{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:PWQPFSHOIT3VB6ASWPXWFNP6ZG","short_pith_number":"pith:PWQPFSHO","canonical_record":{"source":{"id":"1709.03592","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-09-11T20:54:14Z","cross_cats_sorted":[],"title_canon_sha256":"dbbd5861a76d313498764d23eb7654f8be2d6cf2807a4b1505765b93f1be107f","abstract_canon_sha256":"9d1f4ed1141f0e2292969a8feef6bd79e156c4fc6fca53597c3977b919ccffbd"},"schema_version":"1.0"},"canonical_sha256":"7da0f2c8ee44f750f812b3ef62b5fec98946bf9cfa1621ee5221fc1c98cc4f52","source":{"kind":"arxiv","id":"1709.03592","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1709.03592","created_at":"2026-05-18T00:21:54Z"},{"alias_kind":"arxiv_version","alias_value":"1709.03592v1","created_at":"2026-05-18T00:21:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.03592","created_at":"2026-05-18T00:21:54Z"},{"alias_kind":"pith_short_12","alias_value":"PWQPFSHOIT3V","created_at":"2026-05-18T12:31:37Z"},{"alias_kind":"pith_short_16","alias_value":"PWQPFSHOIT3VB6AS","created_at":"2026-05-18T12:31:37Z"},{"alias_kind":"pith_short_8","alias_value":"PWQPFSHO","created_at":"2026-05-18T12:31:37Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:PWQPFSHOIT3VB6ASWPXWFNP6ZG","target":"record","payload":{"canonical_record":{"source":{"id":"1709.03592","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-09-11T20:54:14Z","cross_cats_sorted":[],"title_canon_sha256":"dbbd5861a76d313498764d23eb7654f8be2d6cf2807a4b1505765b93f1be107f","abstract_canon_sha256":"9d1f4ed1141f0e2292969a8feef6bd79e156c4fc6fca53597c3977b919ccffbd"},"schema_version":"1.0"},"canonical_sha256":"7da0f2c8ee44f750f812b3ef62b5fec98946bf9cfa1621ee5221fc1c98cc4f52","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:21:54.664651Z","signature_b64":"E8eElkszctAIECHIKyzU/W1RLx0tZshx4X47cYi8CvAIJCwcA65fU2Y+Tui9eboctFfOmjqwcpJ2ZzSPVEKLCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7da0f2c8ee44f750f812b3ef62b5fec98946bf9cfa1621ee5221fc1c98cc4f52","last_reissued_at":"2026-05-18T00:21:54.663939Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:21:54.663939Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1709.03592","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:21:54Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SFDWXEyvTCE9D/gnSidz+WmyvgjUrlaLAR0+Y4tG/r8gndcto9aSDmWqX4ZcJT80BKcKxhg8X31vWsTo5I+kAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T19:51:59.633216Z"},"content_sha256":"cf6cc8569efce3b5ae0f8b9135822dbb15b4a8ebe8cd7d5db86918145635db3f","schema_version":"1.0","event_id":"sha256:cf6cc8569efce3b5ae0f8b9135822dbb15b4a8ebe8cd7d5db86918145635db3f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:PWQPFSHOIT3VB6ASWPXWFNP6ZG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quantum Monte Carlo calculations of weak transitions in $A\\,$=$\\,$6--10 nuclei","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"A. Baroni, J. Carlson, R.B. Wiringa, R. Schiavilla, S. Gandolfi, S. Pastore, Steven C. Pieper","submitted_at":"2017-09-11T20:54:14Z","abstract_excerpt":"Ab initio calculations of the Gamow-Teller (GT) matrix elements in the $\\beta$ decays of $^6$He and $^{10}$C and electron captures in $^7$Be are carried out using both variational and Green's function Monte Carlo wave functions obtained from the Argonne $v_{18}$ two-nucleon and Illinois-7 three-nucleon interactions, and axial many-body currents derived from either meson-exchange phenomenology or chiral effective field theory. The agreement with experimental data is excellent for the electron captures in $^7$Be, while theory overestimates the $^6$He and $^{10}$C data by $\\sim 2\\%$ and $\\sim 10\\"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.03592","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:21:54Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IU+j5dwiUJ/YW/earhDJ6QDOax+eXwFj/lLcQrYCjfLNJm6HJjRUbInRFw0063/vOyNKXopwsHoFbUfrFmxtAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T19:51:59.633927Z"},"content_sha256":"09a1f2df88bbb26896fdf34b6c08ba6428be942521ad1d36fba24f1f463a0a85","schema_version":"1.0","event_id":"sha256:09a1f2df88bbb26896fdf34b6c08ba6428be942521ad1d36fba24f1f463a0a85"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PWQPFSHOIT3VB6ASWPXWFNP6ZG/bundle.json","state_url":"https://pith.science/pith