{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:Z3FJHTTEUQ2TH3EJ6ETIY6IFBW","short_pith_number":"pith:Z3FJHTTE","canonical_record":{"source":{"id":"1709.06392","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-09-19T13:15:27Z","cross_cats_sorted":["nlin.AO","nlin.CD"],"title_canon_sha256":"ee403bd0115437bcab5d6879f86a36996d69c9327be2047975bc467dfdf36fde","abstract_canon_sha256":"14436a1e7a69bc789c47dc706d87134aefddfc67723e930d7b5810aa47f4dfa5"},"schema_version":"1.0"},"canonical_sha256":"ceca93ce64a43533ec89f1268c79050d85e6ec90c56873de5a6cb2063ca7f3a4","source":{"kind":"arxiv","id":"1709.06392","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1709.06392","created_at":"2026-05-18T00:32:05Z"},{"alias_kind":"arxiv_version","alias_value":"1709.06392v2","created_at":"2026-05-18T00:32:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.06392","created_at":"2026-05-18T00:32:05Z"},{"alias_kind":"pith_short_12","alias_value":"Z3FJHTTEUQ2T","created_at":"2026-05-18T12:31:59Z"},{"alias_kind":"pith_short_16","alias_value":"Z3FJHTTEUQ2TH3EJ","created_at":"2026-05-18T12:31:59Z"},{"alias_kind":"pith_short_8","alias_value":"Z3FJHTTE","created_at":"2026-05-18T12:31:59Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:Z3FJHTTEUQ2TH3EJ6ETIY6IFBW","target":"record","payload":{"canonical_record":{"source":{"id":"1709.06392","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-09-19T13:15:27Z","cross_cats_sorted":["nlin.AO","nlin.CD"],"title_canon_sha256":"ee403bd0115437bcab5d6879f86a36996d69c9327be2047975bc467dfdf36fde","abstract_canon_sha256":"14436a1e7a69bc789c47dc706d87134aefddfc67723e930d7b5810aa47f4dfa5"},"schema_version":"1.0"},"canonical_sha256":"ceca93ce64a43533ec89f1268c79050d85e6ec90c56873de5a6cb2063ca7f3a4","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:32:05.041389Z","signature_b64":"Eerm7RM9ZUgBte7k+r69/+S7tF4jXMjb84QIuuTM8C4oFPytFSd4wQZp//MpevE0l3zofRKUbNyC9sQqvYN4DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ceca93ce64a43533ec89f1268c79050d85e6ec90c56873de5a6cb2063ca7f3a4","last_reissued_at":"2026-05-18T00:32:05.040733Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:32:05.040733Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1709.06392","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:32:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5gIEjGK9dQrir5L/jiuUTOmQr4YS2t059woXAtg2XQ6xBe//iYJLXzZkywqzu2kNSff1YTHVKu0kcPd9XxNJAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T06:12:21.426789Z"},"content_sha256":"2a2efcf73c92f7ddd38b613be705f1563af6b1ebabc50c6eea1aad2b8fe632e2","schema_version":"1.0","event_id":"sha256:2a2efcf73c92f7ddd38b613be705f1563af6b1ebabc50c6eea1aad2b8fe632e2"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:Z3FJHTTEUQ2TH3EJ6ETIY6IFBW","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Equilibration in the Nos\\'e-Hoover isokinetic ensemble: Effect of inter-particle interactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nlin.AO","nlin.CD"],"primary_cat":"cond-mat.stat-mech","authors_text":"Shamik Gupta, Stefano Ruffo","submitted_at":"2017-09-19T13:15:27Z","abstract_excerpt":"We investigate the stationary and dynamic properties of the celebrated Nos\\'e-Hoover dynamics of many-body interacting Hamiltonian systems, with an emphasis on the effect of inter-particle interactions. To this end, we consider a model system with both short- and long-range interactions. The Nos\\'e-Hoover dynamics aims to generate the canonical equilibrium distribution of a system at a desired temperature by employing a set of time-reversible, deterministic equations of motion. A signature of canonical equilibrium is a single-particle momentum distribution that is Gaussian. We find that the eq"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.06392","kind":"arxiv","version":2},"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":"2026-05-18T00:32:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Larokc4qupWBTexZd2dEIySNvyn5jcn2RXIA/3Ts6ecUGRrhid+SPBifnq7lt8xikEowTkFvtlt/TvT0bvYGCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T06:12:21.427478Z"},"content_sha256":"da36da2816171c837d6d47fa4040d4dfe5554e1acd30c16680c97ad0f6684e49","schema_version":"1.0","event_id":"sha256:da36da2816171c837d6d47fa4040d4dfe5554e1acd30c16680c97ad0f6684e49"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/Z3FJHTTEUQ2TH3EJ6ETIY6IFBW/bundle.json","state_url":"https://pith.science/pith/Z3FJHTTEUQ2TH3