{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:Y4EALL7GLVECXPKMTNGEDC3R5N","short_pith_number":"pith:Y4EALL7G","canonical_record":{"source":{"id":"1106.0352","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2011-06-02T00:53:42Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"5e4bd27f648997d6a97daf0334461dff40380fd661a92b3d2b057634802fb228","abstract_canon_sha256":"e3af79d955afa49f58feda33e145d9a8e80fcf1486ae78b7172b18555bc0a35f"},"schema_version":"1.0"},"canonical_sha256":"c70805afe65d482bbd4c9b4c418b71eb6153c4aaff5378e86594e3519e5550f6","source":{"kind":"arxiv","id":"1106.0352","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1106.0352","created_at":"2026-05-18T04:19:13Z"},{"alias_kind":"arxiv_version","alias_value":"1106.0352v2","created_at":"2026-05-18T04:19:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.0352","created_at":"2026-05-18T04:19:13Z"},{"alias_kind":"pith_short_12","alias_value":"Y4EALL7GLVEC","created_at":"2026-05-18T12:26:47Z"},{"alias_kind":"pith_short_16","alias_value":"Y4EALL7GLVECXPKM","created_at":"2026-05-18T12:26:47Z"},{"alias_kind":"pith_short_8","alias_value":"Y4EALL7G","created_at":"2026-05-18T12:26:47Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:Y4EALL7GLVECXPKMTNGEDC3R5N","target":"record","payload":{"canonical_record":{"source":{"id":"1106.0352","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2011-06-02T00:53:42Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"5e4bd27f648997d6a97daf0334461dff40380fd661a92b3d2b057634802fb228","abstract_canon_sha256":"e3af79d955afa49f58feda33e145d9a8e80fcf1486ae78b7172b18555bc0a35f"},"schema_version":"1.0"},"canonical_sha256":"c70805afe65d482bbd4c9b4c418b71eb6153c4aaff5378e86594e3519e5550f6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:19:13.083793Z","signature_b64":"6v6BccnhWBRHUeMgSd7Qd/C/RLuvLbMhwoDwVXHwsMZh7vmArpS4hAc0m7wRrKt1u2fTQvSaUGar5vECE4cHDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c70805afe65d482bbd4c9b4c418b71eb6153c4aaff5378e86594e3519e5550f6","last_reissued_at":"2026-05-18T04:19:13.083283Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:19:13.083283Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1106.0352","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":"2026-05-18T04:19:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tF8DywwDg4zfJxBYiTiX/2LR+Xa6vDDOJEmsYrhlX8nT1kiY/fKgo4ye2G8FF8ITrntf0zvqz+Drc6TyWLxVDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T20:09:56.468905Z"},"content_sha256":"a5d9de6d45e52768f5d5b30fd442c44095f181b51a4432b41dd2c289e7f33f6b","schema_version":"1.0","event_id":"sha256:a5d9de6d45e52768f5d5b30fd442c44095f181b51a4432b41dd2c289e7f33f6b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:Y4EALL7GLVECXPKMTNGEDC3R5N","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Magnetoelectric effects, helical phases, and FFLO phases in superconductors without inversion symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.supr-con","authors_text":"D.F. Agterberg","submitted_at":"2011-06-02T00:53:42Z","abstract_excerpt":"This chapter emphasizes new magnetic properties that arise when inversion symmetry is broken in a superconductor. There are two aspects that will be covered in detail. The first topic encompasses physics related to superconducting magnetoelectric effects that arise from broken inversion symmetry. Broken inversion symmetry allow for Lifshitz invariants in the free energy which can be viewed as a coupling between the magnetic induction and the supercurrent. There are similarities between these invariants and the better known Dzyaloshinskii-Moyira interaction in magnetic systems. These Lifshitz i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.0352","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":"2026-05-18T04:19:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8VSkm61GO+pDry0bYn07e2+6gZP45aE27c/y7iokQUlOZfcGCUBMTLCYAC37+HJzNcRj2KrsGztV2ns4Z+vZCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T20:09:56.469578Z"},"content_sha256":"2f836310fe34451000fa4eb017ba65c2a4adac7c1f8b0d55b07206e515b6f1ef","schema_version":"1.0","event_id":"sha256:2f836310fe34451000fa4eb017ba65c2a4adac7c1f8b0d55b07206e515b6f1ef"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/Y4EALL7GLVECXPKMTNGEDC3R5N/bundle.json","state_url":"https://pith.science/pith/Y4EALL