{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:X25WGCBT352EAVPXLWI6XSQF3D","short_pith_number":"pith:X25WGCBT","schema_version":"1.0","canonical_sha256":"bebb630833df744055f75d91ebca05d8ceb466e3f3ee39656954391dd5650e90","source":{"kind":"arxiv","id":"hep-ph/0503231","version":3},"attestation_state":"computed","paper":{"title":"Sleptonium at the linear collider and the slepton co-next-to-lightest supersymmetric particle scenario in gauge mediated symmetry breaking models","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Nicola Fabiano, Orlando Panella","submitted_at":"2005-03-23T10:20:00Z","abstract_excerpt":"We discuss the possibility of formation and subsequent detection of a supersymmetric bound state composed of a slepton--antislepton pair at the next linear collider. The Green function method is used within a non-relativistic approximation to estimate the threshold production cross-section of the $2P$ bound state. The parameter space of Gauge Mediated Symmetry Breaking (GMSB) models allow a particular scenario in which a charged slepton ($\\widetilde{e}_R, \\widetilde{\\mu}_R$ or $\\widetilde{\\tau}_1$) is the NLSP. Within this scenario the produced $2P$ bound-state decays, through a dipole transit"},"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-ph/0503231","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2005-03-23T10:20:00Z","cross_cats_sorted":[],"title_canon_sha256":"fd1ebd0be8d19e05230d781c0dc47cccd7eb7815c851ba3ebb21890e0ed447a8","abstract_canon_sha256":"4c230cc92dad041475cd45cd51b9c566ec3fbfb78368a234b19d4473fd024740"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:36:20.032761Z","signature_b64":"SuL8ndwHerKxC7r7FFICOO4fLqlobKIJ31qR4cSCE5VIuojNBy5HgXPdjQ948y+WxekJ5J19rdxQbT8xxiF2CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bebb630833df744055f75d91ebca05d8ceb466e3f3ee39656954391dd5650e90","last_reissued_at":"2026-05-18T02:36:20.032162Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:36:20.032162Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Sleptonium at the linear collider and the slepton co-next-to-lightest supersymmetric particle scenario in gauge mediated symmetry breaking models","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Nicola Fabiano, Orlando Panella","submitted_at":"2005-03-23T10:20:00Z","abstract_excerpt":"We discuss the possibility of formation and subsequent detection of a supersymmetric bound state composed of a slepton--antislepton pair at the next linear collider. The Green function method is used within a non-relativistic approximation to estimate the threshold production cross-section of the $2P$ bound state. The parameter space of Gauge Mediated Symmetry Breaking (GMSB) models allow a particular scenario in which a charged slepton ($\\widetilde{e}_R, \\widetilde{\\mu}_R$ or $\\widetilde{\\tau}_1$) is the NLSP. Within this scenario the produced $2P$ bound-state decays, through a dipole transit"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0503231","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":""},"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-ph/0503231","created_at":"2026-05-18T02:36:20.032247+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0503231v3","created_at":"2026-05-18T02:36:20.032247+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0503231","created_at":"2026-05-18T02:36:20.032247+00:00"},{"alias_kind":"pith_short_12","alias_value":"X25WGCBT352E","created_at":"2026-05-18T12:25:53.939244+00:00"},{"alias_kind":"pith_short_16","alias_value":"X25WGCBT352EAVPX","created_at":"2026-05-18T12:25:53.939244+00:00"},{"alias_kind":"pith_short_8","alias_value":"X25WGCBT","created_at":"2026-05-18T12:25:53.939244+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/X25WGCBT352EAVPXLWI6XSQF3D","json":"https://pith.science/pith/X25WGCBT352EAVPXLWI6XSQF3D.json","graph_json":"https://pith.science/api/pith-number/X25WGCBT352EAVPXLWI6XSQF3D/graph.json","events_json":"https://pith.science/api/pith-number/X25WGCBT352EAVPXLWI6XSQF3D/events.json","paper":"https://pith.science/paper/X25WGCBT"},"agent_actions":{"view_html":"https://pith.science/pith/X25WGCBT352EAVPXLWI6XSQF3D","download_json":"https://pith.science/pith/X25WGCBT352EAVPXLWI6XSQF3D.json","view_paper":"https://pith.science/paper/X25WGCBT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0503231&json=true","fetch_graph":"https://pith.science/api/pith-number/X25WGCBT352EAVPXLWI6XSQF3D/graph.json","fetch_events":"https://pith.science/api/pith-number/X25WGCBT352EAVPXLWI6XSQF3D/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/X25WGCBT352EAVPXLWI6XSQF3D/action/timestamp_anchor","attest_storage":"https://pith.science/pith/X25WGCBT352EAVPXLWI6XSQF3D/action/storage_attestation","attest_author":"https://pith.science/pith/X25WGCBT352EAVPXLWI6XSQF3D/action/author_attestation","sign_citation":"https://pith.science/pith/X25WGCBT352EAVPXLWI6XSQF3D/action/citation_signature","submit_replication":"https://pith.science/pith/X25WGCBT352EAVPXLWI6XSQF3D/action/replication_record"}},"created_at":"2026-05-18T02:36:20.032247+00:00","updated_at":"2026-05-18T02:36:20.032247+00:00"}