{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:ZXFPITU3VKF7QIQRHZKYHY6MEI","short_pith_number":"pith:ZXFPITU3","canonical_record":{"source":{"id":"1604.06666","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2016-04-22T14:06:51Z","cross_cats_sorted":[],"title_canon_sha256":"aa1a96e2b37764b9d79fb29fd848b29a7520a8d89d0e66361c34c89d40d3acc9","abstract_canon_sha256":"40bb1e62753feefa94bfd8bd2b1806e5a89a022d751d947b48e72d535c761bda"},"schema_version":"1.0"},"canonical_sha256":"cdcaf44e9baa8bf822113e5583e3cc223ba863342847b038d5187cf5db7d6963","source":{"kind":"arxiv","id":"1604.06666","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.06666","created_at":"2026-05-18T00:48:17Z"},{"alias_kind":"arxiv_version","alias_value":"1604.06666v2","created_at":"2026-05-18T00:48:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.06666","created_at":"2026-05-18T00:48:17Z"},{"alias_kind":"pith_short_12","alias_value":"ZXFPITU3VKF7","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_16","alias_value":"ZXFPITU3VKF7QIQR","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_8","alias_value":"ZXFPITU3","created_at":"2026-05-18T12:30:55Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:ZXFPITU3VKF7QIQRHZKYHY6MEI","target":"record","payload":{"canonical_record":{"source":{"id":"1604.06666","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2016-04-22T14:06:51Z","cross_cats_sorted":[],"title_canon_sha256":"aa1a96e2b37764b9d79fb29fd848b29a7520a8d89d0e66361c34c89d40d3acc9","abstract_canon_sha256":"40bb1e62753feefa94bfd8bd2b1806e5a89a022d751d947b48e72d535c761bda"},"schema_version":"1.0"},"canonical_sha256":"cdcaf44e9baa8bf822113e5583e3cc223ba863342847b038d5187cf5db7d6963","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:48:17.752523Z","signature_b64":"gwgusbDmC3pDEeynwo6Acjc8s55twnXHzXIOTbv4iHXdYdqjg+z1q6Gi+WyJRaU7oVPbY57P5/qgNp+O3dfNAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cdcaf44e9baa8bf822113e5583e3cc223ba863342847b038d5187cf5db7d6963","last_reissued_at":"2026-05-18T00:48:17.751822Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:48:17.751822Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1604.06666","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":"2026-05-18T00:48:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oUH0AVE7veuHtoIDFBwzIlPV2Qyx25mA2Yv+eN7EsgwHen0Yz/GFNYrDt1684GWE3oGZjQ6A2CJqPKA1r7/QAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T18:56:56.016491Z"},"content_sha256":"b7709845c9aafc4e69c3308c0e83e4896f9a0f05a63818b4cf42a785fc855c4e","schema_version":"1.0","event_id":"sha256:b7709845c9aafc4e69c3308c0e83e4896f9a0f05a63818b4cf42a785fc855c4e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:ZXFPITU3VKF7QIQRHZKYHY6MEI","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Theory of the Evolution of Superconductivity in Sr$_2$RuO$_4$ under Anisotropic Strain","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"F. C. Zhang, Q. H. Wang, T. M. Rice, Y. C. Liu","submitted_at":"2016-04-22T14:06:51Z","abstract_excerpt":"Sr$_2$RuO$_4$ is a leading candidate for chiral $p$-wave superconductivity. The detailed mechanism of superconductivity in this material is still the subject of intense investigations. Since superconductivity is sensitive to the topology of the Fermi surface (the contour of zero-energy quasi-particle excitations in the momentum space in the normal state), changing this topology can provide a strong test of theory. Recent experiments tuned the Fermi surface topology efficiently by applying planar anisotropic strain. Using functional renormalization group theory, we study the superconductivity a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.06666","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":"2026-05-18T00:48:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0RJRJg91Lmu0hQYMvAnm0LAxwScrUfGjXgb9qopoCOwWhfqYvs40fP9vrm+AdVfZ++bBESkOvh/J1IzFG659Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T18:56:56.017481Z"},"content_sha256":"ff17838aad5de281bc1dbf42bf1e463a5142f9048bb43024b01f09be9985dc0c","schema_version":"1.0","event_id":"sha256:ff17838aad5de281bc1dbf42bf1e463a5142f9048bb43024b01f09be9985dc0c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZXFPITU3VKF7QIQRHZKYHY6MEI/bundle.json","state_url":"https://pith.science