{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:X6ACIZIRJWU65DN5C6VDX7MKSW","short_pith_number":"pith:X6ACIZIR","schema_version":"1.0","canonical_sha256":"bf802465114da9ee8dbd17aa3bfd8a95a6401e07689355fc6b529aeef9fb61b1","source":{"kind":"arxiv","id":"1412.0138","version":1},"attestation_state":"computed","paper":{"title":"Momentum sharing in imbalanced Fermi systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","nucl-th"],"primary_cat":"nucl-ex","authors_text":"A. Beck, A. Biselli, A. Celentano, A. DAngelo, A. Deur, A. El Alaoui, A. J. R. Puckett, A. Kim, A. Movsisyan, A. Rizzo, A. V. Vlassov, B. Garillon, B. G. Ritchie, B.I. Ishkanov, B. McKinnon, B. Mustapha, C. Djalali, C. E. Hyde, C. Hanretty, C. Munoz Camacho, D. Doughty, D. G. Ireland, D. Keller, D. Protopopescu, D. Rimal, D. S. Carman, D. Schott, D. Sokhan, D. Watts, D. W. Higinbotham, E. L. Isupov, E. Pasyuk, E. Piasetzky, E. Voutier, F. J. Klein, F. Sabatie, F. X. Girod, G. Asryan, G. D. Smith, G. Fedotov, G. Niculescu, G. P. Gilfoyle, G. Rosner, H. Avakian, H. Egiyan, H. Hakobyan, H. Jiang, H. S. Jo, H. Y. Lu, I. Bedlinskiy, I. J. D. MacGregor, I. Korover, I. Niculescu, I. Zonta, J. Arrington, J. Ball, J. T. Goetz, J. W. Price, K. A. Griffioen, K. Hafidi, K. Hicks, K. Joo, K. Livingston, K. P. Adhikari, K. Park, L.B. Weinstein, L. Colaneri, L. El Fassi, L. Elouadrhiri, L. Guo, L. L. Pappalardo, L. Zana, M. Battaglieri, M. Braverman, M. Dugger, M. Garcon, M. Guidal, M. Hattawy, M. Holtrop, M. H. Wood, M. Khandaker, M. Lowry, M. Mayer, M. Osipenko, M. Ripani, M. Sargsian, M. Taiuti, M. Ungaro, N. A. Baltzell, N. Gevorgyan, N. K. Walford, N. Markov, N. Zachariou, O. Hen, O. Pogorelko, P. L. Cole, P. Lenisa, P. Nadel-Turonski, P. Rossi, P. Roy, P. Stoler, R. A. Schumacher, R. De Vita, R. Dupre, R. Paremuzyan, R. Shneor, R. W. Gothe, S. A. Wood, S. Chandavar, S. E. Kuhn, S. Fegan, S. Gilad, S. Koirala, S. May-Tal Beck, S. Niccolai, S. Pisano, S. Procureur, S. S. Stepanyan, S. Stepanyan, S. Strauch, S. Tkachenko, T. Cao, T. FOrest, T. Mineeva, V. Crede, V. D. Burkert, V. Kubarovsky, V. Mokeev, V. Sytnik, W. Bertozzi, W. I. Levine, W.K. Brooks, W. Kim, W. Phelps, X. Wei, X. Zheng, Y. Ghandilyan, Y. G. Sharabian, Y. Ilieva, Y. Prok, Z. W. Zhao","submitted_at":"2014-11-29T18:51:21Z","abstract_excerpt":"The atomic nucleus is composed of two different kinds of fermions, protons and neutrons. If the protons and neutrons did not interact, the Pauli exclusion principle would force the majority fermions (usually neutrons) to have a higher average momentum. Our high-energy electron scattering measurements using 12C, 27Al, 56Fe and 208Pb targets show that, even in heavy neutron-rich nuclei, short-range interactions between the fermions form correlated high-momentum neutron-proton pairs. Thus, in neutron-rich nuclei, protons have a greater probability than neutrons to have momentum greater than the