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K_S^0 K_L^0 \\gamma$, $K_S^0 K_L^0 \\pi^+\\pi^-\\gamma$, $K_S^0 K_S^0 \\pi^+\\pi^-\\gamma$, and $K_S^0 K_S^0 K^+K^-\\gamma$, where the photon is radiated from the initial state, providing cross section measurements for the hadronic states over a continuum of center-of-mass energies. The results are based on 469 fb$^{-1}$ of data collected with the BaBar detector at SLAC. We observe the $\\phi(1020)$ resonance in the $K_S^0 K_L^0$ final state and measure the product of its electronic width and branching fraction with about 3% uncertainty. We present a measurement of the $e^+ e^-\\to K_S^0 K_L^0 $ cross section in the energy range from 1.06 to 2.2 GeV and observe the production of a resonance at 1.67 GeV. We present the first measurements of the $e^+ e^-\\to K_S^0 K_L^0 \\pi^+\\pi^-$, $K_S^0 K_S^0 \\pi^+\\pi^-$, and $K_S^0 K_S^0 K^+K^-$ cross sections, and study the intermediate resonance structures. We obtain the first observations of \\jpsi decay to the $K_S^0 K_L^0 \\pi^+\\pi^-$, $K_S^0 K_S^0 \\pi^+\\pi^-$, and $K_S^0 K_S^0 K^+K^-$ final states.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins1287920/1/csv","json":"https://www.hepdata.net/download/submission/ins1287920/1/json","root":"https://www.hepdata.net/download/submission/ins1287920/1/root","yaml":"https://www.hepdata.net/download/submission/ins1287920/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins1287920/1/yoda"}},"analyses":[{"analysis":"http://rivet.hepforge.org/analyses/BABAR_2014_I1287920","type":"rivet"}],"arxiv_id":"arXiv:1403.7593","authors":["Lees, J.P.","Poireau, V.","Tisserand, V.","Grauges, E.","Palano, A.","Eigen, G.","Stugu, B.","Brown, David Nathan","Kerth, L.T.","Kolomensky, Yu. 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measurement for PHI(1680).\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1287920/Table 6/csv","json":"https://www.hepdata.net/download/table/ins1287920/Table 6/json","root":"https://www.hepdata.net/download/table/ins1287920/Table 6/root","yaml":"https://www.hepdata.net/download/table/ins1287920/Table 6/yaml","yoda":"https://www.hepdata.net/download/table/ins1287920/Table 6/yoda"}},"authors":null,"collaborations":["BaBar"],"control_number":"64511","creation_date":"2014-03-29","data_keywords":{"cmenergies":[{"gte":1.08,"lte":2.16}],"observables":["M"],"phrases":["E+ E- Scattering","Inclusive","Strange production"],"reactions":["E+ E- --> KS KL GAMMA X"]},"date":"29 Mar 2014","doc_type":"datatable","doi":"10.17182/hepdata.64506.v1/t6","first_author":{"affiliation":"Annecy, LAPP","full_name":"Lees, J.P."},"id":64511,"inspire_id":1287920,"journal_info":"Phys.Rev.D 89 (2014) 092002","keywords":[{"name":"reactions","synonyms":"","value":"E+ E- --> KS KL GAMMA 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LAPP","full_name":"Lees, J.P."},{"affiliation":"Annecy, LAPP","full_name":"Poireau, V."},{"affiliation":"Annecy, LAPP","full_name":"Tisserand, V."},{"affiliation":"Barcelona U., ECM","full_name":"Grauges, E."},{"affiliation":"INFN, Bari","full_name":"Palano, A."},{"affiliation":"Bergen U.","full_name":"Eigen, G."},{"affiliation":"Bergen U.","full_name":"Stugu, B."},{"affiliation":"LBL, Berkeley","full_name":"Brown, David Nathan"},{"affiliation":"LBL, Berkeley","full_name":"Kerth, L.T."},{"affiliation":"LBL, Berkeley","full_name":"Kolomensky, Yu. G."