{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:N7HY247C4JSG3EGR24C7KRITPF","short_pith_number":"pith:N7HY247C","canonical_record":{"source":{"id":"1610.00136","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2016-10-01T13:45:51Z","cross_cats_sorted":[],"title_canon_sha256":"4fc3c976b03fc0ec65b747f8d7e6de31909155ba5baed9585b3b94fe70bd2b5c","abstract_canon_sha256":"0836a3fbb10fe356327b6e92b41b6ee8465ece9d3d0545d776441ea223227d17"},"schema_version":"1.0"},"canonical_sha256":"6fcf8d73e2e2646d90d1d705f5451379454dac464c8b00b7b9aede53186b9192","source":{"kind":"arxiv","id":"1610.00136","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1610.00136","created_at":"2026-05-18T00:49:51Z"},{"alias_kind":"arxiv_version","alias_value":"1610.00136v1","created_at":"2026-05-18T00:49:51Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.00136","created_at":"2026-05-18T00:49:51Z"},{"alias_kind":"pith_short_12","alias_value":"N7HY247C4JSG","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_16","alias_value":"N7HY247C4JSG3EGR","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_8","alias_value":"N7HY247C","created_at":"2026-05-18T12:30:32Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:N7HY247C4JSG3EGR24C7KRITPF","target":"record","payload":{"canonical_record":{"source":{"id":"1610.00136","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2016-10-01T13:45:51Z","cross_cats_sorted":[],"title_canon_sha256":"4fc3c976b03fc0ec65b747f8d7e6de31909155ba5baed9585b3b94fe70bd2b5c","abstract_canon_sha256":"0836a3fbb10fe356327b6e92b41b6ee8465ece9d3d0545d776441ea223227d17"},"schema_version":"1.0"},"canonical_sha256":"6fcf8d73e2e2646d90d1d705f5451379454dac464c8b00b7b9aede53186b9192","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:49:51.625079Z","signature_b64":"DGOKvw+Nwn554Gi1sYCQBSUPrpEusiIZDgRWPqaFDZW/okQBD4H2+fAWi8X1ZYREOMbNco8SYPWnACNjXV8WDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6fcf8d73e2e2646d90d1d705f5451379454dac464c8b00b7b9aede53186b9192","last_reissued_at":"2026-05-18T00:49:51.624651Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:49:51.624651Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1610.00136","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:49:51Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9uz+UgwFOSf6dRogtPqpmSH1mcyoCLTMtllOdNuscdLv+H5enRILD6u7kUfltTwlYGfXeCm0v45IdzkCS14xBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T21:18:55.683516Z"},"content_sha256":"0c8bcbe0e006018eba2ec82f2fccb72d3844ea5cf8266e54bce9f0c0473067a8","schema_version":"1.0","event_id":"sha256:0c8bcbe0e006018eba2ec82f2fccb72d3844ea5cf8266e54bce9f0c0473067a8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:N7HY247C4JSG3EGR24C7KRITPF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Locking of length scales in two-band superconductors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"J. Schmalian, M. Ichioka, V. G. Kogan","submitted_at":"2016-10-01T13:45:51Z","abstract_excerpt":"A model of a clean two-band s-wave superconductor with cylindrical Fermi surfaces, different Fermi velocities v_{1,2}, and a general 2x2 coupling matrix V_{alpha beta} is used to study the order parameter distribution in vortex lattices. The Eilenberger weak coupling formalism is used to calculate numerically the spatial distributions of the pairing amplitudes Delta_1_ and Delta_2_ of the two bands for vortices parallel to the Fermi cylinders. For generic values of the interband coupling V_{12}, it is shown that, independently of the couplings V_{alpha beta}, of the ratio v_1 /v_2, of the temp"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.00136","kind":"arxiv","version":1},"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":"2026-05-18T00:49:51Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4GKFqWaGcG6x819iWaUF+WF6pNpzVEcAIJK1gB/skYB13jm0jGEIDqXsk1rT8cOnGdmd60hZnuFfExG3axTUCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T21:18:55.684086Z"},"content_sha256":"36999ccb226aa11d6b4825ccc0e911e2cc16178b559828a8009c9af63e587315","schema_version":"1.0","event_id":"sha256:36999ccb226aa11d6b4825ccc0e911e2cc16178b559828a8009c9af63e587315"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/N7HY247C4JSG3EGR24C7KRITPF/bundle.json","state_url":"https://pith.science/pith/N7HY247C4JSG3EGR24C7KRITPF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/N7HY247C4JSG3EGR24C7KRITPF/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":"2026-05-25T21:18:55Z","links":{"resolver":"https://pith.science/pith/N7HY247C4JSG3EGR24C7KRITPF","bundle":"https://pith.science/pith/N7HY247C4JSG3EGR24C7KRITPF/bundle.json","state":"https://pith.science/pith/N7HY247C4JSG3EGR24C7KRITPF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/N7HY247C4JSG3EGR24C7KRITPF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:N7HY247C4JSG3EGR24C7KRITPF","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":"0836a3fbb10fe356327b6e92b41b6ee8465ece9d3d0545d776441ea223227d17","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2016-10-01T13:45:51Z","title_canon_sha256":"4fc3c976b03fc0ec65b747f8d7e6de31909155ba5baed9585b3b94fe70bd2b5c"},"schema_version":"1.0","source":{"id":"1610.00136","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1610.00136","created_at":"2026-05-18T00:49:51Z"},{"alias_kind":"arxiv_version","alias_value":"1610.00136v1","created_at":"2026-05-18T00:49:51Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.00136","created_at":"2026-05-18T00:49:51Z"},{"alias_kind":"pith_short_12","alias_value":"N7HY247C4JSG","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_16","alias_value":"N7HY247C4JSG3EGR","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_8","alias_value":"N7HY247C","created_at":"2026-05-18T12:30:32Z"}],"graph_snapshots":[{"event_id":"sha256:36999ccb226aa11d6b4825ccc0e911e2cc16178b559828a8009c9af63e587315","target":"graph","created_at":"2026-05-18T00:49:51Z","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":"A model of a clean two-band s-wave superconductor with cylindrical Fermi surfaces, different Fermi velocities v_{1,2}, and a general 2x2 coupling matrix V_{alpha beta} is used to study the order parameter distribution in vortex lattices. The Eilenberger weak coupling formalism is used to calculate numerically the spatial distributions of the pairing amplitudes Delta_1_ and Delta_2_ of the two bands for vortices parallel to the Fermi cylinders. For generic values of the interband coupling V_{12}, it is shown that, independently of the couplings V_{alpha beta}, of the ratio v_1 /v_2, of the temp","authors_text":"J. Schmalian, M. Ichioka, V. G. Kogan","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2016-10-01T13:45:51Z","title":"Locking of length scales in two-band superconductors"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.00136","kind":"arxiv","version":1},"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":"sha256:0c8bcbe0e006018eba2ec82f2fccb72d3844ea5cf8266e54bce9f0c0473067a8","target":"record","created_at":"2026-05-18T00:49:51Z","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":"0836a3fbb10fe356327b6e92b41b6ee8465ece9d3d0545d776441ea223227d17","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2016-10-01T13:45:51Z","title_canon_sha256":"4fc3c976b03fc0ec65b747f8d7e6de31909155ba5baed9585b3b94fe70bd2b5c"},"schema_version":"1.0","source":{"id":"1610.00136","kind":"arxiv","version":1}},"canonical_sha256":"6fcf8d73e2e2646d90d1d705f5451379454dac464c8b00b7b9aede53186b9192","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6fcf8d73e2e2646d90d1d705f5451379454dac464c8b00b7b9aede53186b9192","first_computed_at":"2026-05-18T00:49:51.624651Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:49:51.624651Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"DGOKvw+Nwn554Gi1sYCQBSUPrpEusiIZDgRWPqaFDZW/okQBD4H2+fAWi8X1ZYREOMbNco8SYPWnACNjXV8WDw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:49:51.625079Z","signed_message":"canonical_sha256_bytes"},"source_id":"1610.00136","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0c8bcbe0e006018eba2ec82f2fccb72d3844ea5cf8266e54bce9f0c0473067a8","sha256:36999ccb226aa11d6b4825ccc0e911e2cc16178b559828a8009c9af63e587315"],"state_sha256":"4a5ae5ad79e0a363ff50208a0dde6c5ad01272811e0bfd42408b973ede882cbd"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6wQ6E9vr5JKpLA5T/M47XkVtSUBbfdeKhiTjyVEXC+qhpJAGQH2Uc1EVcnj5jHc21d8XY1x9c/DjSsxFx5iDDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T21:18:55.687853Z","bundle_sha256":"8e08ce1a06753107a181d556809965ca517e6166d56a08ffb083b9298069bc3d"}}