{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:6PTSCJV34KESEW3I7VIKGJIC2K","short_pith_number":"pith:6PTSCJV3","canonical_record":{"source":{"id":"1704.03191","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-04-11T08:24:18Z","cross_cats_sorted":[],"title_canon_sha256":"77ea6d457b46795168f900307c89129fcb87581cff42fd359c9b3ddc8782e583","abstract_canon_sha256":"70385e43621a65572a76bd3fd3a8482565208347134b47b2ddb14f9cc83388b9"},"schema_version":"1.0"},"canonical_sha256":"f3e72126bbe289225b68fd50a32502d2a1be5d8651dbe6bcf5321c5ce6cfada9","source":{"kind":"arxiv","id":"1704.03191","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1704.03191","created_at":"2026-05-18T00:24:17Z"},{"alias_kind":"arxiv_version","alias_value":"1704.03191v3","created_at":"2026-05-18T00:24:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.03191","created_at":"2026-05-18T00:24:17Z"},{"alias_kind":"pith_short_12","alias_value":"6PTSCJV34KES","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_16","alias_value":"6PTSCJV34KESEW3I","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_8","alias_value":"6PTSCJV3","created_at":"2026-05-18T12:31:03Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:6PTSCJV34KESEW3I7VIKGJIC2K","target":"record","payload":{"canonical_record":{"source":{"id":"1704.03191","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-04-11T08:24:18Z","cross_cats_sorted":[],"title_canon_sha256":"77ea6d457b46795168f900307c89129fcb87581cff42fd359c9b3ddc8782e583","abstract_canon_sha256":"70385e43621a65572a76bd3fd3a8482565208347134b47b2ddb14f9cc83388b9"},"schema_version":"1.0"},"canonical_sha256":"f3e72126bbe289225b68fd50a32502d2a1be5d8651dbe6bcf5321c5ce6cfada9","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:24:17.723237Z","signature_b64":"6qGqm61L3aYR8K3mrvPn4BCX4QAAEWvta5UsnSk7gLQ08MY0WfYKgOvzZz3L3TcLjP2Z9/48oeHYFEKoG9pgCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f3e72126bbe289225b68fd50a32502d2a1be5d8651dbe6bcf5321c5ce6cfada9","last_reissued_at":"2026-05-18T00:24:17.722748Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:24:17.722748Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1704.03191","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:24:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"k5Q2inKvdsHnZ3fdLwkGT1bIsOYbmuRj+DeLv2s0Kv7awEUoVNNwzGSy+oISui6BADCy5qTV9q8VZWpYh1fwBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-29T02:20:34.982097Z"},"content_sha256":"119032985eec53ab8051e81e2501867540203b12500b6c3185fbca376071feff","schema_version":"1.0","event_id":"sha256:119032985eec53ab8051e81e2501867540203b12500b6c3185fbca376071feff"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:6PTSCJV34KESEW3I7VIKGJIC2K","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Gluon Spectrum in Quark-Gluon Plasma under Strong Magnetic Fields","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Daisuke Satow, Koichi Hattori","submitted_at":"2017-04-11T08:24:18Z","abstract_excerpt":"We obtain the general expression of the gluon propagator at finite temperature ($T$) and in a magnetic field ($B$), for the case that the four transverse tensor structures appear in the gluon self-energy. By using this expression and a specific form of the one-loop gluon self-energy in the lowest Landau level approximation, we analyze the gluon spectrum in the strong magnetic field limit. As a result, we find that there exist two collective excitations of which the energies are of the order of $p\\sim gT$ with $g$ being the coupling constant. One of the two excitations enjoys properties quite d"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.03191","kind":"arxiv","version":3},"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":"2026-05-18T00:24:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+P9NGmmBxWK79SwRkwY2vfdakJ2aJxHKFxG5WL0MU2wFVkfmO1vVPvd3yFv/ltwwGpmJPH4ASePUA8iZuA92Bw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-29T02:20:34.982452Z"},"content_sha256":"5ef19863289112e9c32d0bee0531f9f6d3739b78b2ae4515d87d3c56dc13616e","schema_version":"1.0","event_id":"sha256:5ef19863289112e9c32d0bee0531f9f6d3739b78b2ae4515d87d3c56dc13616e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6PTSCJV34KESEW3I7VIKGJIC2K/bundle.json","state_url":"https://pith.science/