{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:OOZQHUYXH74D5HHH4DFIQGHKM2","short_pith_number":"pith:OOZQHUYX","canonical_record":{"source":{"id":"1703.00794","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2017-03-02T14:18:44Z","cross_cats_sorted":[],"title_canon_sha256":"d555d71e48d0ebfee5ee400a5898b8ccdc5069663e407f9843687342f96c95e0","abstract_canon_sha256":"5f6f1a15d5869a84b0f2f8e07c873e928b8555d77a762919e5c94b65e503585f"},"schema_version":"1.0"},"canonical_sha256":"73b303d3173ff83e9ce7e0ca8818ea66afd633c2d9445bfe11c3742f6420c310","source":{"kind":"arxiv","id":"1703.00794","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1703.00794","created_at":"2026-05-18T00:33:52Z"},{"alias_kind":"arxiv_version","alias_value":"1703.00794v2","created_at":"2026-05-18T00:33:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.00794","created_at":"2026-05-18T00:33:52Z"},{"alias_kind":"pith_short_12","alias_value":"OOZQHUYXH74D","created_at":"2026-05-18T12:31:34Z"},{"alias_kind":"pith_short_16","alias_value":"OOZQHUYXH74D5HHH","created_at":"2026-05-18T12:31:34Z"},{"alias_kind":"pith_short_8","alias_value":"OOZQHUYX","created_at":"2026-05-18T12:31:34Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:OOZQHUYXH74D5HHH4DFIQGHKM2","target":"record","payload":{"canonical_record":{"source":{"id":"1703.00794","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2017-03-02T14:18:44Z","cross_cats_sorted":[],"title_canon_sha256":"d555d71e48d0ebfee5ee400a5898b8ccdc5069663e407f9843687342f96c95e0","abstract_canon_sha256":"5f6f1a15d5869a84b0f2f8e07c873e928b8555d77a762919e5c94b65e503585f"},"schema_version":"1.0"},"canonical_sha256":"73b303d3173ff83e9ce7e0ca8818ea66afd633c2d9445bfe11c3742f6420c310","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:33:52.508245Z","signature_b64":"HTDRQmrbYRL7m2gbwztGQGlHVDc49CWOKS50Xc9+k0NEqnHeMP1n2TMMR3cjTSrsFVLiGHq46RueZNWz1zlxAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"73b303d3173ff83e9ce7e0ca8818ea66afd633c2d9445bfe11c3742f6420c310","last_reissued_at":"2026-05-18T00:33:52.507729Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:33:52.507729Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1703.00794","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":"2026-05-18T00:33:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"asa6dTkHZc5B8i1YAXbw9TtSnUg3r7gmnXYObS/KGQ10FSvdbRBR5Ct+fklPVoz3eXgwDamH9QqKhzgPqfZLAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T23:42:28.130665Z"},"content_sha256":"b40a4dc53dd8d6c466bf66b811583e3d7fc18499493879928dc8cbd27fb8851a","schema_version":"1.0","event_id":"sha256:b40a4dc53dd8d6c466bf66b811583e3d7fc18499493879928dc8cbd27fb8851a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:OOZQHUYXH74D5HHH4DFIQGHKM2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Vertical temperature-boundary of the pseudogap under the superconducting dome of the Bi2Sr2CaCu2O8+d phase-diagram","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"A. Forget, A. Sacuto, B. Loret, D. Colson, G. D. Gu, I. Paul, J. Schneeloch, M. A. Measson, M. Cazayous, M. Civelli, R. D. Zhong, S. Benhabib, S. Sakai, Y. Gallais","submitted_at":"2017-03-02T14:18:44Z","abstract_excerpt":"Combining electronic Raman scattering experiments with cellular dynamical mean field theory, we present evidence of the pseudogap in the superconducting state of various hole-doped cuprates. In Bi2Sr2CaCu2O8+d we track the superconducting pseudogap hallmark, a peak-dip feature, as a function of temperature T and doping p, well beyond the optimal one. We show that, at all temperatures under the superconducting dome, the pseudogap disappears at the doping pc, between 0.222 and 0.226, where also the normal-state pseudogap collapses at a Lifshitz transition. This demonstrates that the superconduct"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.00794","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":"2026-05-18T00:33:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"iE8IB2lt9Xz2rHlpXrFKR30y8xrjIx+3bVMNL7Io0xVPCacRhrpkcnkRvu3gwxscnjC08LU1XfDFMRKJjDTNCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T23:42:28.131218Z"},"content_sha256":"385caa52e28c20d50badcb42f4adb0ea82fbcdff4f7bdf8ef2801a6bfeb3014c","schema_version":"1.0","event_id":"sha256:385caa52e28c20d50badcb42f4adb0ea82fbcdff4f7bdf8ef2801a6bfeb3014c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/OOZQHUYXH74D5HHH4DFIQGHKM2/bundle.json","state_url":"https://pith.science