest , B. Garillon , M. Garçon , G. Gavalian , N. Gevorgyan , Y. Ghandilyan , G. P. Gilfoyle , K. L. Giovanetti , F. X. Girod , E. Golovatch , R. W. Gothe , K. A. Griffioen , B. Guegan , L. Guo , K. Hafidi , H. Hakobyan , N. Harrison , M. Hattawy , K. Hicks , M. Holtrop , D. G. Ireland , B. S. Ishkhanov , E. L. Isupov , D. Jenkins , H. S. Jo , K. Joo , D. Keller , M. Khandaker , A. Kim , W. Kim , A. Klein , F. J. Klein , S. Koirala , S. E. Kuhn , S. V. Kuleshov , P. Lenisa , W. I. Levine , K. Livingston , H. Y. Lu , I . J . D. MacGregor , N. Markov , M. Mayer , B. McKinnon , M. Mirazita , V. Mokeev , R. A. Montgomery , C. I. Moody , H. Moutarde , A Movsisyan , C. Munoz Camacho , P. Nadel-Turonski , I. Niculescu , M. Osipenko , A. I. Ostrovidov , L. L. Pappalardo , K. Park , S. Park , E. Pasyuk , E. Phelps , W. Phelps , J. J. Phillips , S. Pisano , O. Pogorelko , J. W. Price , Y. Prok , D. Protopopescu , S. Procureur , A. J. R. Puckett , B. A. Raue , M. Ripani , B. G. Ritchie , A. Rizzo , P. Rossi , P. Roy , F. Sabatié , C. Salgado , D. Schott , R. A. Schumacher , E. Seder , I. Senderovich , Y. G. Sharabian , A. Simonyan , G. D. Smith , D. I. Sober , D. Sokhan , S. S. Stepanyan , S. Strauch , V. Sytnik , W. Tang , Ye Tian , M. Ungaro , A. V. Vlassov , H. Voskanyan , E. Voutier , N. K. Walford , D. Watts , X. Wei , L. B. Weinstein , M. Yurov , N. Zachariou , L. Zana , J. Zhang , Z. W. Zhao , I. Zonta

Central exclusive diffractive production of two-pions from continuum and decays of resonances in the Regge-eikonal model

Calculations of central exclusive diffractive production (CEDP) of two pions via continuum and resonance mechanism are presented in the Regge-eikonal approach. Data from STAR, ISR, CDF and CMS were analysed and compared with theoretical…

High Energy Physics - Phenomenology · Physics 2023-02-28 R. A. Ryutin

Mechanisms of high energy polarized photoproduction of $\pi^{-}\Delta^{++}$

We present an amplitude analysis of high-energy polarized photoproduction of $\pi^-\Delta^{++}$ within a Regge exchange framework. A Regge amplitude model incorporating $\pi$, $\rho$, $b_1$, and $a_2$ trajectory exchanges is fit…

High Energy Physics - Phenomenology · Physics 2026-04-27 Vanamali Shastry , Łukasz Bibrzycki , Vincent Mathieu , Glòria Montaña , Alessandro Pilloni , César Fernández-Ramírez , Robert J. Perry , Arkaitz Rodas , Adam P. Szczepaniak , Daniel Winney

Higher Nucleon Resonances in Exclusive $(\gamma, \pi N)$ Reactions on Nuclei

We report calculations for exclusive pion photoproduction on nuclei beyond the first resonance region in the distorted wave impulse approximation. The elementary operator contains contributions from the resonances $P_{33}(1232)$,…

Nuclear Theory · Physics 2009-10-31 Frank X. Lee , C. Bennhold , S. S. Kamalov , L. E. Wright

Exclusive production of pion pairs with large invariant mass in nucleus-nucleus collisions

The cross section for exclusive $\pi^+\pi^-$ and $\pi^0\pi^0$ meson pairs production in peripheral ultrarelativistic heavy-ion collisions is calculated at the energy available at the CERN Large Hadron Collider, i.e., $\sqrt{s_{NN}}=3.5$…

Nuclear Theory · Physics 2011-10-31 Mariola Klusek-Gawenda , Antoni Szczurek

Cross sections and beam asymmetries for $\vev{e}p \to en\pi^+$ in the nucleon resonance region for $1.7 \le Q^2 \le 4.5 (GeV)^2$

The exclusive electroproduction process $\vec{e}p \to e^\prime n \pi^+$ was measured in the range of the photon virtuality $Q^2 = 1.7 - 4.5 \rm{GeV^2}$, and the invariant mass range for the $n\pi^+$ system of $W = 1.15 - 1.7 \rm{GeV}$ using…

Nuclear Experiment · Physics 2010-04-06 K. Park , V. D. Burkert , W. Kim , CLAS Collaboration

Hard exclusive electroproduction of a pion in the backward region

We study the scaling regime of pion electroproduction in the backward region, eN->e'N'pi. We compute the leading-twist amplitude in the kinematical region, where it factorises into a short-distance matrix element and long-distance dominated…

High Energy Physics - Phenomenology · Physics 2014-11-18 J. P. Lansberg , B. Pire , L. Szymanowski

Separated Response Function Ratios in Exclusive, Forward pi^{+/-} Electroproduction

The study of exclusive $\pi^{\pm}$ electroproduction on the nucleon, including separation of the various structure functions, is of interest for a number of reasons. The ratio $R_L=\sigma_L^{\pi^-}/\sigma_L^{\pi^+}$ is sensitive to…

Nuclear Experiment · Physics 2014-07-23 G. M. Huber , H. P. Blok , C. Butuceanu , D. Gaskell , T. Horn , D. J. Mack , D. Abbott , K. Aniol , H. Anklin , C. Armstrong , J. Arrington , K. Assamagan , S. Avery , O. K. Baker , B. Barrett , E. J. Beise , C. Bochna , W. Boeglin , E. J. Brash , H. Breuer , C. C. Chang , N. Chant , M. E. Christy , J. Dunne , T. Eden , R. Ent , H. Fenker , E. F. Gibson , R. Gilman , K. Gustafsson , W. Hinton , R. J. Holt , H. Jackson , S. Jin , M. K. Jones , C. E. Keppel , P. H. Kim , W. Kim , P. M. King , A. Klein , D. Koltenuk , V. Kovaltchouk , M. Liang , J. Liu , G. J. Lolos , A. Lung , D. J. Margaziotis , P. Markowitz , A. Matsumura , D. McKee , D. Meekins , J. Mitchell , T. Miyoshi , H. Mkrtchyan , B. Mueller , G. Niculescu , I. Niculescu , Y. Okayasu , L. Pentchev , C. Perdrisat , D. Pitz , D. Potterveld , V. Punjabi , L. M. Qin , P. E. Reimer , J. Reinhold , J. Roche , P. G. Roos , A. Sarty , I. K. Shin , G. R. Smith , S. Stepanyan , L. G. Tang , V. Tadevosyan , V. Tvaskis , R. L. J. van der Meer , K. Vansyoc , D. Van Westrum , S. Vidakovic , J. Volmer , W. Vulcan , G. Warren , S. A. Wood , C. Xu , C. Yan , W. -X. Zhao , X. Zheng , B. Zihlmann