pith/6PTSCJV34KESEW3I7VIKGJIC2K/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6PTSCJV34KESEW3I7VIKGJIC2K/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":"2026-06-29T02:20:34Z","links":{"resolver":"https://pith.science/pith/6PTSCJV34KESEW3I7VIKGJIC2K","bundle":"https://pith.science/pith/6PTSCJV34KESEW3I7VIKGJIC2K/bundle.json","state":"https://pith.science/pith/6PTSCJV34KESEW3I7VIKGJIC2K/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6PTSCJV34KESEW3I7VIKGJIC2K/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:6PTSCJV34KESEW3I7VIKGJIC2K","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":"70385e43621a65572a76bd3fd3a8482565208347134b47b2ddb14f9cc83388b9","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-04-11T08:24:18Z","title_canon_sha256":"77ea6d457b46795168f900307c89129fcb87581cff42fd359c9b3ddc8782e583"},"schema_version":"1.0","source":{"id":"1704.03191","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1704.03191","created_at":"2026-05-18T00:24:17Z"},{"alias_kind":"arxiv_version","alias_value":"1704.03191v3","created_at":"2026-05-18T00:24:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.03191","created_at":"2026-05-18T00:24:17Z"},{"alias_kind":"pith_short_12","alias_value":"6PTSCJV34KES","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_16","alias_value":"6PTSCJV34KESEW3I","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_8","alias_value":"6PTSCJV3","created_at":"2026-05-18T12:31:03Z"}],"graph_snapshots":[{"event_id":"sha256:5ef19863289112e9c32d0bee0531f9f6d3739b78b2ae4515d87d3c56dc13616e","target":"graph","created_at":"2026-05-18T00:24:17Z","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 obtain the general expression of the gluon propagator at finite temperature ($T$) and in a magnetic field ($B$), for the case that the four transverse tensor structures appear in the gluon self-energy. By using this expression and a specific form of the one-loop gluon self-energy in the lowest Landau level approximation, we analyze the gluon spectrum in the strong magnetic field limit. As a result, we find that there exist two collective excitations of which the energies are of the order of $p\\sim gT$ with $g$ being the coupling constant. One of the two excitations enjoys properties quite d","authors_text":"Daisuke Satow, Koichi Hattori","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-04-11T08:24:18Z","title":"Gluon Spectrum in Quark-Gluon Plasma under Strong Magnetic Fields"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.03191","kind":"arxiv","version":3},"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":"sha256:119032985eec53ab8051e81e2501867540203b12500b6c3185fbca376071feff","target":"record","created_at":"2026-05-18T00:24:17Z","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":"70385e43621a65572a76bd3fd3a8482565208347134b47b2ddb14f9cc83388b9","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-04-11T08:24:18Z","title_canon_sha256":"77ea6d457b46795168f900307c89129fcb87581cff42fd359c9b3ddc8782e583"},"schema_version":"1.0","source":{"id":"1704.03191","kind":"arxiv","version":3}},"canonical_sha256":"f3e72126bbe289225b68fd50a32502d2a1be5d8651dbe6bcf5321c5ce6cfada9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f3e72126bbe289225b68fd50a32502d2a1be5d8651dbe6bcf5321c5ce6cfada9","first_computed_at":"2026-05-18T00:24:17.722748Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:24:17.722748Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"6qGqm61L3aYR8K3mrvPn4BCX4QAAEWvta5UsnSk7gLQ08MY0WfYKgOvzZz3L3TcLjP2Z9/48oeHYFEKoG9pgCg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:24:17.723237Z","signed_message":"canonical_sha256_bytes"},"source_id":"1704.03191","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:119032985eec53ab8051e81e2501867540203b12500b6c3185fbca376071feff","sha256:5ef19863289112e9c32d0bee0531f9f6d3739b78b2ae4515d87d3c56dc13616e"],"state_sha256":"1a3fed4c6096cbef7a1de1f14accfe22ef5a65780dbc440ee7f71cf7d89cf76d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RIjsam/SHpJS4F+uGbSiqAUmCp7Z+24b7GWmYT7QBb39IMJxdWKxZsP9MnSFLlhXfLK4HmmVEC6Wht5dRX2BBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-29T02:20:34.984241Z","bundle_sha256":"0ba543eb7997d984a495d9bc57f0d06d92b69a7ab33548b9910f091a464aba09"}}