{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:ZXMORKMVL34HZKQYUFSBSLQ2MK","short_pith_number":"pith:ZXMORKMV","canonical_record":{"source":{"id":"1008.0128","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2010-07-31T22:15:40Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"a419f807a8de2c7acd09e32b72104fd0efa933561997f903f08c8fae0924cfb0","abstract_canon_sha256":"abee6632fc68292a798cfc0946b41134f635270cd007ce0f8792d443fa88c390"},"schema_version":"1.0"},"canonical_sha256":"cdd8e8a9955ef87caa18a164192e1a6289454f681e401fc9e9fdbef0f847ee94","source":{"kind":"arxiv","id":"1008.0128","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1008.0128","created_at":"2026-05-18T02:33:08Z"},{"alias_kind":"arxiv_version","alias_value":"1008.0128v1","created_at":"2026-05-18T02:33:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1008.0128","created_at":"2026-05-18T02:33:08Z"},{"alias_kind":"pith_short_12","alias_value":"ZXMORKMVL34H","created_at":"2026-05-18T12:26:18Z"},{"alias_kind":"pith_short_16","alias_value":"ZXMORKMVL34HZKQY","created_at":"2026-05-18T12:26:18Z"},{"alias_kind":"pith_short_8","alias_value":"ZXMORKMV","created_at":"2026-05-18T12:26:18Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:ZXMORKMVL34HZKQYUFSBSLQ2MK","target":"record","payload":{"canonical_record":{"source":{"id":"1008.0128","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2010-07-31T22:15:40Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"a419f807a8de2c7acd09e32b72104fd0efa933561997f903f08c8fae0924cfb0","abstract_canon_sha256":"abee6632fc68292a798cfc0946b41134f635270cd007ce0f8792d443fa88c390"},"schema_version":"1.0"},"canonical_sha256":"cdd8e8a9955ef87caa18a164192e1a6289454f681e401fc9e9fdbef0f847ee94","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:33:08.571623Z","signature_b64":"nkRB9BSSWuEtHnyZgsWpUDwrXfru6xyAg3wGlk4k42QFg3IeimSFdAwIHYfGCd+hQ2pAgcH9cr3GpTN96ZvYAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cdd8e8a9955ef87caa18a164192e1a6289454f681e401fc9e9fdbef0f847ee94","last_reissued_at":"2026-05-18T02:33:08.571257Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:33:08.571257Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1008.0128","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":"2026-05-18T02:33:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"g9DlVii39BJ1zfuVTXzZWzmsQPlrxAjEgNRbg/Z1QXcRtQvT5B8UVIZgA6wDbIYX8QhGabjU1bLn1Rw6Or2zBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-12T10:09:21.114634Z"},"content_sha256":"02e8fb400a1c98f2f5a303b4aaa92565dbc60afe67d42c7e5b81c8ff42fa7710","schema_version":"1.0","event_id":"sha256:02e8fb400a1c98f2f5a303b4aaa92565dbc60afe67d42c7e5b81c8ff42fa7710"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:ZXMORKMVL34HZKQYUFSBSLQ2MK","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Highly accurate calculations of the rotationally excited bound states in three-body systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"physics.atom-ph","authors_text":"Alexei M. Frolov, David M. Wardlaw","submitted_at":"2010-07-31T22:15:40Z","abstract_excerpt":"An effective optimization strategy has been developed to construct highly accurate bound state wave functions in various three-body systems. Our procedure appears to be very effective for computations of weakly bound states and various excited states, including rotationally excited states, i.e. states with $L \\ge 1$. The efficiency of our procedure is illustrated by computations of the excited $P^{*}(L = 1)-$states in the $dd\\mu, dt\\mu$ and $tt\\mu$ muonic molecular ions, $P(L = 1)-$states in the non-symmetric $pd\\mu, pt\\mu$ and $dt\\mu$ ions and $2^{1}P(L = 1)-$ and $2^{3}P(L = 1)-$states in He"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1008.0128","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":"2026-05-18T02:33:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7ZnjSb+CbFdtvQ7TkKLl42nt6THxdIVB7ZA04VO5oxTjSldjMGP/p1KQZyyLjTS6CMytdAu8kWnJF9Rn2oBgCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-12T10:09:21.114987Z"},"content_sha256":"8e56f67eb4384f0c1e5075fd5080dc065ff0bc79d3de2f70531beafb31d67936","schema_version":"1.0","event_id":"sha256:8e56f67eb4384f0c1e5075fd5080dc065ff0bc79d3de2f70531beafb31d67936"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZXMORKMVL34HZKQYUFSBSLQ2MK/bundle.json","state_url":"https://