{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:SKSS2HJQGNSCNW525FIGT2XIY4","short_pith_number":"pith:SKSS2HJQ","canonical_record":{"source":{"id":"1208.0880","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-08-04T02:53:33Z","cross_cats_sorted":["cond-mat.soft","physics.bio-ph"],"title_canon_sha256":"e11b9a7998cacfbe9f44a40e09e1c2238baea94752b0097aaf5ffb652d58d437","abstract_canon_sha256":"c2dc63fafce3050a10235b0e3d6c61a13845792ca36beb8ab06ab7efcbb2d4cd"},"schema_version":"1.0"},"canonical_sha256":"92a52d1d30336426dbbae95069eae8c72a06fae5395de2efa99c8a887c03086d","source":{"kind":"arxiv","id":"1208.0880","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1208.0880","created_at":"2026-05-18T03:30:02Z"},{"alias_kind":"arxiv_version","alias_value":"1208.0880v1","created_at":"2026-05-18T03:30:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1208.0880","created_at":"2026-05-18T03:30:02Z"},{"alias_kind":"pith_short_12","alias_value":"SKSS2HJQGNSC","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_16","alias_value":"SKSS2HJQGNSCNW52","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_8","alias_value":"SKSS2HJQ","created_at":"2026-05-18T12:27:20Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:SKSS2HJQGNSCNW525FIGT2XIY4","target":"record","payload":{"canonical_record":{"source":{"id":"1208.0880","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-08-04T02:53:33Z","cross_cats_sorted":["cond-mat.soft","physics.bio-ph"],"title_canon_sha256":"e11b9a7998cacfbe9f44a40e09e1c2238baea94752b0097aaf5ffb652d58d437","abstract_canon_sha256":"c2dc63fafce3050a10235b0e3d6c61a13845792ca36beb8ab06ab7efcbb2d4cd"},"schema_version":"1.0"},"canonical_sha256":"92a52d1d30336426dbbae95069eae8c72a06fae5395de2efa99c8a887c03086d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:30:02.649366Z","signature_b64":"4yCQrz34+LjtCY07TvFedLrclg02RXryD3Q2R9YnqfzawZOMOnRbbQ9ht+SwNolLbCQsjGCQ4OBEoJ9VRQSxCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"92a52d1d30336426dbbae95069eae8c72a06fae5395de2efa99c8a887c03086d","last_reissued_at":"2026-05-18T03:30:02.648522Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:30:02.648522Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1208.0880","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":"2026-05-18T03:30:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Y9f7+2IGDKSmlJGiBfT4Eu5j2QQb0TcHXV0i37Dccsxq1bI0Ql3wXFrxgiqN35rTG8hISNmJq6a0fzl3nB25Aw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T21:25:54.141727Z"},"content_sha256":"e061e7880faa59c7d4339fe2a4505dfc6ac83340fb97397e4e67b55ceef46ea2","schema_version":"1.0","event_id":"sha256:e061e7880faa59c7d4339fe2a4505dfc6ac83340fb97397e4e67b55ceef46ea2"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:SKSS2HJQGNSCNW525FIGT2XIY4","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Microscopic theory of the glassy dynamics of passive and active network materials","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.soft","physics.bio-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Peter G. Wolynes, Shenshen Wang","submitted_at":"2012-08-04T02:53:33Z","abstract_excerpt":"Signatures of glassy dynamics have been identified experimentally for a rich variety of materials in which molecular networks provide rigidity. Here we present a theoretical framework to study the glassy behavior of both passive and active network materials. We construct a general microscopic network model that incorporates nonlinear elasticity of individual filaments and steric constraints due to crowding. Based on constructive analogies between structural glass forming liquids and random field Ising magnets implemented using a heterogeneous self-consistent phonon method, our scheme provides "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1208.0880","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":"2026-05-18T03:30:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mtCEb6jma5rvg9ARuG8/L8moWXmAFmaDDyqoCbgvjCZl2m1blnivEJEFWi5Xauhafx2xFARmn9V1xWta2foSBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T21:25:54.142256Z"},"content_sha256":"2734f2827da7c2ef2218f14bce6614af7f062f851d27c3611e79c6d869dd1589","schema_version":"1.0","event_id":"sha256:2734f2827da7c2ef2218f14bce6614af7f062f851d27c3611e79c6d869dd1589"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/SKSS2HJQGNSCNW525FIGT2XIY4/bundle.json","state_url":"https://pith.science/pith/