}],"title":"Cross sections for the reactions $e^+ e^-\\to K_S^0 K_L^0$, $K_S^0 K_L^0 \\pi^+\\pi^-$, $K_S^0 K_S^0 \\pi^+\\pi^-$, and $K_S^0 K_S^0 K^+K^-$ from events with initial-state radiation","total_tables":8,"type":["article"],"uuid":"53f501c9-838a-4ce3-a58b-d54162766429","version":1,"year":"2014"},{"abstract":"We report results for the virtual photon asymmetry $A_1$ on the nucleon from new Jefferson Lab measurements. The experiment, which used the CEBAF Large Acceptance Spectrometer and longitudinally polarized proton ($^{15}$NH$_3$) and deuteron ($^{15}$ND$_3$) targets, collected data with a longitudinally polarized electron beam at energies between 1.6 GeV and 5.7 GeV. In the present paper, we concentrate on our results for $A_1(x,Q^2)$ and the related ratio $g_1/F_1(x,Q^2)$ in the resonance and the deep inelastic regions for our lowest and highest beam energies, covering a range in momentum transfer $Q^2$ from 0.05 to 5.0 GeV$^2$ and in final-state invariant mass $W$ up to about 3 GeV. Our data show detailed structure in the resonance region, which leads to a strong $Q^2$--dependence of $A_1(x,Q^2)$ for $W$ below 2 GeV. At higher $W$, a smooth approach to the scaling limit, established by earlier experiments, can be seen, but $A_1(x,Q^2)$ is not strictly $Q^2$--independent. We add significantly to the world data set at high $x$, up to $x = 0.6$. Our data exceed the SU(6)-symmetric quark model expectation for both the proton and the deuteron while being consistent with a negative $d$-quark polarization up to our highest $x$. This data setshould improve next-to-leading order (NLO) pQCD fits of the parton polarization distributions.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins717523/1/csv","json":"https://www.hepdata.net/download/submission/ins717523/1/json","root":"https://www.hepdata.net/download/submission/ins717523/1/root","yaml":"https://www.hepdata.net/download/submission/ins717523/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins717523/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:nucl-ex/0605028","authors":["Dharmawardane, K.V.","Kuhn, S.E.","Bosted, Peter E.","Prok, Y.","Adams, G.","Ambrozewicz, P.","Anghinolfi, M.","Asryan, G.","Avakian, H.","Baghdasaryan, Hovhannes"],"collaborations":["CLAS"],"control_number":"6726","creation_date":"2006-05-01","data":[{"abstract":"A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.3100 GeV.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins717523/Table 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The polarization vector is found to be compatible with zero.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins554759/1/csv","json":"https://www.hepdata.net/download/submission/ins554759/1/json","root":"https://www.hepdata.net/download/submission/ins554759/1/root","yaml":"https://www.hepdata.net/download/submission/ins554759/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins554759/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:hep-ex/0103047","authors":["Astier, P.","Autiero, D.","Baldisseri, A.","Baldo-Ceolin, M.","Banner, M.","Bassompierre, G.","Besson, N.","Bird, I.","Blumenfeld, B.","Bobisut, F."],"collaborations":["NOMAD"],"control_number":"48928","creation_date":"2001-03-01","data":[{"abstract":"Lambdabar polarization in regions of the Bjorken scaling variable X.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins554759/Table 2/csv","json":"https://www.hepdata.net/download/table/ins554759/Table 2/json","root":"https://www.hepdata.net/download/table/ins554759/Table 2/root","yaml":"https://www.hepdata.net/download/table/ins554759/Table 2/yaml","yoda":"https://www.hepdata.net/download/table/ins554759/Table 2/yoda"}},"authors":null,"collaborations":["NOMAD"],"control_number":"48938","creation_date":"2001-03-01","data_keywords":{"cmenergies":[{"gte":0.938,"lte":29.07}],"observables":["POL"],"phrases":["Polarization","Deep Inelastic Scattering","Strange production","Charged Current","Muon production","Inclusive"],"reactions":["NUMU NUCLEON --> MU- LAMBDABAR X"]},"date":"01 Mar 2001","doc_type":"datatable","doi":"10.17182/hepdata.48928.v1/t2","first_author":{"affiliation":"","full_name":"Astier, P."