{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:LSNZICECRNCTSUWDM7DA4N43R5","short_pith_number":"pith:LSNZICEC","canonical_record":{"source":{"id":"1711.03071","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-11-08T18:00:49Z","cross_cats_sorted":[],"title_canon_sha256":"799dc4bb5deb7328c4e6b8ae955596fe1831037805e4f768f056d26a9bd3c5c5","abstract_canon_sha256":"dcb53914e5cee202fbf9ab29fc537755d07525cf7ed7c20054b1b73e23dea05b"},"schema_version":"1.0"},"canonical_sha256":"5c9b9408828b453952c367c60e379b8f5f8e7934012342fab99d655e50ff32e8","source":{"kind":"arxiv","id":"1711.03071","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.03071","created_at":"2026-05-18T00:14:06Z"},{"alias_kind":"arxiv_version","alias_value":"1711.03071v2","created_at":"2026-05-18T00:14:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.03071","created_at":"2026-05-18T00:14:06Z"},{"alias_kind":"pith_short_12","alias_value":"LSNZICECRNCT","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_16","alias_value":"LSNZICECRNCTSUWD","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_8","alias_value":"LSNZICEC","created_at":"2026-05-18T12:31:28Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:LSNZICECRNCTSUWDM7DA4N43R5","target":"record","payload":{"canonical_record":{"source":{"id":"1711.03071","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-11-08T18:00:49Z","cross_cats_sorted":[],"title_canon_sha256":"799dc4bb5deb7328c4e6b8ae955596fe1831037805e4f768f056d26a9bd3c5c5","abstract_canon_sha256":"dcb53914e5cee202fbf9ab29fc537755d07525cf7ed7c20054b1b73e23dea05b"},"schema_version":"1.0"},"canonical_sha256":"5c9b9408828b453952c367c60e379b8f5f8e7934012342fab99d655e50ff32e8","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:14:06.580050Z","signature_b64":"XIBBIb5PZQ6raHa61wilUPgtqpStaRd+H8iquHfmY7vpnn4jqwiMIybvtcbwEe9J+swvRFeCnfoZFqYhuFUyAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5c9b9408828b453952c367c60e379b8f5f8e7934012342fab99d655e50ff32e8","last_reissued_at":"2026-05-18T00:14:06.579537Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:14:06.579537Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1711.03071","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:14:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GruTK2UDBAOA8wXduvHRFNt1GH53zkfHA76UJGWqXLIau8beuWB/mBUXjYFUfM6DCdzO663fev1saOwCM8J9AA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-01T20:20:51.669735Z"},"content_sha256":"09897a2fa914152a943e56736b315928dd61f091924ded6b4afb984fae567086","schema_version":"1.0","event_id":"sha256:09897a2fa914152a943e56736b315928dd61f091924ded6b4afb984fae567086"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:LSNZICECRNCTSUWDM7DA4N43R5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Heavy quark complex potential in a strongly magnetized hot QGP medium","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Balbeer Singh, Hiranmaya Mishra, Lata Thakur","submitted_at":"2017-11-08T18:00:49Z","abstract_excerpt":"We study the effect of a strong constant magnetic field, generated in relativistic heavy ion collisions, on the heavy quark complex potential. We work in the strong magnetic field limit with the lowest Landau level approximation. We find that the screening of the real part of the potential increases with the increase in the magnetic field. Therefore, we expect less binding of the $ Q\\bar{Q} $ pair in the presence of a strong magnetic field. The imaginary part of the potential increases in magnitude with the increase in the magnetic field, leading to an increase of the width of the quarkonium s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.03071","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:14:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"q4uZGdFB8h2WWNofaG4ELCKuhxTd5o2NdaDuWbtJpO/FcVFdYRrNDwgywWJEP+NHtEzZ1J2OIb5PprJa1nYvDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-01T20:20:51.670588Z"},"content_sha256":"beaf493856859f968c1635f801f17f8ae24555c92384bff8b16cfdb7df991422","schema_version":"1.0","event_id":"sha256:beaf493856859f968c1635f801f17f8ae24555c92384bff8b16cfdb7df991422"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LSNZICECRNCTSUWDM7DA4N43R5/bundle.json","state_url":"https://pith.