{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:CFA45ZVHNXT2DUDUWHXIJ4OKOA","short_pith_number":"pith:CFA45ZVH","schema_version":"1.0","canonical_sha256":"1141cee6a76de7a1d074b1ee84f1ca70190eb3e9e63904e323246d826a9c3a2e","source":{"kind":"arxiv","id":"hep-th/9612095","version":3},"attestation_state":"computed","paper":{"title":"Multiple Intersections of D-branes and M-branes","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"B. Janssen, E. Bergshoeff, E. Eyras, J. P. van der Schaar, M. de Roo","submitted_at":"1996-12-09T18:11:17Z","abstract_excerpt":"We give a classification of all multiple intersections of D-branes in ten dimensions and M-branes in eleven dimensions that corresponds to threshold BPS bound states. The residual supersymmetry of these composite branes is determined. By dimensional reduction composite p-branes in lower dimensions can be constructed. We emphasize in dimensions D greater or equal than two, those solutions which involve a single scalar and depend on a single harmonic function. For these extremal branes we obtain the strength of the coupling between the scalar and the gauge field. In particular we give a D-brane "},"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/9612095","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1996-12-09T18:11:17Z","cross_cats_sorted":[],"title_canon_sha256":"4f1dec61d6648b965fa5e31daa286a46781ecd99755ec4be84580d1f1f65bbfd","abstract_canon_sha256":"993e1f00da64a81d2fc634b3e1bc61ce33501ca1fd487effcd0de71bf3077120"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:02:27.043111Z","signature_b64":"fWt/IPnrh/bzVF7PvZEx5S7KAzukT1E2jHuIBxYOmdqpC81xNO0MfMZIkPxZqKeYVOG1TaMBgCrpDuMlSENlDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1141cee6a76de7a1d074b1ee84f1ca70190eb3e9e63904e323246d826a9c3a2e","last_reissued_at":"2026-07-04T16:02:27.042752Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:02:27.042752Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Multiple Intersections of D-branes and M-branes","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"B. Janssen, E. Bergshoeff, E. Eyras, J. P. van der Schaar, M. de Roo","submitted_at":"1996-12-09T18:11:17Z","abstract_excerpt":"We give a classification of all multiple intersections of D-branes in ten dimensions and M-branes in eleven dimensions that corresponds to threshold BPS bound states. The residual supersymmetry of these composite branes is determined. By dimensional reduction composite p-branes in lower dimensions can be constructed. We emphasize in dimensions D greater or equal than two, those solutions which involve a single scalar and depend on a single harmonic function. For these extremal branes we obtain the strength of the coupling between the scalar and the gauge field. In particular we give a D-brane "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9612095","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/hep-th/9612095/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/9612095","created_at":"2026-07-04T16:02:27.042807+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9612095v3","created_at":"2026-07-04T16:02:27.042807+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9612095","created_at":"2026-07-04T16:02:27.042807+00:00"},{"alias_kind":"pith_short_12","alias_value":"CFA45ZVHNXT2","created_at":"2026-07-04T16:02:27.042807+00:00"},{"alias_kind":"pith_short_16","alias_value":"CFA45ZVHNXT2DUDU","created_at":"2026-07-04T16:02:27.042807+00:00"},{"alias_kind":"pith_short_8","alias_value":"CFA45ZVH","created_at":"2026-07-04T16:02:27.042807+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2505.21623","citing_title":"New BPS States from Bosonic/Heterotic Duality","ref_index":11,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CFA45ZVHNXT2DUDUWHXIJ4OKOA","json":"https://pith.science/pith/CFA45ZVHNXT2DUDUWHXIJ4OKOA.json","graph_json":"https://pith.science/api/pith-number/CFA45ZVHNXT2DUDUWHXIJ4OKOA/graph.json","events_json":"https://pith.science/api/pith-number/CFA45ZVHNXT2DUDUWHXIJ4OKOA/events.json","paper":"https://pith.science/paper/CFA45ZVH"},"agent_actions":{"view_html":"https://pith.science/pith/CFA45ZVHNXT2DUDUWHXIJ4OKOA","download_json":"https://pith.science/pith/CFA45ZVHNXT2DUDUWHXIJ4OKOA.json","view_paper":"https://pith.science/paper/CFA45ZVH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9612095&json=true","fetch_graph":"https://pith.science/api/pith-number/CFA45ZVHNXT2DUDUWHXIJ4OKOA/graph.json","fetch_events":"https://pith.science/api/pith-number/CFA45ZVHNXT2DUDUWHXIJ4OKOA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CFA45ZVHNXT2DUDUWHXIJ4OKOA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CFA45ZVHNXT2DUDUWHXIJ4OKOA/action/storage_attestation","attest_author":"https://pith.science/pith/CFA45ZVHNXT2DUDUWHXIJ4OKOA/action/author_attestation","sign_citation":"https://pith.science/pith/CFA45ZVHNXT2DUDUWHXIJ4OKOA/action/citation_signature","submit_replication":"https://pith.science/pith/CFA45ZVHNXT2DUDUWHXIJ4OKOA/action/replication_record"}},"created_at":"2026-07-04T16:02:27.042807+00:00","updated_at":"2026-07-04T16:02:27.042807+00:00"}