{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:J7SNZ7USBR5BYN7GDX6QRQUPPN","short_pith_number":"pith:J7SNZ7US","schema_version":"1.0","canonical_sha256":"4fe4dcfe920c7a1c37e61dfd08c28f7b673f4d15066452c958218f82a9556eed","source":{"kind":"arxiv","id":"1510.06405","version":2},"attestation_state":"computed","paper":{"title":"Long-Lived, Colour-Triplet Scalars from Unnaturalness","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Andrew Spray, James Barnard, Peter Cox, Tony Gherghetta","submitted_at":"2015-10-21T20:09:18Z","abstract_excerpt":"Long-lived, colour-triplet scalars are a generic prediction of unnatural, or split, composite Higgs models where the spontaneous global-symmetry breaking scale $f \\gtrsim 10$ TeV and an unbroken $SU(5)$ symmetry is preserved. Since the triplet scalars are pseudo Nambu-Goldstone bosons they are split from the much heavier composite-sector resonances and are the lightest exotic, coloured states. This makes them ideal to search for at colliders. Due to discrete symmetries the triplet scalar decays via a dimension-six term and given the large suppression scale $f$ is often metastable. We show that"},"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":"1510.06405","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-10-21T20:09:18Z","cross_cats_sorted":[],"title_canon_sha256":"b64ef359345bcd9ea0731aa8bf82e7e62c45af3e2bf093bc3a96acc3724aaa39","abstract_canon_sha256":"363f6dd1241cc176b4abb7d4e10d5c92ab59a50647367f6b66d27757a4f1c30f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:19:44.109003Z","signature_b64":"o60PBWy5VxL4CWdzOw95uJhVXC57fvkdSJrrDlSOWQuLMVedGV6Fp3KFtqwi71GAd4OgF88ZoI+UaQ//AOaTDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4fe4dcfe920c7a1c37e61dfd08c28f7b673f4d15066452c958218f82a9556eed","last_reissued_at":"2026-05-18T01:19:44.108527Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:19:44.108527Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Long-Lived, Colour-Triplet Scalars from Unnaturalness","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Andrew Spray, James Barnard, Peter Cox, Tony Gherghetta","submitted_at":"2015-10-21T20:09:18Z","abstract_excerpt":"Long-lived, colour-triplet scalars are a generic prediction of unnatural, or split, composite Higgs models where the spontaneous global-symmetry breaking scale $f \\gtrsim 10$ TeV and an unbroken $SU(5)$ symmetry is preserved. Since the triplet scalars are pseudo Nambu-Goldstone bosons they are split from the much heavier composite-sector resonances and are the lightest exotic, coloured states. This makes them ideal to search for at colliders. Due to discrete symmetries the triplet scalar decays via a dimension-six term and given the large suppression scale $f$ is often metastable. We show that"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1510.06405","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":""},"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":"1510.06405","created_at":"2026-05-18T01:19:44.108604+00:00"},{"alias_kind":"arxiv_version","alias_value":"1510.06405v2","created_at":"2026-05-18T01:19:44.108604+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1510.06405","created_at":"2026-05-18T01:19:44.108604+00:00"},{"alias_kind":"pith_short_12","alias_value":"J7SNZ7USBR5B","created_at":"2026-05-18T12:29:27.538025+00:00"},{"alias_kind":"pith_short_16","alias_value":"J7SNZ7USBR5BYN7G","created_at":"2026-05-18T12:29:27.538025+00:00"},{"alias_kind":"pith_short_8","alias_value":"J7SNZ7US","created_at":"2026-05-18T12:29:27.538025+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.24126","citing_title":"Resonant Enhancement for the transfer of baryon number from a CP-violating hidden sector","ref_index":27,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/J7SNZ7USBR5BYN7GDX6QRQUPPN","json":"https://pith.science/pith/J7SNZ7USBR5BYN7GDX6QRQUPPN.json","graph_json":"https://pith.science/api/pith-number/J7SNZ7USBR5BYN7GDX6QRQUPPN/graph.json","events_json":"https://pith.science/api/pith-number/J7SNZ7USBR5BYN7GDX6QRQUPPN/events.json","paper":"https://pith.science/paper/J7SNZ7US"},"agent_actions":{"view_html":"https://pith.science/pith/J7SNZ7USBR5BYN7GDX6QRQUPPN","download_json":"https://pith.science/pith/J7SNZ7USBR5BYN7GDX6QRQUPPN.json","view_paper":"https://pith.science/paper/J7SNZ7US","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1510.06405&json=true","fetch_graph":"https://pith.science/api/pith-number/J7SNZ7USBR5BYN7GDX6QRQUPPN/graph.json","fetch_events":"https://pith.science/api/pith-number/J7SNZ7USBR5BYN7GDX6QRQUPPN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/J7SNZ7USBR5BYN7GDX6QRQUPPN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/J7SNZ7USBR5BYN7GDX6QRQUPPN/action/storage_attestation","attest_author":"https://pith.science/pith/J7SNZ7USBR5BYN7GDX6QRQUPPN/action/author_attestation","sign_citation":"https://pith.science/pith/J7SNZ7USBR5BYN7GDX6QRQUPPN/action/citation_signature","submit_replication":"https://pith.science/pith/J7SNZ7USBR5BYN7GDX6QRQUPPN/action/replication_record"}},"created_at":"2026-05-18T01:19:44.108604+00:00","updated_at":"2026-05-18T01:19:44.108604+00:00"}