{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:P4AFJN4DO6OCIHSWKFDJFZCHGP","short_pith_number":"pith:P4AFJN4D","canonical_record":{"source":{"id":"1410.0377","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2014-10-01T20:15:44Z","cross_cats_sorted":[],"title_canon_sha256":"12071f8153f9e797b540c2b08936b7ea75804953cfc72e2c647b814dbea178ae","abstract_canon_sha256":"0693292c68c574c183770bdf3ba98490b51865df1ccf97e7ce74f2ae82271372"},"schema_version":"1.0"},"canonical_sha256":"7f0054b783779c241e56514692e44733ca1cbe484aaeded3cb814eb8c33197e4","source":{"kind":"arxiv","id":"1410.0377","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1410.0377","created_at":"2026-05-18T02:30:46Z"},{"alias_kind":"arxiv_version","alias_value":"1410.0377v2","created_at":"2026-05-18T02:30:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.0377","created_at":"2026-05-18T02:30:46Z"},{"alias_kind":"pith_short_12","alias_value":"P4AFJN4DO6OC","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_16","alias_value":"P4AFJN4DO6OCIHSW","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_8","alias_value":"P4AFJN4D","created_at":"2026-05-18T12:28:43Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:P4AFJN4DO6OCIHSWKFDJFZCHGP","target":"record","payload":{"canonical_record":{"source":{"id":"1410.0377","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2014-10-01T20:15:44Z","cross_cats_sorted":[],"title_canon_sha256":"12071f8153f9e797b540c2b08936b7ea75804953cfc72e2c647b814dbea178ae","abstract_canon_sha256":"0693292c68c574c183770bdf3ba98490b51865df1ccf97e7ce74f2ae82271372"},"schema_version":"1.0"},"canonical_sha256":"7f0054b783779c241e56514692e44733ca1cbe484aaeded3cb814eb8c33197e4","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:30:46.910349Z","signature_b64":"be4a7rhsJvOnl8VIsUmV9Fxn3ToKSV0apaITXSHbCqrEg86Q35k+6MB+YYkms8CXWwefhOdrPoHl8HGeE4yMDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7f0054b783779c241e56514692e44733ca1cbe484aaeded3cb814eb8c33197e4","last_reissued_at":"2026-05-18T02:30:46.909871Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:30:46.909871Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1410.0377","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":"2026-05-18T02:30:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YdweWSKAu8QXfTW79PDZEWW+CyyMKftq0c1Ra7ImeARKjiTSChij3vBM/i3NwDL/0iDgoq0MUFVnw9Rbf9v/Dg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T05:23:01.634614Z"},"content_sha256":"194d16f15aeb0eab0cbdc4579d685f0dc808964fc5f9da47c21c317256c6d36c","schema_version":"1.0","event_id":"sha256:194d16f15aeb0eab0cbdc4579d685f0dc808964fc5f9da47c21c317256c6d36c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:P4AFJN4DO6OCIHSWKFDJFZCHGP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Vanishing edge currents in non-$p$-wave topological chiral superconductors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"Catherine Kallin, Edward Taylor, Wen Huang","submitted_at":"2014-10-01T20:15:44Z","abstract_excerpt":"The edge currents of two dimensional topological chiral superconductors with nonzero Cooper pair angular momentum---e.g., chiral $p$-, $d$-, and $f$-wave superconductivity---are studied. Bogoliubov-de Gennes and Ginzburg--Landau calculations are used to show that in the continuum limit, \\emph{only} chiral $p$-wave states have a nonzero edge current. Outside this limit, when lattice effects become important, edge currents in non-$p$-wave superconductors are comparatively smaller, but can be nonzero. Using Ginzburg--Landau theory, a simple criterion is derived for when edge currents vanish for n"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.0377","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":"2026-05-18T02:30:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pbp9XdnJ8KWpNLDK8g1AxwpJBhlp2q8mXnv8cU4KB2AO0euq7OyrFy7bA4bpaONfhE+IfwPX+OFfyybUuTuGCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T05:23:01.634983Z"},"content_sha256":"6b520d5c03b68dc872c5f5fbb839c3c0c172ecd716150e0813f311a725fcc986","schema_version":"1.0","event_id":"sha256:6b520d5c03b68dc872c5f5fbb839c3c0c172ecd716150e0813f311a725fcc986"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/P4AFJN4DO6OCIHSWKFDJFZCHGP/bundle.json","state_url":"https://pith.science/pith/P4AFJN4DO6OCIHSWKFDJFZCHGP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/P4AFJN4DO6OCIHSWKFDJFZCHGP/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":"2026-05-28T05:23:01Z","links":{"resolver":"https://pith.science/pith/P4AFJN4DO6OCIHSWKFDJFZCHGP","bundle":"https://pith.science/pith/P4AFJN4DO6OCIHSWKFDJFZCHGP/bundle.json","state":"https://pith.science/pith/P4AFJN4DO6OCIHSWKFDJFZCHGP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/P4AFJN4DO6OCIHSWKFDJFZCHGP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:P4AFJN4DO6OCIHSWKFDJFZCHGP","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":"0693292c68c574c183770bdf3ba98490b51865df1ccf97e7ce74f2ae82271372","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2014-10-01T20:15:44Z","title_canon_sha256":"12071f8153f9e797b540c2b08936b7ea75804953cfc72e2c647b814dbea178ae"},"schema_version":"1.0","source":{"id":"1410.0377","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1410.0377","created_at":"2026-05-18T02:30:46Z"},{"alias_kind":"arxiv_version","alias_value":"1410.0377v2","created_at":"2026-05-18T02:30:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.0377","created_at":"2026-05-18T02:30:46Z"},{"alias_kind":"pith_short_12","alias_value":"P4AFJN4DO6OC","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_16","alias_value":"P4AFJN4DO6OCIHSW","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_8","alias_value":"P4AFJN4D","created_at":"2026-05-18T12:28:43Z"}],"graph_snapshots":[{"event_id":"sha256:6b520d5c03b68dc872c5f5fbb839c3c0c172ecd716150e0813f311a725fcc986","target":"graph","created_at":"2026-05-18T02:30:46Z","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":"The edge currents of two dimensional topological chiral superconductors with nonzero Cooper pair angular momentum---e.g., chiral $p$-, $d$-, and $f$-wave superconductivity---are studied. Bogoliubov-de Gennes and Ginzburg--Landau calculations are used to show that in the continuum limit, \\emph{only} chiral $p$-wave states have a nonzero edge current. Outside this limit, when lattice effects become important, edge currents in non-$p$-wave superconductors are comparatively smaller, but can be nonzero. Using Ginzburg--Landau theory, a simple criterion is derived for when edge currents vanish for n","authors_text":"Catherine Kallin, Edward Taylor, Wen Huang","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2014-10-01T20:15:44Z","title":"Vanishing edge currents in non-$p$-wave topological chiral superconductors"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.0377","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":"sha256:194d16f15aeb0eab0cbdc4579d685f0dc808964fc5f9da47c21c317256c6d36c","target":"record","created_at":"2026-05-18T02:30:46Z","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":"0693292c68c574c183770bdf3ba98490b51865df1ccf97e7ce74f2ae82271372","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2014-10-01T20:15:44Z","title_canon_sha256":"12071f8153f9e797b540c2b08936b7ea75804953cfc72e2c647b814dbea178ae"},"schema_version":"1.0","source":{"id":"1410.0377","kind":"arxiv","version":2}},"canonical_sha256":"7f0054b783779c241e56514692e44733ca1cbe484aaeded3cb814eb8c33197e4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7f0054b783779c241e56514692e44733ca1cbe484aaeded3cb814eb8c33197e4","first_computed_at":"2026-05-18T02:30:46.909871Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:30:46.909871Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"be4a7rhsJvOnl8VIsUmV9Fxn3ToKSV0apaITXSHbCqrEg86Q35k+6MB+YYkms8CXWwefhOdrPoHl8HGeE4yMDA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:30:46.910349Z","signed_message":"canonical_sha256_bytes"},"source_id":"1410.0377","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:194d16f15aeb0eab0cbdc4579d685f0dc808964fc5f9da47c21c317256c6d36c","sha256:6b520d5c03b68dc872c5f5fbb839c3c0c172ecd716150e0813f311a725fcc986"],"state_sha256":"44a3c39e73375018dd8883deadc0d5d492e076834484a48e43eec7d7ae021df0"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8ccgC1p7xRKx+pGI0I06/P/LxHxTRVJ171fKCI+zk/6zNcmY/Az8yHlxEZ2qSmYqlgx9k+bz194ihx3L/hvYCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T05:23:01.636989Z","bundle_sha256":"2b6b0aa88adb3f5997080b96eee39361d62791ffeca460b6b0eb4af4ed71247e"}}