/pith/OOZQHUYXH74D5HHH4DFIQGHKM2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/OOZQHUYXH74D5HHH4DFIQGHKM2/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":"2026-05-25T23:42:28Z","links":{"resolver":"https://pith.science/pith/OOZQHUYXH74D5HHH4DFIQGHKM2","bundle":"https://pith.science/pith/OOZQHUYXH74D5HHH4DFIQGHKM2/bundle.json","state":"https://pith.science/pith/OOZQHUYXH74D5HHH4DFIQGHKM2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/OOZQHUYXH74D5HHH4DFIQGHKM2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:OOZQHUYXH74D5HHH4DFIQGHKM2","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":"5f6f1a15d5869a84b0f2f8e07c873e928b8555d77a762919e5c94b65e503585f","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2017-03-02T14:18:44Z","title_canon_sha256":"d555d71e48d0ebfee5ee400a5898b8ccdc5069663e407f9843687342f96c95e0"},"schema_version":"1.0","source":{"id":"1703.00794","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1703.00794","created_at":"2026-05-18T00:33:52Z"},{"alias_kind":"arxiv_version","alias_value":"1703.00794v2","created_at":"2026-05-18T00:33:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.00794","created_at":"2026-05-18T00:33:52Z"},{"alias_kind":"pith_short_12","alias_value":"OOZQHUYXH74D","created_at":"2026-05-18T12:31:34Z"},{"alias_kind":"pith_short_16","alias_value":"OOZQHUYXH74D5HHH","created_at":"2026-05-18T12:31:34Z"},{"alias_kind":"pith_short_8","alias_value":"OOZQHUYX","created_at":"2026-05-18T12:31:34Z"}],"graph_snapshots":[{"event_id":"sha256:385caa52e28c20d50badcb42f4adb0ea82fbcdff4f7bdf8ef2801a6bfeb3014c","target":"graph","created_at":"2026-05-18T00:33:52Z","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":"Combining electronic Raman scattering experiments with cellular dynamical mean field theory, we present evidence of the pseudogap in the superconducting state of various hole-doped cuprates. In Bi2Sr2CaCu2O8+d we track the superconducting pseudogap hallmark, a peak-dip feature, as a function of temperature T and doping p, well beyond the optimal one. We show that, at all temperatures under the superconducting dome, the pseudogap disappears at the doping pc, between 0.222 and 0.226, where also the normal-state pseudogap collapses at a Lifshitz transition. This demonstrates that the superconduct","authors_text":"A. Forget, A. Sacuto, B. Loret, D. Colson, G. D. Gu, I. Paul, J. Schneeloch, M. A. Measson, M. Cazayous, M. Civelli, R. D. Zhong, S. Benhabib, S. Sakai, Y. Gallais","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2017-03-02T14:18:44Z","title":"Vertical temperature-boundary of the pseudogap under the superconducting dome of the Bi2Sr2CaCu2O8+d phase-diagram"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.00794","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:b40a4dc53dd8d6c466bf66b811583e3d7fc18499493879928dc8cbd27fb8851a","target":"record","created_at":"2026-05-18T00:33:52Z","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":"5f6f1a15d5869a84b0f2f8e07c873e928b8555d77a762919e5c94b65e503585f","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2017-03-02T14:18:44Z","title_canon_sha256":"d555d71e48d0ebfee5ee400a5898b8ccdc5069663e407f9843687342f96c95e0"},"schema_version":"1.0","source":{"id":"1703.00794","kind":"arxiv","version":2}},"canonical_sha256":"73b303d3173ff83e9ce7e0ca8818ea66afd633c2d9445bfe11c3742f6420c310","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"73b303d3173ff83e9ce7e0ca8818ea66afd633c2d9445bfe11c3742f6420c310","first_computed_at":"2026-05-18T00:33:52.507729Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:33:52.507729Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"HTDRQmrbYRL7m2gbwztGQGlHVDc49CWOKS50Xc9+k0NEqnHeMP1n2TMMR3cjTSrsFVLiGHq46RueZNWz1zlxAA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:33:52.508245Z","signed_message":"canonical_sha256_bytes"},"source_id":"1703.00794","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b40a4dc53dd8d6c466bf66b811583e3d7fc18499493879928dc8cbd27fb8851a","sha256:385caa52e28c20d50badcb42f4adb0ea82fbcdff4f7bdf8ef2801a6bfeb3014c"],"state_sha256":"e38ef2e96dabea604a72fa135586d4fd45b17dbf56b7661c7d0da9bc99dc3ead"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GdFl5vtMmEFMHwj5KTgGIHj101pGuYuk+LKyncWV0ic4ToG6aJUsn/LpCqokFTCh8e1+Tc46KU/xOvbVwm73Ag==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T23:42:28.134452Z","bundle_sha256":"5b40c188b8f3fc28352c4ba7282b68efe1b12b0c59b15223798e55a45cabd617"}}