{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:PBT4APG4IPYUH6XIL4O6V5PIYS","short_pith_number":"pith:PBT4APG4","schema_version":"1.0","canonical_sha256":"7867c03cdc43f143fae85f1deaf5e8c4b8e9ffd06529d406328993d1c890015e","source":{"kind":"arxiv","id":"1103.5216","version":1},"attestation_state":"computed","paper":{"title":"Intrinsic activation energy for twin wall motion","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"E. K. H. Salje, L. Goncalves-Ferreria, M. Daraktchiev, U. Bismayer, W. T. Lee","submitted_at":"2011-03-27T14:33:41Z","abstract_excerpt":"Even in a topologically perfect crystal, a moving twin wall will experience forces due to the discrete nature of the lattice. The potential energy landscape can be described in terms of one of two parameters: the Peierls energy, which is the activation energy for domain wall motion in a perfect crystal; and the Peierls stress, the maximum pinning stress that the potential can exert. We investigate these parameters in a one order parameter discrete Landau-Ginzburg model and a classical potential model of the ferroelastic perovskite CaTiO3. Using the one order parameter model we show that the Pe"},"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":"1103.5216","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2011-03-27T14:33:41Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"3cc89958dae1f328f002a9ac0f0ea7bc185320f837dc674a562588186f07e7c0","abstract_canon_sha256":"9e157121725ab7cdae2eb33b7e423aaa80748c89dd413363a24c5828122ca5a3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:25:38.413917Z","signature_b64":"dZUJcSe3NzCJPScfVPsIp//quVGWU1ViXi+hevg+O0XsyduSAxUnlPMagOOfrokzN7g2oktvj7yVh0h927+ZAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7867c03cdc43f143fae85f1deaf5e8c4b8e9ffd06529d406328993d1c890015e","last_reissued_at":"2026-05-18T04:25:38.413459Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:25:38.413459Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Intrinsic activation energy for twin wall motion","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"E. K. H. Salje, L. Goncalves-Ferreria, M. Daraktchiev, U. Bismayer, W. T. Lee","submitted_at":"2011-03-27T14:33:41Z","abstract_excerpt":"Even in a topologically perfect crystal, a moving twin wall will experience forces due to the discrete nature of the lattice. The potential energy landscape can be described in terms of one of two parameters: the Peierls energy, which is the activation energy for domain wall motion in a perfect crystal; and the Peierls stress, the maximum pinning stress that the potential can exert. We investigate these parameters in a one order parameter discrete Landau-Ginzburg model and a classical potential model of the ferroelastic perovskite CaTiO3. Using the one order parameter model we show that the Pe"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1103.5216","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":"1103.5216","created_at":"2026-05-18T04:25:38.413524+00:00"},{"alias_kind":"arxiv_version","alias_value":"1103.5216v1","created_at":"2026-05-18T04:25:38.413524+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1103.5216","created_at":"2026-05-18T04:25:38.413524+00:00"},{"alias_kind":"pith_short_12","alias_value":"PBT4APG4IPYU","created_at":"2026-05-18T12:26:39.201973+00:00"},{"alias_kind":"pith_short_16","alias_value":"PBT4APG4IPYUH6XI","created_at":"2026-05-18T12:26:39.201973+00:00"},{"alias_kind":"pith_short_8","alias_value":"PBT4APG4","created_at":"2026-05-18T12:26:39.201973+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/PBT4APG4IPYUH6XIL4O6V5PIYS","json":"https://pith.science/pith/PBT4APG4IPYUH6XIL4O6V5PIYS.json","graph_json":"https://pith.science/api/pith-number/PBT4APG4IPYUH6XIL4O6V5PIYS/graph.json","events_json":"https://pith.science/api/pith-number/PBT4APG4IPYUH6XIL4O6V5PIYS/events.json","paper":"https://pith.science/paper/PBT4APG4"},"agent_actions":{"view_html":"https://pith.science/pith/PBT4APG4IPYUH6XIL4O6V5PIYS","download_json":"https://pith.science/pith/PBT4APG4IPYUH6XIL4O6V5PIYS.json","view_paper":"https://pith.science/paper/PBT4APG4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1103.5216&json=true","fetch_graph":"https://pith.science/api/pith-number/PBT4APG4IPYUH6XIL4O6V5PIYS/graph.json","fetch_events":"https://pith.science/api/pith-number/PBT4APG4IPYUH6XIL4O6V5PIYS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PBT4APG4IPYUH6XIL4O6V5PIYS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PBT4APG4IPYUH6XIL4O6V5PIYS/action/storage_attestation","attest_author":"https://pith.science/pith/PBT4APG4IPYUH6XIL4O6V5PIYS/action/author_attestation","sign_citation":"https://pith.science/pith/PBT4APG4IPYUH6XIL4O6V5PIYS/action/citation_signature","submit_replication":"https://pith.science/pith/PBT4APG4IPYUH6XIL4O6V5PIYS/action/replication_record"}},"created_at":"2026-05-18T04:25:38.413524+00:00","updated_at":"2026-05-18T04:25:38.413524+00:00"}