/PWQPFSHOIT3VB6ASWPXWFNP6ZG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PWQPFSHOIT3VB6ASWPXWFNP6ZG/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-25T19:51:59Z","links":{"resolver":"https://pith.science/pith/PWQPFSHOIT3VB6ASWPXWFNP6ZG","bundle":"https://pith.science/pith/PWQPFSHOIT3VB6ASWPXWFNP6ZG/bundle.json","state":"https://pith.science/pith/PWQPFSHOIT3VB6ASWPXWFNP6ZG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PWQPFSHOIT3VB6ASWPXWFNP6ZG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:PWQPFSHOIT3VB6ASWPXWFNP6ZG","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":"9d1f4ed1141f0e2292969a8feef6bd79e156c4fc6fca53597c3977b919ccffbd","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-09-11T20:54:14Z","title_canon_sha256":"dbbd5861a76d313498764d23eb7654f8be2d6cf2807a4b1505765b93f1be107f"},"schema_version":"1.0","source":{"id":"1709.03592","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1709.03592","created_at":"2026-05-18T00:21:54Z"},{"alias_kind":"arxiv_version","alias_value":"1709.03592v1","created_at":"2026-05-18T00:21:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.03592","created_at":"2026-05-18T00:21:54Z"},{"alias_kind":"pith_short_12","alias_value":"PWQPFSHOIT3V","created_at":"2026-05-18T12:31:37Z"},{"alias_kind":"pith_short_16","alias_value":"PWQPFSHOIT3VB6AS","created_at":"2026-05-18T12:31:37Z"},{"alias_kind":"pith_short_8","alias_value":"PWQPFSHO","created_at":"2026-05-18T12:31:37Z"}],"graph_snapshots":[{"event_id":"sha256:09a1f2df88bbb26896fdf34b6c08ba6428be942521ad1d36fba24f1f463a0a85","target":"graph","created_at":"2026-05-18T00:21:54Z","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":"Ab initio calculations of the Gamow-Teller (GT) matrix elements in the $\\beta$ decays of $^6$He and $^{10}$C and electron captures in $^7$Be are carried out using both variational and Green's function Monte Carlo wave functions obtained from the Argonne $v_{18}$ two-nucleon and Illinois-7 three-nucleon interactions, and axial many-body currents derived from either meson-exchange phenomenology or chiral effective field theory. The agreement with experimental data is excellent for the electron captures in $^7$Be, while theory overestimates the $^6$He and $^{10}$C data by $\\sim 2\\%$ and $\\sim 10\\","authors_text":"A. Baroni, J. Carlson, R.B. Wiringa, R. Schiavilla, S. Gandolfi, S. Pastore, Steven C. Pieper","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-09-11T20:54:14Z","title":"Quantum Monte Carlo calculations of weak transitions in $A\\,$=$\\,$6--10 nuclei"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.03592","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:cf6cc8569efce3b5ae0f8b9135822dbb15b4a8ebe8cd7d5db86918145635db3f","target":"record","created_at":"2026-05-18T00:21:54Z","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":"9d1f4ed1141f0e2292969a8feef6bd79e156c4fc6fca53597c3977b919ccffbd","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-09-11T20:54:14Z","title_canon_sha256":"dbbd5861a76d313498764d23eb7654f8be2d6cf2807a4b1505765b93f1be107f"},"schema_version":"1.0","source":{"id":"1709.03592","kind":"arxiv","version":1}},"canonical_sha256":"7da0f2c8ee44f750f812b3ef62b5fec98946bf9cfa1621ee5221fc1c98cc4f52","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7da0f2c8ee44f750f812b3ef62b5fec98946bf9cfa1621ee5221fc1c98cc4f52","first_computed_at":"2026-05-18T00:21:54.663939Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:21:54.663939Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"E8eElkszctAIECHIKyzU/W1RLx0tZshx4X47cYi8CvAIJCwcA65fU2Y+Tui9eboctFfOmjqwcpJ2ZzSPVEKLCw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:21:54.664651Z","signed_message":"canonical_sha256_bytes"},"source_id":"1709.03592","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cf6cc8569efce3b5ae0f8b9135822dbb15b4a8ebe8cd7d5db86918145635db3f","sha256:09a1f2df88bbb26896fdf34b6c08ba6428be942521ad1d36fba24f1f463a0a85"],"state_sha256":"a81cc047bf4672b378d054b5a698d2b95553f8b26809c4261f61182e01d11fdf"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+yHRQ6YXvyCXNkfLkgR9HGNAkc8eKIQG3ZbxGI5nVnRL06AUxAcyFehcl/LkLuVYpWnDdf0m9HdMK9XPVwL8BA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T19:51:59.636987Z","bundle_sha256":"cea0d67b90c76438e2fe3570cb1cd88bb1f1af2df9cc6d351c0cb9d5205bfb53"}}