{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:D4ARGL2AERQFXQIRWGMWBLOXIR","short_pith_number":"pith:D4ARGL2A","canonical_record":{"source":{"id":"1106.5545","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-06-28T00:33:41Z","cross_cats_sorted":[],"title_canon_sha256":"fa3b5e48493f0c624868b0db51fbfdbf384b13a65c019a33976d1acd7a0b5027","abstract_canon_sha256":"d9d0c6b4fd9930f7600469ae9219c2f6a900bd5c091f1bc18b7f0c9ef8029828"},"schema_version":"1.0"},"canonical_sha256":"1f01132f4024605bc111b19960add7446faf5c666d2d25fd770854a9621c569d","source":{"kind":"arxiv","id":"1106.5545","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1106.5545","created_at":"2026-05-18T02:01:30Z"},{"alias_kind":"arxiv_version","alias_value":"1106.5545v1","created_at":"2026-05-18T02:01:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.5545","created_at":"2026-05-18T02:01:30Z"},{"alias_kind":"pith_short_12","alias_value":"D4ARGL2AERQF","created_at":"2026-05-18T12:26:26Z"},{"alias_kind":"pith_short_16","alias_value":"D4ARGL2AERQFXQIR","created_at":"2026-05-18T12:26:26Z"},{"alias_kind":"pith_short_8","alias_value":"D4ARGL2A","created_at":"2026-05-18T12:26:26Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:D4ARGL2AERQFXQIRWGMWBLOXIR","target":"record","payload":{"canonical_record":{"source":{"id":"1106.5545","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-06-28T00:33:41Z","cross_cats_sorted":[],"title_canon_sha256":"fa3b5e48493f0c624868b0db51fbfdbf384b13a65c019a33976d1acd7a0b5027","abstract_canon_sha256":"d9d0c6b4fd9930f7600469ae9219c2f6a900bd5c091f1bc18b7f0c9ef8029828"},"schema_version":"1.0"},"canonical_sha256":"1f01132f4024605bc111b19960add7446faf5c666d2d25fd770854a9621c569d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:01:30.051602Z","signature_b64":"Wo45K1AE69zLVLptX1ntTYKbbBeHIjbeHKCu+CpQUOWaBMhxRE0AJsVcpnWVWlkgNgdbsngORgb1ZY/gW8rECQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1f01132f4024605bc111b19960add7446faf5c666d2d25fd770854a9621c569d","last_reissued_at":"2026-05-18T02:01:30.051046Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:01:30.051046Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1106.5545","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":"2026-05-18T02:01:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UApAK+2epb25APPzT5XvOT5puOxKguB0twe3ndF1CywFKiWGK7Vg/it8uKKrb5pfzcHzN7yZuiqKBrgrDaT7BQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T11:30:02.654021Z"},"content_sha256":"0df09e023d704db3d3f9923ea02e457b816ec7a41f1574b0d15d174795c82179","schema_version":"1.0","event_id":"sha256:0df09e023d704db3d3f9923ea02e457b816ec7a41f1574b0d15d174795c82179"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:D4ARGL2AERQFXQIRWGMWBLOXIR","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Noisy Classical Field Theories with Two Coupled Fields: Dependence of Escape Rates on Relative Field Stiffnesses","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"D. L. Stein, Lan Gong","submitted_at":"2011-06-28T00:33:41Z","abstract_excerpt":"Exit times for stochastic Ginzburg-Landau classical field theories with two or more coupled classical fields depend on the interval length on which the fields are defined, the potential in which the fields deterministically evolve, and the relative stiffness of the fields themselves. The latter is of particular importance in that physical applications will generally require different relative stiffnesses, but the effect of varying field stiffnesses has not heretofore been studied. In this paper, we explore the complete phase diagram of escape times as they depend on the various problem paramet"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.5545","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":"2026-05-18T02:01:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5wr7WWKgyuMM0EMnbjpRmmewMiCLMWXwvchfBLm39gtB/Cwr05z8t9VRzMWcd9vAkJAV7sVm4NNIG68rVpqtAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T11:30:02.654379Z"},"content_sha256":"f6f94e19df504313898f79036f96482d68dfe97804d7c3338bc6ebaa3bc0c20a","schema_version":"1.0","event_id":"sha256:f6f94e19df504313898f79036f96482d68dfe97804d7c3338bc6ebaa3bc0c20a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/D4ARGL2AERQFXQIRWGMWBLOXIR/bundle.json","state_url":"https://pith.science/pith/D4