{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:QBGZ36JAJCR4YALUH5MUZYOGI5","short_pith_number":"pith:QBGZ36JA","canonical_record":{"source":{"id":"1412.5880","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2014-12-18T15:00:53Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"8b63687261a04095d7214d01667ba85ed416e304586b6d3a9fa94f193a92f5b2","abstract_canon_sha256":"22c13f69c32d0d9e600ac081c2fe23eab140198bd7b840be70ab2e66cff07106"},"schema_version":"1.0"},"canonical_sha256":"804d9df92048a3cc01743f594ce1c6474d8f21019e66dcd70447deb08dcc5c2a","source":{"kind":"arxiv","id":"1412.5880","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.5880","created_at":"2026-05-18T02:18:40Z"},{"alias_kind":"arxiv_version","alias_value":"1412.5880v1","created_at":"2026-05-18T02:18:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.5880","created_at":"2026-05-18T02:18:40Z"},{"alias_kind":"pith_short_12","alias_value":"QBGZ36JAJCR4","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_16","alias_value":"QBGZ36JAJCR4YALU","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_8","alias_value":"QBGZ36JA","created_at":"2026-05-18T12:28:43Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:QBGZ36JAJCR4YALUH5MUZYOGI5","target":"record","payload":{"canonical_record":{"source":{"id":"1412.5880","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2014-12-18T15:00:53Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"8b63687261a04095d7214d01667ba85ed416e304586b6d3a9fa94f193a92f5b2","abstract_canon_sha256":"22c13f69c32d0d9e600ac081c2fe23eab140198bd7b840be70ab2e66cff07106"},"schema_version":"1.0"},"canonical_sha256":"804d9df92048a3cc01743f594ce1c6474d8f21019e66dcd70447deb08dcc5c2a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:18:40.573022Z","signature_b64":"f7R3whxl7g+0qVtlTudj8f0oWl9MThmbzmihUfrkil6GAosz7bVsiTHzJUoYx6AOIYdDFOQJBOiwWyY6LBD9DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"804d9df92048a3cc01743f594ce1c6474d8f21019e66dcd70447deb08dcc5c2a","last_reissued_at":"2026-05-18T02:18:40.572367Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:18:40.572367Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1412.5880","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":"2026-05-18T02:18:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+KL9xCOB0CCVVVbaCmZxEdETrxsBs2w6EDNy3Sd6jsvzUsJSuMWYV9tEdpq+Pl15wKl6GJEl2HTYVadIbGGpCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-26T14:33:52.396693Z"},"content_sha256":"6d1539940b266aa12f571d28339672b15d63bb43369dd00ccaf316b93dc18cbd","schema_version":"1.0","event_id":"sha256:6d1539940b266aa12f571d28339672b15d63bb43369dd00ccaf316b93dc18cbd"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:QBGZ36JAJCR4YALUH5MUZYOGI5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Geometric phase in St\\\"uckelberg interferometry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"Gilles Montambaux, Jean-No\\\"el Fuchs, Lih-King Lim","submitted_at":"2014-12-18T15:00:53Z","abstract_excerpt":"We study the time evolution of a two-dimensional quantum particle exhibiting an energy spectrum, made of two bands, with two Dirac cones, as e.g. in the band structure of a honeycomb lattice. A force is applied such that the particle experiences two Landau-Zener transitions in succession. The adiabatic evolution between the two transitions leads to St\\\"uckelberg interferences, due to two possible trajectories in energy space. In addition to well-known dynamical and Stokes phases, the interference pattern reveals a geometric phase which depends on the chirality (winding number) and the mass sig"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.5880","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":"2026-05-18T02:18:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zhcpcnVdBovFZbPfFz4ReHPtdMUNzTcN533pPDyYXn5yCnSThMfaTto6rQMuZOdZgFxOJspzefYksAvoNHInCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-26T14:33:52.397045Z"},"content_sha256":"c378e973eb9ec7af136b16380d16b68a166ccf6ab79a891368c35df9afb3cedb","schema_version":"1.0","event_id":"sha256:c378e973eb9ec7af136b16380d16b68a166ccf6ab79a891368c35df9afb3cedb"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/QBGZ36JAJCR4YALUH5MUZYOGI5/bundle.json","state_url":"https://pith.science/pith/QBGZ36JAJCR4YALUH5MUZYOGI5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/QBGZ36JAJCR4YALUH5MUZYOGI5/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":"2026-06-26T14:33:52Z","links":{"resolver":"https://pith.science/pith/QBGZ36JAJCR4YALUH5MUZYOGI5","bundle":"https://pith.science/pith/QBGZ36JAJCR4YALUH5MUZYOGI5/bundle.json","state":"https://pith.science/pith/QBGZ36JAJCR4YALUH5MUZYOGI5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/QBGZ36JAJCR4YALUH5MUZYOGI5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:QBGZ36JAJCR4YALUH5MUZYOGI5","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":"22c13f69c32d0d9e600ac081c2fe23eab140198bd7b840be70ab2e66cff07106","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2014-12-18T15:00:53Z","title_canon_sha256":"8b63687261a04095d7214d01667ba85ed416e304586b6d3a9fa94f193a92f5b2"},"schema_version":"1.0","source":{"id":"1412.5880","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.5880","created_at":"2026-05-18T02:18:40Z"},{"alias_kind":"arxiv_version","alias_value":"1412.5880v1","created_at":"2026-05-18T02:18:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.5880","created_at":"2026-05-18T02:18:40Z"},{"alias_kind":"pith_short_12","alias_value":"QBGZ36JAJCR4","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_16","alias_value":"QBGZ36JAJCR4YALU","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_8","alias_value":"QBGZ36JA","created_at":"2026-05-18T12:28:43Z"}],"graph_snapshots":[{"event_id":"sha256:c378e973eb9ec7af136b16380d16b68a166ccf6ab79a891368c35df9afb3cedb","target":"graph","created_at":"2026-05-18T02:18:40Z","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 study the time evolution of a two-dimensional quantum particle exhibiting an energy spectrum, made of two bands, with two Dirac cones, as e.g. in the band structure of a honeycomb lattice. A force is applied such that the particle experiences two Landau-Zener transitions in succession. The adiabatic evolution between the two transitions leads to St\\\"uckelberg interferences, due to two possible trajectories in energy space. In addition to well-known dynamical and Stokes phases, the interference pattern reveals a geometric phase which depends on the chirality (winding number) and the mass sig","authors_text":"Gilles Montambaux, Jean-No\\\"el Fuchs, Lih-King Lim","cross_cats":["quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2014-12-18T15:00:53Z","title":"Geometric phase in St\\\"uckelberg interferometry"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.5880","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":"sha256:6d1539940b266aa12f571d28339672b15d63bb43369dd00ccaf316b93dc18cbd","target":"record","created_at":"2026-05-18T02:18:40Z","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":"22c13f69c32d0d9e600ac081c2fe23eab140198bd7b840be70ab2e66cff07106","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2014-12-18T15:00:53Z","title_canon_sha256":"8b63687261a04095d7214d01667ba85ed416e304586b6d3a9fa94f193a92f5b2"},"schema_version":"1.0","source":{"id":"1412.5880","kind":"arxiv","version":1}},"canonical_sha256":"804d9df92048a3cc01743f594ce1c6474d8f21019e66dcd70447deb08dcc5c2a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"804d9df92048a3cc01743f594ce1c6474d8f21019e66dcd70447deb08dcc5c2a","first_computed_at":"2026-05-18T02:18:40.572367Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:18:40.572367Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"f7R3whxl7g+0qVtlTudj8f0oWl9MThmbzmihUfrkil6GAosz7bVsiTHzJUoYx6AOIYdDFOQJBOiwWyY6LBD9DQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:18:40.573022Z","signed_message":"canonical_sha256_bytes"},"source_id":"1412.5880","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6d1539940b266aa12f571d28339672b15d63bb43369dd00ccaf316b93dc18cbd","sha256:c378e973eb9ec7af136b16380d16b68a166ccf6ab79a891368c35df9afb3cedb"],"state_sha256":"ab60a6728214cffe57158b3d294cecb27016c0711d04cf572e0a5e74f8d44313"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oikNTHLtjN8X7CQYlgn36JHEar4AN5ydOTLDutxo3fk0LDhAdFLTzqTgl6qVvI8WOr3g+GGsbrLp2rLX3i74Bg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-26T14:33:52.398934Z","bundle_sha256":"62f4ed0f31530d58df381322ec9e5dbf5fda3787f8fae409b7d26285bb6bcdb3"}}