{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:HKID2JIEPP5P2QBCJU4NFMVTFP","short_pith_number":"pith:HKID2JIE","canonical_record":{"source":{"id":"1311.3978","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-11-15T21:01:03Z","cross_cats_sorted":[],"title_canon_sha256":"d8ffad944e30b1628db554282e340e8f349134344f1e0ac03e91c4bb8f831edd","abstract_canon_sha256":"af32b875999fb0098adbf917d3ca3d1ff122426252f071398dd535007014b054"},"schema_version":"1.0"},"canonical_sha256":"3a903d25047bfafd40224d38d2b2b32bca2738918b11848c783e72ab51e1f491","source":{"kind":"arxiv","id":"1311.3978","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1311.3978","created_at":"2026-05-18T03:06:54Z"},{"alias_kind":"arxiv_version","alias_value":"1311.3978v1","created_at":"2026-05-18T03:06:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.3978","created_at":"2026-05-18T03:06:54Z"},{"alias_kind":"pith_short_12","alias_value":"HKID2JIEPP5P","created_at":"2026-05-18T12:27:46Z"},{"alias_kind":"pith_short_16","alias_value":"HKID2JIEPP5P2QBC","created_at":"2026-05-18T12:27:46Z"},{"alias_kind":"pith_short_8","alias_value":"HKID2JIE","created_at":"2026-05-18T12:27:46Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:HKID2JIEPP5P2QBCJU4NFMVTFP","target":"record","payload":{"canonical_record":{"source":{"id":"1311.3978","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-11-15T21:01:03Z","cross_cats_sorted":[],"title_canon_sha256":"d8ffad944e30b1628db554282e340e8f349134344f1e0ac03e91c4bb8f831edd","abstract_canon_sha256":"af32b875999fb0098adbf917d3ca3d1ff122426252f071398dd535007014b054"},"schema_version":"1.0"},"canonical_sha256":"3a903d25047bfafd40224d38d2b2b32bca2738918b11848c783e72ab51e1f491","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:06:54.040462Z","signature_b64":"vBXF1MqJYeyYItdIZSj/xKwPFZUiVKkeiy3fDUgCznBea9GEMIXeabosk4OBuTmOm3gbxOif5cTSP1tU1vckAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3a903d25047bfafd40224d38d2b2b32bca2738918b11848c783e72ab51e1f491","last_reissued_at":"2026-05-18T03:06:54.039875Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:06:54.039875Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1311.3978","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":"2026-05-18T03:06:54Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"X0LWdGkgVPR68LBg0GDtv+E6UqUUoS9fbUUPRRa4mTxatwtAk7+eUGfY2JQ278bq//xB997Q0uNIq+C/YnQrBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T07:03:45.110525Z"},"content_sha256":"ee542f2b9a1eccb0edee4d4ad0888fa347253396375144392c78078e2ad9b26a","schema_version":"1.0","event_id":"sha256:ee542f2b9a1eccb0edee4d4ad0888fa347253396375144392c78078e2ad9b26a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:HKID2JIEPP5P2QBCJU4NFMVTFP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Emergence of Molecular Chirality by Vibrational Raman Scattering","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Afshin Shafiee, Farhad Taher Ghahramani","submitted_at":"2013-11-15T21:01:03Z","abstract_excerpt":"In this study, we apply the monitoring master equation describing decoherence of internal states to an optically active molecule prepared in a coherent superposition of nondegenerate internal states interacting with thermal photons at low temperatures. We use vibrational Raman scattering theory up to the first chiral-sensitive contribution, i.e., the mixed electric-magnetic interaction, to obtain scattering amplitudes in terms of molecular polarizability tensors. The resulting density matrix is used to obtain elastic decoherence rates."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.3978","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":"2026-05-18T03:06:54Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"stvGY6MuHV4dN1N7VLHXpiFfiLPfVp7Qa5nLb2sWdNV9RzAXVcsL1Ueum6FgCmilperpMwhtB/zK58fUIDRgDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T07:03:45.111229Z"},"content_sha256":"173b74e2b030585baa0ba90ec71035a73e7719cfee4c1f163c7a82b535b864d9","schema_version":"1.0","event_id":"sha256:173b74e2b030585baa0ba90ec71035a73e7719cfee4c1f163c7a82b535b864d9"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HKID2JIEPP5P2QBCJU4NFMVTFP/bundle.json","state_url":"https://pith.science