{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:ZBG6KCPSYS4CGDVPLR5ZZ7AF76","short_pith_number":"pith:ZBG6KCPS","schema_version":"1.0","canonical_sha256":"c84de509f2c4b8230eaf5c7b9cfc05ffb6e452f99464989dfdf41db16c2ffec4","source":{"kind":"arxiv","id":"2407.14184","version":3},"attestation_state":"computed","paper":{"title":"From the Janis-Newman-Winicour naked singularities to Einstein-Maxwell phantom wormholes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"Changjun Gao, Jianhui Qiu","submitted_at":"2024-07-19T10:28:31Z","abstract_excerpt":"The Janis-Newman-Winicour spacetime corresponds to a static spherically symmetric solution of Einstein equations with the energy momentum tensor of a massless quintessence field. It is understood that the spacetime describes a naked singularity. The solution has two parameters, $b$ and $s$. To our knowledge, the exact physical meaning of the two parameters is still unclear. In this paper, starting from the Janis-Newman-Winicour naked singularity solution, we first obtain a wormhole solution by a complex transformation. Then let the parameter $s$ approaching infinity, we obtain the well-known e"},"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":"2407.14184","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2024-07-19T10:28:31Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"23056393d794c32a361a583a1fdea4d5904c803a4214a68cf5af52b9201c3cd8","abstract_canon_sha256":"1a51b0f7fa363b97e03f88ce68882a7797b0ed0fd054c3420a87f73063b5dd82"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:55:51.214826Z","signature_b64":"4lCkm8CJ+z9UZH5qlW+StwFRW/KzD+y1WqAIxQy2DRsDJ9R691v9kJ7qegDqiO5OQtWCb0nfhGyPILQ153lvBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c84de509f2c4b8230eaf5c7b9cfc05ffb6e452f99464989dfdf41db16c2ffec4","last_reissued_at":"2026-07-05T08:55:51.214381Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:55:51.214381Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"From the Janis-Newman-Winicour naked singularities to Einstein-Maxwell phantom wormholes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"Changjun Gao, Jianhui Qiu","submitted_at":"2024-07-19T10:28:31Z","abstract_excerpt":"The Janis-Newman-Winicour spacetime corresponds to a static spherically symmetric solution of Einstein equations with the energy momentum tensor of a massless quintessence field. It is understood that the spacetime describes a naked singularity. The solution has two parameters, $b$ and $s$. To our knowledge, the exact physical meaning of the two parameters is still unclear. In this paper, starting from the Janis-Newman-Winicour naked singularity solution, we first obtain a wormhole solution by a complex transformation. Then let the parameter $s$ approaching infinity, we obtain the well-known e"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2407.14184","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2407.14184/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2407.14184","created_at":"2026-07-05T08:55:51.214438+00:00"},{"alias_kind":"arxiv_version","alias_value":"2407.14184v3","created_at":"2026-07-05T08:55:51.214438+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2407.14184","created_at":"2026-07-05T08:55:51.214438+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZBG6KCPSYS4C","created_at":"2026-07-05T08:55:51.214438+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZBG6KCPSYS4CGDVP","created_at":"2026-07-05T08:55:51.214438+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZBG6KCPS","created_at":"2026-07-05T08:55:51.214438+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.06793","citing_title":"Sharpened Dynamical Cobordism","ref_index":82,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZBG6KCPSYS4CGDVPLR5ZZ7AF76","json":"https://pith.science/pith/ZBG6KCPSYS4CGDVPLR5ZZ7AF76.json","graph_json":"https://pith.science/api/pith-number/ZBG6KCPSYS4CGDVPLR5ZZ7AF76/graph.json","events_json":"https://pith.science/api/pith-number/ZBG6KCPSYS4CGDVPLR5ZZ7AF76/events.json","paper":"https://pith.science/paper/ZBG6KCPS"},"agent_actions":{"view_html":"https://pith.science/pith/ZBG6KCPSYS4CGDVPLR5ZZ7AF76","download_json":"https://pith.science/pith/ZBG6KCPSYS4CGDVPLR5ZZ7AF76.json","view_paper":"https://pith.science/paper/ZBG6KCPS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2407.14184&json=true","fetch_graph":"https://pith.science/api/pith-number/ZBG6KCPSYS4CGDVPLR5ZZ7AF76/graph.json","fetch_events":"https://pith.science/api/pith-number/ZBG6KCPSYS4CGDVPLR5ZZ7AF76/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZBG6KCPSYS4CGDVPLR5ZZ7AF76/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZBG6KCPSYS4CGDVPLR5ZZ7AF76/action/storage_attestation","attest_author":"https://pith.science/pith/ZBG6KCPSYS4CGDVPLR5ZZ7AF76/action/author_attestation","sign_citation":"https://pith.science/pith/ZBG6KCPSYS4CGDVPLR5ZZ7AF76/action/citation_signature","submit_replication":"https://pith.science/pith/ZBG6KCPSYS4CGDVPLR5ZZ7AF76/action/replication_record"}},"created_at":"2026-07-05T08:55:51.214438+00:00","updated_at":"2026-07-05T08:55:51.214438+00:00"}