{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1998:QO7UT5WPAGYLDFZRVEGSTBF67B","short_pith_number":"pith:QO7UT5WP","schema_version":"1.0","canonical_sha256":"83bf49f6cf01b0b19731a90d2984bef87e90f3e588364e1a7b80952bc61d0481","source":{"kind":"arxiv","id":"hep-ph/9803315","version":1},"attestation_state":"computed","paper":{"title":"The Hierarchy Problem and New Dimensions at a Millimeter","license":"","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Gia Dvali, Nima Arkani-Hamed, Savas Dimopoulos","submitted_at":"1998-03-11T23:45:15Z","abstract_excerpt":"We propose a new framework for solving the hierarchy problem which does not rely on either supersymmetry or technicolor. In this framework, the gravitational and gauge interactions become united at the weak scale, which we take as the only fundamental short distance scale in nature. The observed weakness of gravity on distances $\\gsim$ 1 mm is due to the existence of $n \\geq 2$ new compact spatial dimensions large compared to the weak scale. The Planck scale $M_{Pl} \\sim G_N^{-1/2}$ is not a fundamental scale; its enormity is simply a consequence of the large size of the new dimensions. While "},"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/9803315","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1998-03-11T23:45:15Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"1a6d5124f529b3fac116db589727edb5a2b72039f4b28343fb763dc91f9301d1","abstract_canon_sha256":"636e4ae332fce819fa5226758a4519de4a1cb8e84b06285f4096679106a2fa17"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:27:23.940688Z","signature_b64":"cqvtU2uyvFN8DCYn1VXWZMYpVIb6mO83yrx6FC8Ov+Qk1s3+dlNyXv0cWEKOoy4HsJ2q+fYbyGT93wYM6+FHCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"83bf49f6cf01b0b19731a90d2984bef87e90f3e588364e1a7b80952bc61d0481","last_reissued_at":"2026-07-04T15:27:23.939106Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:27:23.939106Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Hierarchy Problem and New Dimensions at a Millimeter","license":"","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Gia Dvali, Nima Arkani-Hamed, Savas Dimopoulos","submitted_at":"1998-03-11T23:45:15Z","abstract_excerpt":"We propose a new framework for solving the hierarchy problem which does not rely on either supersymmetry or technicolor. In this framework, the gravitational and gauge interactions become united at the weak scale, which we take as the only fundamental short distance scale in nature. The observed weakness of gravity on distances $\\gsim$ 1 mm is due to the existence of $n \\geq 2$ new compact spatial dimensions large compared to the weak scale. The Planck scale $M_{Pl} \\sim G_N^{-1/2}$ is not a fundamental scale; its enormity is simply a consequence of the large size of the new dimensions. While "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9803315","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/9803315/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-ph/9803315","created_at":"2026-07-04T15:27:23.940288+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9803315v1","created_at":"2026-07-04T15:27:23.940288+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9803315","created_at":"2026-07-04T15:27:23.940288+00:00"},{"alias_kind":"pith_short_12","alias_value":"QO7UT5WPAGYL","created_at":"2026-07-04T15:27:23.940288+00:00"},{"alias_kind":"pith_short_16","alias_value":"QO7UT5WPAGYLDFZR","created_at":"2026-07-04T15:27:23.940288+00:00"},{"alias_kind":"pith_short_8","alias_value":"QO7UT5WP","created_at":"2026-07-04T15:27:23.940288+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":44,"internal_anchor_count":29,"sample":[{"citing_arxiv_id":"2607.06081","citing_title":"Quasinormal modes of scalar perturbations in Rastall thick brane","ref_index":11,"is_internal_anchor":true},{"citing_arxiv_id":"2606.24486","citing_title":"Reinterpretation of ATLAS and CMS searches in monojet and mono-$V$ final states: prospects of limits on excited neutrinos","ref_index":4,"is_internal_anchor":true},{"citing_arxiv_id":"2606.23178","citing_title":"Signatures of gravity-mediated dark matter interaction in theories with large extra dimensions","ref_index":13,"is_internal_anchor":true},{"citing_arxiv_id":"2606.20486","citing_title":"Cosmological history after higher dimensional inflation","ref_index":2,"is_internal_anchor":true},{"citing_arxiv_id":"2606.20066","citing_title":"Quantization of Brane-Skyrmions via Physics-Informed Neural Networks","ref_index":3,"is_internal_anchor":true},{"citing_arxiv_id":"2606.19440","citing_title":"Moduli