{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:MHRCSMZ6LJMVMTKDBEX6UE5TUD","short_pith_number":"pith:MHRCSMZ6","canonical_record":{"source":{"id":"1407.5997","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-07-22T20:00:04Z","cross_cats_sorted":["cond-mat.dis-nn","hep-lat","hep-th","physics.chem-ph"],"title_canon_sha256":"bf68bc86f30d4924c357b7dad370170a4baf23db63ef52df7f9941f9a90151be","abstract_canon_sha256":"4e92d7a698aa9b523bb1019c21dd40d2501b890529a3087cdb5d8cf69057df70"},"schema_version":"1.0"},"canonical_sha256":"61e229333e5a59564d43092fea13b3a0d6147a7fd212dc6dd4df3e3477b6da06","source":{"kind":"arxiv","id":"1407.5997","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.5997","created_at":"2026-05-18T02:46:38Z"},{"alias_kind":"arxiv_version","alias_value":"1407.5997v1","created_at":"2026-05-18T02:46:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.5997","created_at":"2026-05-18T02:46:38Z"},{"alias_kind":"pith_short_12","alias_value":"MHRCSMZ6LJMV","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"MHRCSMZ6LJMVMTKD","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"MHRCSMZ6","created_at":"2026-05-18T12:28:38Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:MHRCSMZ6LJMVMTKDBEX6UE5TUD","target":"record","payload":{"canonical_record":{"source":{"id":"1407.5997","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-07-22T20:00:04Z","cross_cats_sorted":["cond-mat.dis-nn","hep-lat","hep-th","physics.chem-ph"],"title_canon_sha256":"bf68bc86f30d4924c357b7dad370170a4baf23db63ef52df7f9941f9a90151be","abstract_canon_sha256":"4e92d7a698aa9b523bb1019c21dd40d2501b890529a3087cdb5d8cf69057df70"},"schema_version":"1.0"},"canonical_sha256":"61e229333e5a59564d43092fea13b3a0d6147a7fd212dc6dd4df3e3477b6da06","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:46:38.874854Z","signature_b64":"i9+MOwv5btgQ2HennZiWKgHIgWyfy3kjRxyyH0BRisaMRMOacJ5xWTKMnJGCOOdUVBksqRedg6Ry4EJ81nQhDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"61e229333e5a59564d43092fea13b3a0d6147a7fd212dc6dd4df3e3477b6da06","last_reissued_at":"2026-05-18T02:46:38.874453Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:46:38.874453Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1407.5997","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":"2026-05-18T02:46:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"X+XwFsIo0rYdr9rtvy9jPWecHJJnBzEHXuPQXUVQx5gSoRKhUPGRSN9ewaGSpHE0SdI3n3rbE2FcAFIquM3cDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T13:47:06.249798Z"},"content_sha256":"469c477db30b4e4741ea4f96660fb7e9a1b9aaa9f18947315c12136186190512","schema_version":"1.0","event_id":"sha256:469c477db30b4e4741ea4f96660fb7e9a1b9aaa9f18947315c12136186190512"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:MHRCSMZ6LJMVMTKDBEX6UE5TUD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"An Inversion-Relaxation Approach for Sampling Stationary Points of Spin Model Hamiltonians","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn","hep-lat","hep-th","physics.chem-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Ciaran Hughes, David J Wales, Dhagash Mehta","submitted_at":"2014-07-22T20:00:04Z","abstract_excerpt":"Sampling the stationary points of a complicated potential energy landscape is a challenging problem. Here we introduce a sampling method based on relaxation from stationary points of the highest index of the Hessian matrix. We illustrate how this approach can find all the stationary points for potentials or Hamiltonians bounded from above, which includes a large class of important spin models, and we show that it is far more efficient than previous methods. For potentials unbounded from above, the relaxation part of the method is still efficient in finding minima and transition states, which