{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:C5WQYY7BIHSIHI7FZVE6EXU4A4","short_pith_number":"pith:C5WQYY7B","canonical_record":{"source":{"id":"1602.00876","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-02-02T10:59:05Z","cross_cats_sorted":["cond-mat.soft"],"title_canon_sha256":"2ca17d68b0c97709e096366c6a651fd3a82c61808db0ee9e95f78ae88bdf177d","abstract_canon_sha256":"a174b4847cba140614a6ab08231b2705ff15a534097ec94602ce88f35728f97a"},"schema_version":"1.0"},"canonical_sha256":"176d0c63e141e483a3e5cd49e25e9c07199fb5c51496598d062fed02271e23b5","source":{"kind":"arxiv","id":"1602.00876","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1602.00876","created_at":"2026-05-18T00:42:51Z"},{"alias_kind":"arxiv_version","alias_value":"1602.00876v2","created_at":"2026-05-18T00:42:51Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1602.00876","created_at":"2026-05-18T00:42:51Z"},{"alias_kind":"pith_short_12","alias_value":"C5WQYY7BIHSI","created_at":"2026-05-18T12:30:09Z"},{"alias_kind":"pith_short_16","alias_value":"C5WQYY7BIHSIHI7F","created_at":"2026-05-18T12:30:09Z"},{"alias_kind":"pith_short_8","alias_value":"C5WQYY7B","created_at":"2026-05-18T12:30:09Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:C5WQYY7BIHSIHI7FZVE6EXU4A4","target":"record","payload":{"canonical_record":{"source":{"id":"1602.00876","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-02-02T10:59:05Z","cross_cats_sorted":["cond-mat.soft"],"title_canon_sha256":"2ca17d68b0c97709e096366c6a651fd3a82c61808db0ee9e95f78ae88bdf177d","abstract_canon_sha256":"a174b4847cba140614a6ab08231b2705ff15a534097ec94602ce88f35728f97a"},"schema_version":"1.0"},"canonical_sha256":"176d0c63e141e483a3e5cd49e25e9c07199fb5c51496598d062fed02271e23b5","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:42:51.841568Z","signature_b64":"AvY+Xg2MCozsp9bNw/YJogvHKsCZusXFQUq4yShqFNFfsgP/PJaDRDI23xsqIoocmPfKdxrI6f3RLcdEFuuDAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"176d0c63e141e483a3e5cd49e25e9c07199fb5c51496598d062fed02271e23b5","last_reissued_at":"2026-05-18T00:42:51.840712Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:42:51.840712Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1602.00876","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":"2026-05-18T00:42:51Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0K3MqGVjyreKv/H8u8AyZjNkwAZD/l4dx7p63E+dnW6OdNsuS1U8AtoOMxTrKh+QgmlARuAcocCY1qV4SRDKAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T08:41:03.965679Z"},"content_sha256":"f9411f0c93d6002804774f949e66c937cf3eb165c7f2f90c1c6b3ae5b8b83361","schema_version":"1.0","event_id":"sha256:f9411f0c93d6002804774f949e66c937cf3eb165c7f2f90c1c6b3ae5b8b83361"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:C5WQYY7BIHSIHI7FZVE6EXU4A4","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Jamming vs. Caging in Three Dimensional Jamming Percolation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.soft"],"primary_cat":"cond-mat.stat-mech","authors_text":"Eial Teomy, Nimrod Segall, Yair Shokef","submitted_at":"2016-02-02T10:59:05Z","abstract_excerpt":"We investigate a three-dimensional kinetically-constrained model that exhibits two types of phase transitions at different densities. At the jamming density $ \\rho_J $ there is a mixed-order phase transition in which a finite fraction of the particles become frozen, but the other particles may still diffuse throughout the system. At the caging density $ \\rho_C > \\rho_J $, the mobile particles are trapped in finite cages and no longer diffuse. The caging transition occurs due to a percolation transition of the unfrozen sites, and we numerically find that it is a continuous transition with the s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1602.00876","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":"2026-05-18T00:42:51Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/VxS6ECpv0zSESW5WuItk7sLGOCXRaMi+rHTbpn++1bIA2a2f7eQXtAqu4JzIvDOH6W7r2e/uXILEWmOktAhDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T08:41:03.966031Z"},"content_sha256":"6db384cc29874b5a3dd2fdc3363bd13b0a289a7167bfef7df8002e2e8a58da43","schema_version":"1.0","event_id":"sha256:6db384cc29874b5a3dd2fdc3363bd13b0a289a7167bfef7df8002e2e8a58da43"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/C5WQYY7BIHSIHI7FZVE6EXU4A4/bundle.json","state_url":"https://pith.science/pith/