{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2005:X25WGCBT352EAVPXLWI6XSQF3D","short_pith_number":"pith:X25WGCBT","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"},"canonical_sha256":"bebb630833df744055f75d91ebca05d8ceb466e3f3ee39656954391dd5650e90","source":{"kind":"arxiv","id":"hep-ph/0503231","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0503231","created_at":"2026-05-18T02:36:20Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0503231v3","created_at":"2026-05-18T02:36:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0503231","created_at":"2026-05-18T02:36:20Z"},{"alias_kind":"pith_short_12","alias_value":"X25WGCBT352E","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_16","alias_value":"X25WGCBT352EAVPX","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_8","alias_value":"X25WGCBT","created_at":"2026-05-18T12:25:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2005:X25WGCBT352EAVPXLWI6XSQF3D","target":"record","payload":{"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"},"canonical_sha256":"bebb630833df744055f75d91ebca05d8ceb466e3f3ee39656954391dd5650e90","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"},"source_kind":"arxiv","source_id":"hep-ph/0503231","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:36:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"MhIZwHkRlKL7VIHP+kDvR44tarMUoah+1dO0bptgWgPxwDFP/M3I/zdYkkWNVG2ZIYj/+/KIz4b+zZSdW6Z+DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T22:45:03.030259Z"},"content_sha256":"18afb69e3a000a48bc5f33c1d41c332d107e14c89ff5dfc270e5216b518076d0","schema_version":"1.0","event_id":"sha256:18afb69e3a000a48bc5f33c1d41c332d107e14c89ff5dfc270e5216b518076d0"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2005:X25WGCBT352EAVPXLWI6XSQF3D","target":"graph","payload":{"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:36:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IFOCnpa+Z/kbcVtXWE3cZl0w06nYvfZbq+q75XxV3P3V54rYI3bhNLWbj4CVq806xyHjdwtOfoTcNxORuYrNBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T22:45:03.030609Z"},"content_sha256":"d5e962b00b80f1cf558c5a06b80cf76908409fda354f74df70f10d8d8823805a","schema_version":"1.0","event_id":"sha256:d5e962b00b80f1cf558c5a06b80cf76908409fda354f74df70f10d8d8823805a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/X25WGCBT352EAVPXLWI6XSQF3D/bundle.json","state_url":"https://pith.science/pith/X25WGCBT352EAVPXLWI6XSQF3D/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/X25WGCBT352EAVPXLWI6XSQF3D/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-04T22:45:03Z","links":{"resolver":"https://pith.science/pith/X25WGCBT352EAVPXLWI6XSQF3D","bundle":"https://pith.science/pith/X25WGCBT352EAVPXLWI6XSQF3D/bundle.json","state":"https://pith.science/pith/X25WGCBT352EAVPXLWI6XSQF3D/state.json","well_known_bundle":"https://pith.science/.well-known/pith/X25WGCBT352EAVPXLWI6XSQF3D/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2005:X25WGCBT352EAVPXLWI6XSQF3D","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"4c230cc92dad041475cd45cd51b9c566ec3fbfb78368a234b19d4473fd024740","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2005-03-23T10:20:00Z","title_canon_sha256":"fd1ebd0be8d19e05230d781c0dc47cccd7eb7815c851ba3ebb21890e0ed447a8"},"schema_version":"1.0","source":{"id":"hep-ph/0503231","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0503231","created_at":"2026-05-18T02:36:20Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0503231v3","created_at":"2026-05-18T02:36:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0503231","created_at":"2026-05-18T02:36:20Z"},{"alias_kind":"pith_short_12","alias_value":"X25WGCBT352E","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_16","alias_value":"X25WGCBT352EAVPX","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_8","alias_value":"X25WGCBT","created_at":"2026-05-18T12:25:53Z"}],"graph_snapshots":[{"event_id":"sha256:d5e962b00b80f1cf558c5a06b80cf76908409fda354f74df70f10d8d8823805a","target":"graph","created_at":"2026-05-18T02:36:20Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"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","authors_text":"Nicola Fabiano, Orlando Panella","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2005-03-23T10:20:00Z","title":"Sleptonium at the linear collider and the slepton co-next-to-lightest supersymmetric particle scenario in gauge mediated symmetry breaking models"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0503231","kind":"arxiv","version":3},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:18afb69e3a000a48bc5f33c1d41c332d107e14c89ff5dfc270e5216b518076d0","target":"record","created_at":"2026-05-18T02:36:20Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"4c230cc92dad041475cd45cd51b9c566ec3fbfb78368a234b19d4473fd024740","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2005-03-23T10:20:00Z","title_canon_sha256":"fd1ebd0be8d19e05230d781c0dc47cccd7eb7815c851ba3ebb21890e0ed447a8"},"schema_version":"1.0","source":{"id":"hep-ph/0503231","kind":"arxiv","version":3}},"canonical_sha256":"bebb630833df744055f75d91ebca05d8ceb466e3f3ee39656954391dd5650e90","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"bebb630833df744055f75d91ebca05d8ceb466e3f3ee39656954391dd5650e90","first_computed_at":"2026-05-18T02:36:20.032162Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:36:20.032162Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"SuL8ndwHerKxC7r7FFICOO4fLqlobKIJ31qR4cSCE5VIuojNBy5HgXPdjQ948y+WxekJ5J19rdxQbT8xxiF2CA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:36:20.032761Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/0503231","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:18afb69e3a000a48bc5f33c1d41c332d107e14c89ff5dfc270e5216b518076d0","sha256:d5e962b00b80f1cf558c5a06b80cf76908409fda354f74df70f10d8d8823805a"],"state_sha256":"e3f7e370a9952be4adc32fb8efdc0d1b2673721083e837362ae83458456d9acc"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ocpb0TYYgiaovVMH6u0MNCH4xpWeMGz6Io6sgN3hm14DUbJYHFZF8J8ZlqQx+XxJSnsAcbjKzfVcmznJ3UvVAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-04T22:45:03.032493Z","bundle_sha256":"d46fc50ca697448be24f69ad6690daca3c7bc5e22071c1a8fd3d18100b65ccfe"}}