{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:VAWJPQYUA33TUIVORTQFUE5FWZ","short_pith_number":"pith:VAWJPQYU","canonical_record":{"source":{"id":"1301.2395","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2013-01-11T06:26:02Z","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.str-el"],"title_canon_sha256":"e604ba657bfe4a9bc9d3aa8c3afc32c49029ecc9279e891d4e485df21abf2449","abstract_canon_sha256":"53e1c6ee87778dc309c4937397fe44e10e34700b56e6d62005c4c8181c0e4645"},"schema_version":"1.0"},"canonical_sha256":"a82c97c31406f73a22ae8ce05a13a5b6708f425bd46a45c7d9a4fc0a0cf87bee","source":{"kind":"arxiv","id":"1301.2395","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1301.2395","created_at":"2026-05-18T01:52:13Z"},{"alias_kind":"arxiv_version","alias_value":"1301.2395v1","created_at":"2026-05-18T01:52:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1301.2395","created_at":"2026-05-18T01:52:13Z"},{"alias_kind":"pith_short_12","alias_value":"VAWJPQYUA33T","created_at":"2026-05-18T12:28:04Z"},{"alias_kind":"pith_short_16","alias_value":"VAWJPQYUA33TUIVO","created_at":"2026-05-18T12:28:04Z"},{"alias_kind":"pith_short_8","alias_value":"VAWJPQYU","created_at":"2026-05-18T12:28:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:VAWJPQYUA33TUIVORTQFUE5FWZ","target":"record","payload":{"canonical_record":{"source":{"id":"1301.2395","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2013-01-11T06:26:02Z","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.str-el"],"title_canon_sha256":"e604ba657bfe4a9bc9d3aa8c3afc32c49029ecc9279e891d4e485df21abf2449","abstract_canon_sha256":"53e1c6ee87778dc309c4937397fe44e10e34700b56e6d62005c4c8181c0e4645"},"schema_version":"1.0"},"canonical_sha256":"a82c97c31406f73a22ae8ce05a13a5b6708f425bd46a45c7d9a4fc0a0cf87bee","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:52:13.560092Z","signature_b64":"aOHg1oZhGDiGKOgQ0r+Vl7DZNGJ8ElH79T2V+GOoTAkxAh1FsYybyvB7rZWdEKF2iGg2kwLtGBRpuMH8D0V7CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a82c97c31406f73a22ae8ce05a13a5b6708f425bd46a45c7d9a4fc0a0cf87bee","last_reissued_at":"2026-05-18T01:52:13.559377Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:52:13.559377Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1301.2395","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":"2026-05-18T01:52:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+MvZiQvDlgTva4YClRLJII3cNUHdwWCqUadCn6XJYzjl48OZVCNmyjw+5hJFapMTswnnmu2ftMVVw82AXarOBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T00:24:52.669290Z"},"content_sha256":"fc2134ae5b71c41a63519d3a29165ba4cc9ae42a3e395ecfc9559ba6f9e780d0","schema_version":"1.0","event_id":"sha256:fc2134ae5b71c41a63519d3a29165ba4cc9ae42a3e395ecfc9559ba6f9e780d0"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:VAWJPQYUA33TUIVORTQFUE5FWZ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Perspectives of the disproportionation driven superconductivity in strongly correlated 3d compounds","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci","cond-mat.str-el"],"primary_cat":"cond-mat.supr-con","authors_text":"A.S. Moskvin","submitted_at":"2013-01-11T06:26:02Z","abstract_excerpt":"Disproportionation in 3d compounds can give rise to an unconventional electron-hole Bose liquid with a very rich phase diagram from a Bose metal, charge ordering insulator to an inhomogeneous Bose superfluid. Optimal conditions for the disproportionation driven high-T_c superconductivity are shown to realize only for several Jahn-Teller d^n configurations that permit the formation of well defined local composite bosons. These are the high-spin d^4, low-spin d^7, and d^9 configurations given the octahedral crystal field, and the d^1, high-spin d^6 configurations given the tetrahedral crystal