pith.science/pith/ZXMORKMVL34HZKQYUFSBSLQ2MK/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZXMORKMVL34HZKQYUFSBSLQ2MK/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":"2026-06-12T10:09:21Z","links":{"resolver":"https://pith.science/pith/ZXMORKMVL34HZKQYUFSBSLQ2MK","bundle":"https://pith.science/pith/ZXMORKMVL34HZKQYUFSBSLQ2MK/bundle.json","state":"https://pith.science/pith/ZXMORKMVL34HZKQYUFSBSLQ2MK/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZXMORKMVL34HZKQYUFSBSLQ2MK/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:ZXMORKMVL34HZKQYUFSBSLQ2MK","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":"abee6632fc68292a798cfc0946b41134f635270cd007ce0f8792d443fa88c390","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2010-07-31T22:15:40Z","title_canon_sha256":"a419f807a8de2c7acd09e32b72104fd0efa933561997f903f08c8fae0924cfb0"},"schema_version":"1.0","source":{"id":"1008.0128","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1008.0128","created_at":"2026-05-18T02:33:08Z"},{"alias_kind":"arxiv_version","alias_value":"1008.0128v1","created_at":"2026-05-18T02:33:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1008.0128","created_at":"2026-05-18T02:33:08Z"},{"alias_kind":"pith_short_12","alias_value":"ZXMORKMVL34H","created_at":"2026-05-18T12:26:18Z"},{"alias_kind":"pith_short_16","alias_value":"ZXMORKMVL34HZKQY","created_at":"2026-05-18T12:26:18Z"},{"alias_kind":"pith_short_8","alias_value":"ZXMORKMV","created_at":"2026-05-18T12:26:18Z"}],"graph_snapshots":[{"event_id":"sha256:8e56f67eb4384f0c1e5075fd5080dc065ff0bc79d3de2f70531beafb31d67936","target":"graph","created_at":"2026-05-18T02:33:08Z","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":"An effective optimization strategy has been developed to construct highly accurate bound state wave functions in various three-body systems. Our procedure appears to be very effective for computations of weakly bound states and various excited states, including rotationally excited states, i.e. states with $L \\ge 1$. The efficiency of our procedure is illustrated by computations of the excited $P^{*}(L = 1)-$states in the $dd\\mu, dt\\mu$ and $tt\\mu$ muonic molecular ions, $P(L = 1)-$states in the non-symmetric $pd\\mu, pt\\mu$ and $dt\\mu$ ions and $2^{1}P(L = 1)-$ and $2^{3}P(L = 1)-$states in He","authors_text":"Alexei M. Frolov, David M. Wardlaw","cross_cats":["hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2010-07-31T22:15:40Z","title":"Highly accurate calculations of the rotationally excited bound states in three-body systems"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1008.0128","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":"sha256:02e8fb400a1c98f2f5a303b4aaa92565dbc60afe67d42c7e5b81c8ff42fa7710","target":"record","created_at":"2026-05-18T02:33:08Z","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":"abee6632fc68292a798cfc0946b41134f635270cd007ce0f8792d443fa88c390","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2010-07-31T22:15:40Z","title_canon_sha256":"a419f807a8de2c7acd09e32b72104fd0efa933561997f903f08c8fae0924cfb0"},"schema_version":"1.0","source":{"id":"1008.0128","kind":"arxiv","version":1}},"canonical_sha256":"cdd8e8a9955ef87caa18a164192e1a6289454f681e401fc9e9fdbef0f847ee94","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"cdd8e8a9955ef87caa18a164192e1a6289454f681e401fc9e9fdbef0f847ee94","first_computed_at":"2026-05-18T02:33:08.571257Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:33:08.571257Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"nkRB9BSSWuEtHnyZgsWpUDwrXfru6xyAg3wGlk4k42QFg3IeimSFdAwIHYfGCd+hQ2pAgcH9cr3GpTN96ZvYAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:33:08.571623Z","signed_message":"canonical_sha256_bytes"},"source_id":"1008.0128","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:02e8fb400a1c98f2f5a303b4aaa92565dbc60afe67d42c7e5b81c8ff42fa7710","sha256:8e56f67eb4384f0c1e5075fd5080dc065ff0bc79d3de2f70531beafb31d67936"],"state_sha256":"afd32d2058a319009993dab88bacb2ebac8292897f6923ac5abf2d682df4b93c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CANBYekjypil74CLwKRADayrv3BamE+dJYw3sNMYkoTD09wphJlwlXO8SBgw3IClogcVOrIsRiMNYLG1zeJZBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-12T10:09:21.117566Z","bundle_sha256":"2c7be477572c446092248126f4a3155a0b70200b42d1ed2983c400a72aec4fa9"}}