{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:IHSPN7YBYFX5GGGWCFRR7AK72D","short_pith_number":"pith:IHSPN7YB","schema_version":"1.0","canonical_sha256":"41e4f6ff01c16fd318d611631f815fd0f1ec10c2822ba7daf98be7d5547e0150","source":{"kind":"arxiv","id":"2312.07655","version":1},"attestation_state":"computed","paper":{"title":"Bjorken $x$ weighted Energy-Energy Correlators from the Target Fragmentation Region to the Current Fragmentation Region","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex","nucl-ex"],"primary_cat":"hep-ph","authors_text":"Hai Tao Li, Haotian Cao, Zihao Mi","submitted_at":"2023-12-12T19:00:01Z","abstract_excerpt":"We present the complete spectrum for the Bjorken $x$ weighted Energy-Energy Correlation in the deep inelastic scattering (DIS) process, from the target fragmentation region to the current fragmentation region, in the Breit frame. The corresponding collinear and transverse momentum-dependent logarithms are resummed to all orders with the accuracy of NLL and N$^3$LL, respectively. And the results in the full region are matched with ${\\cal O}(\\alpha^2_s)$ fixed-order calculation. The final numerical predictions are presented for both EIC and CEBAF kinematics."},"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":"2312.07655","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-12-12T19:00:01Z","cross_cats_sorted":["hep-ex","nucl-ex"],"title_canon_sha256":"d25003f6c0e8a6b6c61be4e6c3eb879f84b0c98ed3855b267f94165423300005","abstract_canon_sha256":"da28c733ea7be795b61e55cd4a1dcc743cdf2faba35aaf0ccaaf3ea2c45d4b6b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:23:34.248364Z","signature_b64":"matao5bloRv8rWyflctfZ3Swz0teQxJoP9KSOZv2v20EqkHz8euMnWSsvTSvXYxRdLvcRosBVT6OvXzP8abZAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"41e4f6ff01c16fd318d611631f815fd0f1ec10c2822ba7daf98be7d5547e0150","last_reissued_at":"2026-07-05T07:23:34.247888Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:23:34.247888Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Bjorken $x$ weighted Energy-Energy Correlators from the Target Fragmentation Region to the Current Fragmentation Region","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex","nucl-ex"],"primary_cat":"hep-ph","authors_text":"Hai Tao Li, Haotian Cao, Zihao Mi","submitted_at":"2023-12-12T19:00:01Z","abstract_excerpt":"We present the complete spectrum for the Bjorken $x$ weighted Energy-Energy Correlation in the deep inelastic scattering (DIS) process, from the target fragmentation region to the current fragmentation region, in the Breit frame. The corresponding collinear and transverse momentum-dependent logarithms are resummed to all orders with the accuracy of NLL and N$^3$LL, respectively. And the results in the full region are matched with ${\\cal O}(\\alpha^2_s)$ fixed-order calculation. The final numerical predictions are presented for both EIC and CEBAF kinematics."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2312.07655","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/2312.07655/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":"2312.07655","created_at":"2026-07-05T07:23:34.247949+00:00"},{"alias_kind":"arxiv_version","alias_value":"2312.07655v1","created_at":"2026-07-05T07:23:34.247949+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2312.07655","created_at":"2026-07-05T07:23:34.247949+00:00"},{"alias_kind":"pith_short_12","alias_value":"IHSPN7YBYFX5","created_at":"2026-07-05T07:23:34.247949+00:00"},{"alias_kind":"pith_short_16","alias_value":"IHSPN7YBYFX5GGGW","created_at":"2026-07-05T07:23:34.247949+00:00"},{"alias_kind":"pith_short_8","alias_value":"IHSPN7YB","created_at":"2026-07-05T07:23:34.247949+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2509.17596","citing_title":"Energy Correlators Resolving Proton Spin","ref_index":87,"is_internal_anchor":false},{"citing_arxiv_id":"2605.15280","citing_title":"Sivers Tomography from Charge and Angle Only","ref_index":55,"is_internal_anchor":false},{"citing_arxiv_id":"2508.08516","citing_title":"Nucleon Energy Correlators as a Probe of Light-Quark Dipole Operators at the Electron-Ion Collider","ref_index":37,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/IHSPN7YBYFX5GGGWCFRR7AK72D","json":"https://pith.science/pith/IHSPN7YBYFX5GGGWCFRR7AK72D.json","graph_json":"https://pith.science/api/pith-number/IHSPN7YBYFX5GGGWCFRR7AK72D/graph.json","events_json":"https://pith.science/api/pith-number/IHSPN7YBYFX5GGGWCFRR7AK72D/events.json","paper":"https://pith.science/paper/IHSPN7YB"},"agent_actions":{"view_html":"https://pith.science/pith/IHSPN7YBYFX5GGGWCFRR7AK72D","download_json":"https://pith.science/pith/IHSPN7YBYFX5GGGWCFRR7AK72D.json","view_paper":"https://pith.science/paper/IHSPN7YB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2312.07655&json=true","fetch_graph":"https://pith.science/api/pith-number/IHSPN7YBYFX5GGGWCFRR7AK72D/graph.json","fetch_events":"https://pith.science/api/pith-number/IHSPN7YBYFX5GGGWCFRR7AK72D/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IHSPN7YBYFX5GGGWCFRR7AK72D/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IHSPN7YBYFX5GGGWCFRR7AK72D/action/storage_attestation","attest_author":"https://pith.science/pith/IHSPN7YBYFX5GGGWCFRR7AK72D/action/author_attestation","sign_citation":"https://pith.science/pith/IHSPN7YBYFX5GGGWCFRR7AK72D/action/citation_signature","submit_replication":"https://pith.science/pith/IHSPN7YBYFX5GGGWCFRR7AK72D/action/replication_record"}},"created_at":"2026-07-05T07:23:34.247949+00:00","updated_at":"2026-07-05T07:23:34.247949+00:00"}