fi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1301.2395","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":"2026-05-18T01:52:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OmGsbJImeX0F6/I+0OIeI+XwvuBxWQPbGLFaXo2tfktloz9/7aZKw+WBTHOo/vr34I2MjGXsDvwRgn7OYTyACA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T00:24:52.669987Z"},"content_sha256":"8ada3398faead7a2d98b08efa1262979b5dc2d1b588dd99e2b7f743a1cd83708","schema_version":"1.0","event_id":"sha256:8ada3398faead7a2d98b08efa1262979b5dc2d1b588dd99e2b7f743a1cd83708"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/VAWJPQYUA33TUIVORTQFUE5FWZ/bundle.json","state_url":"https://pith.science/pith/VAWJPQYUA33TUIVORTQFUE5FWZ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/VAWJPQYUA33TUIVORTQFUE5FWZ/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":"2026-06-08T00:24:52Z","links":{"resolver":"https://pith.science/pith/VAWJPQYUA33TUIVORTQFUE5FWZ","bundle":"https://pith.science/pith/VAWJPQYUA33TUIVORTQFUE5FWZ/bundle.json","state":"https://pith.science/pith/VAWJPQYUA33TUIVORTQFUE5FWZ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/VAWJPQYUA33TUIVORTQFUE5FWZ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:VAWJPQYUA33TUIVORTQFUE5FWZ","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":"53e1c6ee87778dc309c4937397fe44e10e34700b56e6d62005c4c8181c0e4645","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2013-01-11T06:26:02Z","title_canon_sha256":"e604ba657bfe4a9bc9d3aa8c3afc32c49029ecc9279e891d4e485df21abf2449"},"schema_version":"1.0","source":{"id":"1301.2395","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1301.2395","created_at":"2026-05-18T01:52:13Z"},{"alias_kind":"arxiv_version","alias_value":"1301.2395v1","created_at":"2026-05-18T01:52:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1301.2395","created_at":"2026-05-18T01:52:13Z"},{"alias_kind":"pith_short_12","alias_value":"VAWJPQYUA33T","created_at":"2026-05-18T12:28:04Z"},{"alias_kind":"pith_short_16","alias_value":"VAWJPQYUA33TUIVO","created_at":"2026-05-18T12:28:04Z"},{"alias_kind":"pith_short_8","alias_value":"VAWJPQYU","created_at":"2026-05-18T12:28:04Z"}],"graph_snapshots":[{"event_id":"sha256:8ada3398faead7a2d98b08efa1262979b5dc2d1b588dd99e2b7f743a1cd83708","target":"graph","created_at":"2026-05-18T01:52:13Z","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":"Disproportionation in 3d compounds can give rise to an unconventional electron-hole Bose liquid with a very rich phase diagram from a Bose metal, charge ordering insulator to an inhomogeneous Bose superfluid. Optimal conditions for the disproportionation driven high-T_c superconductivity are shown to realize only for several Jahn-Teller d^n configurations that permit the formation of well defined local composite bosons. These are the high-spin d^4, low-spin d^7, and d^9 configurations given the octahedral crystal field, and the d^1, high-spin d^6 configurations given the tetrahedral crystal fi","authors_text":"A.S. Moskvin","cross_cats":["cond-mat.mtrl-sci","cond-mat.str-el"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2013-01-11T06:26:02Z","title":"Perspectives of the disproportionation driven superconductivity in strongly correlated 3d compounds"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1301.2395","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:fc2134ae5b71c41a63519d3a29165ba4cc9ae42a3e395ecfc9559ba6f9e780d0","target":"record","created_at":"2026-05-18T01:52:13Z","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":"53e1c6ee87778dc309c4937397fe44e10e34700b56e6d62005c4c8181c0e4645","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2013-01-11T06:26:02Z","title_canon_sha256":"e604ba657bfe4a9bc9d3aa8c3afc32c49029ecc9279e891d4e485df21abf2449"},"schema_version":"1.0","source":{"id":"1301.2395","kind":"arxiv","version":1}},"canonical_sha256":"a82c97c31406f73a22ae8ce05a13a5b6708f425bd46a45c7d9a4fc0a0cf87bee","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a82c97c31406f73a22ae8ce05a13a5b6708f425bd46a45c7d9a4fc0a0cf87bee","first_computed_at":"2026-05-18T01:52:13.559377Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:52:13.559377Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"aOHg1oZhGDiGKOgQ0r+Vl7DZNGJ8ElH79T2V+GOoTAkxAh1FsYybyvB7rZWdEKF2iGg2kwLtGBRpuMH8D0V7CQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:52:13.560092Z","signed_message":"canonical_sha256_bytes"},"source_id":"1301.2395","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:fc2134ae5b71c41a63519d3a29165ba4cc9ae42a3e395ecfc9559ba6f9e780d0","sha256:8ada3398faead7a2d98b08efa1262979b5dc2d1b588dd99e2b7f743a1cd83708"],"state_sha256":"188aa7c1a6b93b3d2fec5ae8c0ff9296ba9e350750ea32dddc28b5dc2ef946c9"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yQhnu0u25/gsFqEdteuFIKV4qTUk6UVEc5pCtSfgMTMjaMAJWW7TVWn6lOJ1XTM7XohtnQk/SbpI4yTLOL0iDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-08T00:24:52.673384Z","bundle_sha256":"1be4ef778f841f397af9d00867e0e979d3625d9a77e4fee40a0d7b4258f4ba2a"}}