{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:VACQF5NE5XSSRW5HI3CUPLVT5L","short_pith_number":"pith:VACQF5NE","schema_version":"1.0","canonical_sha256":"a80502f5a4ede528dba746c547aeb3eade879b657aedcc5a3ef1c07992bdcd70","source":{"kind":"arxiv","id":"1607.08160","version":1},"attestation_state":"computed","paper":{"title":"Magnetic field effects on the static quark potential at zero and finite temperature","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Andrea Rucci, Claudio Bonati, Francesco Negro, Francesco Sanfilippo, Marco Mariti, Massimo D'Elia, Michele Mesiti","submitted_at":"2016-07-27T15:52:21Z","abstract_excerpt":"We investigate the static $Q\\bar{Q}$ potential at zero and finite temperature in the presence of a constant and uniform external magnetic field $\\vec{B}$, for several values of the lattice spacing and for different orientations with respect to $\\vec{B}$. As a byproduct, we provide continuum limit extrapolated results for the string tension, the Coulomb coupling and the Sommer parameter at $T = 0$ and $B = 0$. We confirm the presence in the continuum of a $B$-induced anisotropy, regarding essentially the string tension, for which it is of the order of 15\\% at $|e| B \\sim 1~{\\rm GeV}^2$ and woul"},"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":"1607.08160","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2016-07-27T15:52:21Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"977a50f045eec7985d10cff11d6514704aac7936ad649f7e8cce0cb20c0ab476","abstract_canon_sha256":"1055cf71aad3a57058693e7ba82647a92a380330f8eb92d7a05a6fecb3ea868a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:59:20.101587Z","signature_b64":"D7wPV+7pCNz+IFyjWWOR+jo57DMoKMjMgjjtmiuC16aDgwuJM0tLJIYY3YXu0+ADLDYbXbKPG77oA+5oCphqDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a80502f5a4ede528dba746c547aeb3eade879b657aedcc5a3ef1c07992bdcd70","last_reissued_at":"2026-05-18T00:59:20.100805Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:59:20.100805Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Magnetic field effects on the static quark potential at zero and finite temperature","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Andrea Rucci, Claudio Bonati, Francesco Negro, Francesco Sanfilippo, Marco Mariti, Massimo D'Elia, Michele Mesiti","submitted_at":"2016-07-27T15:52:21Z","abstract_excerpt":"We investigate the static $Q\\bar{Q}$ potential at zero and finite temperature in the presence of a constant and uniform external magnetic field $\\vec{B}$, for several values of the lattice spacing and for different orientations with respect to $\\vec{B}$. As a byproduct, we provide continuum limit extrapolated results for the string tension, the Coulomb coupling and the Sommer parameter at $T = 0$ and $B = 0$. We confirm the presence in the continuum of a $B$-induced anisotropy, regarding essentially the string tension, for which it is of the order of 15\\% at $|e| B \\sim 1~{\\rm GeV}^2$ and woul"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1607.08160","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":"1607.08160","created_at":"2026-05-18T00:59:20.100932+00:00"},{"alias_kind":"arxiv_version","alias_value":"1607.08160v1","created_at":"2026-05-18T00:59:20.100932+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1607.08160","created_at":"2026-05-18T00:59:20.100932+00:00"},{"alias_kind":"pith_short_12","alias_value":"VACQF5NE5XSS","created_at":"2026-05-18T12:30:48.956258+00:00"},{"alias_kind":"pith_short_16","alias_value":"VACQF5NE5XSSRW5H","created_at":"2026-05-18T12:30:48.956258+00:00"},{"alias_kind":"pith_short_8","alias_value":"VACQF5NE","created_at":"2026-05-18T12:30:48.956258+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2601.18354","citing_title":"Chiral Properties of $(2\\!+\\!1)$-Flavor QCD in Magnetic Fields at Zero Temperature","ref_index":36,"is_internal_anchor":true},{"citing_arxiv_id":"2605.17438","citing_title":"Holographic entanglement entropy in the QCD phase diagram under external magnetic field","ref_index":49,"is_internal_anchor":true},{"citing_arxiv_id":"2604.15897","citing_title":"Delineating neutral and charged mesons in magnetic fields","ref_index":63,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VACQF5NE5XSSRW5HI3CUPLVT5L","json":"https://pith.science/pith/VACQF5NE5XSSRW5HI3CUPLVT5L.json","graph_json":"https://pith.science/api/pith-number/VACQF5NE5XSSRW5HI3CUPLVT5L/graph.json","events_json":"https://pith.science/api/pith-number/VACQF5NE5XSSRW5HI3CUPLVT5L/events.json","paper":"https://pith.science/paper/VACQF5NE"},"agent_actions":{"view_html":"https://pith.science/pith/VACQF5NE5XSSRW5HI3CUPLVT5L","download_json":"https://pith.science/pith/VACQF5NE5XSSRW5HI3CUPLVT5L.json","view_paper":"https://pith.science/paper/VACQF5NE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1607.08160&json=true","fetch_graph":"https://pith.science/api/pith-number/VACQF5NE5XSSRW5HI3CUPLVT5L/graph.json","fetch_events":"https://pith.science/api/pith-number/VACQF5NE5XSSRW5HI3CUPLVT5L/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VACQF5NE5XSSRW5HI3CUPLVT5L/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VACQF5NE5XSSRW5HI3CUPLVT5L/action/storage_attestation","attest_author":"https://pith.science/pith/VACQF5NE5XSSRW5HI3CUPLVT5L/action/author_attestation","sign_citation":"https://pith.science/pith/VACQF5NE5XSSRW5HI3CUPLVT5L/action/citation_signature","submit_replication":"https://pith.science/pith/VACQF5NE5XSSRW5HI3CUPLVT5L/action/replication_record"}},"created_at":"2026-05-18T00:59:20.100932+00:00","updated_at":"2026-05-18T00:59:20.100932+00:00"}