{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1998:KPJ6WAN2RRSQYQCDB5LGEE5B7V","short_pith_number":"pith:KPJ6WAN2","schema_version":"1.0","canonical_sha256":"53d3eb01ba8c650c40430f566213a1fd6895391b6583f00d2857745ac3e7ae22","source":{"kind":"arxiv","id":"hep-ph/9804398","version":1},"attestation_state":"computed","paper":{"title":"New Dimensions at a Millimeter to a Fermi and Superstrings at a TeV","license":"","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"G. Dvali, I. Antoniadis, N. Arkani-Hamed, S. Dimopoulos","submitted_at":"1998-04-24T23:43:55Z","abstract_excerpt":"Recently, a new framework for solving the hierarchy problem has been proposed which does not rely on low energy supersymmetry or technicolor. The gravitational and gauge interactions unite at the electroweak scale, and the observed weakness of gravity at long distances is due the existence of large new spatial dimensions. In this letter, we show that this framework can be embedded in string theory. These models have a perturbative description in the context of type I string theory. The gravitational sector consists of closed strings propagating in the higher-dimensional bulk, while ordinary ma"},"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/9804398","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1998-04-24T23:43:55Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"a06dba81f1bb849d2036d1bb464b1c669ca40152c0ee1ec282631160218a8352","abstract_canon_sha256":"491044c7565649087940eb9e737b8ec50aa2611c0bdaabc21b36327c5d5cb54b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:27:24.096459Z","signature_b64":"zApePER8YRsCugSLqtyUzigbETanXik1nEP4iw7PQ+xabMtmi+JgGp7M3YzqX3nE8VMyO1WzlyxyPuTv+UigDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"53d3eb01ba8c650c40430f566213a1fd6895391b6583f00d2857745ac3e7ae22","last_reissued_at":"2026-07-04T15:27:24.094835Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:27:24.094835Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"New Dimensions at a Millimeter to a Fermi and Superstrings at a TeV","license":"","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"G. Dvali, I. Antoniadis, N. Arkani-Hamed, S. Dimopoulos","submitted_at":"1998-04-24T23:43:55Z","abstract_excerpt":"Recently, a new framework for solving the hierarchy problem has been proposed which does not rely on low energy supersymmetry or technicolor. The gravitational and gauge interactions unite at the electroweak scale, and the observed weakness of gravity at long distances is due the existence of large new spatial dimensions. In this letter, we show that this framework can be embedded in string theory. These models have a perturbative description in the context of type I string theory. The gravitational sector consists of closed strings propagating in the higher-dimensional bulk, while ordinary ma"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9804398","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/9804398/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/9804398","created_at":"2026-07-04T15:27:24.096059+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9804398v1","created_at":"2026-07-04T15:27:24.096059+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9804398","created_at":"2026-07-04T15:27:24.096059+00:00"},{"alias_kind":"pith_short_12","alias_value":"KPJ6WAN2RRSQ","created_at":"2026-07-04T15:27:24.096059+00:00"},{"alias_kind":"pith_short_16","alias_value":"KPJ6WAN2RRSQYQCD","created_at":"2026-07-04T15:27:24.096059+00:00"},{"alias_kind":"pith_short_8","alias_value":"KPJ6WAN2","created_at":"2026-07-04T15:27:24.096059+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":24,"internal_anchor_count":17,"sample":[{"citing_arxiv_id":"2607.06081","citing_title":"Quasinormal modes of scalar perturbations in Rastall thick brane","ref_index":12,"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":12,"is_internal_anchor":true},{"citing_arxiv_id":"2606.20486","citing_title":"Cosmological history after higher dimensional