{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2008:BWOVF7CRLRNMQGQULZM74AZ7VY","short_pith_number":"pith:BWOVF7CR","canonical_record":{"source":{"id":"0812.4984","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2008-12-29T22:58:32Z","cross_cats_sorted":[],"title_canon_sha256":"607ac7d2b54b75f06705b53ef4262aa22b88ecb7841f394df43fed15098a1686","abstract_canon_sha256":"0e8a3867d9f684cd2a6a952a82bb90993716cc3d26a1e1e2e76a5d434713d428"},"schema_version":"1.0"},"canonical_sha256":"0d9d52fc515c5ac81a145e59fe033fae3ab288e866e1f03f356ffee057cfda13","source":{"kind":"arxiv","id":"0812.4984","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0812.4984","created_at":"2026-07-04T17:26:24Z"},{"alias_kind":"arxiv_version","alias_value":"0812.4984v2","created_at":"2026-07-04T17:26:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0812.4984","created_at":"2026-07-04T17:26:24Z"},{"alias_kind":"pith_short_12","alias_value":"BWOVF7CRLRNM","created_at":"2026-07-04T17:26:24Z"},{"alias_kind":"pith_short_16","alias_value":"BWOVF7CRLRNMQGQU","created_at":"2026-07-04T17:26:24Z"},{"alias_kind":"pith_short_8","alias_value":"BWOVF7CR","created_at":"2026-07-04T17:26:24Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2008:BWOVF7CRLRNMQGQULZM74AZ7VY","target":"record","payload":{"canonical_record":{"source":{"id":"0812.4984","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2008-12-29T22:58:32Z","cross_cats_sorted":[],"title_canon_sha256":"607ac7d2b54b75f06705b53ef4262aa22b88ecb7841f394df43fed15098a1686","abstract_canon_sha256":"0e8a3867d9f684cd2a6a952a82bb90993716cc3d26a1e1e2e76a5d434713d428"},"schema_version":"1.0"},"canonical_sha256":"0d9d52fc515c5ac81a145e59fe033fae3ab288e866e1f03f356ffee057cfda13","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:26:24.363036Z","signature_b64":"v3Q+e2Kwoe0b8bVMU6LvllYl5WBt6rF1W8zIuNZ9/svsmc6Vlj6G1CRxOEW1YFM5NMxDqqVuN7vAiFCtWU5eCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0d9d52fc515c5ac81a145e59fe033fae3ab288e866e1f03f356ffee057cfda13","last_reissued_at":"2026-07-04T17:26:24.362647Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:26:24.362647Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"0812.4984","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":"2026-07-04T17:26:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"prgu1Ze5kwZpP9UL8Tu/HvomD8xOOCp6F56Xwo6z0BKqx9wYvIX0x7KnY8ZNquMRvMjKBQZyvcfmwThsHCihCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-13T21:47:55.859175Z"},"content_sha256":"2bd4f0b97d8627acd6341d0f9788a4c37326d6404162a30c123c6b59eb914f41","schema_version":"1.0","event_id":"sha256:2bd4f0b97d8627acd6341d0f9788a4c37326d6404162a30c123c6b59eb914f41"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2008:BWOVF7CRLRNMQGQULZM74AZ7VY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Towards thermal evolution of the most general 2HDM","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"I. P. Ivanov","submitted_at":"2008-12-29T22:58:32Z","abstract_excerpt":"We consider the scalar sector of the most general renormalizable two-Higgs-doublet model at non-zero temperature. We calculate the largest finite temperature corrections to the free-energy density and study thermal evolution of the ground state. Within the approximation chosen, we establish all possible sequences of thermal phase transitions and study their relation with the symmetries of the model. We show, in particular, that a charge-breaking or a CP-violating vacuum can arise at intermediate stages of thermal evolution, and that the first-order phase transition is associated with a discret"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0812.4984","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/0812.4984/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-04T17:26:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BKWJKCq7VJEvjdzGkNeku1SCQkPXUwWVY2i4Mp05qesYcnNNHKgIwyXZNgG5+mzj5abALe6cS25PNFPji8OcAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-13T21:47:55.859738Z"},"content_sha256":"188c0fc1363dd1584e96a26927333e40554ecfae6c8b76408bf4c4a49194109f","schema_version":"1.0","event_id":"sha256:188c0fc1363dd1584e96a26927333e40554ecfae6c8b76408bf4c4a49194109f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/BWOVF7CRLRNMQGQULZM74AZ7VY/bundle.json","state_url":"https://pith.science/pith