F"},"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":"1412.0138","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2014-11-29T18:51:21Z","cross_cats_sorted":["cond-mat.quant-gas","nucl-th"],"title_canon_sha256":"36a0d5c208c19579f0ffe86e5baeff3e0fdea131fce1f38fec5288672e3aff9b","abstract_canon_sha256":"b585f3b142e3a9816ee6eaf95990c1afc3d4050da0f06071757691a2bde4bdf7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:32:30.241704Z","signature_b64":"tU3Ui173CGGLj5wmG9jq5RS6tNGDikfMceraM0DxMNQOoGuaoAu4YysUiedtnQuFUVk2D21NB83A6YEQPInoBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bf802465114da9ee8dbd17aa3bfd8a95a6401e07689355fc6b529aeef9fb61b1","last_reissued_at":"2026-05-18T02:32:30.241145Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:32:30.241145Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Momentum sharing in imbalanced Fermi systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","nucl-th"],"primary_cat":"nucl-ex","authors_text":"A. Beck, A. Biselli, A. Celentano, A. DAngelo, A. Deur, A. El Alaoui, A. J. R. Puckett, A. Kim, A. Movsisyan, A. Rizzo, A. V. Vlassov, B. Garillon, B. G. Ritchie, B.I. Ishkanov, B. McKinnon, B. Mustapha, C. Djalali, C. E. Hyde, C. Hanretty, C. Munoz Camacho, D. Doughty, D. G. Ireland, D. Keller, D. Protopopescu, D. Rimal, D. S. Carman, D. Schott, D. Sokhan, D. Watts, D. W. Higinbotham, E. L. Isupov, E. Pasyuk, E. Piasetzky, E. Voutier, F. J. Klein, F. Sabatie, F. X. Girod, G. Asryan, G. D. Smith, G. Fedotov, G. Niculescu, G. P. Gilfoyle, G. Rosner, H. Avakian, H. Egiyan, H. Hakobyan, H. Jiang, H. S. Jo, H. Y. Lu, I. Bedlinskiy, I. J. D. MacGregor, I. Korover, I. Niculescu, I. Zonta, J. Arrington, J. Ball, J. T. Goetz, J. W. Price, K. A. Griffioen, K. Hafidi, K. Hicks, K. Joo, K. Livingston, K. P. Adhikari, K. Park, L.B. Weinstein, L. Colaneri, L. El Fassi, L. Elouadrhiri, L. Guo, L. L. Pappalardo, L. Zana, M. Battaglieri, M. Braverman, M. Dugger, M. Garcon, M. Guidal, M. Hattawy, M. Holtrop, M. H. Wood, M. Khandaker, M. Lowry, M. Mayer, M. Osipenko, M. Ripani, M. Sargsian, M. Taiuti, M. Ungaro, N. A. Baltzell, N. Gevorgyan, N. K. Walford, N. Markov, N. Zachariou, O. Hen, O. Pogorelko, P. L. Cole, P. Lenisa, P. Nadel-Turonski, P. Rossi, P. Roy, P. Stoler, R. A. Schumacher, R. De Vita, R. Dupre, R. Paremuzyan, R. Shneor, R. W. Gothe, S. A. Wood, S. Chandavar, S. E. Kuhn, S. Fegan, S. Gilad, S. Koirala, S. May-Tal Beck, S. Niccolai, S. Pisano, S. Procureur, S. S. Stepanyan, S. Stepanyan, S. Strauch, S. Tkachenko, T. Cao, T. FOrest, T. Mineeva, V. Crede, V. D. Burkert, V. Kubarovsky, V. Mokeev, V. Sytnik, W. Bertozzi, W. I. Levine, W.K. Brooks, W. Kim, W. Phelps, X. Wei, X. Zheng, Y. Ghandilyan, Y. G. Sharabian, Y. Ilieva, Y. Prok, Z. W. Zhao","submitted_at":"2014-11-29T18:51:21Z","abstract_excerpt":"The atomic nucleus is composed of two different kinds of fermions, protons and neutrons. If the protons and neutrons did not interact, the Pauli exclusion principle would force the majority fermions (usually neutrons) to have a higher average momentum. Our high-energy electron scattering measurements using 12C, 27Al, 56Fe and 208Pb targets show that, even in heavy neutron-rich nuclei, short-range interactions between the fermions form correlated high-momentum neutron-proton pairs. Thus, in neutron-rich nuclei, protons have a greater probability than neutrons to have momentum greater than the