{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2009:3KQJ3HOBMCSLEYWM3XK2EZKRGF","short_pith_number":"pith:3KQJ3HOB","canonical_record":{"source":{"id":"0912.3531","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2009-12-17T21:02:24Z","cross_cats_sorted":["cond-mat.quant-gas","quant-ph"],"title_canon_sha256":"8c52c32eb2707a75f512753b27c18c2612821e871a5ec411cc09161555d1caa7","abstract_canon_sha256":"102310f1c2ec3cd1eac87f09d11f310b82a465b1b08c8894a3e75895a1bec333"},"schema_version":"1.0"},"canonical_sha256":"daa09d9dc160a4b262ccddd5a265513173703491254482a8212c969b3bf61f6f","source":{"kind":"arxiv","id":"0912.3531","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0912.3531","created_at":"2026-05-18T04:39:59Z"},{"alias_kind":"arxiv_version","alias_value":"0912.3531v4","created_at":"2026-05-18T04:39:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0912.3531","created_at":"2026-05-18T04:39:59Z"},{"alias_kind":"pith_short_12","alias_value":"3KQJ3HOBMCSL","created_at":"2026-05-18T12:25:58Z"},{"alias_kind":"pith_short_16","alias_value":"3KQJ3HOBMCSLEYWM","created_at":"2026-05-18T12:25:58Z"},{"alias_kind":"pith_short_8","alias_value":"3KQJ3HOB","created_at":"2026-05-18T12:25:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2009:3KQJ3HOBMCSLEYWM3XK2EZKRGF","target":"record","payload":{"canonical_record":{"source":{"id":"0912.3531","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2009-12-17T21:02:24Z","cross_cats_sorted":["cond-mat.quant-gas","quant-ph"],"title_canon_sha256":"8c52c32eb2707a75f512753b27c18c2612821e871a5ec411cc09161555d1caa7","abstract_canon_sha256":"102310f1c2ec3cd1eac87f09d11f310b82a465b1b08c8894a3e75895a1bec333"},"schema_version":"1.0"},"canonical_sha256":"daa09d9dc160a4b262ccddd5a265513173703491254482a8212c969b3bf61f6f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:39:59.392924Z","signature_b64":"5QdFp7XzjLd6hCJyxqjkSyj+z31AfcHFnlWOw1M7e6UoU5n4KfdzoNi936nvibb8GGnoddKQkKgKkAssI+eZBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"daa09d9dc160a4b262ccddd5a265513173703491254482a8212c969b3bf61f6f","last_reissued_at":"2026-05-18T04:39:59.392412Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:39:59.392412Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"0912.3531","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:39:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"MtY2uiijoRMFstT6pz1x74UR/i+ev/PJU0bdpRTWPTQxRchwZDA9pACSbZILsu1IhN6Y5B1zY4BES6yXaHucBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T19:54:00.631752Z"},"content_sha256":"48325f4f8150c7ec0b58ede01a3cdb17e5ea108a71743f387ab3ba031477d48d","schema_version":"1.0","event_id":"sha256:48325f4f8150c7ec0b58ede01a3cdb17e5ea108a71743f387ab3ba031477d48d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2009:3KQJ3HOBMCSLEYWM3XK2EZKRGF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Universality in dissipative Landau-Zener transitions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","quant-ph"],"primary_cat":"cond-mat.other","authors_text":"Adilet Imambekov, Karyn Le Hur, Peter P. Orth","submitted_at":"2009-12-17T21:02:24Z","abstract_excerpt":"We introduce a random variable approach to investigate the dynamics of a dissipative two-state system. Based on an exact functional integral description, our method reformulates the problem as that of the time evolution of a quantum state vector subject to a Hamiltonian containing random noise fields. This numerically exact, non-perturbative formalism is particularly well suited in the context of time-dependent Hamiltonians, both at zero and finite temperature. As an important example, we consider the renowned Landau-Zener problem in the presence of an Ohmic environment with a large cutoff fre"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0912.3531","kind":"arxiv","version":4},"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":"2026-05-18T04:39:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"iWQ3qqzCNGe7lUj52WQMmCDw+hPICA5yw1h7YtDRyMJLElT6PTVLfRr8gHq1+v9GkrlDCjAaanmToFaNhqF7Dg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T19:54:00.632125Z"},"content_sha256":"b3af31aadde70e81729267dfe836abddf723882e47d44fe76817c4ae71e255a1","schema_version":"1.0","event_id":"sha256:b3af31aadde70e81729267dfe836abddf723882e47d44fe76817c4ae71e255a1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3KQJ3HOBMCSLEYWM3XK2EZKRGF/bundle.json","state_url":"https://pith.science/pith/3KQJ3HOBMCSLEYWM3XK2EZKRGF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3KQJ3HOBMCSLEYWM3XK2EZKRGF/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":"2026-06-06T19:54:00Z","links":{"resolver":"https://pith.science/pith/3KQJ3HOBMCSLEYWM3XK2EZKRGF","bundle":"https://pith.science/pith/3KQJ3HOBMCSLEYWM3XK2EZKRGF/bundle.json","state":"https://pith.science/pith/3KQJ3HOBMCSLEYWM3XK2EZKRGF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3KQJ3HOBMCSLEYWM3XK2EZKRGF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2009:3KQJ3HOBMCSLEYWM3XK2EZKRGF","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":"102310f1c2ec3cd1eac87f09d11f310b82a465b1b08c8894a3e75895a1bec333","cross_cats_sorted":["cond-mat.quant-gas","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2009-12-17T21:02:24Z","title_canon_sha256":"8c52c32eb2707a75f512753b27c18c2612821e871a5ec411cc09161555d1caa7"},"schema_version":"1.0","source":{"id":"0912.3531","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0912.3531","created_at":"2026-05-18T04:39:59Z"},{"alias_kind":"arxiv_version","alias_value":"0912.3531v4","created_at":"2026-05-18T04:39:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0912.3531","created_at":"2026-05-18T04:39:59Z"},{"alias_kind":"pith_short_12","alias_value":"3KQJ3HOBMCSL","created_at":"2026-05-18T12:25:58Z"},{"alias_kind":"pith_short_16","alias_value":"3KQJ3HOBMCSLEYWM","created_at":"2026-05-18T12:25:58Z"},{"alias_kind":"pith_short_8","alias_value":"3KQJ3HOB","created_at":"2026-05-18T12:25:58Z"}],"graph_snapshots":[{"event_id":"sha256:b3af31aadde70e81729267dfe836abddf723882e47d44fe76817c4ae71e255a1","target":"graph","created_at":"2026-05-18T04:39:59Z","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 introduce a random variable approach to investigate the dynamics of a dissipative two-state system. Based on an exact functional integral description, our method reformulates the problem as that of the time evolution of a quantum state vector subject to a Hamiltonian containing random noise fields. This numerically exact, non-perturbative formalism is particularly well suited in the context of time-dependent Hamiltonians, both at zero and finite temperature. As an important example, we consider the renowned Landau-Zener problem in the presence of an Ohmic environment with a large cutoff fre","authors_text":"Adilet Imambekov, Karyn Le Hur, Peter P. Orth","cross_cats":["cond-mat.quant-gas","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2009-12-17T21:02:24Z","title":"Universality in dissipative Landau-Zener transitions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0912.3531","kind":"arxiv","version":4},"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":"sha256:48325f4f8150c7ec0b58ede01a3cdb17e5ea108a71743f387ab3ba031477d48d","target":"record","created_at":"2026-05-18T04:39:59Z","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":"102310f1c2ec3cd1eac87f09d11f310b82a465b1b08c8894a3e75895a1bec333","cross_cats_sorted":["cond-mat.quant-gas","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2009-12-17T21:02:24Z","title_canon_sha256":"8c52c32eb2707a75f512753b27c18c2612821e871a5ec411cc09161555d1caa7"},"schema_version":"1.0","source":{"id":"0912.3531","kind":"arxiv","version":4}},"canonical_sha256":"daa09d9dc160a4b262ccddd5a265513173703491254482a8212c969b3bf61f6f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"daa09d9dc160a4b262ccddd5a265513173703491254482a8212c969b3bf61f6f","first_computed_at":"2026-05-18T04:39:59.392412Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:39:59.392412Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"5QdFp7XzjLd6hCJyxqjkSyj+z31AfcHFnlWOw1M7e6UoU5n4KfdzoNi936nvibb8GGnoddKQkKgKkAssI+eZBA==","signature_status":"signed_v1","signed_at":"2026-05-18T04:39:59.392924Z","signed_message":"canonical_sha256_bytes"},"source_id":"0912.3531","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:48325f4f8150c7ec0b58ede01a3cdb17e5ea108a71743f387ab3ba031477d48d","sha256:b3af31aadde70e81729267dfe836abddf723882e47d44fe76817c4ae71e255a1"],"state_sha256":"3d2f73fbd252ff0a8b396424744c2a4ac3944487bf5fc369b17ae5c00ef7a82c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rBxJ8f+dSeB9pCeDGNZvLG8pJ61b2MvQXcaA21XFUA8PB7G/yfPdrzN63npSKOk+fCK9liOHKdUhojDX5q6eDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-06T19:54:00.634780Z","bundle_sha256":"9adfed54e9b4979b5cd659c71b6e0ac18112c59b7c8a2bc1dbd062ad394e9d0d"}}