{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:ENZHZ535M26F4BMX7JOBXM65EF","short_pith_number":"pith:ENZHZ535","canonical_record":{"source":{"id":"1407.2960","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-07-10T20:53:33Z","cross_cats_sorted":["physics.comp-ph"],"title_canon_sha256":"fa373666d956e1d0af95306927e3029131335bd3c34e48dbcc71d96c855fa704","abstract_canon_sha256":"7bd987a4b8e8b41385120d201bc7181df920448227407bdddd7f3f6fc698a300"},"schema_version":"1.0"},"canonical_sha256":"23727cf77d66bc5e0597fa5c1bb3dd216fdb8ca927ea09e77eb0c0c7e041a3bb","source":{"kind":"arxiv","id":"1407.2960","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.2960","created_at":"2026-05-18T02:47:52Z"},{"alias_kind":"arxiv_version","alias_value":"1407.2960v1","created_at":"2026-05-18T02:47:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.2960","created_at":"2026-05-18T02:47:52Z"},{"alias_kind":"pith_short_12","alias_value":"ENZHZ535M26F","created_at":"2026-05-18T12:28:28Z"},{"alias_kind":"pith_short_16","alias_value":"ENZHZ535M26F4BMX","created_at":"2026-05-18T12:28:28Z"},{"alias_kind":"pith_short_8","alias_value":"ENZHZ535","created_at":"2026-05-18T12:28:28Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:ENZHZ535M26F4BMX7JOBXM65EF","target":"record","payload":{"canonical_record":{"source":{"id":"1407.2960","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-07-10T20:53:33Z","cross_cats_sorted":["physics.comp-ph"],"title_canon_sha256":"fa373666d956e1d0af95306927e3029131335bd3c34e48dbcc71d96c855fa704","abstract_canon_sha256":"7bd987a4b8e8b41385120d201bc7181df920448227407bdddd7f3f6fc698a300"},"schema_version":"1.0"},"canonical_sha256":"23727cf77d66bc5e0597fa5c1bb3dd216fdb8ca927ea09e77eb0c0c7e041a3bb","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:47:52.349424Z","signature_b64":"7DDuh5FybPuFb/rpaa+EWp+X8HXLks0JR3IW4QMXt6LsOIFGQkL9xYfQx0JRZT3KizK9HiqDaF9HpQmhKpTqDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"23727cf77d66bc5e0597fa5c1bb3dd216fdb8ca927ea09e77eb0c0c7e041a3bb","last_reissued_at":"2026-05-18T02:47:52.348953Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:47:52.348953Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1407.2960","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":"2026-05-18T02:47:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"uIKLzl1lttaXlZDbRpn8SS1FrHChYdtiesyi+3COWe6xQHTAoXrH1lHQs8UHNVyPRipjKetFbhfAQasofIJhDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T13:25:40.231212Z"},"content_sha256":"96d61e9739afb5f905a6413fbdaa15d340cd767c4b5b1067d69e5406bbf676f7","schema_version":"1.0","event_id":"sha256:96d61e9739afb5f905a6413fbdaa15d340cd767c4b5b1067d69e5406bbf676f7"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:ENZHZ535M26F4BMX7JOBXM65EF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Explosive metallic breakdown","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.comp-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Cl\\'audio L. N. Oliveira, Hans J. Herrmann, Jos\\'e S. Andrade Jr., Nuno A. M. Ara\\'ujo","submitted_at":"2014-07-10T20:53:33Z","abstract_excerpt":"We investigate the metallic breakdown of a substrate on which highly conducting particles are adsorbed and desorbed with a probability that depends on the local electric field. We find that, by tuning the relative strength $q$ of this dependence, the breakdown can change from continuous to explosive. Precisely, in the limit in which the adsorption probability is the same for any finite voltage drop, we can map our model exactly onto the $q$-state Potts model and thus the transition to a jump occurs at $q=4$. In another limit, where the adsorption probability becomes independent of the local