{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:CPUS6JXK5X7KNSTXA6TUGZ2XL6","short_pith_number":"pith:CPUS6JXK","schema_version":"1.0","canonical_sha256":"13e92f26eaedfea6ca7707a74367575fafc3b02ab6594486c2315a2b43aa663d","source":{"kind":"arxiv","id":"1312.3047","version":3},"attestation_state":"computed","paper":{"title":"Measurement of pretzelosity asymmetry of charged pion production in Semi-Inclusive Deep Inelastic Scattering on a polarized $^3$He target","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"A. Camsonne, A. Deur, A. J. R. Puckett, A. Kelleher, A. Kolarkar, A. Narayan, A. Rakhman, A. Saha, A. Shahinyan, B. Moffit, B. Norum, B. Sawatzky, B. Wojtsekhowski, B. Zhao, C. Chen, C. Dutta, C. Mu\\~noz Camacho, C.W. de Jager, D. Dutta, D. Gaskell, D. Hamilton, D.J. Margaziotis, D. McNulty, D. Parno, D.W. Higinbotham, E. Chudakov, E. Cisbani, E. Long, E. Schulte, F. Benmokhtar, F. Cusanno, F. Garibaldi, G.D. Cates, G. Jin, G. M. Urciuoli, H. Ding, H. F. Ibrahim, H. Gao, H.-J. Lu, H. Yao, I. Vilardi, J.C. Cornejo, J. C. Peng, J. Huang, J.J. LeRose, J. Katich, J.-P. Chen, J.R.M. Annand, K. Allada, K. Aniol, K. Chirapatpimol, K. Wang, L. El Fassi, L.-G. Tang, L. Guo, L. Yuan, L. Zhu, M. Canan, M. H. Shabestari, M. Huang, M. Iodice, M.K. Jones, M. M. Dalton, M. Osipenko, M. Posik, N. Liyanage, O. Glamazdin, O. Hansen, P. A. M. Dolph, P. Bosted, P.C. Bradshaw, P. Markowitz, R. De Leo, R. D. Ransome, R. Gilman, R. Lindgren, R. Michaels, R. Subedi, S. Frullani, S. Gilad, S. Golge, S. K. Phillips, S. Marrone, S. Nanda, S. Riordan, S. Sirca, S. Stepanyan, T. Averett, T. Holmstrom, V. Nelyubin, V. Sulkosky, W.A. Tobias, W. Bertozzi, W. Chen, W. Deconinck, W. Kim, W. Korsch, X. Deng, X. Jiang, X. Li, X. Qian, X. Yan, X. Zhan, X. Zheng, X. Zhu, X. Zong, Y. Li, Y. Oh, Y. Qiang, Y. Wang, Y.-W. Zhang, Y. Ye, Y. Zhang, Z.-E. Meziani, Z. Ye","submitted_at":"2013-12-11T06:47:39Z","abstract_excerpt":"An experiment to measure single-spin asymmetries in semi-inclusive production of charged pions in deep-inelastic scattering on a transversely polarized $^3$He target was performed at Jefferson Lab in the kinematic region of $0.16<x<0.35$ and $1.4<Q^2<2.7$ ${\\rm GeV^2}$. The pretzelosity asymmetries on $^3$He, which can be expressed as the convolution of the $h^\\perp_{1T}$ transverse momentum dependent distribution functions and the Collins fragmentation functions in the leading order, were measured for the first time. Using the effective polarization approximation, we extracted the correspondi"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1312.3047","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2013-12-11T06:47:39Z","cross_cats_sorted":[],"title_canon_sha256":"32599738790cb7f97913230460d4887bfe6bba7451fc32429ecec481636b6928","abstract_canon_sha256":"a63db4f76e634d47c1b8303e75621880b35ca38b2885f1541e0f7b51cf2bb82d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:24:21.874121Z","signature_b64":"XKBtx5JimG43doaaDvUjdepaLx/cENOeNWklirJi/hdnjjweDsSJC/gYlXt8X3SPspAQt/OSXmnpuRc4xADEBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"13e92f26eaedfea6ca7707a74367575fafc3b02ab6594486c2315a2b43aa663d","last_reissued_at":"2026-05-18T01:24:21.873490Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:24:21.873490Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurement of pretzelosity asymmetry of charged pion production in Semi-Inclusive Deep Inelastic Scattering on a polarized $^3$He target","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"A. Camsonne, A. Deur, A. J. R. Puckett, A. Kelleher, A. Kolarkar, A. Narayan, A. Rakhman, A. Saha, A. Shahinyan, B. Moffit, B. Norum, B. Sawatzky, B. Wojtsekhowski, B. Zhao, C. Chen, C. Dutta, C. Mu\\~noz Camacho, C.W. de Jager, D. Dutta, D. Gaskell, D. Hamilton, D.J. Margaziotis, D. McNulty, D. Parno, D.W. Higinbotham, E. Chudakov, E. Cisbani, E. Long, E. Schulte, F. Benmokhtar, F. Cusanno, F. Garibaldi, G.D. Cates, G. Jin, G. M. Urciuoli, H. Ding, H. F. Ibrahim, H. Gao, H.