science/pith/LSNZICECRNCTSUWDM7DA4N43R5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LSNZICECRNCTSUWDM7DA4N43R5/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-07-01T20:20:51Z","links":{"resolver":"https://pith.science/pith/LSNZICECRNCTSUWDM7DA4N43R5","bundle":"https://pith.science/pith/LSNZICECRNCTSUWDM7DA4N43R5/bundle.json","state":"https://pith.science/pith/LSNZICECRNCTSUWDM7DA4N43R5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LSNZICECRNCTSUWDM7DA4N43R5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:LSNZICECRNCTSUWDM7DA4N43R5","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"dcb53914e5cee202fbf9ab29fc537755d07525cf7ed7c20054b1b73e23dea05b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-11-08T18:00:49Z","title_canon_sha256":"799dc4bb5deb7328c4e6b8ae955596fe1831037805e4f768f056d26a9bd3c5c5"},"schema_version":"1.0","source":{"id":"1711.03071","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.03071","created_at":"2026-05-18T00:14:06Z"},{"alias_kind":"arxiv_version","alias_value":"1711.03071v2","created_at":"2026-05-18T00:14:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.03071","created_at":"2026-05-18T00:14:06Z"},{"alias_kind":"pith_short_12","alias_value":"LSNZICECRNCT","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_16","alias_value":"LSNZICECRNCTSUWD","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_8","alias_value":"LSNZICEC","created_at":"2026-05-18T12:31:28Z"}],"graph_snapshots":[{"event_id":"sha256:beaf493856859f968c1635f801f17f8ae24555c92384bff8b16cfdb7df991422","target":"graph","created_at":"2026-05-18T00:14:06Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We study the effect of a strong constant magnetic field, generated in relativistic heavy ion collisions, on the heavy quark complex potential. We work in the strong magnetic field limit with the lowest Landau level approximation. We find that the screening of the real part of the potential increases with the increase in the magnetic field. Therefore, we expect less binding of the $ Q\\bar{Q} $ pair in the presence of a strong magnetic field. The imaginary part of the potential increases in magnitude with the increase in the magnetic field, leading to an increase of the width of the quarkonium s","authors_text":"Balbeer Singh, Hiranmaya Mishra, Lata Thakur","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-11-08T18:00:49Z","title":"Heavy quark complex potential in a strongly magnetized hot QGP medium"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.03071","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:09897a2fa914152a943e56736b315928dd61f091924ded6b4afb984fae567086","target":"record","created_at":"2026-05-18T00:14:06Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"dcb53914e5cee202fbf9ab29fc537755d07525cf7ed7c20054b1b73e23dea05b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-11-08T18:00:49Z","title_canon_sha256":"799dc4bb5deb7328c4e6b8ae955596fe1831037805e4f768f056d26a9bd3c5c5"},"schema_version":"1.0","source":{"id":"1711.03071","kind":"arxiv","version":2}},"canonical_sha256":"5c9b9408828b453952c367c60e379b8f5f8e7934012342fab99d655e50ff32e8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5c9b9408828b453952c367c60e379b8f5f8e7934012342fab99d655e50ff32e8","first_computed_at":"2026-05-18T00:14:06.579537Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:14:06.579537Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"XIBBIb5PZQ6raHa61wilUPgtqpStaRd+H8iquHfmY7vpnn4jqwiMIybvtcbwEe9J+swvRFeCnfoZFqYhuFUyAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:14:06.580050Z","signed_message":"canonical_sha256_bytes"},"source_id":"1711.03071","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:09897a2fa914152a943e56736b315928dd61f091924ded6b4afb984fae567086","sha256:beaf493856859f968c1635f801f17f8ae24555c92384bff8b16cfdb7df991422"],"state_sha256":"75b0bbaf1ec4a07bc8bc427cfd3a46986aca5d0fa6188c72e33fab94be5907cf"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mT7jCKhn6I7xq/OJuMj3mmriaYpa/VOFL+4/BU9dOoy14Shl/9EevAL35Xjyzg/X8suxCgpQLxETF+UKGIzIAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-01T20:20:51.675257Z","bundle_sha256":"bc8f048970c2baad8cb70bc40ceb97e2455cb91dd650347afee74031f3311331"}}