},"id":48938,"inspire_id":554759,"journal_info":"Nucl.Phys.B 605 (2001) 3-14","keywords":[{"name":"reactions","synonyms":"","value":"NUMU NUCLEON --> MU- LAMBDABAR X"},{"name":"observables","synonyms":"","value":"POL"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"phrases","synonyms":"","value":"Polarization"},{"name":"phrases","synonyms":"","value":"Strange production"},{"name":"phrases","synonyms":"","value":"Muon production"},{"name":"phrases","synonyms":"","value":"Charged Current"},{"name":"phrases","synonyms":"","value":"Deep Inelastic Scattering"},{"name":"cmenergies","synonyms":"","value":"0.938-29.07"}],"last_updated":"2016-10-14T15:50:07","parent_child_join":{"name":"child_datatable","parent":"48928"},"recid":48938,"related_publication":48928,"title":"Table 2","uuid":"ad1a9590-e9c3-4f0f-8607-5ce603d7cafb"}],"data_keywords":{"cmenergies":[{"gte":31.872,"lte":31.872},{"gte":0.938,"lte":29.07}],"observables":["POL"],"phrases":["Polarization","Deep Inelastic Scattering","Strange production","Charged Current","Muon production","Inclusive"],"reactions":["NUMU NUCLEON --> MU- LAMBDABAR X"]},"date":"01 Mar 2001","doc_type":"publication","doi":"10.1016/S0550-3213(01)00181-X","first_author":{"affiliation":"Paris U., VI-VII","full_name":"Astier, P."},"hepdata_doi":"10.17182/hepdata.48928","id":48928,"inspire_id":554759,"journal_info":"Nucl.Phys.B 605 (2001) 3-14","keywords":[{"schema":"INSPIRE","value":"neutrino nucleon: interaction"},{"schema":"INSPIRE","value":"neutrino/mu"},{"schema":"INSPIRE","value":"charged current"},{"schema":"INSPIRE","value":"Antilambda: neutrinoproduction"},{"schema":"INSPIRE","value":"Antilambda: hadronic decay"},{"schema":"INSPIRE","value":"Antilambda: polarization"},{"schema":"INSPIRE","value":"polarization: vector"},{"schema":"INSPIRE","value":"angular distribution"},{"schema":"INSPIRE","value":"magnetic detector: experimental results"},{"schema":"INSPIRE","value":"CERN SPS"},{"schema":"INSPIRE","value":"neutrino/mu nucleon --> Antilambda anything"},{"schema":"INSPIRE","value":"Antilambda --> anti-p pi+"}],"last_updated":"1993-11-02T00:00:00","parent_child_join":{"name":"parent_publication"},"publication_date":"2001-12-11T00:00:00","recid":48928,"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Paris U., VI-VII","full_name":"Astier, P."},{"affiliation":"CERN","full_name":"Autiero, D."},{"affiliation":"DAPNIA, Saclay","full_name":"Baldisseri, A."},{"affiliation":"INFN, Padua","full_name":"Baldo-Ceolin, M."},{"affiliation":"Paris U., VI-VII","full_name":"Banner, M."},{"affiliation":"Annecy, LAPP","full_name":"Bassompierre, G."},{"affiliation":"DAPNIA, Saclay","full_name":"Besson, N."},{"affiliation":"CERN","full_name":"Bird, I."},{"affiliation":"Johns Hopkins U.","full_name":"Blumenfeld, B."},{"affiliation":"INFN, Padua","full_name":"Bobisut, F."}],"title":"Measurement of the Antilambda polarization in nu/mu charged current interactions in the NOMAD experiment.","total_tables":1,"type":["article"],"uuid":"33762679-148d-40a8-b1dd-aba5b69ef10d","version":1,"year":"2001"},{"abstract":"We report measurements of the asymmetry A_parallel for inclusive hadron production on longitudinally polarized proton and deuteron targets by circularly polarized photons. The photons were produced via internal and external bremsstrahlung from an electron beam of 48.35 GeV. Asymmetries for both positive and negative signed hadrons, and a subset of identified pions, were measured in the momentum range 10