a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.5997","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":"2026-05-18T02:46:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mDtgjYG/Gc46b1HixJDr5cRfjFKcBS4jTibXbGGJkCjSdTWKkDiu9xig4PgJgdOueb1FO9CXEIUyEwfTyrWTCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T13:47:06.250194Z"},"content_sha256":"3cbba2623a8780b01a59341ab4ab02058034d6952b8a150d289f3b35363d1ae6","schema_version":"1.0","event_id":"sha256:3cbba2623a8780b01a59341ab4ab02058034d6952b8a150d289f3b35363d1ae6"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/MHRCSMZ6LJMVMTKDBEX6UE5TUD/bundle.json","state_url":"https://pith.science/pith/MHRCSMZ6LJMVMTKDBEX6UE5TUD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/MHRCSMZ6LJMVMTKDBEX6UE5TUD/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":"2026-05-27T13:47:06Z","links":{"resolver":"https://pith.science/pith/MHRCSMZ6LJMVMTKDBEX6UE5TUD","bundle":"https://pith.science/pith/MHRCSMZ6LJMVMTKDBEX6UE5TUD/bundle.json","state":"https://pith.science/pith/MHRCSMZ6LJMVMTKDBEX6UE5TUD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/MHRCSMZ6LJMVMTKDBEX6UE5TUD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:MHRCSMZ6LJMVMTKDBEX6UE5TUD","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":"4e92d7a698aa9b523bb1019c21dd40d2501b890529a3087cdb5d8cf69057df70","cross_cats_sorted":["cond-mat.dis-nn","hep-lat","hep-th","physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-07-22T20:00:04Z","title_canon_sha256":"bf68bc86f30d4924c357b7dad370170a4baf23db63ef52df7f9941f9a90151be"},"schema_version":"1.0","source":{"id":"1407.5997","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.5997","created_at":"2026-05-18T02:46:38Z"},{"alias_kind":"arxiv_version","alias_value":"1407.5997v1","created_at":"2026-05-18T02:46:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.5997","created_at":"2026-05-18T02:46:38Z"},{"alias_kind":"pith_short_12","alias_value":"MHRCSMZ6LJMV","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"MHRCSMZ6LJMVMTKD","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"MHRCSMZ6","created_at":"2026-05-18T12:28:38Z"}],"graph_snapshots":[{"event_id":"sha256:3cbba2623a8780b01a59341ab4ab02058034d6952b8a150d289f3b35363d1ae6","target":"graph","created_at":"2026-05-18T02:46:38Z","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":"Sampling the stationary points of a complicated potential energy landscape is a challenging problem. Here we introduce a sampling method based on relaxation from stationary points of the highest index of the Hessian matrix. We illustrate how this approach can find all the stationary points for potentials or Hamiltonians bounded from above, which includes a large class of important spin models, and we show that it is far more efficient than previous methods. For potentials unbounded from above, the relaxation part of the method is still efficient in finding minima and transition states, which a","authors_text":"Ciaran Hughes, David J Wales, Dhagash Mehta","cross_cats":["cond-mat.dis-nn","hep-lat","hep-th","physics.chem-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-07-22T20:00:04Z","title":"An Inversion-Relaxation Approach for Sampling Stationary Points of Spin Model Hamiltonians"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.5997","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":"sha256:469c477db30b4e4741ea4f96660fb7e9a1b9aaa9f18947315c12136186190512","target":"record","created_at":"2026-05-18T02:46:38Z","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":"4e92d7a698aa9b523bb1019c21dd40d2501b890529a3087cdb5d8cf69057df70","cross_cats_sorted":["cond-mat.dis-nn","hep-lat","hep-th","physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-07-22T20:00:04Z","title_canon_sha256":"bf68bc86f30d4924c357b7dad370170a4baf23db63ef52df7f9941f9a90151be"},"schema_version":"1.0","source":{"id":"1407.5997","kind":"arxiv","version":1}},"canonical_sha256":"61e229333e5a59564d43092fea13b3a0d6147a7fd212dc6dd4df3e3477b6da06","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"61e229333e5a59564d43092fea13b3a0d6147a7fd212dc6dd4df3e3477b6da06","first_computed_at":"2026-05-18T02:46:38.874453Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:46:38.874453Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"i9+MOwv5btgQ2HennZiWKgHIgWyfy3kjRxyyH0BRisaMRMOacJ5xWTKMnJGCOOdUVBksqRedg6Ry4EJ81nQhDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:46:38.874854Z","signed_message":"canonical_sha256_bytes"},"source_id":"1407.5997","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:469c477db30b4e4741ea4f96660fb7e9a1b9aaa9f18947315c12136186190512","sha256:3cbba2623a8780b01a59341ab4ab02058034d6952b8a150d289f3b35363d1ae6"],"state_sha256":"7c3eac39bfc38707631333d895c6c0719cfe17500a9612b1428d53c83e0b915b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"O1VG55ec8NgW2d/fcX42wvCgawv4iiDOhHYxygCXQqTCXpQbkCspDJ1u67WAtQFoo8f5Fu52VOrkg3jnDD0ECg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T13:47:06.253980Z","bundle_sha256":"aec33ac7c612bc53c2f5174f950f73289e9c63b06b33d5023743fc6d76d8ff56"}}