{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:I6UETFXLWGNDAIOCGD3BB26G3T","short_pith_number":"pith:I6UETFXL","canonical_record":{"source":{"id":"1703.02170","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2017-03-07T01:25:59Z","cross_cats_sorted":[],"title_canon_sha256":"eb96724eef7425146aa87385afe32a3a92bb428111f153c16e9bf641bd18f6f9","abstract_canon_sha256":"540d5519c85149dbfc5b1c0356f790c7b09b4acc27c65a4cf9de0785107f5449"},"schema_version":"1.0"},"canonical_sha256":"47a84996ebb19a3021c230f610ebc6dcd10bae29cf6c139f8c258f9c8a0f80a8","source":{"kind":"arxiv","id":"1703.02170","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1703.02170","created_at":"2026-05-18T00:40:30Z"},{"alias_kind":"arxiv_version","alias_value":"1703.02170v2","created_at":"2026-05-18T00:40:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.02170","created_at":"2026-05-18T00:40:30Z"},{"alias_kind":"pith_short_12","alias_value":"I6UETFXLWGND","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_16","alias_value":"I6UETFXLWGNDAIOC","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_8","alias_value":"I6UETFXL","created_at":"2026-05-18T12:31:21Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:I6UETFXLWGNDAIOCGD3BB26G3T","target":"record","payload":{"canonical_record":{"source":{"id":"1703.02170","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2017-03-07T01:25:59Z","cross_cats_sorted":[],"title_canon_sha256":"eb96724eef7425146aa87385afe32a3a92bb428111f153c16e9bf641bd18f6f9","abstract_canon_sha256":"540d5519c85149dbfc5b1c0356f790c7b09b4acc27c65a4cf9de0785107f5449"},"schema_version":"1.0"},"canonical_sha256":"47a84996ebb19a3021c230f610ebc6dcd10bae29cf6c139f8c258f9c8a0f80a8","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:40:30.519090Z","signature_b64":"FcEUuwu9iztbNN9UTSU+N+Fi204se5Q1ZZb+FA2xFLqVfCTyhsbh7qmW6frGnAx3TTpDzkkAVqUDsobQP6aHDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"47a84996ebb19a3021c230f610ebc6dcd10bae29cf6c139f8c258f9c8a0f80a8","last_reissued_at":"2026-05-18T00:40:30.518696Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:40:30.518696Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1703.02170","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":"2026-05-18T00:40:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yRRASKV9AioRzsRSfY9yo4ZYYoqKZ3uQNx/ls9EwvWthLnebxEZ2G1TLhYhufW8ZDlNmLMYv8H3AnlPjyfuLAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T23:24:46.187572Z"},"content_sha256":"7d135ccc2960158e29208e42201706d909a89358d61c074c7dfa396faaa366bb","schema_version":"1.0","event_id":"sha256:7d135ccc2960158e29208e42201706d909a89358d61c074c7dfa396faaa366bb"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:I6UETFXLWGNDAIOCGD3BB26G3T","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Conservation laws, vertex corrections, and screening in Raman spectroscopy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"Andrey Chubukov, P. J. Hirschfeld, Saurabh Maiti","submitted_at":"2017-03-07T01:25:59Z","abstract_excerpt":"We present a microscopic theory for the Raman response of a clean multiband superconductor accounting for the effects of vertex corrections and long-range Coulomb interaction. The measured Raman intensity, $R(\\Omega)$, is proportional to the imaginary part of the fully renormalized particle-hole correlator with Raman form-factors $\\gamma(\\vec k)$. In a BCS superconductor, a bare Raman bubble is non-zero for any $\\gamma(\\vec k)$ and diverges at $\\Omega = 2\\Delta +0$, where $\\Delta$ is the largest gap along the Fermi surface. However, for $\\gamma(\\vec k) =$ const, the full $R(\\Omega)$ is expecte"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.02170","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":"2026-05-18T00:40:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Kq+mdaD1dK15GxE6Dk4u++vD7B0SGHfGL3PMC3IMmVz1fTFZx0GLRxgvEMyu6aLintl3lKdyrNs8WB57wud7DA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T23:24:46.187916Z"},"content_sha256":"9b116db8467ebb70806be7a17793b35204f4ba63be59d2b5e0389d9575e9ace8","schema_version":"1.0","event_id":"sha256:9b116db8467ebb70806be7a17793b35204f4ba63be59d2b5e0389d9575e9ace8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/I6UETFXLWGNDAIOCGD3BB26G3T/bundle.json","state_url":"https://pith.science/pith/I6UETFXLWGNDAIOCGD3BB26G3T/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/I6UETFXLWGNDAIOCGD3BB26G3T/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":"2026-06-02T23:24:46Z","links":{"resolver":"https://pith.science/pith/I6UETFXLWGNDAIOCGD3BB26G3T","bundle":"https://pith.science/pith/I6UETFXLWGNDAIOCGD3BB26G3T/bundle.json","state":"https://pith.science/pith/I6UETFXLWGNDAIOCGD3BB26G3T/state.json","well_known_bundle":"https://pith.science/.well-known/pith/I6UETFXLWGNDAIOCGD3BB26G3T/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:I6UETFXLWGNDAIOCGD3BB26G3T","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":"540d5519c85149dbfc5b1c0356f790c7b09b4acc27c65a4cf9de0785107f5449","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2017-03-07T01:25:59Z","title_canon_sha256":"eb96724eef7425146aa87385afe32a3a92bb428111f153c16e9bf641bd18f6f9"},"schema_version":"1.0","source":{"id":"1703.02170","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1703.02170","created_at":"2026-05-18T00:40:30Z"},{"alias_kind":"arxiv_version","alias_value":"1703.02170v2","created_at":"2026-05-18T00:40:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.02170","created_at":"2026-05-18T00:40:30Z"},{"alias_kind":"pith_short_12","alias_value":"I6UETFXLWGND","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_16","alias_value":"I6UETFXLWGNDAIOC","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_8","alias_value":"I6UETFXL","created_at":"2026-05-18T12:31:21Z"}],"graph_snapshots":[{"event_id":"sha256:9b116db8467ebb70806be7a17793b35204f4ba63be59d2b5e0389d9575e9ace8","target":"graph","created_at":"2026-05-18T00:40:30Z","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":"We present a microscopic theory for the Raman response of a clean multiband superconductor accounting for the effects of vertex corrections and long-range Coulomb interaction. The measured Raman intensity, $R(\\Omega)$, is proportional to the imaginary part of the fully renormalized particle-hole correlator with Raman form-factors $\\gamma(\\vec k)$. In a BCS superconductor, a bare Raman bubble is non-zero for any $\\gamma(\\vec k)$ and diverges at $\\Omega = 2\\Delta +0$, where $\\Delta$ is the largest gap along the Fermi surface. However, for $\\gamma(\\vec k) =$ const, the full $R(\\Omega)$ is expecte","authors_text":"Andrey Chubukov, P. J. Hirschfeld, Saurabh Maiti","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2017-03-07T01:25:59Z","title":"Conservation laws, vertex corrections, and screening in Raman spectroscopy"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.02170","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":"sha256:7d135ccc2960158e29208e42201706d909a89358d61c074c7dfa396faaa366bb","target":"record","created_at":"2026-05-18T00:40:30Z","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":"540d5519c85149dbfc5b1c0356f790c7b09b4acc27c65a4cf9de0785107f5449","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2017-03-07T01:25:59Z","title_canon_sha256":"eb96724eef7425146aa87385afe32a3a92bb428111f153c16e9bf641bd18f6f9"},"schema_version":"1.0","source":{"id":"1703.02170","kind":"arxiv","version":2}},"canonical_sha256":"47a84996ebb19a3021c230f610ebc6dcd10bae29cf6c139f8c258f9c8a0f80a8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"47a84996ebb19a3021c230f610ebc6dcd10bae29cf6c139f8c258f9c8a0f80a8","first_computed_at":"2026-05-18T00:40:30.518696Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:40:30.518696Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"FcEUuwu9iztbNN9UTSU+N+Fi204se5Q1ZZb+FA2xFLqVfCTyhsbh7qmW6frGnAx3TTpDzkkAVqUDsobQP6aHDw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:40:30.519090Z","signed_message":"canonical_sha256_bytes"},"source_id":"1703.02170","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7d135ccc2960158e29208e42201706d909a89358d61c074c7dfa396faaa366bb","sha256:9b116db8467ebb70806be7a17793b35204f4ba63be59d2b5e0389d9575e9ace8"],"state_sha256":"33988399f659f94fafd2bd225074de82c39c8dea30f65be2308239999e9e9f53"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DfsLqYUayCyXNpjyjxa7EixzGxuBVMq+N+uWjodqY8uV2nPGSrHLN3GwV3p+VnJpnwTN0noVyLoAE+NPA9KrBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T23:24:46.189878Z","bundle_sha256":"c8c3a00d1766a8632fb28f10171a8adc2cf02e629385805a5a8a72352758877a"}}