{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:S7YR5B2ZJWMZ4DA5OYSS5SVECQ","short_pith_number":"pith:S7YR5B2Z","schema_version":"1.0","canonical_sha256":"97f11e87594d999e0c1d76252ecaa4141da91091529e8a914656e6e46e5be2a4","source":{"kind":"arxiv","id":"1106.2179","version":2},"attestation_state":"computed","paper":{"title":"Isovector soft dipole mode in 6Be","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"nucl-ex","authors_text":"A. S. Fomichev, A. V. Gorshkov, G. Kami\\'nski, G. M. Ter-Akopian, I. A. Egorova, I. G. Mukha, L. Standy{\\l}o, L. V. Grigorenko, M. S. Golovkov, M. V. Zhukov, R. S. Slepnev, R. Wolski, S. A. Krupko, S. I. Sidorchuk, S. N. Ershov, S. V. Stepantsov, V. A. Gorshkov, V. Chudoba, Yu. L. Parfenova","submitted_at":"2011-06-10T21:41:15Z","abstract_excerpt":"By using the 1H(6Li,6Be)n charge-exchange reaction, continuum states in 6Be were populated up to E_t=16 MeV, E_t being the 6Be energy above its three-body decay threshold. In kinematically complete measurements performed by detecting alpha+p+p coincidences, an E_t spectrum of high statistics was obtained, containing approximately ~5x10^6 events. The spectrum provides detailed correlation information about the well-known 0^+ ground state of 6Be at E_t=1.37 MeV and its 2^+ state at E_t=3.05 MeV. Moreover, a broad structure extending from 4 to 16 MeV was observed. It contains negative parity stat"},"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":"1106.2179","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2011-06-10T21:41:15Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"e9afecf6fd9d905fe9101d76a3f1f9bba3e84a8ea38b67894f9a9de3b8fe76ec","abstract_canon_sha256":"90d9cd5623eedfbea31464a59ff48555c72e702540029c90cbdb3bf0c7021476"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:01:39.814027Z","signature_b64":"bV8G3auMAzam6kJtecjIdXR8JLl/LaOsMGZfTQOpeJblJis0rSFh0aLApsH+CHuLpkOMwz/Y9Ljf5awqDJuyDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"97f11e87594d999e0c1d76252ecaa4141da91091529e8a914656e6e46e5be2a4","last_reissued_at":"2026-05-18T02:01:39.813580Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:01:39.813580Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Isovector soft dipole mode in 6Be","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"nucl-ex","authors_text":"A. S. Fomichev, A. V. Gorshkov, G. Kami\\'nski, G. M. Ter-Akopian, I. A. Egorova, I. G. Mukha, L. Standy{\\l}o, L. V. Grigorenko, M. S. Golovkov, M. V. Zhukov, R. S. Slepnev, R. Wolski, S. A. Krupko, S. I. Sidorchuk, S. N. Ershov, S. V. Stepantsov, V. A. Gorshkov, V. Chudoba, Yu. L. Parfenova","submitted_at":"2011-06-10T21:41:15Z","abstract_excerpt":"By using the 1H(6Li,6Be)n charge-exchange reaction, continuum states in 6Be were populated up to E_t=16 MeV, E_t being the 6Be energy above its three-body decay threshold. In kinematically complete measurements performed by detecting alpha+p+p coincidences, an E_t spectrum of high statistics was obtained, containing approximately ~5x10^6 events. The spectrum provides detailed correlation information about the well-known 0^+ ground state of 6Be at E_t=1.37 MeV and its 2^+ state at E_t=3.05 MeV. Moreover, a broad structure extending from 4 to 16 MeV was observed. It contains negative parity stat"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.2179","kind":"arxiv","version":2},"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":"1106.2179","created_at":"2026-05-18T02:01:39.813648+00:00"},{"alias_kind":"arxiv_version","alias_value":"1106.2179v2","created_at":"2026-05-18T02:01:39.813648+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.2179","created_at":"2026-05-18T02:01:39.813648+00:00"},{"alias_kind":"pith_short_12","alias_value":"S7YR5B2ZJWMZ","created_at":"2026-05-18T12:26:41.206345+00:00"},{"alias_kind":"pith_short_16","alias_value":"S7YR5B2ZJWMZ4DA5","created_at":"2026-05-18T12:26:41.206345+00:00"},{"alias_kind":"pith_short_8","alias_value":"S7YR5B2Z","created_at":"2026-05-18T12:26:41.206345+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/S7YR5B2ZJWMZ4DA5OYSS5SVECQ","json":"https://pith.science/pith/S7YR5B2ZJWMZ4DA5OYSS5SVECQ.json","graph_json":"https://pith.science/api/pith-number/S7YR5B2ZJWMZ4DA5OYSS5SVECQ/graph.json","events_json":"https://pith.science/api/pith-number/S7YR5B2ZJWMZ4DA5OYSS5SVECQ/events.json","paper":"https://pith.science/paper/S7YR5B2Z"},"agent_actions":{"view_html":"https://pith.science/pith/S7YR5B2ZJWMZ4DA5OYSS5SVECQ","download_json":"https://pith.science/pith/S7YR5B2ZJWMZ4DA5OYSS5SVECQ.json","view_paper":"https://pith.science/paper/S7YR5B2Z","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1106.2179&json=true","fetch_graph":"https://pith.science/api/pith-number/S7YR5B2ZJWMZ4DA5OYSS5SVECQ/graph.json","fetch_events":"https://pith.science/api/pith-number/S7YR5B2ZJWMZ4DA5OYSS5SVECQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/S7YR5B2ZJWMZ4DA5OYSS5SVECQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/S7YR5B2ZJWMZ4DA5OYSS5SVECQ/action/storage_attestation","attest_author":"https://pith.science/pith/S7YR5B2ZJWMZ4DA5OYSS5SVECQ/action/author_attestation","sign_citation":"https://pith.science/pith/S7YR5B2ZJWMZ4DA5OYSS5SVECQ/action/citation_signature","submit_replication":"https://pith.science/pith/S7YR5B2ZJWMZ4DA5OYSS5SVECQ/action/replication_record"}},"created_at":"2026-05-18T02:01:39.813648+00:00","updated_at":"2026-05-18T02:01:39.813648+00:00"}