{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2000:GOFT4PNRUGDMZRCQ63TJVQI6GM","short_pith_number":"pith:GOFT4PNR","canonical_record":{"source":{"id":"cond-mat/0005385","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.str-el","submitted_at":"2000-05-23T14:25:58Z","cross_cats_sorted":[],"title_canon_sha256":"ea106c4fc95ea3f15f0440ff3901031381e835da0dd7bcc53c115315c34bf7c7","abstract_canon_sha256":"17b890a589c17c03a8f2a2b15762e97560c795da26595018f9f44b632c65d24c"},"schema_version":"1.0"},"canonical_sha256":"338b3e3db1a186ccc450f6e69ac11e33187cc9cf19e6c11167514062ee58a957","source":{"kind":"arxiv","id":"cond-mat/0005385","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0005385","created_at":"2026-07-04T16:18:30Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0005385v1","created_at":"2026-07-04T16:18:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0005385","created_at":"2026-07-04T16:18:30Z"},{"alias_kind":"pith_short_12","alias_value":"GOFT4PNRUGDM","created_at":"2026-07-04T16:18:30Z"},{"alias_kind":"pith_short_16","alias_value":"GOFT4PNRUGDMZRCQ","created_at":"2026-07-04T16:18:30Z"},{"alias_kind":"pith_short_8","alias_value":"GOFT4PNR","created_at":"2026-07-04T16:18:30Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2000:GOFT4PNRUGDMZRCQ63TJVQI6GM","target":"record","payload":{"canonical_record":{"source":{"id":"cond-mat/0005385","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.str-el","submitted_at":"2000-05-23T14:25:58Z","cross_cats_sorted":[],"title_canon_sha256":"ea106c4fc95ea3f15f0440ff3901031381e835da0dd7bcc53c115315c34bf7c7","abstract_canon_sha256":"17b890a589c17c03a8f2a2b15762e97560c795da26595018f9f44b632c65d24c"},"schema_version":"1.0"},"canonical_sha256":"338b3e3db1a186ccc450f6e69ac11e33187cc9cf19e6c11167514062ee58a957","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:18:30.994115Z","signature_b64":"g6uY5A1c45W7CnaElqlKpCsIs3dqLNTz5hH5mB5wtto5yyBtm2cRMvp5Vmx0+S+FxICjYZUQHFyTEtT9Su/fAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"338b3e3db1a186ccc450f6e69ac11e33187cc9cf19e6c11167514062ee58a957","last_reissued_at":"2026-07-04T16:18:30.993701Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:18:30.993701Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"cond-mat/0005385","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":"2026-07-04T16:18:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"srcR7JEUT4+gWBMi/KslySD7wlcpbGtL2u03+yAZ2V5Chd0AT6pGBEHlVee+EbNT/BR8HKciwbIeqM7mlTVPBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-07T07:22:51.410741Z"},"content_sha256":"1ad8ffdec51784b73dbae954abcdcfb3baeac2b462a7776bbc4c6925cb9209e3","schema_version":"1.0","event_id":"sha256:1ad8ffdec51784b73dbae954abcdcfb3baeac2b462a7776bbc4c6925cb9209e3"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2000:GOFT4PNRUGDMZRCQ63TJVQI6GM","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Critical properties of projected SO(5) models at finite temperatures","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"E. Arrigoni, W. Hanke (University of Wuerzburg - Germany)","submitted_at":"2000-05-23T14:25:58Z","abstract_excerpt":"We consider the projected SO(5) bosonic model introduced in order to connect the SO(5) theory of high-T$_c$ superconductivity with the physics of the Mott-insulating gap, and derive the corresponding effective functional describing low-energy degrees of freedom. At the antiferromagnetic-superconducting transition, SO(5) symmetry-breaking effects due to the gap are purely quantum mechanical and become irrelevant in the neighborhood of a possible finite-temperature multicritical point separating the normal from the antiferromagnetic and the superconducting phases. A difference in the magnon and "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0005385","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/cond-mat/0005385/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":"2026-07-04T16:18:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CRwHUoOwXysZDEPQT3/U+fghLxggisVC4t+uJSk7Hk9BY/uSK4xRad+dDfibKqavkcLvkxGHL3NGxIK8UlsSBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-07T07:22:51.411158Z"},"content_sha256":"ab5c97a715b317e2266bd8c7f27d89d07a85f54c0a8e957ea0b70b791c037187","schema_version":"1.0","event_id":"sha256:ab5c97a715b317e2266bd8c7f27d89d07a85f54c0a8e957ea0b70b791c037187"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GOFT4PNRUGDMZRCQ63TJVQI6GM/bundle.json","state_url":"https://pith.science/pith/GOFT4PNRUGDMZRCQ63TJVQI6GM/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GOFT4PNRUGDMZRCQ63TJVQI6GM/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":"2026-07-07T07:22:51Z","links":{"resolver":"https://pith.science/pith/GOFT4PNRUGDMZRCQ63TJVQI6GM","bundle":"https://pith.science/pith/GOFT4PNRUGDMZRCQ63TJVQI6GM/bundle.json","state":"https://pith.science/pith/GOFT4PNRUGDMZRCQ63TJVQI6GM/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GOFT4PNRUGDMZRCQ63TJVQI6GM/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2000:GOFT4PNRUGDMZRCQ63TJVQI6GM","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":"17b890a589c17c03a8f2a2b15762e97560c795da26595018f9f44b632c65d24c","cross_cats_sorted":[],"license":"","primary_cat":"cond-mat.str-el","submitted_at":"2000-05-23T14:25:58Z","title_canon_sha256":"ea106c4fc95ea3f15f0440ff3901031381e835da0dd7bcc53c115315c34bf7c7"},"schema_version":"1.0","source":{"id":"cond-mat/0005385","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0005385","created_at":"2026-07-04T16:18:30Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0005385v1","created_at":"2026-07-04T16:18:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0005385","created_at":"2026-07-04T16:18:30Z"},{"alias_kind":"pith_short_12","alias_value":"GOFT4PNRUGDM","created_at":"2026-07-04T16:18:30Z"},{"alias_kind":"pith_short_16","alias_value":"GOFT4PNRUGDMZRCQ","created_at":"2026-07-04T16:18:30Z"},{"alias_kind":"pith_short_8","alias_value":"GOFT4PNR","created_at":"2026-07-04T16:18:30Z"}],"graph_snapshots":[{"event_id":"sha256:ab5c97a715b317e2266bd8c7f27d89d07a85f54c0a8e957ea0b70b791c037187","target":"graph","created_at":"2026-07-04T16:18:30Z","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/cond-mat/0005385/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We consider the projected SO(5) bosonic model introduced in order to connect the SO(5) theory of high-T$_c$ superconductivity with the physics of the Mott-insulating gap, and derive the corresponding effective functional describing low-energy degrees of freedom. At the antiferromagnetic-superconducting transition, SO(5) symmetry-breaking effects due to the gap are purely quantum mechanical and become irrelevant in the neighborhood of a possible finite-temperature multicritical point separating the normal from the antiferromagnetic and the superconducting phases. A difference in the magnon and ","authors_text":"E. Arrigoni, W. Hanke (University of Wuerzburg - Germany)","cross_cats":[],"headline":"","license":"","primary_cat":"cond-mat.str-el","submitted_at":"2000-05-23T14:25:58Z","title":"Critical properties of projected SO(5) models at finite temperatures"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0005385","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":"sha256:1ad8ffdec51784b73dbae954abcdcfb3baeac2b462a7776bbc4c6925cb9209e3","target":"record","created_at":"2026-07-04T16:18:30Z","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":"17b890a589c17c03a8f2a2b15762e97560c795da26595018f9f44b632c65d24c","cross_cats_sorted":[],"license":"","primary_cat":"cond-mat.str-el","submitted_at":"2000-05-23T14:25:58Z","title_canon_sha256":"ea106c4fc95ea3f15f0440ff3901031381e835da0dd7bcc53c115315c34bf7c7"},"schema_version":"1.0","source":{"id":"cond-mat/0005385","kind":"arxiv","version":1}},"canonical_sha256":"338b3e3db1a186ccc450f6e69ac11e33187cc9cf19e6c11167514062ee58a957","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"338b3e3db1a186ccc450f6e69ac11e33187cc9cf19e6c11167514062ee58a957","first_computed_at":"2026-07-04T16:18:30.993701Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:18:30.993701Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"g6uY5A1c45W7CnaElqlKpCsIs3dqLNTz5hH5mB5wtto5yyBtm2cRMvp5Vmx0+S+FxICjYZUQHFyTEtT9Su/fAg==","signature_status":"signed_v1","signed_at":"2026-07-04T16:18:30.994115Z","signed_message":"canonical_sha256_bytes"},"source_id":"cond-mat/0005385","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1ad8ffdec51784b73dbae954abcdcfb3baeac2b462a7776bbc4c6925cb9209e3","sha256:ab5c97a715b317e2266bd8c7f27d89d07a85f54c0a8e957ea0b70b791c037187"],"state_sha256":"34f5be60fc80274f9b5c55ba8b15cd11df493ac71d921c10e0f7fc5e321ee70b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vN4sBRAcQKGjbnJzW+4hmtEKjno7XJT8goAw695HCqS+wYVbICPOoISUxTWbU+tl4oKRlPpZGmUc5hy7wmPVDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-07T07:22:51.413340Z","bundle_sha256":"1f3e1e27baea2a1a42d3d6bf2cfc32718e4b7de689139ebc024f11697608a1ad"}}