{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:FILHIRDMIDZ3XWMMS44W3ITRWP","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"b5dfb6aec4c13e14d1731cbb3851e56e7bd4833a0660ce219d4be35a6c38e7f3","cross_cats_sorted":["math-ph","math.MP","nucl-th","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-04-23T14:30:53Z","title_canon_sha256":"84083bc644dcc9942632e318b2ea5939b87e7c8ffadba88fb7bbce701eed4852"},"schema_version":"1.0","source":{"id":"1604.06910","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.06910","created_at":"2026-05-18T01:04:27Z"},{"alias_kind":"arxiv_version","alias_value":"1604.06910v1","created_at":"2026-05-18T01:04:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.06910","created_at":"2026-05-18T01:04:27Z"},{"alias_kind":"pith_short_12","alias_value":"FILHIRDMIDZ3","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_16","alias_value":"FILHIRDMIDZ3XWMM","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_8","alias_value":"FILHIRDM","created_at":"2026-05-18T12:30:15Z"}],"graph_snapshots":[{"event_id":"sha256:d4b80baf5e00de6c63e6a8692706eed6453e0b98bc140e6ea810951ab7e2f09b","target":"graph","created_at":"2026-05-18T01:04:27Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"In a recent paper [Nuc. Phys. A {\\bf 948}, (2016) 19] we have demonstrated the possible existence of Tsallis' q-Gamow states. Now, accelerators' experimental evidence for Tsallis' distributions has been ascertained only at very high energies. Here, instead, we develop a different set of q-Gamow states for which the associated q-Breit-Wigner distribution could easily be found at intermediate energies, for which accelerators are available at many locations. In this context, it should be strongly emphasized [Physica A {\\bf 388} (2009) 601] that, empirically, one never exactly and unambiguously \"d","authors_text":"A. Plastino, D. J. Zamora, M. C. Rocca","cross_cats":["math-ph","math.MP","nucl-th","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-04-23T14:30:53Z","title":"q-Gamow States for intermediate energies"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.06910","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:f1f102a09201bd4cf08a226f97894d7f3375f02450ab66c5ea12636d4ba0d687","target":"record","created_at":"2026-05-18T01:04:27Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"b5dfb6aec4c13e14d1731cbb3851e56e7bd4833a0660ce219d4be35a6c38e7f3","cross_cats_sorted":["math-ph","math.MP","nucl-th","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-04-23T14:30:53Z","title_canon_sha256":"84083bc644dcc9942632e318b2ea5939b87e7c8ffadba88fb7bbce701eed4852"},"schema_version":"1.0","source":{"id":"1604.06910","kind":"arxiv","version":1}},"canonical_sha256":"2a1674446c40f3bbd98c97396da271b3c806209537bb49d94b7b8bcf1773823e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2a1674446c40f3bbd98c97396da271b3c806209537bb49d94b7b8bcf1773823e","first_computed_at":"2026-05-18T01:04:27.743428Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:04:27.743428Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ptwRI4wV95f3SNxb3slqeG5seqA6Z0hOI9OXUq7zVM+vXE2HP/qX9GMRYS1vAypG3Y9Vt5Y9NWVI8/hOaB6+BA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:04:27.744120Z","signed_message":"canonical_sha256_bytes"},"source_id":"1604.06910","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f1f102a09201bd4cf08a226f97894d7f3375f02450ab66c5ea12636d4ba0d687","sha256:d4b80baf5e00de6c63e6a8692706eed6453e0b98bc140e6ea810951ab7e2f09b"],"state_sha256":"b8ffcb4f2c43aea4cdd37787bf6fee6a0260369cbcb84915c014ba2009993858"}