{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:ILRGVPK67NWVZI6I2IHV7O3DZH","short_pith_number":"pith:ILRGVPK6","schema_version":"1.0","canonical_sha256":"42e26abd5efb6d5ca3c8d20f5fbb63c9e166f54b339db01e88b54d21b08c27eb","source":{"kind":"arxiv","id":"hep-th/9603037","version":2},"attestation_state":"computed","paper":{"title":"Heterotic phase transitions and singularities of the gauge dyonic string","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"C.N. Pope, H. Lu, M.J. Duff","submitted_at":"1996-03-07T04:06:33Z","abstract_excerpt":"Heterotic strings on $R^6 \\times K3$ generically appear to undergo some interesting new phase transition at that value of the string coupling for which the one of the six-dimensional gauge field kinetic energies changes sign. An exception is the $E_8 \\times E_8$ string with equal instanton numbers in the two $E_8$'s, which admits a heterotic/heterotic self-duality. In this paper, we generalize the dyonic string solution of the six-dimensional heterotic string to include non-trivial gauge field configurations corresponding to self-dual Yang-Mills instantons in the four transverse dimensions. We"},"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":"hep-th/9603037","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1996-03-07T04:06:33Z","cross_cats_sorted":[],"title_canon_sha256":"6f750942b829c4c8dfdcad8108c89fc214e94f5ce72836fd73368424f1e6630f","abstract_canon_sha256":"063edbaeb631977d763bae32cabe3129adbd05b7ce27a01a966a18ddcd206cec"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:53:52.627611Z","signature_b64":"USsTfvKbcX+G2fwLhxdm+scMQiu99hbYm2IBqg9vw8G8uXG8qs/ArubWC3NvhB6W67JhM6bLmXnqw3vjYTIrBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"42e26abd5efb6d5ca3c8d20f5fbb63c9e166f54b339db01e88b54d21b08c27eb","last_reissued_at":"2026-07-04T15:53:52.627195Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:53:52.627195Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Heterotic phase transitions and singularities of the gauge dyonic string","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"C.N. Pope, H. Lu, M.J. Duff","submitted_at":"1996-03-07T04:06:33Z","abstract_excerpt":"Heterotic strings on $R^6 \\times K3$ generically appear to undergo some interesting new phase transition at that value of the string coupling for which the one of the six-dimensional gauge field kinetic energies changes sign. An exception is the $E_8 \\times E_8$ string with equal instanton numbers in the two $E_8$'s, which admits a heterotic/heterotic self-duality. In this paper, we generalize the dyonic string solution of the six-dimensional heterotic string to include non-trivial gauge field configurations corresponding to self-dual Yang-Mills instantons in the four transverse dimensions. We"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9603037","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/9603037/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":"hep-th/9603037","created_at":"2026-07-04T15:53:52.627260+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9603037v2","created_at":"2026-07-04T15:53:52.627260+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9603037","created_at":"2026-07-04T15:53:52.627260+00:00"},{"alias_kind":"pith_short_12","alias_value":"ILRGVPK67NWV","created_at":"2026-07-04T15:53:52.627260+00:00"},{"alias_kind":"pith_short_16","alias_value":"ILRGVPK67NWVZI6I","created_at":"2026-07-04T15:53:52.627260+00:00"},{"alias_kind":"pith_short_8","alias_value":"ILRGVPK6","created_at":"2026-07-04T15:53:52.627260+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2605.17643","citing_title":"Anomaly-Free Spectra, Unimodular Lattices and 6D R-Symmetry Gauged Supergravity","ref_index":22,"is_internal_anchor":true},{"citing_arxiv_id":"2605.17643","citing_title":"Anomaly-Free Spectra, Unimodular Lattices and 6D R-Symmetry Gauged Supergravity","ref_index":22,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ILRGVPK67NWVZI6I2IHV7O3DZH","json":"https://pith.science/pith/ILRGVPK67NWVZI6I2IHV7O3DZH.json","graph_json":"https://pith.science/api/pith-number/ILRGVPK67NWVZI6I2IHV7O3DZH/graph.json","events_json":"https://pith.science/api/pith-number/ILRGVPK67NWVZI6I2IHV7O3DZH/events.json","paper":"https://pith.science/paper/ILRGVPK6"},"agent_actions":{"view_html":"https://pith.science/pith/ILRGVPK67NWVZI6I2IHV7O3DZH","download_json":"https://pith.science/pith/ILRGVPK67NWVZI6I2IHV7O3DZH.json","view_paper":"https://pith.science/paper/ILRGVPK6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9603037&json=true","fetch_graph":"https://pith.science/api/pith-number/ILRGVPK67NWVZI6I2IHV7O3DZH/graph.json","fetch_events":"https://pith.science/api/pith-number/ILRGVPK67NWVZI6I2IHV7O3DZH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ILRGVPK67NWVZI6I2IHV7O3DZH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ILRGVPK67NWVZI6I2IHV7O3DZH/action/storage_attestation","attest_author":"https://pith.science/pith/ILRGVPK67NWVZI6I2IHV7O3DZH/action/author_attestation","sign_citation":"https://pith.science/pith/ILRGVPK67NWVZI6I2IHV7O3DZH/action/citation_signature","submit_replication":"https://pith.science/pith/ILRGVPK67NWVZI6I2IHV7O3DZH/action/replication_record"}},"created_at":"2026-07-04T15:53:52.627260+00:00","updated_at":"2026-07-04T15:53:52.627260+00:00"}