Stabilisation for ADD and the Dark Dimension Scenario","ref_index":4,"is_internal_anchor":true},{"citing_arxiv_id":"2606.05086","citing_title":"Fermionic Kaluza-Klein mode mixing in braneworlds","ref_index":1,"is_internal_anchor":true},{"citing_arxiv_id":"2606.04424","citing_title":"Real Part Emergence in Purely Imaginary Quasinormal Modes in Perturbed de Sitter Braneworlds","ref_index":5,"is_internal_anchor":true},{"citing_arxiv_id":"2606.02708","citing_title":"Supersymmetry, Large Extra Dimensions and the Gravitino Conjecture","ref_index":9,"is_internal_anchor":true},{"citing_arxiv_id":"2606.31330","citing_title":"Two-scalar-field $f(R)$ Thick Branes, Gravitational Resonances and Quasinormal Modes","ref_index":42,"is_internal_anchor":true},{"citing_arxiv_id":"2605.10476","citing_title":"Breaking Free from the Swampland of Impossible Universes through the DESI Portal","ref_index":127,"is_internal_anchor":true},{"citing_arxiv_id":"2605.25015","citing_title":"Emerging Nonlocal K\\\"{a}ll\\`{e}n-Lehmann Higgs Spectra at the LHC","ref_index":6,"is_internal_anchor":true},{"citing_arxiv_id":"2606.19839","citing_title":"Constraining ADD black holes at the LHC with $\\sqrt{s} = 14$ TeV","ref_index":9,"is_internal_anchor":true},{"citing_arxiv_id":"1907.04517","citing_title":"Extra dimension of space-time exposed by anomalies at low energy","ref_index":14,"is_internal_anchor":true},{"citing_arxiv_id":"2502.09538","citing_title":"Neutrino Masses and Phenomenology in Nnaturalness","ref_index":15,"is_internal_anchor":true},{"citing_arxiv_id":"2509.05233","citing_title":"Searching for a Dark Dimension Right-handed Neutrino in KATRIN","ref_index":3,"is_internal_anchor":true},{"citing_arxiv_id":"2512.02101","citing_title":"Do neutrinos dream in 5D? Towards a comprehensive extra-dimensional neutrino phenomenology","ref_index":7,"is_internal_anchor":true},{"citing_arxiv_id":"2601.00790","citing_title":"Dark Dimension Right-handed Neutrinos Confronted with Long-Baseline Oscillation Experiments","ref_index":2,"is_internal_anchor":true},{"citing_arxiv_id":"2605.19221","citing_title":"Thick branes and fermion localization in five-dimensional $f(T,T_G)$ gravity","ref_index":3,"is_internal_anchor":true},{"citing_arxiv_id":"2605.08642","citing_title":"Polydoxon Transformations and Scientific Reward in Physics","ref_index":6,"is_internal_anchor":true},{"citing_arxiv_id":"2506.05472","citing_title":"The Intrinsic and Extrinsic Hierarchy Problems","ref_index":13,"is_internal_anchor":true},{"citing_arxiv_id":"2510.21420","citing_title":"The Standard Model partial unification scale as a guide to new physics model building","ref_index":36,"is_internal_anchor":true},{"citing_arxiv_id":"2512.11113","citing_title":"TeV Scale Quark-Lepton Unification","ref_index":30,"is_internal_anchor":true},{"citing_arxiv_id":"2601.01527","citing_title":"Top-quark pair production in electron-positron collisions within the minimal noncommutative Standard Model","ref_index":6,"is_internal_anchor":true},{"citing_arxiv_id":"2601.18613","citing_title":"Correspondence between quasinormal modes and grey-body factors of Schwarzschild--Tangherlini black holes","ref_index":9,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QO7UT5WPAGYLDFZRVEGSTBF67B","json":"https://pith.science/pith/QO7UT5WPAGYLDFZRVEGSTBF67B.json","graph_json":"https://pith.science/api/pith-number/QO7UT5WPAGYLDFZRVEGSTBF67B/graph.json","events_json":"https://pith.science/api/pith-number/QO7UT5WPAGYLDFZRVEGSTBF67B/events.json","paper":"https://pith.science/paper/QO7UT5WP"},"agent_actions":{"view_html":"https://pith.science/pith/QO7UT5WPAGYLDFZRVEGSTBF67B","download_json":"https://pith.science/pith/QO7UT5WPAGYLDFZRVEGSTBF67B.json","view_paper":"https://pith.science/paper/QO7UT5WP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9803315&json=true","fetch_graph":"https://pith.science/api/pith-number/QO7UT5WPAGYLDFZRVEGSTBF67B/graph.json","fetch_events":"https://pith.science/api/pith-number/QO7UT5WPAGYLDFZRVEGSTBF67B/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QO7UT5WPAGYLDFZRVEGSTBF67B/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QO7UT5WPAGYLDFZRVEGSTBF67B/action/storage_attestation","attest_author":"https://pith.science/pith/QO7UT5WPAGYLDFZRVEGSTBF67B/action/author_attestation","sign_citation":"https://pith.science/pith/QO7UT5WPAGYLDFZRVEGSTBF67B/action/citation_signature","submit_replication":"https://pith.science/pith/QO7UT5WPAGYLDFZRVEGSTBF67B/action/replication_record"}},"created_at":"2026-07-04T15:27:23.940288+00:00","updated_at":"2026-07-04T15:27:23.940288+00:00"}