{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:X5SBWUMDLZAWYH2MY75FRQP6VA","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":"e6eaf13636cdd9140a6b90f5ee412b7705f6bdefd123236dc18d0c5c43d22461","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2026-06-30T17:59:29Z","title_canon_sha256":"6bbcfa71d4f7bf6a4c2523040cb5238773477f3dcfc779447fb25d1bbdfc43be"},"schema_version":"1.0","source":{"id":"2606.32037","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2606.32037","created_at":"2026-07-01T02:17:47Z"},{"alias_kind":"arxiv_version","alias_value":"2606.32037v1","created_at":"2026-07-01T02:17:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.32037","created_at":"2026-07-01T02:17:47Z"},{"alias_kind":"pith_short_12","alias_value":"X5SBWUMDLZAW","created_at":"2026-07-01T02:17:47Z"},{"alias_kind":"pith_short_16","alias_value":"X5SBWUMDLZAWYH2M","created_at":"2026-07-01T02:17:47Z"},{"alias_kind":"pith_short_8","alias_value":"X5SBWUMD","created_at":"2026-07-01T02:17:47Z"}],"graph_snapshots":[{"event_id":"sha256:b50239fa33a80d30c1ba8156c1b8397617ce1b790f39bc42bde25905cd447fe1","target":"graph","created_at":"2026-07-01T02:17:47Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2606.32037/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Halo effective field theory (Halo EFT) is a powerful tool to describe halo nuclei and predict low-energy observables with quantified uncertainties. However, in the case that there is a leading-order interaction determined by two or more effective-range parameters, such as the $^2P_{3/2}$ $n\\alpha$ interaction in $^6$He, the standard implementation in the dimer formalism leads to an energy-dependent interaction. This complicates the construction of a Hilbert space of states, especially beyond the two-body problem. As an alternative, we propose the use of a finite-range formulation of Halo EFT, ","authors_text":"Daniel R. Phillips, Hans-Werner Hammer, Matthias G\\\"obel","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2026-06-30T17:59:29Z","title":"Finite-range EFT for the $E1$ strength distribution of ${}^6$He"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.32037","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":"sha256:3a067c103c08b4448f444bdc16f3bf9a0cba6812bc09a6b5548b358a6551ba58","target":"record","created_at":"2026-07-01T02:17:47Z","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":"e6eaf13636cdd9140a6b90f5ee412b7705f6bdefd123236dc18d0c5c43d22461","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2026-06-30T17:59:29Z","title_canon_sha256":"6bbcfa71d4f7bf6a4c2523040cb5238773477f3dcfc779447fb25d1bbdfc43be"},"schema_version":"1.0","source":{"id":"2606.32037","kind":"arxiv","version":1}},"canonical_sha256":"bf641b51835e416c1f4cc7fa58c1fea81c95af404d1408c42449eae90870ac9a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"bf641b51835e416c1f4cc7fa58c1fea81c95af404d1408c42449eae90870ac9a","first_computed_at":"2026-07-01T02:17:47.949188Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-01T02:17:47.949188Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"DmMqwnyw+7Pgsl2a3MkVc5Ri3vScHHQ2y7CRUl9I0KDznvF2JIpYBmktK3EPy2l09mnQ/1EZmU0qdauyDhXtBQ==","signature_status":"signed_v1","signed_at":"2026-07-01T02:17:47.949580Z","signed_message":"canonical_sha256_bytes"},"source_id":"2606.32037","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3a067c103c08b4448f444bdc16f3bf9a0cba6812bc09a6b5548b358a6551ba58","sha256:b50239fa33a80d30c1ba8156c1b8397617ce1b790f39bc42bde25905cd447fe1"],"state_sha256":"6c7960faeb674152843a4809994c62f7974944836d708942e4bccf46e15cd351"}