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The transverse and longitudinal structure functions have been separated by varying the polarization of the virtual photon (Rosenbluth plot) with a 3 to 4% error. In addition the longitudinal-transverse interference term has been determined measuring the right-left asymmetry with an accuracy of 3%. 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U.","full_name":"Beery, P.D."},{"affiliation":"Fermilab","full_name":"Bhat, P"},{"affiliation":"Notre Dame U.","full_name":"Bishop, J.M."},{"affiliation":"Notre Dame U.","full_name":"Biswas, N.N."},{"affiliation":"Purdue U.","full_name":"Bujak, A."}],"title":"Mass identified particle production in proton anti-proton collisions at s**(1/2) = 300-GeV, 540-GeV, 1000-GeV, and 1800-GeV","total_tables":2,"type":["article"],"uuid":"12c5d15b-7f51-4a20-997f-d37f3aa48972","version":1,"year":"1993"},{"abstract":"None","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins364824/1/csv","json":"https://www.hepdata.net/download/submission/ins364824/1/json","root":"https://www.hepdata.net/download/submission/ins364824/1/root","yaml":"https://www.hepdata.net/download/submission/ins364824/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins364824/1/yoda"}},"analyses":[],"arxiv_id":null,"authors":["Aleev, A.N.","Arefev, V.A.","Balandin, V.P.","Berdyshev, 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Jan 1993","doc_type":"publication","doi":null,"first_author":{"affiliation":"Dubna, JINR","full_name":"Aleev, A.N."},"hepdata_doi":"10.17182/hepdata.17203","id":17203,"inspire_id":364824,"journal_info":"Phys.Atom.Nucl. 56 (1993) 1235-1240","keywords":[{"schema":"INSPIRE","value":"p n: inclusive reaction"},{"schema":"INSPIRE","value":"p nucleus: inclusive reaction"},{"schema":"INSPIRE","value":"carbon"},{"schema":"INSPIRE","value":"aluminum"},{"schema":"INSPIRE","value":"anti-D0: hadroproduction"},{"schema":"INSPIRE","value":"hadroproduction: anti-D0"},{"schema":"INSPIRE","value":"anti-D0: nonleptonic decay"},{"schema":"INSPIRE","value":"nonleptonic decay: anti-D0"},{"schema":"INSPIRE","value":"mass spectrum: (K+ pi+ 2pi-)"},{"schema":"INSPIRE","value":"(K+ pi+ 2pi-): mass spectrum"},{"schema":"INSPIRE","value":"channel cross section: mass number"},{"schema":"INSPIRE","value":"mass number: channel cross section"},{"schema":"INSPIRE","value":"transverse momentum: 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JINR","full_name":"Berdyshev, V.K."},{"affiliation":"Dubna, JINR","full_name":"Birulev, V.K."},{"affiliation":"Dubna, JINR","full_name":"Guskov, B.N."},{"affiliation":"Dubna, JINR","full_name":"Eviskov, I.I."},{"affiliation":"Dubna, JINR","full_name":"Zinchenko, A.I."},{"affiliation":"Dubna, JINR","full_name":"Kapishin, M.N."},{"affiliation":"Dubna, JINR","full_name":"Karpenko, N.N."