{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:G5UBGLL233T74Q4TNCZUTOZTZ4","short_pith_number":"pith:G5UBGLL2","canonical_record":{"source":{"id":"1612.01737","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-12-06T10:29:57Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"fc5b2187ae59c526cc227ea7f272b733ebd30fa3429c1403bdac1c642a9b61f6","abstract_canon_sha256":"286bd8f2878fc1c7f66a7849ac1d3271e60791d4b026f64653d4a8980e752841"},"schema_version":"1.0"},"canonical_sha256":"3768132d7adee7fe439368b349bb33cf14d1116cb31e0b2da6b28523c4617801","source":{"kind":"arxiv","id":"1612.01737","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1612.01737","created_at":"2026-05-18T00:55:47Z"},{"alias_kind":"arxiv_version","alias_value":"1612.01737v1","created_at":"2026-05-18T00:55:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1612.01737","created_at":"2026-05-18T00:55:47Z"},{"alias_kind":"pith_short_12","alias_value":"G5UBGLL233T7","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_16","alias_value":"G5UBGLL233T74Q4T","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_8","alias_value":"G5UBGLL2","created_at":"2026-05-18T12:30:15Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:G5UBGLL233T74Q4TNCZUTOZTZ4","target":"record","payload":{"canonical_record":{"source":{"id":"1612.01737","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-12-06T10:29:57Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"fc5b2187ae59c526cc227ea7f272b733ebd30fa3429c1403bdac1c642a9b61f6","abstract_canon_sha256":"286bd8f2878fc1c7f66a7849ac1d3271e60791d4b026f64653d4a8980e752841"},"schema_version":"1.0"},"canonical_sha256":"3768132d7adee7fe439368b349bb33cf14d1116cb31e0b2da6b28523c4617801","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:55:47.731157Z","signature_b64":"bzO+Xp6C/jZaU+9RXTgX6nX0nyJHtHf49Z4CFsGq56kJhcHSRlXIHbxsnouyXKbf1M4GygWdmZixTeRZQfMNAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3768132d7adee7fe439368b349bb33cf14d1116cb31e0b2da6b28523c4617801","last_reissued_at":"2026-05-18T00:55:47.730702Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:55:47.730702Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1612.01737","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":"2026-05-18T00:55:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UVytSMQ6Oy5s7lAwENi1d5VWZs26j2muVx1S5aFZz5fCmjFh0xmoEEz9w9Nij4b5BrJext55ryZ4Mt894DDtBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T03:24:02.129522Z"},"content_sha256":"38941a6d495d2278b50dd4ee99fae9cd8280d1f420d2766b91b785f2f1066be7","schema_version":"1.0","event_id":"sha256:38941a6d495d2278b50dd4ee99fae9cd8280d1f420d2766b91b785f2f1066be7"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:G5UBGLL233T74Q4TNCZUTOZTZ4","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dynamical scaling for underdamped strain order parameters quenched below first-order phase transitions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.stat-mech","authors_text":"Awadhesh K. Dubey, N. Shankaraiah, Sanjay Puri, Subodh R. Shenoy","submitted_at":"2016-12-06T10:29:57Z","abstract_excerpt":"In the conceptual framework of phase ordering after temperature quenches below transition, we consider the underdamped Bales-Gooding-type 'momentum conserving' dynamics of a 2D martensitic structural transition from a square-to-rectangle unit cell. The one-component or $N_{\\rm OP} =1$ order parameter is one of the physical strains, and the Landau free energy has a triple well, describing a first-order transition. We numerically study the evolution of the strain-strain correlation, and find that it exhibits dynamical scaling, with a coarsening length $L(t) \\sim t^{\\alpha}$. We find at intermedi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1612.01737","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":"2026-05-18T00:55:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QifNQDeimeWc/gElcr11+vUHBgSNBr/SqgL6H25D4GbT4XOpOus754eH5w8jvn3vR8XvBQAW16tCfn/PznmDAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T03:24:02.130295Z"},"content_sha256":"c44278d5213bd7aa74f29e72f2a1a1133b127ed04831d2a8dc133c161384759e","schema_version":"1.0","event_id":"sha256:c44278d5213bd7aa74f29e72f2a1a1133b127ed04831d2a8dc133c161384759e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/G5UBGLL233T74Q4TNCZUTOZTZ4/bundle.json","state_url":"https://pith.science/pith/G5