{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:MYSFPBE3DNVBMSQFKKDLWBLCER","short_pith_number":"pith:MYSFPBE3","canonical_record":{"source":{"id":"1501.00004","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-30T21:00:06Z","cross_cats_sorted":["cond-mat.supr-con","gr-qc"],"title_canon_sha256":"465e4e2960772ccfcf0b7e2f96631cd730fd54420dd356d0f1dcba77dcea21bf","abstract_canon_sha256":"5644961ab0c48b78407c3dcd208e89e6b959b7f60c71cfd5b2fd12acb7b533f0"},"schema_version":"1.0"},"canonical_sha256":"662457849b1b6a164a055286bb0562244ccd95634e07f197ba2b182a27f814fe","source":{"kind":"arxiv","id":"1501.00004","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1501.00004","created_at":"2026-05-18T00:27:22Z"},{"alias_kind":"arxiv_version","alias_value":"1501.00004v2","created_at":"2026-05-18T00:27:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1501.00004","created_at":"2026-05-18T00:27:22Z"},{"alias_kind":"pith_short_12","alias_value":"MYSFPBE3DNVB","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"MYSFPBE3DNVBMSQF","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"MYSFPBE3","created_at":"2026-05-18T12:28:38Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:MYSFPBE3DNVBMSQFKKDLWBLCER","target":"record","payload":{"canonical_record":{"source":{"id":"1501.00004","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-30T21:00:06Z","cross_cats_sorted":["cond-mat.supr-con","gr-qc"],"title_canon_sha256":"465e4e2960772ccfcf0b7e2f96631cd730fd54420dd356d0f1dcba77dcea21bf","abstract_canon_sha256":"5644961ab0c48b78407c3dcd208e89e6b959b7f60c71cfd5b2fd12acb7b533f0"},"schema_version":"1.0"},"canonical_sha256":"662457849b1b6a164a055286bb0562244ccd95634e07f197ba2b182a27f814fe","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:27:22.686067Z","signature_b64":"EGLKDhPBBSZmbmJWQOfsGZoSAr6hbogbhtMBT9oInw5uKa5OqEBrMg4byi5+uXxOWIwQE8eaj83gbaHxoDoJCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"662457849b1b6a164a055286bb0562244ccd95634e07f197ba2b182a27f814fe","last_reissued_at":"2026-05-18T00:27:22.685368Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:27:22.685368Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1501.00004","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":"2026-05-18T00:27:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lbFhYVF27o/sa7htqgirLVOKBEZ1qD8QcwhaEa/Ztmad09ZO29GF3nhyJDgoUjDwt1I+jc0i+S5P0eHIF2G7BQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-23T22:26:10.206492Z"},"content_sha256":"65e44e5884ca3c781d5c7bb8c81cdc76cd2c0723f88d95fbe1be3a1ba12b915f","schema_version":"1.0","event_id":"sha256:65e44e5884ca3c781d5c7bb8c81cdc76cd2c0723f88d95fbe1be3a1ba12b915f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:MYSFPBE3DNVBMSQFKKDLWBLCER","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Phase transitions in a holographic s+p model with backreaction","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con","gr-qc"],"primary_cat":"hep-th","authors_text":"Hui Zeng, Li Li, Rong-Gen Cai, Xin Gao, Zhang-Yu Nie","submitted_at":"2014-12-30T21:00:06Z","abstract_excerpt":"In a previous paper (arXiv:1309.2204, JHEP 1311 (2013) 087), we present a holographic s+p superconductor model with a scalar triplet charged under an SU(2) gauge field in the bulk. We also study the competition and coexistence of the s-wave and p-wave orders in the probe limit. In this work we continue to study the model by considering the full back-reaction The model shows a rich phase structure and various condensate behaviors such as the \"n-type\" and \"u-type\" ones, which are also known as reentrant phase transitions in condensed matter physics. The phase transitions to the p-wave phase or s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1501.00004","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":"2026-05-18T00:27:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AFzPNI3EyP8CBJ2LxfkOXNG3sa0JNC60ZjmGVFQQjabQDxgZ7KwqwHZZ8mh3v+OY13S3DSBDo5PT/EZ6W/RLCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-23T22:26:10.207184Z"},"content_sha256":"be7ebc5e008aa28ff17f5a7a884ef05fd58db57e129e9d857f8a351529f6f662","schema_version":"1.0","event_id":"sha256:be7ebc5e008aa28ff17f5a7a884ef05fd58db57e129e9d857f8a351529f6f662"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/MYSFPBE3DNVBMSQFKKDLWBLCER/bundle.json","state_url":"https://pith.science/pith/MYSFPBE3DNVBMSQFKKDLWBLCER/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/MYSFPBE3DNVBMSQFKKDLWBLCER/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":"2026-05-23T22:26:10Z","links":{"resolver":"https://pith.science/pith/MYSFPBE3DNVBMSQFKKDLWBLCER","bundle":"https://pith.science/pith/MYSFPBE3DNVBMSQFKKDLWBLCER/bundle.json","state":"https://pith.science/pith/MYSFPBE3DNVBMSQFKKDLWBLCER/state.json","well_known_bundle":"https://pith.science/.well-known/pith/MYSFPBE3DNVBMSQFKKDLWBLCER/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:MYSFPBE3DNVBMSQFKKDLWBLCER","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":"5644961ab0c48b78407c3dcd208e89e6b959b7f60c71cfd5b2fd12acb7b533f0","cross_cats_sorted":["cond-mat.supr-con","gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-30T21:00:06Z","title_canon_sha256":"465e4e2960772ccfcf0b7e2f96631cd730fd54420dd356d0f1dcba77dcea21bf"},"schema_version":"1.0","source":{"id":"1501.00004","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1501.00004","created_at":"2026-05-18T00:27:22Z"},{"alias_kind":"arxiv_version","alias_value":"1501.00004v2","created_at":"2026-05-18T00:27:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1501.00004","created_at":"2026-05-18T00:27:22Z"},{"alias_kind":"pith_short_12","alias_value":"MYSFPBE3DNVB","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"MYSFPBE3DNVBMSQF","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"MYSFPBE3","created_at":"2026-05-18T12:28:38Z"}],"graph_snapshots":[{"event_id":"sha256:be7ebc5e008aa28ff17f5a7a884ef05fd58db57e129e9d857f8a351529f6f662","target":"graph","created_at":"2026-05-18T00:27:22Z","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":"In a previous paper (arXiv:1309.2204, JHEP 1311 (2013) 087), we present a holographic s+p superconductor model with a scalar triplet charged under an SU(2) gauge field in the bulk. We also study the competition and coexistence of the s-wave and p-wave orders in the probe limit. In this work we continue to study the model by considering the full back-reaction The model shows a rich phase structure and various condensate behaviors such as the \"n-type\" and \"u-type\" ones, which are also known as reentrant phase transitions in condensed matter physics. The phase transitions to the p-wave phase or s","authors_text":"Hui Zeng, Li Li, Rong-Gen Cai, Xin Gao, Zhang-Yu Nie","cross_cats":["cond-mat.supr-con","gr-qc"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-30T21:00:06Z","title":"Phase transitions in a holographic s+p model with backreaction"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1501.00004","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":"sha256:65e44e5884ca3c781d5c7bb8c81cdc76cd2c0723f88d95fbe1be3a1ba12b915f","target":"record","created_at":"2026-05-18T00:27:22Z","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":"5644961ab0c48b78407c3dcd208e89e6b959b7f60c71cfd5b2fd12acb7b533f0","cross_cats_sorted":["cond-mat.supr-con","gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-30T21:00:06Z","title_canon_sha256":"465e4e2960772ccfcf0b7e2f96631cd730fd54420dd356d0f1dcba77dcea21bf"},"schema_version":"1.0","source":{"id":"1501.00004","kind":"arxiv","version":2}},"canonical_sha256":"662457849b1b6a164a055286bb0562244ccd95634e07f197ba2b182a27f814fe","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"662457849b1b6a164a055286bb0562244ccd95634e07f197ba2b182a27f814fe","first_computed_at":"2026-05-18T00:27:22.685368Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:27:22.685368Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"EGLKDhPBBSZmbmJWQOfsGZoSAr6hbogbhtMBT9oInw5uKa5OqEBrMg4byi5+uXxOWIwQE8eaj83gbaHxoDoJCA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:27:22.686067Z","signed_message":"canonical_sha256_bytes"},"source_id":"1501.00004","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:65e44e5884ca3c781d5c7bb8c81cdc76cd2c0723f88d95fbe1be3a1ba12b915f","sha256:be7ebc5e008aa28ff17f5a7a884ef05fd58db57e129e9d857f8a351529f6f662"],"state_sha256":"fde1f16564de1fb657b99b95810b5dd4ecbbda80215ae1dcfbac2d687b76c411"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"X5bY0a8Lh/QwXzpRdKND/GpGurpZEvRzBzl3Gswtm6zoBpMcib8EIZBceQmMPyMRvludPlnySpF8lgdfH0xeBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-23T22:26:10.211272Z","bundle_sha256":"11a87fd5b5a00c2c75c50047b683f656094dc0b90bdd163ad017a7ac2c6c782d"}}