}],"title":"Anti-D0 meson production in interactions of neutrons with hydrogen, carbon, and aluminum nuclei at 37.5-GeV to 70-GeV","total_tables":6,"type":["article"],"uuid":"5527a6d4-eab6-4947-8891-506ffd98838a","version":1,"year":"1993"},{"abstract":"Using data onvp and\\(\\bar vp\\) charged current interactions from a bubble chamber experiment with BEBC at CERN, the average multiplicities of charged hadrons and pions are determined as functions ofW2 andQ2. The analysis is based on \u223c20000 events with incidentv and \u223c10000 events with incident\\(\\bar v\\). In addition to the known dependence of the average multiplicity onW2 a weak dependence onQ2 for fixed intervals ofW is observed. ForW>2 GeV andQ2>0.1 GeV2 the average multiplicity of charged hadrons is well described by\u3008n\u3009=a1+a2ln(W2/GeV2)+a3ln(Q2/GeV2) witha1=0.465\u00b10.053,a2=1.211\u00b10.021,a3=0.103\u00b10.014 for thevp anda1=\u22120.372\u00b10.073,a2=1.245\u00b10.028,a3=0.093\u00b10.015 for the\\(\\bar vp\\) reaction.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins305244/1/csv","json":"https://www.hepdata.net/download/submission/ins305244/1/json","root":"https://www.hepdata.net/download/submission/ins305244/1/root","yaml":"https://www.hepdata.net/download/submission/ins305244/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins305244/1/yoda"}},"analyses":[],"arxiv_id":null,"authors":["Jones, G.T.","Jones, R.W.L.","Morrison, Douglas R.O.","Mobayyen, M.M.","Wainstein, S.","Aderholz, M.","Hantke, D.","Hoffmann, E.","Katz, U.F.","Kern, J."],"collaborations":["WA21"],"control_number":"1699","creation_date":"1990-01-01","data":[{"abstract":"No description 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Semileptonic B Decay","total_tables":2,"type":["article"],"uuid":"b4276bb2-2254-4913-a580-2ef7ba846787","version":1,"year":"1984"},{"abstract":"We present new high statistics data on hadron production in photon-photon reactions. The data are analyzed in terms of an electron-photon scattering formalism. The dependence of the total cross section of Q 2 , the four-momentum transfer squared of the scattered electron, and on the mass W of the hadronic system is investigated. The data are compared to predictions from Vector-Meson Dominance and the quark model.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins155594/1/csv","json":"https://www.hepdata.net/download/submission/ins155594/1/json","root":"https://www.hepdata.net/download/submission/ins155594/1/root","yaml":"https://www.hepdata.net/download/submission/ins155594/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins155594/1/yoda"}},"analyses":[],"arxiv_id":null,"authors":["Berger, Christoph","Genzel, H.","Grigull, R.","Lackas, W.","Raupach, F.","Klovning, A.","Lillestol, E.","Skard, J.A.","Ackermann, H.","Burger, J."],"collaborations":["PLUTO"],"control_number":"27125","creation_date":"1980-10-01","data":[{"abstract":"DEPENDENCE ON VISIBLE HADRONIC INVARIANT MASS.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins155594/Table 2/csv","json":"https://www.hepdata.net/download/table/ins155594/Table 2/json","root":"https://www.hepdata.net/download/table/ins155594/Table 2/root","yaml":"https://www.hepdata.net/download/table/ins155594/Table 2/yaml","yoda":"https://www.hepdata.net/download/table/ins155594/Table 2/yoda"}},"authors":null,"collaborations":["PLUTO"],"control_number":"27132","creation_date":"1980-10-01","data_keywords":{"cmenergies":[{"gte":1.0,"lte":7.0}],"observables":["SIG"],"phrases":["Exclusive","Integrated Cross Section","Cross Section","Photoproduction"],"reactions":["GAMMA* GAMMA --> HADRONS"]},"date":"01 Oct 1980","doc_type":"datatable","doi":"10.17182/hepdata.27125.v1/t2","first_author":{"affiliation":"Aachen, Tech. Hochsch.","full_name":"Berger, Christoph"},"id":27132,"inspire_id":155594,"journal_info":"Phys.Lett.B 99 (1981) 287-291","keywords":[{"name":"reactions","synonyms":"","value":"GAMMA* GAMMA --> HADRONS"},{"name":"observables","synonyms":"","value":"SIG"},{"name":"phrases","synonyms":"","value":"Exclusive"},{"name":"phrases","synonyms":"","value":"Integrated