/pith/HKID2JIEPP5P2QBCJU4NFMVTFP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HKID2JIEPP5P2QBCJU4NFMVTFP/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":"2026-05-25T07:03:45Z","links":{"resolver":"https://pith.science/pith/HKID2JIEPP5P2QBCJU4NFMVTFP","bundle":"https://pith.science/pith/HKID2JIEPP5P2QBCJU4NFMVTFP/bundle.json","state":"https://pith.science/pith/HKID2JIEPP5P2QBCJU4NFMVTFP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HKID2JIEPP5P2QBCJU4NFMVTFP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:HKID2JIEPP5P2QBCJU4NFMVTFP","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":"af32b875999fb0098adbf917d3ca3d1ff122426252f071398dd535007014b054","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-11-15T21:01:03Z","title_canon_sha256":"d8ffad944e30b1628db554282e340e8f349134344f1e0ac03e91c4bb8f831edd"},"schema_version":"1.0","source":{"id":"1311.3978","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1311.3978","created_at":"2026-05-18T03:06:54Z"},{"alias_kind":"arxiv_version","alias_value":"1311.3978v1","created_at":"2026-05-18T03:06:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.3978","created_at":"2026-05-18T03:06:54Z"},{"alias_kind":"pith_short_12","alias_value":"HKID2JIEPP5P","created_at":"2026-05-18T12:27:46Z"},{"alias_kind":"pith_short_16","alias_value":"HKID2JIEPP5P2QBC","created_at":"2026-05-18T12:27:46Z"},{"alias_kind":"pith_short_8","alias_value":"HKID2JIE","created_at":"2026-05-18T12:27:46Z"}],"graph_snapshots":[{"event_id":"sha256:173b74e2b030585baa0ba90ec71035a73e7719cfee4c1f163c7a82b535b864d9","target":"graph","created_at":"2026-05-18T03:06:54Z","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 this study, we apply the monitoring master equation describing decoherence of internal states to an optically active molecule prepared in a coherent superposition of nondegenerate internal states interacting with thermal photons at low temperatures. We use vibrational Raman scattering theory up to the first chiral-sensitive contribution, i.e., the mixed electric-magnetic interaction, to obtain scattering amplitudes in terms of molecular polarizability tensors. The resulting density matrix is used to obtain elastic decoherence rates.","authors_text":"Afshin Shafiee, Farhad Taher Ghahramani","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-11-15T21:01:03Z","title":"Emergence of Molecular Chirality by Vibrational Raman Scattering"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.3978","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:ee542f2b9a1eccb0edee4d4ad0888fa347253396375144392c78078e2ad9b26a","target":"record","created_at":"2026-05-18T03:06:54Z","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":"af32b875999fb0098adbf917d3ca3d1ff122426252f071398dd535007014b054","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-11-15T21:01:03Z","title_canon_sha256":"d8ffad944e30b1628db554282e340e8f349134344f1e0ac03e91c4bb8f831edd"},"schema_version":"1.0","source":{"id":"1311.3978","kind":"arxiv","version":1}},"canonical_sha256":"3a903d25047bfafd40224d38d2b2b32bca2738918b11848c783e72ab51e1f491","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3a903d25047bfafd40224d38d2b2b32bca2738918b11848c783e72ab51e1f491","first_computed_at":"2026-05-18T03:06:54.039875Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:06:54.039875Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"vBXF1MqJYeyYItdIZSj/xKwPFZUiVKkeiy3fDUgCznBea9GEMIXeabosk4OBuTmOm3gbxOif5cTSP1tU1vckAg==","signature_status":"signed_v1","signed_at":"2026-05-18T03:06:54.040462Z","signed_message":"canonical_sha256_bytes"},"source_id":"1311.3978","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ee542f2b9a1eccb0edee4d4ad0888fa347253396375144392c78078e2ad9b26a","sha256:173b74e2b030585baa0ba90ec71035a73e7719cfee4c1f163c7a82b535b864d9"],"state_sha256":"fdd8c6a0208d94f817f63e5b4f04b3ef8ec6080841d1816f452bd00f8011f15d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cEG5Lv2lqLKlXUDIjde1mdoVvY/zwEZ3k0hVqK0FmHpAJYPTWrkbpLoIyOSd+kJrqRGAI5N69L0GZdemBSX6Cg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T07:03:45.115203Z","bundle_sha256":"9367bf8d77889006a39a3f689c6744a364d8fa6e733ca19e2038c6120a2969b8"}}