7GLVECXPKMTNGEDC3R5N/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/Y4EALL7GLVECXPKMTNGEDC3R5N/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":"2026-05-31T20:09:56Z","links":{"resolver":"https://pith.science/pith/Y4EALL7GLVECXPKMTNGEDC3R5N","bundle":"https://pith.science/pith/Y4EALL7GLVECXPKMTNGEDC3R5N/bundle.json","state":"https://pith.science/pith/Y4EALL7GLVECXPKMTNGEDC3R5N/state.json","well_known_bundle":"https://pith.science/.well-known/pith/Y4EALL7GLVECXPKMTNGEDC3R5N/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:Y4EALL7GLVECXPKMTNGEDC3R5N","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":"e3af79d955afa49f58feda33e145d9a8e80fcf1486ae78b7172b18555bc0a35f","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2011-06-02T00:53:42Z","title_canon_sha256":"5e4bd27f648997d6a97daf0334461dff40380fd661a92b3d2b057634802fb228"},"schema_version":"1.0","source":{"id":"1106.0352","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1106.0352","created_at":"2026-05-18T04:19:13Z"},{"alias_kind":"arxiv_version","alias_value":"1106.0352v2","created_at":"2026-05-18T04:19:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.0352","created_at":"2026-05-18T04:19:13Z"},{"alias_kind":"pith_short_12","alias_value":"Y4EALL7GLVEC","created_at":"2026-05-18T12:26:47Z"},{"alias_kind":"pith_short_16","alias_value":"Y4EALL7GLVECXPKM","created_at":"2026-05-18T12:26:47Z"},{"alias_kind":"pith_short_8","alias_value":"Y4EALL7G","created_at":"2026-05-18T12:26:47Z"}],"graph_snapshots":[{"event_id":"sha256:2f836310fe34451000fa4eb017ba65c2a4adac7c1f8b0d55b07206e515b6f1ef","target":"graph","created_at":"2026-05-18T04:19:13Z","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":"This chapter emphasizes new magnetic properties that arise when inversion symmetry is broken in a superconductor. There are two aspects that will be covered in detail. The first topic encompasses physics related to superconducting magnetoelectric effects that arise from broken inversion symmetry. Broken inversion symmetry allow for Lifshitz invariants in the free energy which can be viewed as a coupling between the magnetic induction and the supercurrent. There are similarities between these invariants and the better known Dzyaloshinskii-Moyira interaction in magnetic systems. These Lifshitz i","authors_text":"D.F. Agterberg","cross_cats":["cond-mat.mtrl-sci"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2011-06-02T00:53:42Z","title":"Magnetoelectric effects, helical phases, and FFLO phases in superconductors without inversion symmetry"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.0352","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:a5d9de6d45e52768f5d5b30fd442c44095f181b51a4432b41dd2c289e7f33f6b","target":"record","created_at":"2026-05-18T04:19:13Z","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":"e3af79d955afa49f58feda33e145d9a8e80fcf1486ae78b7172b18555bc0a35f","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2011-06-02T00:53:42Z","title_canon_sha256":"5e4bd27f648997d6a97daf0334461dff40380fd661a92b3d2b057634802fb228"},"schema_version":"1.0","source":{"id":"1106.0352","kind":"arxiv","version":2}},"canonical_sha256":"c70805afe65d482bbd4c9b4c418b71eb6153c4aaff5378e86594e3519e5550f6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c70805afe65d482bbd4c9b4c418b71eb6153c4aaff5378e86594e3519e5550f6","first_computed_at":"2026-05-18T04:19:13.083283Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:19:13.083283Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"6v6BccnhWBRHUeMgSd7Qd/C/RLuvLbMhwoDwVXHwsMZh7vmArpS4hAc0m7wRrKt1u2fTQvSaUGar5vECE4cHDg==","signature_status":"signed_v1","signed_at":"2026-05-18T04:19:13.083793Z","signed_message":"canonical_sha256_bytes"},"source_id":"1106.0352","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a5d9de6d45e52768f5d5b30fd442c44095f181b51a4432b41dd2c289e7f33f6b","sha256:2f836310fe34451000fa4eb017ba65c2a4adac7c1f8b0d55b07206e515b6f1ef"],"state_sha256":"649566a4cf331030d7a0a8b9afb9974d80f893871f18f9fd1384503d6c064fed"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"k6YY7eSOkj6+w8Gp2IikMNwZQcg93DYZZ2vgzJLHW3tWYoB5Ty+mDq1NsB6aaNCc3EeLbgpHTYqZsllREnNGCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T20:09:56.473012Z","bundle_sha256":"aaae635d4c791806ad04548b7a2d79fc8068050b508426082af3646ad14be96e"}}