SKSS2HJQGNSCNW525FIGT2XIY4/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/SKSS2HJQGNSCNW525FIGT2XIY4/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":"2026-05-26T21:25:54Z","links":{"resolver":"https://pith.science/pith/SKSS2HJQGNSCNW525FIGT2XIY4","bundle":"https://pith.science/pith/SKSS2HJQGNSCNW525FIGT2XIY4/bundle.json","state":"https://pith.science/pith/SKSS2HJQGNSCNW525FIGT2XIY4/state.json","well_known_bundle":"https://pith.science/.well-known/pith/SKSS2HJQGNSCNW525FIGT2XIY4/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:SKSS2HJQGNSCNW525FIGT2XIY4","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":"c2dc63fafce3050a10235b0e3d6c61a13845792ca36beb8ab06ab7efcbb2d4cd","cross_cats_sorted":["cond-mat.soft","physics.bio-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-08-04T02:53:33Z","title_canon_sha256":"e11b9a7998cacfbe9f44a40e09e1c2238baea94752b0097aaf5ffb652d58d437"},"schema_version":"1.0","source":{"id":"1208.0880","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1208.0880","created_at":"2026-05-18T03:30:02Z"},{"alias_kind":"arxiv_version","alias_value":"1208.0880v1","created_at":"2026-05-18T03:30:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1208.0880","created_at":"2026-05-18T03:30:02Z"},{"alias_kind":"pith_short_12","alias_value":"SKSS2HJQGNSC","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_16","alias_value":"SKSS2HJQGNSCNW52","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_8","alias_value":"SKSS2HJQ","created_at":"2026-05-18T12:27:20Z"}],"graph_snapshots":[{"event_id":"sha256:2734f2827da7c2ef2218f14bce6614af7f062f851d27c3611e79c6d869dd1589","target":"graph","created_at":"2026-05-18T03:30:02Z","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":"Signatures of glassy dynamics have been identified experimentally for a rich variety of materials in which molecular networks provide rigidity. Here we present a theoretical framework to study the glassy behavior of both passive and active network materials. We construct a general microscopic network model that incorporates nonlinear elasticity of individual filaments and steric constraints due to crowding. Based on constructive analogies between structural glass forming liquids and random field Ising magnets implemented using a heterogeneous self-consistent phonon method, our scheme provides ","authors_text":"Peter G. Wolynes, Shenshen Wang","cross_cats":["cond-mat.soft","physics.bio-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-08-04T02:53:33Z","title":"Microscopic theory of the glassy dynamics of passive and active network materials"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1208.0880","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:e061e7880faa59c7d4339fe2a4505dfc6ac83340fb97397e4e67b55ceef46ea2","target":"record","created_at":"2026-05-18T03:30:02Z","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":"c2dc63fafce3050a10235b0e3d6c61a13845792ca36beb8ab06ab7efcbb2d4cd","cross_cats_sorted":["cond-mat.soft","physics.bio-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-08-04T02:53:33Z","title_canon_sha256":"e11b9a7998cacfbe9f44a40e09e1c2238baea94752b0097aaf5ffb652d58d437"},"schema_version":"1.0","source":{"id":"1208.0880","kind":"arxiv","version":1}},"canonical_sha256":"92a52d1d30336426dbbae95069eae8c72a06fae5395de2efa99c8a887c03086d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"92a52d1d30336426dbbae95069eae8c72a06fae5395de2efa99c8a887c03086d","first_computed_at":"2026-05-18T03:30:02.648522Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:30:02.648522Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"4yCQrz34+LjtCY07TvFedLrclg02RXryD3Q2R9YnqfzawZOMOnRbbQ9ht+SwNolLbCQsjGCQ4OBEoJ9VRQSxCw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:30:02.649366Z","signed_message":"canonical_sha256_bytes"},"source_id":"1208.0880","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e061e7880faa59c7d4339fe2a4505dfc6ac83340fb97397e4e67b55ceef46ea2","sha256:2734f2827da7c2ef2218f14bce6614af7f062f851d27c3611e79c6d869dd1589"],"state_sha256":"6b26d21492e5a6e48f14dc4d8956a6c105a37c4769cf78836dcaeb0690e55613"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"55+jVHSk2iGE/L6QI8zFelbKRYlOgzP7AdN/sacrJx1IgerAWzQPgFZ3iHBJCoR+2JObtv2iWAYD7fwX0b3nDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T21:25:54.145262Z","bundle_sha256":"1ee3ce68522000d588b3e3f14b2d1f00abc8a793d7858e6dc0bca011a7d365f7"}}