{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:2CIWVCN2JPGGWFCWD6YEBBM734","short_pith_number":"pith:2CIWVCN2","schema_version":"1.0","canonical_sha256":"d0916a89ba4bcc6b14561fb040859fdf1ac08166109f593d20332c6b85390691","source":{"kind":"arxiv","id":"1207.1303","version":2},"attestation_state":"computed","paper":{"title":"Parton distributions with LHC data","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alberto Guffanti, Christopher S.Deans, Jose I.Latorre, Juan Rojo, Luigi Del Debbio, Maria Ubiali, Nathan P.Hartland, Richard D. Ball, Stefano Carrazza, Stefano Forte, Valerio Bertone","submitted_at":"2012-07-05T17:23:49Z","abstract_excerpt":"We present the first determination of parton distributions of the nucleon at NLO and NNLO based on a global data set which includes LHC data: NNPDF2.3. Our data set includes, besides the deep inelastic, Drell-Yan, gauge boson production and jet data already used in previous global PDF determinations, all the relevant LHC data for which experimental systematic uncertainties are currently available: ATLAS and LHCb W and Z lepton rapidity distributions from the 2010 run, CMS W electron asymmetry data from the 2011 run, and ATLAS inclusive jet cross-sections from the 2010 run. We introduce an impr"},"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":"1207.1303","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-07-05T17:23:49Z","cross_cats_sorted":[],"title_canon_sha256":"948f6598504dee8f923a61e7d7fbd6ad6d814840682fba6ac2533cb639512a40","abstract_canon_sha256":"4a09bbbd666b542a5f7a86a1f26c83f2c6007bcafd5fdba783894e561615a2d0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:56:34.256595Z","signature_b64":"lr3/DsdSYbPMmzi3Mu5tDSk1zwWmUiJ1+KaLT5Vm8Tj9/08IjiAvGcX6Jtj91cA0QEY/RhbMF4sbRLLoSw4oAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d0916a89ba4bcc6b14561fb040859fdf1ac08166109f593d20332c6b85390691","last_reissued_at":"2026-05-18T01:56:34.255949Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:56:34.255949Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Parton distributions with LHC data","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alberto Guffanti, Christopher S.Deans, Jose I.Latorre, Juan Rojo, Luigi Del Debbio, Maria Ubiali, Nathan P.Hartland, Richard D. Ball, Stefano Carrazza, Stefano Forte, Valerio Bertone","submitted_at":"2012-07-05T17:23:49Z","abstract_excerpt":"We present the first determination of parton distributions of the nucleon at NLO and NNLO based on a global data set which includes LHC data: NNPDF2.3. Our data set includes, besides the deep inelastic, Drell-Yan, gauge boson production and jet data already used in previous global PDF determinations, all the relevant LHC data for which experimental systematic uncertainties are currently available: ATLAS and LHCb W and Z lepton rapidity distributions from the 2010 run, CMS W electron asymmetry data from the 2011 run, and ATLAS inclusive jet cross-sections from the 2010 run. We introduce an impr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1207.1303","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":"1207.1303","created_at":"2026-05-18T01:56:34.256041+00:00"},{"alias_kind":"arxiv_version","alias_value":"1207.1303v2","created_at":"2026-05-18T01:56:34.256041+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1207.1303","created_at":"2026-05-18T01:56:34.256041+00:00"},{"alias_kind":"pith_short_12","alias_value":"2CIWVCN2JPGG","created_at":"2026-05-18T12:26:50.516681+00:00"},{"alias_kind":"pith_short_16","alias_value":"2CIWVCN2JPGGWFCW","created_at":"2026-05-18T12:26:50.516681+00:00"},{"alias_kind":"pith_short_8","alias_value":"2CIWVCN2","created_at":"2026-05-18T12:26:50.516681+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":29,"internal_anchor_count":22,"sample":[{"citing_arxiv_id":"2510.02857","citing_title":"Search for a resonance decaying into a scalar particle and a Higgs boson in the final state with two bottom quarks and two photons with 199 fb$^{-1}$ of data collected at $\\sqrt{s}$=13 and 13.6 TeV wi","ref_index":31,"is_internal_anchor":true},{"citing_arxiv_id":"2503.05463","citing_title":"Search for Higgs boson exotic decays into Lorentz-boosted light bosons in the four-$\\tau$ final state at $\\sqrt{s}=13$ TeV with the ATLAS detector","ref_index":61,"is_internal_anchor":true},{"citing_arxiv_id":"2503.17461","citing_title":"Electroweak diboson production in association with a high-mass dijet system in semileptonic final states from $pp$ collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector","ref_index":64,"is_internal_anchor":true},{"citing_arxiv_id":"2504.02638","citing_title":"Characterization of nuclear breakup as a function of hard-scattering kinematics using dijets measured by ATLAS in $p$+Pb collisions","ref_index":47,"is_internal_anchor":true},{"citing_arxiv_id":"2504.02958","citing_title":"Combined effective field theory interpretation of Higgs boson, electroweak vector boson, top quark, and multi-jet measurements","ref_index":72,"is_internal_anchor":true},{"citing_arxiv_id":"2505.03724","citing_title":"Stay Positive: Neural Refinement of Sample Weights","ref_index":13,"is_internal_anchor":true},{"citing_arxiv_id":"2510.02857","citing_title":"Search for a resonance decaying into a scalar particle and a Higgs boson in the final state with two bottom quarks