C5WQYY7BIHSIHI7FZVE6EXU4A4/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/C5WQYY7BIHSIHI7FZVE6EXU4A4/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":"2026-05-28T08:41:03Z","links":{"resolver":"https://pith.science/pith/C5WQYY7BIHSIHI7FZVE6EXU4A4","bundle":"https://pith.science/pith/C5WQYY7BIHSIHI7FZVE6EXU4A4/bundle.json","state":"https://pith.science/pith/C5WQYY7BIHSIHI7FZVE6EXU4A4/state.json","well_known_bundle":"https://pith.science/.well-known/pith/C5WQYY7BIHSIHI7FZVE6EXU4A4/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:C5WQYY7BIHSIHI7FZVE6EXU4A4","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":"a174b4847cba140614a6ab08231b2705ff15a534097ec94602ce88f35728f97a","cross_cats_sorted":["cond-mat.soft"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-02-02T10:59:05Z","title_canon_sha256":"2ca17d68b0c97709e096366c6a651fd3a82c61808db0ee9e95f78ae88bdf177d"},"schema_version":"1.0","source":{"id":"1602.00876","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1602.00876","created_at":"2026-05-18T00:42:51Z"},{"alias_kind":"arxiv_version","alias_value":"1602.00876v2","created_at":"2026-05-18T00:42:51Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1602.00876","created_at":"2026-05-18T00:42:51Z"},{"alias_kind":"pith_short_12","alias_value":"C5WQYY7BIHSI","created_at":"2026-05-18T12:30:09Z"},{"alias_kind":"pith_short_16","alias_value":"C5WQYY7BIHSIHI7F","created_at":"2026-05-18T12:30:09Z"},{"alias_kind":"pith_short_8","alias_value":"C5WQYY7B","created_at":"2026-05-18T12:30:09Z"}],"graph_snapshots":[{"event_id":"sha256:6db384cc29874b5a3dd2fdc3363bd13b0a289a7167bfef7df8002e2e8a58da43","target":"graph","created_at":"2026-05-18T00:42:51Z","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":"We investigate a three-dimensional kinetically-constrained model that exhibits two types of phase transitions at different densities. At the jamming density $ \\rho_J $ there is a mixed-order phase transition in which a finite fraction of the particles become frozen, but the other particles may still diffuse throughout the system. At the caging density $ \\rho_C > \\rho_J $, the mobile particles are trapped in finite cages and no longer diffuse. The caging transition occurs due to a percolation transition of the unfrozen sites, and we numerically find that it is a continuous transition with the s","authors_text":"Eial Teomy, Nimrod Segall, Yair Shokef","cross_cats":["cond-mat.soft"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-02-02T10:59:05Z","title":"Jamming vs. Caging in Three Dimensional Jamming Percolation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1602.00876","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:f9411f0c93d6002804774f949e66c937cf3eb165c7f2f90c1c6b3ae5b8b83361","target":"record","created_at":"2026-05-18T00:42:51Z","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":"a174b4847cba140614a6ab08231b2705ff15a534097ec94602ce88f35728f97a","cross_cats_sorted":["cond-mat.soft"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-02-02T10:59:05Z","title_canon_sha256":"2ca17d68b0c97709e096366c6a651fd3a82c61808db0ee9e95f78ae88bdf177d"},"schema_version":"1.0","source":{"id":"1602.00876","kind":"arxiv","version":2}},"canonical_sha256":"176d0c63e141e483a3e5cd49e25e9c07199fb5c51496598d062fed02271e23b5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"176d0c63e141e483a3e5cd49e25e9c07199fb5c51496598d062fed02271e23b5","first_computed_at":"2026-05-18T00:42:51.840712Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:42:51.840712Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"AvY+Xg2MCozsp9bNw/YJogvHKsCZusXFQUq4yShqFNFfsgP/PJaDRDI23xsqIoocmPfKdxrI6f3RLcdEFuuDAA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:42:51.841568Z","signed_message":"canonical_sha256_bytes"},"source_id":"1602.00876","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f9411f0c93d6002804774f949e66c937cf3eb165c7f2f90c1c6b3ae5b8b83361","sha256:6db384cc29874b5a3dd2fdc3363bd13b0a289a7167bfef7df8002e2e8a58da43"],"state_sha256":"c5023ff7bb8117c80f2f82f4cb1cd270445951155f52f73c5c353398b184e9b9"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ya7Nm9lnqlfm8AQz9vzIMUtA8Jeqru3yFk/HL7/i/uNuIguKZTMGvOt5KJ58IBeBTSh8SQtPYvnMd8Vgs/ygBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T08:41:03.968459Z","bundle_sha256":"782fa1212ff3102fe395d3bc6cfbaa131275e9fea599ad570289d83118ff2a0e"}}