-J. Lu, H. Yao, I. Vilardi, J.C. Cornejo, J. C. Peng, J. Huang, J.J. LeRose, J. Katich, J.-P. Chen, J.R.M. Annand, K. Allada, K. Aniol, K. Chirapatpimol, K. Wang, L. El Fassi, L.-G. Tang, L. Guo, L. Yuan, L. Zhu, M. Canan, M. H. Shabestari, M. Huang, M. Iodice, M.K. Jones, M. M. Dalton, M. Osipenko, M. Posik, N. Liyanage, O. Glamazdin, O. Hansen, P. A. M. Dolph, P. Bosted, P.C. Bradshaw, P. Markowitz, R. De Leo, R. D. Ransome, R. Gilman, R. Lindgren, R. Michaels, R. Subedi, S. Frullani, S. Gilad, S. Golge, S. K. Phillips, S. Marrone, S. Nanda, S. Riordan, S. Sirca, S. Stepanyan, T. Averett, T. Holmstrom, V. Nelyubin, V. Sulkosky, W.A. Tobias, W. Bertozzi, W. Chen, W. Deconinck, W. Kim, W. Korsch, X. Deng, X. Jiang, X. Li, X. Qian, X. Yan, X. Zhan, X. Zheng, X. Zhu, X. Zong, Y. Li, Y. Oh, Y. Qiang, Y. Wang, Y.-W. Zhang, Y. Ye, Y. Zhang, Z.-E. Meziani, Z. Ye","submitted_at":"2013-12-11T06:47:39Z","abstract_excerpt":"An experiment to measure single-spin asymmetries in semi-inclusive production of charged pions in deep-inelastic scattering on a transversely polarized $^3$He target was performed at Jefferson Lab in the kinematic region of $0.16<x<0.35$ and $1.4<Q^2<2.7$ ${\\rm GeV^2}$. The pretzelosity asymmetries on $^3$He, which can be expressed as the convolution of the $h^\\perp_{1T}$ transverse momentum dependent distribution functions and the Collins fragmentation functions in the leading order, were measured for the first time. Using the effective polarization approximation, we extracted the correspondi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.3047","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"1312.3047","created_at":"2026-05-18T01:24:21.873589+00:00"},{"alias_kind":"arxiv_version","alias_value":"1312.3047v3","created_at":"2026-05-18T01:24:21.873589+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.3047","created_at":"2026-05-18T01:24:21.873589+00:00"},{"alias_kind":"pith_short_12","alias_value":"CPUS6JXK5X7K","created_at":"2026-05-18T12:27:40.988391+00:00"},{"alias_kind":"pith_short_16","alias_value":"CPUS6JXK5X7KNSTX","created_at":"2026-05-18T12:27:40.988391+00:00"},{"alias_kind":"pith_short_8","alias_value":"CPUS6JXK","created_at":"2026-05-18T12:27:40.988391+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CPUS6JXK5X7KNSTXA6TUGZ2XL6","json":"https://pith.science/pith/CPUS6JXK5X7KNSTXA6TUGZ2XL6.json","graph_json":"https://pith.science/api/pith-number/CPUS6JXK5X7KNSTXA6TUGZ2XL6/graph.json","events_json":"https://pith.science/api/pith-number/CPUS6JXK5X7KNSTXA6TUGZ2XL6/events.json","paper":"https://pith.science/paper/CPUS6JXK"},"agent_actions":{"view_html":"https://pith.science/pith/CPUS6JXK5X7KNSTXA6TUGZ2XL6","download_json":"https://pith.science/pith/CPUS6JXK5X7KNSTXA6TUGZ2XL6.json","view_paper":"https://pith.science/paper/CPUS6JXK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1312.3047&json=true","fetch_graph":"https://pith.science/api/pith-number/CPUS6JXK5X7KNSTXA6TUGZ2XL6/graph.json","fetch_events":"https://pith.science/api/pith-number/CPUS6JXK5X7KNSTXA6TUGZ2XL6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CPUS6JXK5X7KNSTXA6TUGZ2XL6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CPUS6JXK5X7KNSTXA6TUGZ2XL6/action/storage_attestation","attest_author":"https://pith.science/pith/CPUS6JXK5X7KNSTXA6TUGZ2XL6/action/author_attestation","sign_citation":"https://pith.science/pith/CPUS6JXK5X7KNSTXA6TUGZ2XL6/action/citation_signature","submit_replication":"https://pith.science/pith/CPUS6JXK5X7KNSTXA6TUGZ2XL6/action/replication_record"}},"created_at":"2026-05-18T01:24:21.873589+00:00","updated_at":"2026-05-18T01:24:21.873589+00:00"}