and two photons with 199 fb$^{-1}$ of data collected at $\\sqrt{s}$=13 and 13.6 TeV wi","ref_index":31,"is_internal_anchor":true},{"citing_arxiv_id":"2601.11780","citing_title":"Observation of a cross-section enhancement near the $t\\bar{t}$ production threshold in $\\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector","ref_index":48,"is_internal_anchor":true},{"citing_arxiv_id":"2601.11986","citing_title":"Prospects for discovering strongly decaying doubly heavy $T_{bc}$ tetraquark states at LHCb","ref_index":15,"is_internal_anchor":true},{"citing_arxiv_id":"2605.19016","citing_title":"Measurements of the Higgs boson production, fiducial and differential cross-sections in the four lepton decay channel using 164 fb$^{-1}$ of data collected at $\\sqrt{s}$ = 13.6 TeV with the ATLAS dete","ref_index":47,"is_internal_anchor":true},{"citing_arxiv_id":"2605.19144","citing_title":"Search for Higgs boson decays into two neutral scalars with unequal masses in final states with b quarks and tau leptons in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","ref_index":86,"is_internal_anchor":true},{"citing_arxiv_id":"2605.20015","citing_title":"Search for soft unclustered energy patterns containing muons in the final state in $pp$ collisions at $\\sqrt{s}$ = 13 TeV with the ATLAS detector","ref_index":53,"is_internal_anchor":true},{"citing_arxiv_id":"2509.13759","citing_title":"Measurement of the $W$-boson angular coefficients and transverse momentum in $pp$ collisions at $\\sqrt{s}=$ 13 TeV with the ATLAS detector","ref_index":38,"is_internal_anchor":true},{"citing_arxiv_id":"2509.14070","citing_title":"Observation of $W^{+}W^{-}\\gamma$ production in $pp$ collisions at $\\sqrt{s}$ = 13 TeV with the ATLAS detector and constraints on anomalous quartic gauge-boson couplings","ref_index":26,"is_internal_anchor":true},{"citing_arxiv_id":"2510.17730","citing_title":"Automated computation of spin-density matrices and quantum observables for collider physics","ref_index":135,"is_internal_anchor":true},{"citing_arxiv_id":"2511.07224","citing_title":"Bridging the divide: axion searches and axino phenomenology at colliders","ref_index":49,"is_internal_anchor":true},{"citing_arxiv_id":"2511.21240","citing_title":"Search for signatures of electroweakinos with photons, jets, and large missing transverse momentum in $\\sqrt{s}=13$ TeV pp collisions with the ATLAS detector","ref_index":43,"is_internal_anchor":true},{"citing_arxiv_id":"2511.23091","citing_title":"Measurement of the top-quark mass using decays with a $J/\\psi$ meson at $\\sqrt{s}=$13 TeV with the ATLAS detector","ref_index":34,"is_internal_anchor":true},{"citing_arxiv_id":"2601.11780","citing_title":"Observation of a cross-section enhancement near the $t\\bar{t}$ production threshold in $\\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector","ref_index":48,"is_internal_anchor":true},{"citing_arxiv_id":"2601.17119","citing_title":"NO LESS: Novel Opportunities for Light Exotic Searches at the SPS","ref_index":17,"is_internal_anchor":true},{"citing_arxiv_id":"2603.15882","citing_title":"Probing compressed triplet scalars with ISR jets and soft leptons at the LHC","ref_index":32,"is_internal_anchor":true},{"citing_arxiv_id":"2605.13819","citing_title":"Search for charginos and neutralinos with $B-L$ $R$-parity violating decays in $\\sqrt{s}=13$ TeV and $13.6$ TeV $pp$ collisions with the ATLAS detector","ref_index":66,"is_internal_anchor":true},{"citing_arxiv_id":"2604.02906","citing_title":"Probing Proton Structure via Physics-Guided Neural Networks in Holographic QCD","ref_index":56,"is_internal_anchor":false},{"citing_arxiv_id":"2604.28154","citing_title":"Mapping data sensitivities in global QCD analysis with linear response and influence functions","ref_index":22,"is_internal_anchor":false},{"citing_arxiv_id":"2605.10287","citing_title":"Phenomenology of electroweak spin-1 resonances","ref_index":54,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/2CIWVCN2JPGGWFCWD6YEBBM734","json":"https://pith.science/pith/2CIWVCN2JPGGWFCWD6YEBBM734.json","graph_json":"https://pith.science/api/pith-number/2CIWVCN2JPGGWFCWD6YEBBM734/graph.json","events_json":"https://pith.science/api/pith-number/2CIWVCN2JPGGWFCWD6YEBBM734/events.json","paper":"https://pith.science/paper/2CIWVCN2"},"agent_actions":{"view_html":"https://pith.science/pith/2CIWVCN2JPGGWFCWD6YEBBM734","download_json":"https://pith.science/pith/2CIWVCN2JPGGWFCWD6YEBBM734.json","view_paper":"https://pith.science/paper/2CIWVCN2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1207.1303&json=true","fetch_graph":"https://pith.science/api/pith-number/2CIWVCN2JPGGWFCWD6YEBBM734/graph.json","fetch_events":"https://pith.science/api/pith-number/2CIWVCN2JPGGWFCWD6YEBBM734/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2CIWVCN2JPGGWFCWD6YEBBM734/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2CIWVCN2JPGGWFCWD6YEBBM734/action/storage_attestation","attest_author":"https://pith.science/pith/2CIWVCN2JPGGWFCWD6YEBBM734/action/author_attestation","sign_citation":"https://pith.science/pith/2CIWVCN2JPGGWFCWD6YEBBM734/action/citation_signature","submit_replication":"https://pith.science/pith/2CIWVCN2JPGGWFCWD6YEBBM734/action/replication_record"}},"created_at":"2026-05-18T01:56:34.256041+00:00","updated_at":"2026-05-18T01:56:34.256041+00:00"}