{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:LPFZOSBPVEVFN2JC5IJIAKEHHR","short_pith_number":"pith:LPFZOSBP","schema_version":"1.0","canonical_sha256":"5bcb97482fa92a56e922ea128028873c7421c90821b330f851d6312a509a7c64","source":{"kind":"arxiv","id":"1704.03447","version":1},"attestation_state":"computed","paper":{"title":"Higgsplosion: Solving the Hierarchy Problem via rapid decays of heavy states into multiple Higgs bosons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Michael Spannowsky, Valentin V. Khoze","submitted_at":"2017-04-11T17:50:59Z","abstract_excerpt":"We introduce and discuss two inter-related mechanisms operative in the electroweak sector of the Standard Model at high energies. Higgsplosion, the first mechanism, occurs at some critical energy in the 25 to 10^3 TeV range, and leads to an exponentially growing decay rate of highly energetic particles into multiple Higgs bosons. We argue that this a well-controlled non-perturbative phenomenon in the Higgs-sector which involves the final state Higgs multiplicities n in the regime n \\lambda >> 1 where \\lambda is the Higgs self-coupling. If this mechanism is realised in nature, the cross-section"},"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":"1704.03447","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-04-11T17:50:59Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"6a43aa0fe60c9438261aa6f08d652c4e3c267a3382907fd852a33cc696698ccf","abstract_canon_sha256":"b09053d8db0508e3ecdda1846f009c0f5d3092548e06914adc952f070608666f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:30:28.355392Z","signature_b64":"qjBMOIYz+h+pwZTtWFNtzVa+sdL7Wdj0DeXAOk/PvqEDCjwvBqMQKsiZ7AX9DLlM3Xo0YlE5v+huwNOYXQflCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5bcb97482fa92a56e922ea128028873c7421c90821b330f851d6312a509a7c64","last_reissued_at":"2026-05-18T00:30:28.354819Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:30:28.354819Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Higgsplosion: Solving the Hierarchy Problem via rapid decays of heavy states into multiple Higgs bosons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Michael Spannowsky, Valentin V. Khoze","submitted_at":"2017-04-11T17:50:59Z","abstract_excerpt":"We introduce and discuss two inter-related mechanisms operative in the electroweak sector of the Standard Model at high energies. Higgsplosion, the first mechanism, occurs at some critical energy in the 25 to 10^3 TeV range, and leads to an exponentially growing decay rate of highly energetic particles into multiple Higgs bosons. We argue that this a well-controlled non-perturbative phenomenon in the Higgs-sector which involves the final state Higgs multiplicities n in the regime n \\lambda >> 1 where \\lambda is the Higgs self-coupling. If this mechanism is realised in nature, the cross-section"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.03447","kind":"arxiv","version":1},"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":"1704.03447","created_at":"2026-05-18T00:30:28.354891+00:00"},{"alias_kind":"arxiv_version","alias_value":"1704.03447v1","created_at":"2026-05-18T00:30:28.354891+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.03447","created_at":"2026-05-18T00:30:28.354891+00:00"},{"alias_kind":"pith_short_12","alias_value":"LPFZOSBPVEVF","created_at":"2026-05-18T12:31:28.150371+00:00"},{"alias_kind":"pith_short_16","alias_value":"LPFZOSBPVEVFN2JC","created_at":"2026-05-18T12:31:28.150371+00:00"},{"alias_kind":"pith_short_8","alias_value":"LPFZOSBP","created_at":"2026-05-18T12:31:28.150371+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.25015","citing_title":"Emerging Nonlocal K\\\"{a}ll\\`{e}n-Lehmann Higgs Spectra at the LHC","ref_index":18,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LPFZOSBPVEVFN2JC5IJIAKEHHR","json":"https://pith.science/pith/LPFZOSBPVEVFN2JC5IJIAKEHHR.json","graph_json":"https://pith.science/api/pith-number/LPFZOSBPVEVFN2JC5IJIAKEHHR/graph.json","events_json":"https://pith.science/api/pith-number/LPFZOSBPVEVFN2JC5IJIAKEHHR/events.json","paper":"https://pith.science/paper/LPFZOSBP"},"agent_actions":{"view_html":"https://pith.science/pith/LPFZOSBPVEVFN2JC5IJIAKEHHR","download_json":"https://pith.science/pith/LPFZOSBPVEVFN2JC5IJIAKEHHR.json","view_paper":"https://pith.science/paper/LPFZOSBP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1704.03447&json=true","fetch_graph":"https://pith.science/api/pith-number/LPFZOSBPVEVFN2JC5IJIAKEHHR/graph.json","fetch_events":"https://pith.science/api/pith-number/LPFZOSBPVEVFN2JC5IJIAKEHHR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LPFZOSBPVEVFN2JC5IJIAKEHHR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LPFZOSBPVEVFN2JC5IJIAKEHHR/action/storage_attestation","attest_author":"https://pith.science/pith/LPFZOSBPVEVFN2JC5IJIAKEHHR/action/author_attestation","sign_citation":"https://pith.science/pith/LPFZOSBPVEVFN2JC5IJIAKEHHR/action/citation_signature","submit_replication":"https://pith.science/pith/LPFZOSBPVEVFN2JC5IJIAKEHHR/action/replication_record"}},"created_at":"2026-05-18T00:30:28.354891+00:00","updated_at":"2026-05-18T00:30:28.354891+00:00"}