inflation","ref_index":3,"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":6,"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":43,"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":128,"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":8,"is_internal_anchor":true},{"citing_arxiv_id":"2502.09538","citing_title":"Neutrino Masses and Phenomenology in Nnaturalness","ref_index":16,"is_internal_anchor":true},{"citing_arxiv_id":"2509.05233","citing_title":"Searching for a Dark Dimension Right-handed Neutrino in KATRIN","ref_index":4,"is_internal_anchor":true},{"citing_arxiv_id":"2601.00790","citing_title":"Dark Dimension Right-handed Neutrinos Confronted with Long-Baseline Oscillation Experiments","ref_index":3,"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":4,"is_internal_anchor":true},{"citing_arxiv_id":"2605.08642","citing_title":"Polydoxon Transformations and Scientific Reward in Physics","ref_index":5,"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":37,"is_internal_anchor":true},{"citing_arxiv_id":"2512.16941","citing_title":"Constructing de Sitter space and Dark Matter with Dynamical Tension Strings","ref_index":42,"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":7,"is_internal_anchor":true},{"citing_arxiv_id":"2603.04101","citing_title":"Scattering of kinks in Frankensteinian potentials: Kinks as bubbles of exotic mass and phase transitions in oscillon production","ref_index":10,"is_internal_anchor":true},{"citing_arxiv_id":"2605.00252","citing_title":"Micron-sized Extra Dimensions and Primordial Black Holes: Charged, Rotating, and Memory Burdened","ref_index":5,"is_internal_anchor":true},{"citing_arxiv_id":"1106.2476","citing_title":"Modified Gravity and Cosmology","ref_index":52,"is_internal_anchor":false},{"citing_arxiv_id":"1403.7377","citing_title":"The Confrontation between General Relativity and Experiment","ref_index":16,"is_internal_anchor":false},{"citing_arxiv_id":"2604.23364","citing_title":"Spectral Butterfly Effect and Resilient Ringdown in Thick Braneworlds","ref_index":2,"is_internal_anchor":false},{"citing_arxiv_id":"2605.00749","citing_title":"Entanglement probes of gravitational Kaluza-Klein spectra: signal hierarchy and model discrimination","ref_index":5,"is_internal_anchor":false},{"citing_arxiv_id":"2605.00252","citing_title":"Micron-sized Extra Dimensions and Primordial Black Holes: Charged, Rotating, and Memory Burdened","ref_index":5,"is_internal_anchor":false},{"citing_arxiv_id":"2604.05041","citing_title":"Aspects of a Five-Dimensional $U(1)_{L_\\mu - L_\\tau}$ Model at Future Muon-Based Colliders","ref_index":65,"is_internal_anchor":false},{"citing_arxiv_id":"2604.19495","citing_title":"Search for quantum black holes in lepton+jet final states using proton-proton collisions at $\\sqrt{s}=13.6$ TeV with the ATLAS detector","ref_index":2,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KPJ6WAN2RRSQYQCDB5LGEE5B7V","json":"https://pith.science/pith/KPJ6WAN2RRSQYQCDB5LGEE5B7V.json","graph_json":"https://pith.science/api/pith-number/KPJ6WAN2RRSQYQCDB5LGEE5B7V/graph.json","events_json":"https://pith.science/api/pith-number/KPJ6WAN2RRSQYQCDB5LGEE5B7V/events.json","paper":"https://pith.science/paper/KPJ6WAN2"},"agent_actions":{"view_html":"https://pith.science/pith/KPJ6WAN2RRSQYQCDB5LGEE5B7V","download_json":"https://pith.science/pith/KPJ6WAN2RRSQYQCDB5LGEE5B7V.json","view_paper":"https://pith.science/paper/KPJ6WAN2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9804398&json=true","fetch_graph":"https://pith.science/api/pith-number/KPJ6WAN2RRSQYQCDB5LGEE5B7V/graph.json","fetch_events":"https://pith.science/api/pith-number/KPJ6WAN2RRSQYQCDB5LGEE5B7V/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KPJ6WAN2RRSQYQCDB5LGEE5B7V/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KPJ6WAN2RRSQYQCDB5LGEE5B7V/action/storage_attestation","attest_author":"https://pith.science/pith/KPJ6WAN2RRSQYQCDB5LGEE5B7V/action/author_attestation","sign_citation":"https://pith.science/pith/KPJ6WAN2RRSQYQCDB5LGEE5B7V/action/citation_signature","submit_replication":"https://pith.science/pith/KPJ6WAN2RRSQYQCDB5LGEE5B7V/action/replication_record"}},"created_at":"2026-07-04T15:27:24.096059+00:00","updated_at":"2026-07-04T15:27:24.096059+00:00"}