F"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.0138","kind":"arxiv","version":1},"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":"1412.0138","created_at":"2026-05-18T02:32:30.241223+00:00"},{"alias_kind":"arxiv_version","alias_value":"1412.0138v1","created_at":"2026-05-18T02:32:30.241223+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.0138","created_at":"2026-05-18T02:32:30.241223+00:00"},{"alias_kind":"pith_short_12","alias_value":"X6ACIZIRJWU6","created_at":"2026-05-18T12:28:57.508820+00:00"},{"alias_kind":"pith_short_16","alias_value":"X6ACIZIRJWU65DN5","created_at":"2026-05-18T12:28:57.508820+00:00"},{"alias_kind":"pith_short_8","alias_value":"X6ACIZIR","created_at":"2026-05-18T12:28:57.508820+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":6,"internal_anchor_count":5,"sample":[{"citing_arxiv_id":"2606.07754","citing_title":"Short-range correlated pair formation and nuclear shell structure","ref_index":15,"is_internal_anchor":true},{"citing_arxiv_id":"2604.25106","citing_title":"Relaxation Kernel, Spectral Dissipation, and Global Convergence of Blahut--Arimoto Dynamics","ref_index":6,"is_internal_anchor":true},{"citing_arxiv_id":"2605.28671","citing_title":"CP-violation or Nuclear Excitation: Reviewing the Role of Neutrino Interaction Model Uncertainties on Accelerator-Based Neutrino Oscillation Measurements","ref_index":47,"is_internal_anchor":true},{"citing_arxiv_id":"2508.04550","citing_title":"Experimental Study of Bremsstrahlung Gamma Ray Emission and Short-Range Correlations in $^{124}$Sn+$^{124}$Sn Collisions at 25 MeV/u","ref_index":19,"is_internal_anchor":true},{"citing_arxiv_id":"2605.12626","citing_title":"Short-range correlations in nuclei","ref_index":116,"is_internal_anchor":true},{"citing_arxiv_id":"2604.25107","citing_title":"Large amplification of the isospin-dependence of proton emitting source size in radioactive heavy-ion collisions: a signal of n-p correlation","ref_index":6,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/X6ACIZIRJWU65DN5C6VDX7MKSW","json":"https://pith.science/pith/X6ACIZIRJWU65DN5C6VDX7MKSW.json","graph_json":"https://pith.science/api/pith-number/X6ACIZIRJWU65DN5C6VDX7MKSW/graph.json","events_json":"https://pith.science/api/pith-number/X6ACIZIRJWU65DN5C6VDX7MKSW/events.json","paper":"https://pith.science/paper/X6ACIZIR"},"agent_actions":{"view_html":"https://pith.science/pith/X6ACIZIRJWU65DN5C6VDX7MKSW","download_json":"https://pith.science/pith/X6ACIZIRJWU65DN5C6VDX7MKSW.json","view_paper":"https://pith.science/paper/X6ACIZIR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1412.0138&json=true","fetch_graph":"https://pith.science/api/pith-number/X6ACIZIRJWU65DN5C6VDX7MKSW/graph.json","fetch_events":"https://pith.science/api/pith-number/X6ACIZIRJWU65DN5C6VDX7MKSW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/X6ACIZIRJWU65DN5C6VDX7MKSW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/X6ACIZIRJWU65DN5C6VDX7MKSW/action/storage_attestation","attest_author":"https://pith.science/pith/X6ACIZIRJWU65DN5C6VDX7MKSW/action/author_attestation","sign_citation":"https://pith.science/pith/X6ACIZIRJWU65DN5C6VDX7MKSW/action/citation_signature","submit_replication":"https://pith.science/pith/X6ACIZIRJWU65DN5C6VDX7MKSW/action/replication_record"}},"created_at":"2026-05-18T02:32:30.241223+00:00","updated_at":"2026-05-18T02:32:30.241223+00:00"}