/pith/ZXFPITU3VKF7QIQRHZKYHY6MEI/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZXFPITU3VKF7QIQRHZKYHY6MEI/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":"2026-05-25T18:56:56Z","links":{"resolver":"https://pith.science/pith/ZXFPITU3VKF7QIQRHZKYHY6MEI","bundle":"https://pith.science/pith/ZXFPITU3VKF7QIQRHZKYHY6MEI/bundle.json","state":"https://pith.science/pith/ZXFPITU3VKF7QIQRHZKYHY6MEI/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZXFPITU3VKF7QIQRHZKYHY6MEI/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:ZXFPITU3VKF7QIQRHZKYHY6MEI","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":"40bb1e62753feefa94bfd8bd2b1806e5a89a022d751d947b48e72d535c761bda","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2016-04-22T14:06:51Z","title_canon_sha256":"aa1a96e2b37764b9d79fb29fd848b29a7520a8d89d0e66361c34c89d40d3acc9"},"schema_version":"1.0","source":{"id":"1604.06666","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.06666","created_at":"2026-05-18T00:48:17Z"},{"alias_kind":"arxiv_version","alias_value":"1604.06666v2","created_at":"2026-05-18T00:48:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.06666","created_at":"2026-05-18T00:48:17Z"},{"alias_kind":"pith_short_12","alias_value":"ZXFPITU3VKF7","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_16","alias_value":"ZXFPITU3VKF7QIQR","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_8","alias_value":"ZXFPITU3","created_at":"2026-05-18T12:30:55Z"}],"graph_snapshots":[{"event_id":"sha256:ff17838aad5de281bc1dbf42bf1e463a5142f9048bb43024b01f09be9985dc0c","target":"graph","created_at":"2026-05-18T00:48:17Z","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":"Sr$_2$RuO$_4$ is a leading candidate for chiral $p$-wave superconductivity. The detailed mechanism of superconductivity in this material is still the subject of intense investigations. Since superconductivity is sensitive to the topology of the Fermi surface (the contour of zero-energy quasi-particle excitations in the momentum space in the normal state), changing this topology can provide a strong test of theory. Recent experiments tuned the Fermi surface topology efficiently by applying planar anisotropic strain. Using functional renormalization group theory, we study the superconductivity a","authors_text":"F. C. Zhang, Q. H. Wang, T. M. Rice, Y. C. Liu","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2016-04-22T14:06:51Z","title":"Theory of the Evolution of Superconductivity in Sr$_2$RuO$_4$ under Anisotropic Strain"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.06666","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:b7709845c9aafc4e69c3308c0e83e4896f9a0f05a63818b4cf42a785fc855c4e","target":"record","created_at":"2026-05-18T00:48:17Z","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":"40bb1e62753feefa94bfd8bd2b1806e5a89a022d751d947b48e72d535c761bda","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2016-04-22T14:06:51Z","title_canon_sha256":"aa1a96e2b37764b9d79fb29fd848b29a7520a8d89d0e66361c34c89d40d3acc9"},"schema_version":"1.0","source":{"id":"1604.06666","kind":"arxiv","version":2}},"canonical_sha256":"cdcaf44e9baa8bf822113e5583e3cc223ba863342847b038d5187cf5db7d6963","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"cdcaf44e9baa8bf822113e5583e3cc223ba863342847b038d5187cf5db7d6963","first_computed_at":"2026-05-18T00:48:17.751822Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:48:17.751822Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"gwgusbDmC3pDEeynwo6Acjc8s55twnXHzXIOTbv4iHXdYdqjg+z1q6Gi+WyJRaU7oVPbY57P5/qgNp+O3dfNAg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:48:17.752523Z","signed_message":"canonical_sha256_bytes"},"source_id":"1604.06666","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b7709845c9aafc4e69c3308c0e83e4896f9a0f05a63818b4cf42a785fc855c4e","sha256:ff17838aad5de281bc1dbf42bf1e463a5142f9048bb43024b01f09be9985dc0c"],"state_sha256":"0725a2ac605e5ae95b9d1e54627b1cfc83ad7993fdc326b7adf84fec4f444bb9"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8w4Igan5+jWn1IEY26edVTXEp8ca5iy/VyQNWjcWxiL9XXHKjCmegswGO6k7cdvpbO5TP8Ef+pQB2ISamGaZAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T18:56:56.020932Z","bundle_sha256":"0cf41bea90354984c91f7b44aaaa67256ba543a5d66a66be554da61e7df89505"}}