ARGL2AERQFXQIRWGMWBLOXIR/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/D4ARGL2AERQFXQIRWGMWBLOXIR/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":"2026-05-28T11:30:02Z","links":{"resolver":"https://pith.science/pith/D4ARGL2AERQFXQIRWGMWBLOXIR","bundle":"https://pith.science/pith/D4ARGL2AERQFXQIRWGMWBLOXIR/bundle.json","state":"https://pith.science/pith/D4ARGL2AERQFXQIRWGMWBLOXIR/state.json","well_known_bundle":"https://pith.science/.well-known/pith/D4ARGL2AERQFXQIRWGMWBLOXIR/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:D4ARGL2AERQFXQIRWGMWBLOXIR","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":"d9d0c6b4fd9930f7600469ae9219c2f6a900bd5c091f1bc18b7f0c9ef8029828","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-06-28T00:33:41Z","title_canon_sha256":"fa3b5e48493f0c624868b0db51fbfdbf384b13a65c019a33976d1acd7a0b5027"},"schema_version":"1.0","source":{"id":"1106.5545","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1106.5545","created_at":"2026-05-18T02:01:30Z"},{"alias_kind":"arxiv_version","alias_value":"1106.5545v1","created_at":"2026-05-18T02:01:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.5545","created_at":"2026-05-18T02:01:30Z"},{"alias_kind":"pith_short_12","alias_value":"D4ARGL2AERQF","created_at":"2026-05-18T12:26:26Z"},{"alias_kind":"pith_short_16","alias_value":"D4ARGL2AERQFXQIR","created_at":"2026-05-18T12:26:26Z"},{"alias_kind":"pith_short_8","alias_value":"D4ARGL2A","created_at":"2026-05-18T12:26:26Z"}],"graph_snapshots":[{"event_id":"sha256:f6f94e19df504313898f79036f96482d68dfe97804d7c3338bc6ebaa3bc0c20a","target":"graph","created_at":"2026-05-18T02:01:30Z","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":"Exit times for stochastic Ginzburg-Landau classical field theories with two or more coupled classical fields depend on the interval length on which the fields are defined, the potential in which the fields deterministically evolve, and the relative stiffness of the fields themselves. The latter is of particular importance in that physical applications will generally require different relative stiffnesses, but the effect of varying field stiffnesses has not heretofore been studied. In this paper, we explore the complete phase diagram of escape times as they depend on the various problem paramet","authors_text":"D. L. Stein, Lan Gong","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-06-28T00:33:41Z","title":"Noisy Classical Field Theories with Two Coupled Fields: Dependence of Escape Rates on Relative Field Stiffnesses"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.5545","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":"sha256:0df09e023d704db3d3f9923ea02e457b816ec7a41f1574b0d15d174795c82179","target":"record","created_at":"2026-05-18T02:01:30Z","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":"d9d0c6b4fd9930f7600469ae9219c2f6a900bd5c091f1bc18b7f0c9ef8029828","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-06-28T00:33:41Z","title_canon_sha256":"fa3b5e48493f0c624868b0db51fbfdbf384b13a65c019a33976d1acd7a0b5027"},"schema_version":"1.0","source":{"id":"1106.5545","kind":"arxiv","version":1}},"canonical_sha256":"1f01132f4024605bc111b19960add7446faf5c666d2d25fd770854a9621c569d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1f01132f4024605bc111b19960add7446faf5c666d2d25fd770854a9621c569d","first_computed_at":"2026-05-18T02:01:30.051046Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:01:30.051046Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Wo45K1AE69zLVLptX1ntTYKbbBeHIjbeHKCu+CpQUOWaBMhxRE0AJsVcpnWVWlkgNgdbsngORgb1ZY/gW8rECQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:01:30.051602Z","signed_message":"canonical_sha256_bytes"},"source_id":"1106.5545","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0df09e023d704db3d3f9923ea02e457b816ec7a41f1574b0d15d174795c82179","sha256:f6f94e19df504313898f79036f96482d68dfe97804d7c3338bc6ebaa3bc0c20a"],"state_sha256":"3b34ed813a923be2ebac51931e3360923c470e92409c0bb74bbad76767e9a9ba"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5MxmhCwFePdTnGlkgmP7tREI7BeiUVSbMbf9pjUizN18utiUKzEwUGGqvjoJbFYaUF7xNU52up/4sQ/E2MOOBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T11:30:02.656373Z","bundle_sha256":"8bc239987d6cc728c23bbc019946b640c7f27056f9d7c8fe660c5a0c9361ff5d"}}