{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:YD4DKEZVHLW4RLNHACK33ZHKVJ","short_pith_number":"pith:YD4DKEZV","canonical_record":{"source":{"id":"1609.00485","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-09-02T07:29:52Z","cross_cats_sorted":[],"title_canon_sha256":"d1d7ecb6311acce943d20fdc3603ff30efb13d781ddb61d8f9922e168fbd16a4","abstract_canon_sha256":"b06da3ce43686fd99cfe4bc5f04134c783a0d201567c2f8b815d8b5dfe0ed8b8"},"schema_version":"1.0"},"canonical_sha256":"c0f83513353aedc8ada70095bde4eaaa6501925971d4082fd8678da16cfe38dc","source":{"kind":"arxiv","id":"1609.00485","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1609.00485","created_at":"2026-05-18T01:06:23Z"},{"alias_kind":"arxiv_version","alias_value":"1609.00485v1","created_at":"2026-05-18T01:06:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.00485","created_at":"2026-05-18T01:06:23Z"},{"alias_kind":"pith_short_12","alias_value":"YD4DKEZVHLW4","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_16","alias_value":"YD4DKEZVHLW4RLNH","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_8","alias_value":"YD4DKEZV","created_at":"2026-05-18T12:30:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:YD4DKEZVHLW4RLNHACK33ZHKVJ","target":"record","payload":{"canonical_record":{"source":{"id":"1609.00485","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-09-02T07:29:52Z","cross_cats_sorted":[],"title_canon_sha256":"d1d7ecb6311acce943d20fdc3603ff30efb13d781ddb61d8f9922e168fbd16a4","abstract_canon_sha256":"b06da3ce43686fd99cfe4bc5f04134c783a0d201567c2f8b815d8b5dfe0ed8b8"},"schema_version":"1.0"},"canonical_sha256":"c0f83513353aedc8ada70095bde4eaaa6501925971d4082fd8678da16cfe38dc","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:06:23.826543Z","signature_b64":"ZArhwB0ZTUud8NWv/GUIYhxe2sJS6srqdXEGxT1VaHh0AbsFf+qTs6MbwqhxlEAdgfYzaPB2YX4iYt/n95QgDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c0f83513353aedc8ada70095bde4eaaa6501925971d4082fd8678da16cfe38dc","last_reissued_at":"2026-05-18T01:06:23.826028Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:06:23.826028Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1609.00485","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":"2026-05-18T01:06:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jyrupx2ge4L8ifYi/WtV4F2UofRrDjBXYXo92XwsPHR72D1hImgIUVjusfG4beFa+RL49i2cE8HEZpFlF/wJBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T05:29:44.045438Z"},"content_sha256":"e31057a325c803cafa016fe334ca90363b417f81212e27ad9b249b7503cbb5f7","schema_version":"1.0","event_id":"sha256:e31057a325c803cafa016fe334ca90363b417f81212e27ad9b249b7503cbb5f7"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:YD4DKEZVHLW4RLNHACK33ZHKVJ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"A microscopic model for the magnetic field driven breakdown of the dissipationless state in the integer and fractional quantum Hall effect","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"A. Poux, D. K. Maude, K. H. Ploog, K. J. Friedland, P. Plochocka, R. Airey, R. Hey, Z. R. Wasilewski","submitted_at":"2016-09-02T07:29:52Z","abstract_excerpt":"Intra Landau level thermal activation, from localized states in the tail, to delocalized states above the mobility edge in the same Landau level, explains the $B_c(T)$ (half width of the dissipationless state) phase diagram for a number of different quantum Hall samples with widely ranging carrier density, mobility and disorder. Good agreement is achieved over $2-3$ orders of magnitude in temperature and magnetic field for a wide range of filling factors. The Landau level width is found to be independent of magnetic field. The mobility edge moves, in the case of changing Landau level overlap t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.00485","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":"2026-05-18T01:06:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"e5DWTR6X9JB/I888nhTpS57veIeqrVFa/AdWj5aiC99AsikgLY41MK4lj29pxtwajk/n4FedbqlB0JK5Ab2WDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T05:29:44.046085Z"},"content_sha256":"bf89c72d02baed3ffb0a2ed44183fca1f0be7d734286b317cf16c7805cf75acc","schema_version":"1.0","event_id":"sha256:bf89c72d02baed3ffb0a2ed44183fca1f0be7d734286b317cf16c7805cf75acc"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YD4DKEZVHLW4RLNHACK33ZHKVJ/bundle.json","state_url":"https://pith.science