fi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.2960","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":"2026-05-18T02:47:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QDIKC8/d2rvpSXMXRel17PXtJ4clK36an03X33ab4K92cMJNRN715XFODad7nn4qTfMHRZix20ibFVvzL2aZCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T13:25:40.231916Z"},"content_sha256":"8636bad898eb03e2c62e8bedec0db1567e89fdffd570649b7ef89fac95eb0a09","schema_version":"1.0","event_id":"sha256:8636bad898eb03e2c62e8bedec0db1567e89fdffd570649b7ef89fac95eb0a09"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ENZHZ535M26F4BMX7JOBXM65EF/bundle.json","state_url":"https://pith.science/pith/ENZHZ535M26F4BMX7JOBXM65EF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ENZHZ535M26F4BMX7JOBXM65EF/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":"2026-05-27T13:25:40Z","links":{"resolver":"https://pith.science/pith/ENZHZ535M26F4BMX7JOBXM65EF","bundle":"https://pith.science/pith/ENZHZ535M26F4BMX7JOBXM65EF/bundle.json","state":"https://pith.science/pith/ENZHZ535M26F4BMX7JOBXM65EF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ENZHZ535M26F4BMX7JOBXM65EF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:ENZHZ535M26F4BMX7JOBXM65EF","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":"7bd987a4b8e8b41385120d201bc7181df920448227407bdddd7f3f6fc698a300","cross_cats_sorted":["physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-07-10T20:53:33Z","title_canon_sha256":"fa373666d956e1d0af95306927e3029131335bd3c34e48dbcc71d96c855fa704"},"schema_version":"1.0","source":{"id":"1407.2960","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.2960","created_at":"2026-05-18T02:47:52Z"},{"alias_kind":"arxiv_version","alias_value":"1407.2960v1","created_at":"2026-05-18T02:47:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.2960","created_at":"2026-05-18T02:47:52Z"},{"alias_kind":"pith_short_12","alias_value":"ENZHZ535M26F","created_at":"2026-05-18T12:28:28Z"},{"alias_kind":"pith_short_16","alias_value":"ENZHZ535M26F4BMX","created_at":"2026-05-18T12:28:28Z"},{"alias_kind":"pith_short_8","alias_value":"ENZHZ535","created_at":"2026-05-18T12:28:28Z"}],"graph_snapshots":[{"event_id":"sha256:8636bad898eb03e2c62e8bedec0db1567e89fdffd570649b7ef89fac95eb0a09","target":"graph","created_at":"2026-05-18T02:47:52Z","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 investigate the metallic breakdown of a substrate on which highly conducting particles are adsorbed and desorbed with a probability that depends on the local electric field. We find that, by tuning the relative strength $q$ of this dependence, the breakdown can change from continuous to explosive. Precisely, in the limit in which the adsorption probability is the same for any finite voltage drop, we can map our model exactly onto the $q$-state Potts model and thus the transition to a jump occurs at $q=4$. In another limit, where the adsorption probability becomes independent of the local fi","authors_text":"Cl\\'audio L. N. Oliveira, Hans J. Herrmann, Jos\\'e S. Andrade Jr., Nuno A. M. Ara\\'ujo","cross_cats":["physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-07-10T20:53:33Z","title":"Explosive metallic breakdown"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.2960","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":"sha256:96d61e9739afb5f905a6413fbdaa15d340cd767c4b5b1067d69e5406bbf676f7","target":"record","created_at":"2026-05-18T02:47:52Z","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":"7bd987a4b8e8b41385120d201bc7181df920448227407bdddd7f3f6fc698a300","cross_cats_sorted":["physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-07-10T20:53:33Z","title_canon_sha256":"fa373666d956e1d0af95306927e3029131335bd3c34e48dbcc71d96c855fa704"},"schema_version":"1.0","source":{"id":"1407.2960","kind":"arxiv","version":1}},"canonical_sha256":"23727cf77d66bc5e0597fa5c1bb3dd216fdb8ca927ea09e77eb0c0c7e041a3bb","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"23727cf77d66bc5e0597fa5c1bb3dd216fdb8ca927ea09e77eb0c0c7e041a3bb","first_computed_at":"2026-05-18T02:47:52.348953Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:47:52.348953Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"7DDuh5FybPuFb/rpaa+EWp+X8HXLks0JR3IW4QMXt6LsOIFGQkL9xYfQx0JRZT3KizK9HiqDaF9HpQmhKpTqDA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:47:52.349424Z","signed_message":"canonical_sha256_bytes"},"source_id":"1407.2960","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:96d61e9739afb5f905a6413fbdaa15d340cd767c4b5b1067d69e5406bbf676f7","sha256:8636bad898eb03e2c62e8bedec0db1567e89fdffd570649b7ef89fac95eb0a09"],"state_sha256":"6b547a5369f786b1380723a0d03046fa64c34aaa1a917725c8f7793a25b4352c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VVI3F8kSh24FsML+jNwFQpuah5SnLqzBepKf6TppmxEsMcexvvKQK3kJoL4QwnfWoYLqX7OPaVao9I3NWKrUBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T13:25:40.234699Z","bundle_sha256":"b18a03b96b9dfe3da7c4b2badcfce1c384811bdb70d79764531c41a95282ba25"}}