{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:YOTMOL34PISM6AHNBHC6JWE6L3","short_pith_number":"pith:YOTMOL34","canonical_record":{"source":{"id":"1305.7299","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2013-05-31T04:14:08Z","cross_cats_sorted":[],"title_canon_sha256":"4217b4f648b743bfd0626a3b35851731515d27240f2c8173dc9550ad864973b1","abstract_canon_sha256":"5bcb0efd87a15b2cda41f27d625b2f665b2498bf0fe39cf84ef4f037c14a9342"},"schema_version":"1.0"},"canonical_sha256":"c3a6c72f7c7a24cf00ed09c5e4d89e5eca8bfcab0c05452c17234e42c82cc2c7","source":{"kind":"arxiv","id":"1305.7299","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1305.7299","created_at":"2026-05-18T01:49:39Z"},{"alias_kind":"arxiv_version","alias_value":"1305.7299v2","created_at":"2026-05-18T01:49:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1305.7299","created_at":"2026-05-18T01:49:39Z"},{"alias_kind":"pith_short_12","alias_value":"YOTMOL34PISM","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_16","alias_value":"YOTMOL34PISM6AHN","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_8","alias_value":"YOTMOL34","created_at":"2026-05-18T12:28:06Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:YOTMOL34PISM6AHNBHC6JWE6L3","target":"record","payload":{"canonical_record":{"source":{"id":"1305.7299","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2013-05-31T04:14:08Z","cross_cats_sorted":[],"title_canon_sha256":"4217b4f648b743bfd0626a3b35851731515d27240f2c8173dc9550ad864973b1","abstract_canon_sha256":"5bcb0efd87a15b2cda41f27d625b2f665b2498bf0fe39cf84ef4f037c14a9342"},"schema_version":"1.0"},"canonical_sha256":"c3a6c72f7c7a24cf00ed09c5e4d89e5eca8bfcab0c05452c17234e42c82cc2c7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:49:39.361664Z","signature_b64":"72YZnfKwNsrwdIUwyAcniRQXhDXSrcHvvR3TUmBgfAulYoypkralOtckuFhKovMKOmhoEUgkvVm8z5+N3700CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c3a6c72f7c7a24cf00ed09c5e4d89e5eca8bfcab0c05452c17234e42c82cc2c7","last_reissued_at":"2026-05-18T01:49:39.361095Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:49:39.361095Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1305.7299","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:49:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DnwZ6oEUPtY86nhGspYFVh3gnnM3/UnBhAS2PHIGSJiAvVLtrDLgj06YO7X1D4hEHH8TMBbbWzdkl/49VquDCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T08:05:19.453805Z"},"content_sha256":"ebcd364933c85823d3b1d3490d20c1dbf8960da2569ceca13a53d6f2eb01a806","schema_version":"1.0","event_id":"sha256:ebcd364933c85823d3b1d3490d20c1dbf8960da2569ceca13a53d6f2eb01a806"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:YOTMOL34PISM6AHNBHC6JWE6L3","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Role of pairing in the description of Giant Monopole Resonances","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Carlos A. Bertulani, Paolo Avogadro","submitted_at":"2013-05-31T04:14:08Z","abstract_excerpt":"We compare the results obtained in the framework of the quasiparticle random phase approximation (QRPA) on top of a Hartree-Fock-Bogoliubov (HFB) with the most recent experiments on giant monopole resonances in Pb, Sn, Zr, Sm, Mo and Cd. Our calculations are fully self consistent and the density dependence of pairing interactions is, for the first time in this framework, properly taken into account. In the particle-hole (ph) channel we employ different Skyrme functionals (SLy5, SkM* and Skxs20) while in the particle-particle (pp) channel we make use of density dependent contact interactions. W"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1305.7299","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:49:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"03FTiws1x3zu8FSZGlBEgo75j587/BCabfUvuA650KJNciIAYK+1Pe246EI5yrYjH3ZiYPn1C+TuUhyjazl0DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T08:05:19.454491Z"},"content_sha256":"fc1f060fc4ebe6c91c38b9494567a5e446fd41cd4b6620217de5d6177d9e5f28","schema_version":"1.0","event_id":"sha256:fc1f060fc4ebe6c91c38b9494567a5e446fd41cd4b6620217de5d6177d9e5f28"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YOTMOL34PISM6AHNBHC6JWE6L3/bundle.json","state_url":"https://pith.science/pith/YOTMOL34PISM6AHNBHC6JWE6L3/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YOTMOL34PISM6AHNBHC6JWE6L3/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":"2026-05-27T08:05:19Z","links":{"resolver":"https://pith.science/pith/YOTMOL34PISM6AHNBHC6JWE6L3","bundle":"https://pith.science/pith/YOTMOL34PISM6AHNBHC6JWE6L3/bundle.json","state":"https://pith.science/pith/YOTMOL34PISM6AHNBHC6JWE6L3/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YOTMOL34PISM6AHNBHC6JWE6L3/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:YOTMOL34PISM6AHNBHC6JWE6L3","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":"5bcb0efd87a15b2cda41f27d625b2f665b2498bf0fe39cf84ef4f037c14a9342","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2013-05-31T04:14:08Z","title_canon_sha256":"4217b4f648b743bfd0626a3b35851731515d27240f2c8173dc9550ad864973b1"},"schema_version":"1.0","source":{"id":"1305.7299","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1305.7299","created_at":"2026-05-18T01:49:39Z"},{"alias_kind":"arxiv_version","alias_value":"1305.7299v2","created_at":"2026-05-18T01:49:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1305.7299","created_at":"2026-05-18T01:49:39Z"},{"alias_kind":"pith_short_12","alias_value":"YOTMOL34PISM","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_16","alias_value":"YOTMOL34PISM6AHN","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_8","alias_value":"YOTMOL34","created_at":"2026-05-18T12:28:06Z"}],"graph_snapshots":[{"event_id":"sha256:fc1f060fc4ebe6c91c38b9494567a5e446fd41cd4b6620217de5d6177d9e5f28","target":"graph","created_at":"2026-05-18T01:49:39Z","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":"We compare the results obtained in the framework of the quasiparticle random phase approximation (QRPA) on top of a Hartree-Fock-Bogoliubov (HFB) with the most recent experiments on giant monopole resonances in Pb, Sn, Zr, Sm, Mo and Cd. Our calculations are fully self consistent and the density dependence of pairing interactions is, for the first time in this framework, properly taken into account. In the particle-hole (ph) channel we employ different Skyrme functionals (SLy5, SkM* and Skxs20) while in the particle-particle (pp) channel we make use of density dependent contact interactions. W","authors_text":"Carlos A. Bertulani, Paolo Avogadro","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2013-05-31T04:14:08Z","title":"Role of pairing in the description of Giant Monopole Resonances"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1305.7299","kind":"arxiv","version":2},"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:ebcd364933c85823d3b1d3490d20c1dbf8960da2569ceca13a53d6f2eb01a806","target":"record","created_at":"2026-05-18T01:49:39Z","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":"5bcb0efd87a15b2cda41f27d625b2f665b2498bf0fe39cf84ef4f037c14a9342","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2013-05-31T04:14:08Z","title_canon_sha256":"4217b4f648b743bfd0626a3b35851731515d27240f2c8173dc9550ad864973b1"},"schema_version":"1.0","source":{"id":"1305.7299","kind":"arxiv","version":2}},"canonical_sha256":"c3a6c72f7c7a24cf00ed09c5e4d89e5eca8bfcab0c05452c17234e42c82cc2c7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c3a6c72f7c7a24cf00ed09c5e4d89e5eca8bfcab0c05452c17234e42c82cc2c7","first_computed_at":"2026-05-18T01:49:39.361095Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:49:39.361095Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"72YZnfKwNsrwdIUwyAcniRQXhDXSrcHvvR3TUmBgfAulYoypkralOtckuFhKovMKOmhoEUgkvVm8z5+N3700CQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:49:39.361664Z","signed_message":"canonical_sha256_bytes"},"source_id":"1305.7299","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ebcd364933c85823d3b1d3490d20c1dbf8960da2569ceca13a53d6f2eb01a806","sha256:fc1f060fc4ebe6c91c38b9494567a5e446fd41cd4b6620217de5d6177d9e5f28"],"state_sha256":"a1e7e115879b545b1c2433d9e1397fb0ff5d52506eab1d91d97ad9eb93f1b32c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HMG+k/NFB7sAqvm8kDQfLHgfr6WG9p6Oggnfv010VKKAW0QeTORDIwc41IMvNMLJ2/Tn9m300YMC1jPhHmWuBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T08:05:19.458366Z","bundle_sha256":"f2615e36cf9177fb06073a47ebfdd5a8f21f7d75a0eecf178cc4b0dfc67f8317"}}