EJ6ETIY6IFBW/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/Z3FJHTTEUQ2TH3EJ6ETIY6IFBW/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":"2026-06-07T06:12:21Z","links":{"resolver":"https://pith.science/pith/Z3FJHTTEUQ2TH3EJ6ETIY6IFBW","bundle":"https://pith.science/pith/Z3FJHTTEUQ2TH3EJ6ETIY6IFBW/bundle.json","state":"https://pith.science/pith/Z3FJHTTEUQ2TH3EJ6ETIY6IFBW/state.json","well_known_bundle":"https://pith.science/.well-known/pith/Z3FJHTTEUQ2TH3EJ6ETIY6IFBW/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:Z3FJHTTEUQ2TH3EJ6ETIY6IFBW","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":"14436a1e7a69bc789c47dc706d87134aefddfc67723e930d7b5810aa47f4dfa5","cross_cats_sorted":["nlin.AO","nlin.CD"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-09-19T13:15:27Z","title_canon_sha256":"ee403bd0115437bcab5d6879f86a36996d69c9327be2047975bc467dfdf36fde"},"schema_version":"1.0","source":{"id":"1709.06392","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1709.06392","created_at":"2026-05-18T00:32:05Z"},{"alias_kind":"arxiv_version","alias_value":"1709.06392v2","created_at":"2026-05-18T00:32:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.06392","created_at":"2026-05-18T00:32:05Z"},{"alias_kind":"pith_short_12","alias_value":"Z3FJHTTEUQ2T","created_at":"2026-05-18T12:31:59Z"},{"alias_kind":"pith_short_16","alias_value":"Z3FJHTTEUQ2TH3EJ","created_at":"2026-05-18T12:31:59Z"},{"alias_kind":"pith_short_8","alias_value":"Z3FJHTTE","created_at":"2026-05-18T12:31:59Z"}],"graph_snapshots":[{"event_id":"sha256:da36da2816171c837d6d47fa4040d4dfe5554e1acd30c16680c97ad0f6684e49","target":"graph","created_at":"2026-05-18T00:32:05Z","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":"We investigate the stationary and dynamic properties of the celebrated Nos\\'e-Hoover dynamics of many-body interacting Hamiltonian systems, with an emphasis on the effect of inter-particle interactions. To this end, we consider a model system with both short- and long-range interactions. The Nos\\'e-Hoover dynamics aims to generate the canonical equilibrium distribution of a system at a desired temperature by employing a set of time-reversible, deterministic equations of motion. A signature of canonical equilibrium is a single-particle momentum distribution that is Gaussian. We find that the eq","authors_text":"Shamik Gupta, Stefano Ruffo","cross_cats":["nlin.AO","nlin.CD"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-09-19T13:15:27Z","title":"Equilibration in the Nos\\'e-Hoover isokinetic ensemble: Effect of inter-particle interactions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.06392","kind":"arxiv","version":2},"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":"sha256:2a2efcf73c92f7ddd38b613be705f1563af6b1ebabc50c6eea1aad2b8fe632e2","target":"record","created_at":"2026-05-18T00:32:05Z","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":"14436a1e7a69bc789c47dc706d87134aefddfc67723e930d7b5810aa47f4dfa5","cross_cats_sorted":["nlin.AO","nlin.CD"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-09-19T13:15:27Z","title_canon_sha256":"ee403bd0115437bcab5d6879f86a36996d69c9327be2047975bc467dfdf36fde"},"schema_version":"1.0","source":{"id":"1709.06392","kind":"arxiv","version":2}},"canonical_sha256":"ceca93ce64a43533ec89f1268c79050d85e6ec90c56873de5a6cb2063ca7f3a4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ceca93ce64a43533ec89f1268c79050d85e6ec90c56873de5a6cb2063ca7f3a4","first_computed_at":"2026-05-18T00:32:05.040733Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:32:05.040733Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Eerm7RM9ZUgBte7k+r69/+S7tF4jXMjb84QIuuTM8C4oFPytFSd4wQZp//MpevE0l3zofRKUbNyC9sQqvYN4DA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:32:05.041389Z","signed_message":"canonical_sha256_bytes"},"source_id":"1709.06392","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2a2efcf73c92f7ddd38b613be705f1563af6b1ebabc50c6eea1aad2b8fe632e2","sha256:da36da2816171c837d6d47fa4040d4dfe5554e1acd30c16680c97ad0f6684e49"],"state_sha256":"59c2d6a58e34c29d8e68808808ee96171ac552f0608cd14a8a25906e4bcb3f22"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7fVFyJrdFrFJZKyjjQpjcvOOxBF22oy2264QiEd/R3s2e87xRsNZC9pOT6wpboLMgLyKMaFANj5h4iYX+lpECQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-07T06:12:21.430999Z","bundle_sha256":"42329e51719974adc6f073a2179f98b401b82ae3ae5b8fa3a96ff0607c9d1829"}}