/BWOVF7CRLRNMQGQULZM74AZ7VY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/BWOVF7CRLRNMQGQULZM74AZ7VY/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":"2026-08-13T21:47:55Z","links":{"resolver":"https://pith.science/pith/BWOVF7CRLRNMQGQULZM74AZ7VY","bundle":"https://pith.science/pith/BWOVF7CRLRNMQGQULZM74AZ7VY/bundle.json","state":"https://pith.science/pith/BWOVF7CRLRNMQGQULZM74AZ7VY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/BWOVF7CRLRNMQGQULZM74AZ7VY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2008:BWOVF7CRLRNMQGQULZM74AZ7VY","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":"0e8a3867d9f684cd2a6a952a82bb90993716cc3d26a1e1e2e76a5d434713d428","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2008-12-29T22:58:32Z","title_canon_sha256":"607ac7d2b54b75f06705b53ef4262aa22b88ecb7841f394df43fed15098a1686"},"schema_version":"1.0","source":{"id":"0812.4984","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0812.4984","created_at":"2026-07-04T17:26:24Z"},{"alias_kind":"arxiv_version","alias_value":"0812.4984v2","created_at":"2026-07-04T17:26:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0812.4984","created_at":"2026-07-04T17:26:24Z"},{"alias_kind":"pith_short_12","alias_value":"BWOVF7CRLRNM","created_at":"2026-07-04T17:26:24Z"},{"alias_kind":"pith_short_16","alias_value":"BWOVF7CRLRNMQGQU","created_at":"2026-07-04T17:26:24Z"},{"alias_kind":"pith_short_8","alias_value":"BWOVF7CR","created_at":"2026-07-04T17:26:24Z"}],"graph_snapshots":[{"event_id":"sha256:188c0fc1363dd1584e96a26927333e40554ecfae6c8b76408bf4c4a49194109f","target":"graph","created_at":"2026-07-04T17:26:24Z","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/0812.4984/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We consider the scalar sector of the most general renormalizable two-Higgs-doublet model at non-zero temperature. We calculate the largest finite temperature corrections to the free-energy density and study thermal evolution of the ground state. Within the approximation chosen, we establish all possible sequences of thermal phase transitions and study their relation with the symmetries of the model. We show, in particular, that a charge-breaking or a CP-violating vacuum can arise at intermediate stages of thermal evolution, and that the first-order phase transition is associated with a discret","authors_text":"I. P. Ivanov","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2008-12-29T22:58:32Z","title":"Towards thermal evolution of the most general 2HDM"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0812.4984","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":"sha256:2bd4f0b97d8627acd6341d0f9788a4c37326d6404162a30c123c6b59eb914f41","target":"record","created_at":"2026-07-04T17:26:24Z","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":"0e8a3867d9f684cd2a6a952a82bb90993716cc3d26a1e1e2e76a5d434713d428","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2008-12-29T22:58:32Z","title_canon_sha256":"607ac7d2b54b75f06705b53ef4262aa22b88ecb7841f394df43fed15098a1686"},"schema_version":"1.0","source":{"id":"0812.4984","kind":"arxiv","version":2}},"canonical_sha256":"0d9d52fc515c5ac81a145e59fe033fae3ab288e866e1f03f356ffee057cfda13","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0d9d52fc515c5ac81a145e59fe033fae3ab288e866e1f03f356ffee057cfda13","first_computed_at":"2026-07-04T17:26:24.362647Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T17:26:24.362647Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"v3Q+e2Kwoe0b8bVMU6LvllYl5WBt6rF1W8zIuNZ9/svsmc6Vlj6G1CRxOEW1YFM5NMxDqqVuN7vAiFCtWU5eCQ==","signature_status":"signed_v1","signed_at":"2026-07-04T17:26:24.363036Z","signed_message":"canonical_sha256_bytes"},"source_id":"0812.4984","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2bd4f0b97d8627acd6341d0f9788a4c37326d6404162a30c123c6b59eb914f41","sha256:188c0fc1363dd1584e96a26927333e40554ecfae6c8b76408bf4c4a49194109f"],"state_sha256":"92a249ffa4a1847d5934b3a013381baffb93201a7ac5cecf26cd43529277b5ea"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/Ae7o7n+YeUsAJSH9FUiDGXjz8Ijh3cWoTLmfZQceriLWgyXEM5bbQ3Upx3pDXnCkBpA7z9eMwh2U/JtxX5KAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-13T21:47:55.869455Z","bundle_sha256":"a24cfdc529a1aaf2ccfc32d04e2cc7b013bd0b2446f8b27c567837ccdfe36005"}}