{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:EKDQH7Q4XLYPMAB3GDRHD5HYBE","short_pith_number":"pith:EKDQH7Q4","canonical_record":{"source":{"id":"1212.4838","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-12-19T21:00:02Z","cross_cats_sorted":["hep-ph","physics.flu-dyn"],"title_canon_sha256":"73fe5c098dd4de451e02fbf65986f55c9d0f2f8680d7bf3ebdd0a1851824ce6b","abstract_canon_sha256":"0114d43dc31bb1d79dff4cfb97c414090c6803282dde90c8cb005ddc61ba4176"},"schema_version":"1.0"},"canonical_sha256":"228703fe1cbaf0f6003b30e271f4f80909756e8bb4c5fa9f64c0e0f8a3a4af54","source":{"kind":"arxiv","id":"1212.4838","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1212.4838","created_at":"2026-05-18T01:52:30Z"},{"alias_kind":"arxiv_version","alias_value":"1212.4838v2","created_at":"2026-05-18T01:52:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1212.4838","created_at":"2026-05-18T01:52:30Z"},{"alias_kind":"pith_short_12","alias_value":"EKDQH7Q4XLYP","created_at":"2026-05-18T12:27:04Z"},{"alias_kind":"pith_short_16","alias_value":"EKDQH7Q4XLYPMAB3","created_at":"2026-05-18T12:27:04Z"},{"alias_kind":"pith_short_8","alias_value":"EKDQH7Q4","created_at":"2026-05-18T12:27:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:EKDQH7Q4XLYPMAB3GDRHD5HYBE","target":"record","payload":{"canonical_record":{"source":{"id":"1212.4838","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-12-19T21:00:02Z","cross_cats_sorted":["hep-ph","physics.flu-dyn"],"title_canon_sha256":"73fe5c098dd4de451e02fbf65986f55c9d0f2f8680d7bf3ebdd0a1851824ce6b","abstract_canon_sha256":"0114d43dc31bb1d79dff4cfb97c414090c6803282dde90c8cb005ddc61ba4176"},"schema_version":"1.0"},"canonical_sha256":"228703fe1cbaf0f6003b30e271f4f80909756e8bb4c5fa9f64c0e0f8a3a4af54","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:52:30.203152Z","signature_b64":"lRtMnWbg+3jeipK6cCes/Qqd79SggEJ3cmQioP5+jr2/B522tRVeuPCiAA7jEwMb3lAAx1ByyL1TL0k3KYkOAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"228703fe1cbaf0f6003b30e271f4f80909756e8bb4c5fa9f64c0e0f8a3a4af54","last_reissued_at":"2026-05-18T01:52:30.202565Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:52:30.202565Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1212.4838","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":"2026-05-18T01:52:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0SKA7t0vPCtkrTU6+56mgdVej4i61bkSw+EppSaaDViz8BEThCqrxggsQWMwVCLmm7hukOLJcaDMb98KWnDsAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T22:43:39.136548Z"},"content_sha256":"ff1a450bcb18b7ba594ae0e5ca1dfdbdd41b21427e1a5cb56fdae89ea746f4ce","schema_version":"1.0","event_id":"sha256:ff1a450bcb18b7ba594ae0e5ca1dfdbdd41b21427e1a5cb56fdae89ea746f4ce"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:EKDQH7Q4XLYPMAB3GDRHD5HYBE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"New Transport Properties of Anisotropic Holographic Superfluids","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","physics.flu-dyn"],"primary_cat":"hep-th","authors_text":"Daniel Fernandez, Hansj\\\"org Zeller, Johanna Erdmenger","submitted_at":"2012-12-19T21:00:02Z","abstract_excerpt":"We complete the analysis of transport phenomena in p-wave superfluids within gauge/gravity duality, using the SU(2) Einstein-Yang-Mills model with backreaction. In particular, we analyze the fluctuation modes of helicity zero in addition to the helicity one and two modes studied earlier. We compute a further transport coefficient, associated to the first normal stress difference, not previously considered in the holographic context. In the unbroken phase this is related to a minimally coupled scalar on the gravity side. Moreover we find transport phenomena related to the thermoelectric and pie"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1212.4838","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":"2026-05-18T01:52:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vBbGqglahOPoL+aJ70MQs67YQ0Nm5i15hyHqWB6m21qmf0NZMNX6ionpZkOS5NkBqch8qcHtu895C5jW81LrCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T22:43:39.137225Z"},"content_sha256":"342154d15d15c577eaf1f98c33423f27481c593d1797d80fc32306914c157139","schema_version":"1.0","event_id":"sha256:342154d15d15c577eaf1f98c33423f27481c593d1797d80fc32306914c157139"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/EKDQH7Q4XLYPMAB3GDRHD5HYBE/bundle.json","state_url":"https://pith.science/pith/EKDQH7Q4XLYPMAB3GDRHD5HYBE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/EKDQH7Q4XLYPMAB3GDRHD5HYBE/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":"2026-06-06T22:43:39Z","links":{"resolver":"https://pith.science/pith/EKDQH7Q4XLYPMAB3GDRHD5HYBE","bundle":"https://pith.science/pith/EKDQH7Q4XLYPMAB3GDRHD5HYBE/bundle.json","state":"https://pith.science/pith/EKDQH7Q4XLYPMAB3GDRHD5HYBE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/EKDQH7Q4XLYPMAB3GDRHD5HYBE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:EKDQH7Q4XLYPMAB3GDRHD5HYBE","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":"0114d43dc31bb1d79dff4cfb97c414090c6803282dde90c8cb005ddc61ba4176","cross_cats_sorted":["hep-ph","physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-12-19T21:00:02Z","title_canon_sha256":"73fe5c098dd4de451e02fbf65986f55c9d0f2f8680d7bf3ebdd0a1851824ce6b"},"schema_version":"1.0","source":{"id":"1212.4838","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1212.4838","created_at":"2026-05-18T01:52:30Z"},{"alias_kind":"arxiv_version","alias_value":"1212.4838v2","created_at":"2026-05-18T01:52:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1212.4838","created_at":"2026-05-18T01:52:30Z"},{"alias_kind":"pith_short_12","alias_value":"EKDQH7Q4XLYP","created_at":"2026-05-18T12:27:04Z"},{"alias_kind":"pith_short_16","alias_value":"EKDQH7Q4XLYPMAB3","created_at":"2026-05-18T12:27:04Z"},{"alias_kind":"pith_short_8","alias_value":"EKDQH7Q4","created_at":"2026-05-18T12:27:04Z"}],"graph_snapshots":[{"event_id":"sha256:342154d15d15c577eaf1f98c33423f27481c593d1797d80fc32306914c157139","target":"graph","created_at":"2026-05-18T01:52:30Z","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"},"paper":{"abstract_excerpt":"We complete the analysis of transport phenomena in p-wave superfluids within gauge/gravity duality, using the SU(2) Einstein-Yang-Mills model with backreaction. In particular, we analyze the fluctuation modes of helicity zero in addition to the helicity one and two modes studied earlier. We compute a further transport coefficient, associated to the first normal stress difference, not previously considered in the holographic context. In the unbroken phase this is related to a minimally coupled scalar on the gravity side. Moreover we find transport phenomena related to the thermoelectric and pie","authors_text":"Daniel Fernandez, Hansj\\\"org Zeller, Johanna Erdmenger","cross_cats":["hep-ph","physics.flu-dyn"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-12-19T21:00:02Z","title":"New Transport Properties of Anisotropic Holographic Superfluids"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1212.4838","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:ff1a450bcb18b7ba594ae0e5ca1dfdbdd41b21427e1a5cb56fdae89ea746f4ce","target":"record","created_at":"2026-05-18T01:52:30Z","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":"0114d43dc31bb1d79dff4cfb97c414090c6803282dde90c8cb005ddc61ba4176","cross_cats_sorted":["hep-ph","physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-12-19T21:00:02Z","title_canon_sha256":"73fe5c098dd4de451e02fbf65986f55c9d0f2f8680d7bf3ebdd0a1851824ce6b"},"schema_version":"1.0","source":{"id":"1212.4838","kind":"arxiv","version":2}},"canonical_sha256":"228703fe1cbaf0f6003b30e271f4f80909756e8bb4c5fa9f64c0e0f8a3a4af54","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"228703fe1cbaf0f6003b30e271f4f80909756e8bb4c5fa9f64c0e0f8a3a4af54","first_computed_at":"2026-05-18T01:52:30.202565Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:52:30.202565Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"lRtMnWbg+3jeipK6cCes/Qqd79SggEJ3cmQioP5+jr2/B522tRVeuPCiAA7jEwMb3lAAx1ByyL1TL0k3KYkOAw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:52:30.203152Z","signed_message":"canonical_sha256_bytes"},"source_id":"1212.4838","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ff1a450bcb18b7ba594ae0e5ca1dfdbdd41b21427e1a5cb56fdae89ea746f4ce","sha256:342154d15d15c577eaf1f98c33423f27481c593d1797d80fc32306914c157139"],"state_sha256":"4eec58e28b7da4eb38684532ae858f57b8fb697c09144d2476bfd488f215e2e4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"EKp5uJWFqGgik546VBwciO7/t/eTyDMiaqzHx2QftjBXxqlBeciMiKxwfrZfOYwhdLXhBcgIL5Fw76uWCUHFAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-06T22:43:39.141097Z","bundle_sha256":"e41d59ed03c1b752c4ed6e189ef075249f047a7fa0044347501eb41362d70380"}}