{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:DZEPCXO5PMXUVXB65ED3D4FV7I","short_pith_number":"pith:DZEPCXO5","schema_version":"1.0","canonical_sha256":"1e48f15ddd7b2f4adc3ee907b1f0b5fa37644a8dab78cfaab3560be11f34a23b","source":{"kind":"arxiv","id":"1202.0086","version":1},"attestation_state":"computed","paper":{"title":"Shear-Transformation-Zone Theory of Viscosity, Diffusion, and Stretched Exponential Relaxation in Amorphous Solids","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"J. S. Langer","submitted_at":"2012-02-01T03:19:33Z","abstract_excerpt":"The shear-transformation-zone (STZ) theory has been remarkably successful in accounting for broadly peaked, frequency-dependent, viscoelastic responses of amorphous systems near their glass temperatures $T_g$. This success is based on the theory's first-principles prediction of a wide range of internal STZ transition rates. Here, I show that the STZ rate-distribution causes the Newtonian viscosity to be strongly temperature dependent; and I propose that it is this temperature dependence, rather than any heterogeneity-induced enhancement of diffusion, that is responsible for Stokes-Einstein vio"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1202.0086","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-02-01T03:19:33Z","cross_cats_sorted":[],"title_canon_sha256":"dfc1a512bb8cdf47f9263853fb2618917ca1b4594c189dfe5ea80bc19fa4f186","abstract_canon_sha256":"b4836a0ac5cb9a88b76275379a2af43c6c9a3f2d913697f0cfe4b6c58a560042"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:03:20.554159Z","signature_b64":"cYALeib9FGNZ3SWQA9Z0OQacNlIQHbSRS9YkTht6vCKoi2q0A3zFlTqJfi8YsN89/hnyPW9WXwHTLD+1e9VTDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1e48f15ddd7b2f4adc3ee907b1f0b5fa37644a8dab78cfaab3560be11f34a23b","last_reissued_at":"2026-05-18T04:03:20.553753Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:03:20.553753Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Shear-Transformation-Zone Theory of Viscosity, Diffusion, and Stretched Exponential Relaxation in Amorphous Solids","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"J. S. Langer","submitted_at":"2012-02-01T03:19:33Z","abstract_excerpt":"The shear-transformation-zone (STZ) theory has been remarkably successful in accounting for broadly peaked, frequency-dependent, viscoelastic responses of amorphous systems near their glass temperatures $T_g$. This success is based on the theory's first-principles prediction of a wide range of internal STZ transition rates. Here, I show that the STZ rate-distribution causes the Newtonian viscosity to be strongly temperature dependent; and I propose that it is this temperature dependence, rather than any heterogeneity-induced enhancement of diffusion, that is responsible for Stokes-Einstein vio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1202.0086","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1202.0086","created_at":"2026-05-18T04:03:20.553803+00:00"},{"alias_kind":"arxiv_version","alias_value":"1202.0086v1","created_at":"2026-05-18T04:03:20.553803+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1202.0086","created_at":"2026-05-18T04:03:20.553803+00:00"},{"alias_kind":"pith_short_12","alias_value":"DZEPCXO5PMXU","created_at":"2026-05-18T12:27:04.183437+00:00"},{"alias_kind":"pith_short_16","alias_value":"DZEPCXO5PMXUVXB6","created_at":"2026-05-18T12:27:04.183437+00:00"},{"alias_kind":"pith_short_8","alias_value":"DZEPCXO5","created_at":"2026-05-18T12:27:04.183437+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/DZEPCXO5PMXUVXB65ED3D4FV7I","json":"https://pith.science/pith/DZEPCXO5PMXUVXB65ED3D4FV7I.json","graph_json":"https://pith.science/api/pith-number/DZEPCXO5PMXUVXB65ED3D4FV7I/graph.json","events_json":"https://pith.science/api/pith-number/DZEPCXO5PMXUVXB65ED3D4FV7I/events.json","paper":"https://pith.science/paper/DZEPCXO5"},"agent_actions":{"view_html":"https://pith.science/pith/DZEPCXO5PMXUVXB65ED3D4FV7I","download_json":"https://pith.science/pith/DZEPCXO5PMXUVXB65ED3D4FV7I.json","view_paper":"https://pith.science/paper/DZEPCXO5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1202.0086&json=true","fetch_graph":"https://pith.science/api/pith-number/DZEPCXO5PMXUVXB65ED3D4FV7I/graph.json","fetch_events":"https://pith.science/api/pith-number/DZEPCXO5PMXUVXB65ED3D4FV7I/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DZEPCXO5PMXUVXB65ED3D4FV7I/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DZEPCXO5PMXUVXB65ED3D4FV7I/action/storage_attestation","attest_author":"https://pith.science/pith/DZEPCXO5PMXUVXB65ED3D4FV7I/action/author_attestation","sign_citation":"https://pith.science/pith/DZEPCXO5PMXUVXB65ED3D4FV7I/action/citation_signature","submit_replication":"https://pith.science/pith/DZEPCXO5PMXUVXB65ED3D4FV7I/action/replication_record"}},"created_at":"2026-05-18T04:03:20.553803+00:00","updated_at":"2026-05-18T04:03:20.553803+00:00"}