{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:USPXZPBZZRUAYEGRTU7V5YCDZ4","short_pith_number":"pith:USPXZPBZ","schema_version":"1.0","canonical_sha256":"a49f7cbc39cc680c10d19d3f5ee043cf192331d9049bc0c1855894fb055a851b","source":{"kind":"arxiv","id":"2507.13960","version":1},"attestation_state":"computed","paper":{"title":"Predicting temperature-dependent failure and transformation zones in 2D silica glass through quasistatic Gaussian Phase Packets","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.dis-nn","authors_text":"Dennis M. Kochmann, Franz Bamer, Miguel Sp\\'inola, Shashank Saxena","submitted_at":"2025-07-18T14:24:22Z","abstract_excerpt":"The athermal quasistatic (AQS) method is a powerful technique to study the mechanical behavior of disordered systems. However, its applicability is limited to temperatures near zero, where thermal activation is unlikely. In this work, we extend the AQS method to finite temperatures, based on a formulation that describes atoms as temperature-dependent Gaussian packets (GPPs) in phase space under quasistatic conditions, thus equivalent to minimum free energy conditions. This framework is used to study the effect of temperature on the onset of inelasticity and fracture in amorphous two-dimensiona"},"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":"2507.13960","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2025-07-18T14:24:22Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"ce2ced02017fcb701e44fda83965b17f59dd4134478370cde9aed738bb41c677","abstract_canon_sha256":"50d59b4dcafff3728f0f50591c768c288e775640c77381c3ab744e0b73561a66"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:39:26.096290Z","signature_b64":"iET5tgX0iSB9ISZX37cSHBw2XfpLYqR+HHNfYdEL/oS3Q/ikaTGLBbW3ghVlZf4bmXNfkHyOnJZXYo7T6oLvCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a49f7cbc39cc680c10d19d3f5ee043cf192331d9049bc0c1855894fb055a851b","last_reissued_at":"2026-07-05T11:39:26.095794Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:39:26.095794Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Predicting temperature-dependent failure and transformation zones in 2D silica glass through quasistatic Gaussian Phase Packets","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.dis-nn","authors_text":"Dennis M. Kochmann, Franz Bamer, Miguel Sp\\'inola, Shashank Saxena","submitted_at":"2025-07-18T14:24:22Z","abstract_excerpt":"The athermal quasistatic (AQS) method is a powerful technique to study the mechanical behavior of disordered systems. However, its applicability is limited to temperatures near zero, where thermal activation is unlikely. In this work, we extend the AQS method to finite temperatures, based on a formulation that describes atoms as temperature-dependent Gaussian packets (GPPs) in phase space under quasistatic conditions, thus equivalent to minimum free energy conditions. This framework is used to study the effect of temperature on the onset of inelasticity and fracture in amorphous two-dimensiona"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2507.13960","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2507.13960/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2507.13960","created_at":"2026-07-05T11:39:26.095867+00:00"},{"alias_kind":"arxiv_version","alias_value":"2507.13960v1","created_at":"2026-07-05T11:39:26.095867+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2507.13960","created_at":"2026-07-05T11:39:26.095867+00:00"},{"alias_kind":"pith_short_12","alias_value":"USPXZPBZZRUA","created_at":"2026-07-05T11:39:26.095867+00:00"},{"alias_kind":"pith_short_16","alias_value":"USPXZPBZZRUAYEGR","created_at":"2026-07-05T11:39:26.095867+00:00"},{"alias_kind":"pith_short_8","alias_value":"USPXZPBZ","created_at":"2026-07-05T11:39:26.095867+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/USPXZPBZZRUAYEGRTU7V5YCDZ4","json":"https://pith.science/pith/USPXZPBZZRUAYEGRTU7V5YCDZ4.json","graph_json":"https://pith.science/api/pith-number/USPXZPBZZRUAYEGRTU7V5YCDZ4/graph.json","events_json":"https://pith.science/api/pith-number/USPXZPBZZRUAYEGRTU7V5YCDZ4/events.json","paper":"https://pith.science/paper/USPXZPBZ"},"agent_actions":{"view_html":"https://pith.science/pith/USPXZPBZZRUAYEGRTU7V5YCDZ4","download_json":"https://pith.science/pith/USPXZPBZZRUAYEGRTU7V5YCDZ4.json","view_paper":"https://pith.science/paper/USPXZPBZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2507.13960&json=true","fetch_graph":"https://pith.science/api/pith-number/USPXZPBZZRUAYEGRTU7V5YCDZ4/graph.json","fetch_events":"https://pith.science/api/pith-number/USPXZPBZZRUAYEGRTU7V5YCDZ4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/USPXZPBZZRUAYEGRTU7V5YCDZ4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/USPXZPBZZRUAYEGRTU7V5YCDZ4/action/storage_attestation","attest_author":"https://pith.science/pith/USPXZPBZZRUAYEGRTU7V5YCDZ4/action/author_attestation","sign_citation":"https://pith.science/pith/USPXZPBZZRUAYEGRTU7V5YCDZ4/action/citation_signature","submit_replication":"https://pith.science/pith/USPXZPBZZRUAYEGRTU7V5YCDZ4/action/replication_record"}},"created_at":"2026-07-05T11:39:26.095867+00:00","updated_at":"2026-07-05T11:39:26.095867+00:00"}