UBGLL233T74Q4TNCZUTOZTZ4/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/G5UBGLL233T74Q4TNCZUTOZTZ4/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":"2026-06-08T03:24:02Z","links":{"resolver":"https://pith.science/pith/G5UBGLL233T74Q4TNCZUTOZTZ4","bundle":"https://pith.science/pith/G5UBGLL233T74Q4TNCZUTOZTZ4/bundle.json","state":"https://pith.science/pith/G5UBGLL233T74Q4TNCZUTOZTZ4/state.json","well_known_bundle":"https://pith.science/.well-known/pith/G5UBGLL233T74Q4TNCZUTOZTZ4/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:G5UBGLL233T74Q4TNCZUTOZTZ4","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":"286bd8f2878fc1c7f66a7849ac1d3271e60791d4b026f64653d4a8980e752841","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-12-06T10:29:57Z","title_canon_sha256":"fc5b2187ae59c526cc227ea7f272b733ebd30fa3429c1403bdac1c642a9b61f6"},"schema_version":"1.0","source":{"id":"1612.01737","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1612.01737","created_at":"2026-05-18T00:55:47Z"},{"alias_kind":"arxiv_version","alias_value":"1612.01737v1","created_at":"2026-05-18T00:55:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1612.01737","created_at":"2026-05-18T00:55:47Z"},{"alias_kind":"pith_short_12","alias_value":"G5UBGLL233T7","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_16","alias_value":"G5UBGLL233T74Q4T","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_8","alias_value":"G5UBGLL2","created_at":"2026-05-18T12:30:15Z"}],"graph_snapshots":[{"event_id":"sha256:c44278d5213bd7aa74f29e72f2a1a1133b127ed04831d2a8dc133c161384759e","target":"graph","created_at":"2026-05-18T00:55:47Z","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":"In the conceptual framework of phase ordering after temperature quenches below transition, we consider the underdamped Bales-Gooding-type 'momentum conserving' dynamics of a 2D martensitic structural transition from a square-to-rectangle unit cell. The one-component or $N_{\\rm OP} =1$ order parameter is one of the physical strains, and the Landau free energy has a triple well, describing a first-order transition. We numerically study the evolution of the strain-strain correlation, and find that it exhibits dynamical scaling, with a coarsening length $L(t) \\sim t^{\\alpha}$. We find at intermedi","authors_text":"Awadhesh K. Dubey, N. Shankaraiah, Sanjay Puri, Subodh R. Shenoy","cross_cats":["cond-mat.mtrl-sci"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-12-06T10:29:57Z","title":"Dynamical scaling for underdamped strain order parameters quenched below first-order phase transitions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1612.01737","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":"sha256:38941a6d495d2278b50dd4ee99fae9cd8280d1f420d2766b91b785f2f1066be7","target":"record","created_at":"2026-05-18T00:55:47Z","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":"286bd8f2878fc1c7f66a7849ac1d3271e60791d4b026f64653d4a8980e752841","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-12-06T10:29:57Z","title_canon_sha256":"fc5b2187ae59c526cc227ea7f272b733ebd30fa3429c1403bdac1c642a9b61f6"},"schema_version":"1.0","source":{"id":"1612.01737","kind":"arxiv","version":1}},"canonical_sha256":"3768132d7adee7fe439368b349bb33cf14d1116cb31e0b2da6b28523c4617801","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3768132d7adee7fe439368b349bb33cf14d1116cb31e0b2da6b28523c4617801","first_computed_at":"2026-05-18T00:55:47.730702Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:55:47.730702Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"bzO+Xp6C/jZaU+9RXTgX6nX0nyJHtHf49Z4CFsGq56kJhcHSRlXIHbxsnouyXKbf1M4GygWdmZixTeRZQfMNAw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:55:47.731157Z","signed_message":"canonical_sha256_bytes"},"source_id":"1612.01737","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:38941a6d495d2278b50dd4ee99fae9cd8280d1f420d2766b91b785f2f1066be7","sha256:c44278d5213bd7aa74f29e72f2a1a1133b127ed04831d2a8dc133c161384759e"],"state_sha256":"8f473342023e233aa76e4c698b9800ef11fe6ba5c966e88a26c96ee9f8feae49"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Pfw6oKSG0AVz3w4dQORlM8i2WSKs0IgXNo+K4/gCK9bA90QuhmKQ8GgnoJ64VtpB/DU/FmX/P+0I6xry6/UlBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-08T03:24:02.133933Z","bundle_sha256":"d9e5c0fc4d90c950fcca2610a9ffdd583e6782de565a944a7fe021b4614d27c6"}}