{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:OFLWZ4PV3Z6Z5QQKOVU2IOHAS4","short_pith_number":"pith:OFLWZ4PV","schema_version":"1.0","canonical_sha256":"71576cf1f5de7d9ec20a7569a438e097257aa5c4a3f7f3ba58c7eb157f2e9ad3","source":{"kind":"arxiv","id":"1010.3101","version":1},"attestation_state":"computed","paper":{"title":"The electrostatic view on M-theory LLM geometries","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Aristomenis Donos, Joan Simon","submitted_at":"2010-10-15T09:09:06Z","abstract_excerpt":"We describe the geometry of the R x SO(3) x SO(6) x U(1) invariant half-BPS M-theory configurations considered in LLM in terms of their electrostatic variables. We discuss both regular configurations, such as AdS_4 x S^7 and AdS_7 x S^4 vacua or simple excited solutions, and singular ones such as the superstar geometries. This allows us to identify the appropriate boundary conditions describing the most general smooth and superstar-like singular configurations. We also compute their masses, matching the expected result from their microscopic interpretation, but now at finite radius of curvatur"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1010.3101","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-10-15T09:09:06Z","cross_cats_sorted":[],"title_canon_sha256":"1e86c08da53696f95613be62185849438f31ebfa09b33dde8417bf5b68a6fb34","abstract_canon_sha256":"5dd6c301b3c53be6f0ac00538d6e6575964f6d75d9a2882651c2e493cd776311"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:30:47.928051Z","signature_b64":"+Juxx0Naz7t6OM9ap5pdcrbdOhemq41VQv5QwnYINrSbC+8ee5yvvPHPIwETdjdK/1zFerKL8UdEkfFG5iGbCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"71576cf1f5de7d9ec20a7569a438e097257aa5c4a3f7f3ba58c7eb157f2e9ad3","last_reissued_at":"2026-05-18T04:30:47.927426Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:30:47.927426Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The electrostatic view on M-theory LLM geometries","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Aristomenis Donos, Joan Simon","submitted_at":"2010-10-15T09:09:06Z","abstract_excerpt":"We describe the geometry of the R x SO(3) x SO(6) x U(1) invariant half-BPS M-theory configurations considered in LLM in terms of their electrostatic variables. We discuss both regular configurations, such as AdS_4 x S^7 and AdS_7 x S^4 vacua or simple excited solutions, and singular ones such as the superstar geometries. This allows us to identify the appropriate boundary conditions describing the most general smooth and superstar-like singular configurations. We also compute their masses, matching the expected result from their microscopic interpretation, but now at finite radius of curvatur"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1010.3101","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1010.3101","created_at":"2026-05-18T04:30:47.927532+00:00"},{"alias_kind":"arxiv_version","alias_value":"1010.3101v1","created_at":"2026-05-18T04:30:47.927532+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1010.3101","created_at":"2026-05-18T04:30:47.927532+00:00"},{"alias_kind":"pith_short_12","alias_value":"OFLWZ4PV3Z6Z","created_at":"2026-05-18T12:26:12.377268+00:00"},{"alias_kind":"pith_short_16","alias_value":"OFLWZ4PV3Z6Z5QQK","created_at":"2026-05-18T12:26:12.377268+00:00"},{"alias_kind":"pith_short_8","alias_value":"OFLWZ4PV","created_at":"2026-05-18T12:26:12.377268+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/OFLWZ4PV3Z6Z5QQKOVU2IOHAS4","json":"https://pith.science/pith/OFLWZ4PV3Z6Z5QQKOVU2IOHAS4.json","graph_json":"https://pith.science/api/pith-number/OFLWZ4PV3Z6Z5QQKOVU2IOHAS4/graph.json","events_json":"https://pith.science/api/pith-number/OFLWZ4PV3Z6Z5QQKOVU2IOHAS4/events.json","paper":"https://pith.science/paper/OFLWZ4PV"},"agent_actions":{"view_html":"https://pith.science/pith/OFLWZ4PV3Z6Z5QQKOVU2IOHAS4","download_json":"https://pith.science/pith/OFLWZ4PV3Z6Z5QQKOVU2IOHAS4.json","view_paper":"https://pith.science/paper/OFLWZ4PV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1010.3101&json=true","fetch_graph":"https://pith.science/api/pith-number/OFLWZ4PV3Z6Z5QQKOVU2IOHAS4/graph.json","fetch_events":"https://pith.science/api/pith-number/OFLWZ4PV3Z6Z5QQKOVU2IOHAS4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OFLWZ4PV3Z6Z5QQKOVU2IOHAS4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OFLWZ4PV3Z6Z5QQKOVU2IOHAS4/action/storage_attestation","attest_author":"https://pith.science/pith/OFLWZ4PV3Z6Z5QQKOVU2IOHAS4/action/author_attestation","sign_citation":"https://pith.science/pith/OFLWZ4PV3Z6Z5QQKOVU2IOHAS4/action/citation_signature","submit_replication":"https://pith.science/pith/OFLWZ4PV3Z6Z5QQKOVU2IOHAS4/action/replication_record"}},"created_at":"2026-05-18T04:30:47.927532+00:00","updated_at":"2026-05-18T04:30:47.927532+00:00"}