/pith/YD4DKEZVHLW4RLNHACK33ZHKVJ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YD4DKEZVHLW4RLNHACK33ZHKVJ/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":"2026-05-28T05:29:44Z","links":{"resolver":"https://pith.science/pith/YD4DKEZVHLW4RLNHACK33ZHKVJ","bundle":"https://pith.science/pith/YD4DKEZVHLW4RLNHACK33ZHKVJ/bundle.json","state":"https://pith.science/pith/YD4DKEZVHLW4RLNHACK33ZHKVJ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YD4DKEZVHLW4RLNHACK33ZHKVJ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:YD4DKEZVHLW4RLNHACK33ZHKVJ","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":"b06da3ce43686fd99cfe4bc5f04134c783a0d201567c2f8b815d8b5dfe0ed8b8","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-09-02T07:29:52Z","title_canon_sha256":"d1d7ecb6311acce943d20fdc3603ff30efb13d781ddb61d8f9922e168fbd16a4"},"schema_version":"1.0","source":{"id":"1609.00485","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1609.00485","created_at":"2026-05-18T01:06:23Z"},{"alias_kind":"arxiv_version","alias_value":"1609.00485v1","created_at":"2026-05-18T01:06:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.00485","created_at":"2026-05-18T01:06:23Z"},{"alias_kind":"pith_short_12","alias_value":"YD4DKEZVHLW4","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_16","alias_value":"YD4DKEZVHLW4RLNH","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_8","alias_value":"YD4DKEZV","created_at":"2026-05-18T12:30:53Z"}],"graph_snapshots":[{"event_id":"sha256:bf89c72d02baed3ffb0a2ed44183fca1f0be7d734286b317cf16c7805cf75acc","target":"graph","created_at":"2026-05-18T01:06:23Z","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":"Intra Landau level thermal activation, from localized states in the tail, to delocalized states above the mobility edge in the same Landau level, explains the $B_c(T)$ (half width of the dissipationless state) phase diagram for a number of different quantum Hall samples with widely ranging carrier density, mobility and disorder. Good agreement is achieved over $2-3$ orders of magnitude in temperature and magnetic field for a wide range of filling factors. The Landau level width is found to be independent of magnetic field. The mobility edge moves, in the case of changing Landau level overlap t","authors_text":"A. Poux, D. K. Maude, K. H. Ploog, K. J. Friedland, P. Plochocka, R. Airey, R. Hey, Z. R. Wasilewski","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-09-02T07:29:52Z","title":"A microscopic model for the magnetic field driven breakdown of the dissipationless state in the integer and fractional quantum Hall effect"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.00485","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:e31057a325c803cafa016fe334ca90363b417f81212e27ad9b249b7503cbb5f7","target":"record","created_at":"2026-05-18T01:06:23Z","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":"b06da3ce43686fd99cfe4bc5f04134c783a0d201567c2f8b815d8b5dfe0ed8b8","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-09-02T07:29:52Z","title_canon_sha256":"d1d7ecb6311acce943d20fdc3603ff30efb13d781ddb61d8f9922e168fbd16a4"},"schema_version":"1.0","source":{"id":"1609.00485","kind":"arxiv","version":1}},"canonical_sha256":"c0f83513353aedc8ada70095bde4eaaa6501925971d4082fd8678da16cfe38dc","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c0f83513353aedc8ada70095bde4eaaa6501925971d4082fd8678da16cfe38dc","first_computed_at":"2026-05-18T01:06:23.826028Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:06:23.826028Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ZArhwB0ZTUud8NWv/GUIYhxe2sJS6srqdXEGxT1VaHh0AbsFf+qTs6MbwqhxlEAdgfYzaPB2YX4iYt/n95QgDw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:06:23.826543Z","signed_message":"canonical_sha256_bytes"},"source_id":"1609.00485","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e31057a325c803cafa016fe334ca90363b417f81212e27ad9b249b7503cbb5f7","sha256:bf89c72d02baed3ffb0a2ed44183fca1f0be7d734286b317cf16c7805cf75acc"],"state_sha256":"e9168a565de35aec18b7ee84dd00c6617677f2d6409e0f29d03311e0463d8fc7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"iOXb/rxzxHtzb5X6D99fEDP2SDekK6Bl2F/j8a4xSEZeP1DjQduRWmgAeAG1aXWozsoQ1Jjg3NJCHCyJcOrGAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T05:29:44.049310Z","bundle_sha256":"f1cd0dc75df2da724ef45de9a723cf8074e24fec704105fbc51ec3bfd17eaf9a"}}