Cross Section"},{"name":"phrases","synonyms":"","value":"Cross Section"},{"name":"phrases","synonyms":"","value":"Photoproduction"},{"name":"cmenergies","synonyms":"","value":"1.0-7.0"}],"last_updated":"2016-10-14T14:18:20","parent_child_join":{"name":"child_datatable","parent":"27125"},"recid":27132,"related_publication":27125,"title":"Table 2","uuid":"5f17a895-a3ec-4690-ab76-f3cad9236b53"}],"data_keywords":{"cmenergies":[{"gte":31.0,"lte":32.0},{"gte":1.0,"lte":7.0},{"gte":0.0,"lte":0.0}],"observables":["DN/DPT**2","SIG"],"phrases":["Two-Photon","Transverse Momentum Dependence","Exclusive","Integrated Cross Section","Cross Section","Photoproduction","Single Differential Distribution","E+ E- Scattering","Inclusive"],"reactions":["GAMMA* GAMMA --> HADRONS","E+ E- --> HADRON- X","E+ E- --> HADRON+ X","GAMMA GAMMA --> HADRONS"]},"date":"01 Oct 1980","doc_type":"publication","doi":"10.1016/0370-2693(81)91127-8","first_author":{"affiliation":"Aachen, Tech. Hochsch.","full_name":"Berger, Christoph"},"hepdata_doi":"10.17182/hepdata.27125","id":27125,"inspire_id":155594,"journal_info":"Phys.Lett.B 99 (1981) 287-291","keywords":[{"schema":"INSPIRE","value":"ELECTRON POSITRON: INCLUSIVE REACTION"},{"schema":"INSPIRE","value":"ELECTRON POSITRON: COLLIDING BEAMS"},{"schema":"INSPIRE","value":"COLLIDING BEAMS: ELECTRON POSITRON"},{"schema":"INSPIRE","value":"HADRON: ELECTROPRODUCTION"},{"schema":"INSPIRE","value":"ELECTROPRODUCTION: HADRON"},{"schema":"INSPIRE","value":"EXCHANGE: TWO-PHOTON"},{"schema":"INSPIRE","value":"TWO-PHOTON: EXCHANGE"},{"schema":"INSPIRE","value":"PHOTON PHOTON: INTERACTION"},{"schema":"INSPIRE","value":"INTERACTION: PHOTON PHOTON"},{"schema":"INSPIRE","value":"CHANNEL CROSS SECTION: MOMENTUM TRANSFER"},{"schema":"INSPIRE","value":"MOMENTUM TRANSFER: CHANNEL CROSS SECTION"},{"schema":"INSPIRE","value":"CHANNEL CROSS SECTION: MASS"},{"schema":"INSPIRE","value":"MASS: CHANNEL CROSS SECTION"},{"schema":"INSPIRE","value":"SPECTRUM: TRANSVERSE MOMENTUM"},{"schema":"INSPIRE","value":"TRANSVERSE MOMENTUM: SPECTRUM"},{"schema":"INSPIRE","value":"MODEL: VECTOR DOMINANCE"},{"schema":"INSPIRE","value":"PLUTO"},{"schema":"INSPIRE","value":"EXPERIMENTAL RESULTS"},{"schema":"INSPIRE","value":"DESY PETRA STOR"},{"schema":"INSPIRE","value":"ELECTRON POSITRON --> (N)HADRON POSITRON ELECTRON"},{"schema":"INSPIRE","value":"30-32 GEV-CM"}],"last_updated":"1981-10-26T00:00:00","parent_child_join":{"name":"parent_publication"},"publication_date":"1981-12-11T00:00:00","recid":27125,"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Aachen, Tech. Hochsch.","full_name":"Berger, Christoph"},{"affiliation":"Aachen, Tech. Hochsch.","full_name":"Genzel, H."},{"affiliation":"Aachen, Tech. Hochsch.","full_name":"Grigull, R."},{"affiliation":"Aachen, Tech. Hochsch.","full_name":"Lackas, W."},{"affiliation":"Aachen, Tech. Hochsch.","full_name":"Raupach, F."},{"affiliation":"Bergen U.","full_name":"Klovning, A."},{"affiliation":"Bergen U.","full_name":"Lillestol, E."},{"affiliation":"Bergen U.","full_name":"Skard, J.A."},{"affiliation":"DESY","full_name":"Ackermann, H."},{"affiliation":"DESY","full_name":"Burger, J."}],"title":"INELASTIC ELECTRON PHOTON SCATTERING AT MODERATE FOUR MOMENTUM TRANSFERS","total_tables":1,"type":["article"],"uuid":"0e7d3197-3e4a-407b-912f-18a1682de440","version":1,"year":"1981"},{"abstract":"To complete data on resonance electroproduction we constructed an electron spectrometer with large angular and momentum acceptance. As a first result inclusive cross sections for an invariant hadronic mass 1.2