{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1997:2LLPB74T2X4OOG245EEWSMYBAA","short_pith_number":"pith:2LLPB74T","schema_version":"1.0","canonical_sha256":"d2d6f0ff93d5f8e71b5ce9096933010014023dc000683e4f1487487f95d2601e","source":{"kind":"arxiv","id":"hep-th/9702006","version":2},"attestation_state":"computed","paper":{"title":"Bound States of Type I' D-particles and Enhanced Gauge Symmetry","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"David A. Lowe","submitted_at":"1997-01-31T23:03:41Z","abstract_excerpt":"Duality between the E_8 x E_8 heterotic string and Type I' theory predicts a tower of D(irichlet)-particle bound states corresponding to perturbative heterotic string states. In the limit of infinite Type I' coupling, some of these bound states become massless, giving rise to enhanced E_8 x E_8 gauge symmetry. By taking a different infinite coupling limit, one can recover the E_8 x E_8 gauge bosons of M-theory, compactified on S^1/Z_2. In this paper we use the matrix model description of the D-particle dynamics to study these bound states. We find results consistent with the chain of dualities"},"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/9702006","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1997-01-31T23:03:41Z","cross_cats_sorted":[],"title_canon_sha256":"0a28060407a43cb3f21ff7e0bc8f0aaf3a6876cc6feb3dfb0a6943311471a0ee","abstract_canon_sha256":"91a9ed5f3c5e7ac8f1cf4108dabc99bd9fae4512fc09d32a1c02540a4f952e82"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:05:23.280881Z","signature_b64":"QmqFr/CI1T0zl2cUhjBBppf/cliksDSqvSW7dDPxycwF4Wm4mg6b/IU8o/UBeNjky1E+27g3TRygNwuALBtuAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d2d6f0ff93d5f8e71b5ce9096933010014023dc000683e4f1487487f95d2601e","last_reissued_at":"2026-07-04T16:05:23.280487Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:05:23.280487Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Bound States of Type I' D-particles and Enhanced Gauge Symmetry","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"David A. Lowe","submitted_at":"1997-01-31T23:03:41Z","abstract_excerpt":"Duality between the E_8 x E_8 heterotic string and Type I' theory predicts a tower of D(irichlet)-particle bound states corresponding to perturbative heterotic string states. In the limit of infinite Type I' coupling, some of these bound states become massless, giving rise to enhanced E_8 x E_8 gauge symmetry. By taking a different infinite coupling limit, one can recover the E_8 x E_8 gauge bosons of M-theory, compactified on S^1/Z_2. In this paper we use the matrix model description of the D-particle dynamics to study these bound states. We find results consistent with the chain of dualities"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9702006","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/9702006/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/9702006","created_at":"2026-07-04T16:05:23.280547+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9702006v2","created_at":"2026-07-04T16:05:23.280547+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9702006","created_at":"2026-07-04T16:05:23.280547+00:00"},{"alias_kind":"pith_short_12","alias_value":"2LLPB74T2X4O","created_at":"2026-07-04T16:05:23.280547+00:00"},{"alias_kind":"pith_short_16","alias_value":"2LLPB74T2X4OOG24","created_at":"2026-07-04T16:05:23.280547+00:00"},{"alias_kind":"pith_short_8","alias_value":"2LLPB74T","created_at":"2026-07-04T16:05:23.280547+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/2LLPB74T2X4OOG245EEWSMYBAA","json":"https://pith.science/pith/2LLPB74T2X4OOG245EEWSMYBAA.json","graph_json":"https://pith.science/api/pith-number/2LLPB74T2X4OOG245EEWSMYBAA/graph.json","events_json":"https://pith.science/api/pith-number/2LLPB74T2X4OOG245EEWSMYBAA/events.json","paper":"https://pith.science/paper/2LLPB74T"},"agent_actions":{"view_html":"https://pith.science/pith/2LLPB74T2X4OOG245EEWSMYBAA","download_json":"https://pith.science/pith/2LLPB74T2X4OOG245EEWSMYBAA.json","view_paper":"https://pith.science/paper/2LLPB74T","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9702006&json=true","fetch_graph":"https://pith.science/api/pith-number/2LLPB74T2X4OOG245EEWSMYBAA/graph.json","fetch_events":"https://pith.science/api/pith-number/2LLPB74T2X4OOG245EEWSMYBAA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2LLPB74T2X4OOG245EEWSMYBAA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2LLPB74T2X4OOG245EEWSMYBAA/action/storage_attestation","attest_author":"https://pith.science/pith/2LLPB74T2X4OOG245EEWSMYBAA/action/author_attestation","sign_citation":"https://pith.science/pith/2LLPB74T2X4OOG245EEWSMYBAA/action/citation_signature","submit_replication":"https://pith.science/pith/2LLPB74T2X4OOG245EEWSMYBAA/action/replication_record"}},"created_at":"2026-07-04T16:05:23.280547+00:00","updated_at":"2026-07-04T16:05:23.280547+00:00"}