{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:S6NZQZ3SUNPPWIVM25DFTHGRS6","short_pith_number":"pith:S6NZQZ3S","canonical_record":{"source":{"id":"1312.0895","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-12-03T18:19:43Z","cross_cats_sorted":[],"title_canon_sha256":"f50892492da4c630c40bffd349d31c28cddf183589a3d3d146b468cdd1bec9ef","abstract_canon_sha256":"39cefeb63484e10b2c3b114677a35aa00dae51adee364f096d319fe45b536356"},"schema_version":"1.0"},"canonical_sha256":"979b986772a35efb22acd746599cd197b1b856cfe01e52c4551c9777bee133a9","source":{"kind":"arxiv","id":"1312.0895","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1312.0895","created_at":"2026-05-18T00:37:02Z"},{"alias_kind":"arxiv_version","alias_value":"1312.0895v1","created_at":"2026-05-18T00:37:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.0895","created_at":"2026-05-18T00:37:02Z"},{"alias_kind":"pith_short_12","alias_value":"S6NZQZ3SUNPP","created_at":"2026-05-18T12:27:59Z"},{"alias_kind":"pith_short_16","alias_value":"S6NZQZ3SUNPPWIVM","created_at":"2026-05-18T12:27:59Z"},{"alias_kind":"pith_short_8","alias_value":"S6NZQZ3S","created_at":"2026-05-18T12:27:59Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:S6NZQZ3SUNPPWIVM25DFTHGRS6","target":"record","payload":{"canonical_record":{"source":{"id":"1312.0895","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-12-03T18:19:43Z","cross_cats_sorted":[],"title_canon_sha256":"f50892492da4c630c40bffd349d31c28cddf183589a3d3d146b468cdd1bec9ef","abstract_canon_sha256":"39cefeb63484e10b2c3b114677a35aa00dae51adee364f096d319fe45b536356"},"schema_version":"1.0"},"canonical_sha256":"979b986772a35efb22acd746599cd197b1b856cfe01e52c4551c9777bee133a9","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:37:02.131847Z","signature_b64":"+z4UpjfcAKX/Oz/c2dxwnaT6hNV0+p32E066bMZ+kGfQkQwnmD/hZu4GB0fJnLln0iPqDKG8+Hxr66wyn0fTBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"979b986772a35efb22acd746599cd197b1b856cfe01e52c4551c9777bee133a9","last_reissued_at":"2026-05-18T00:37:02.131112Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:37:02.131112Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1312.0895","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:37:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+4IuDrudD1y5uJWAeppsPUfQ1UK+AfwxDfezyw1CEfeVcZIHKBjXaIbxkaAd64FcI5UCwz6Rmc0CGUcd2/S1Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T12:38:31.393768Z"},"content_sha256":"26f4ebcb475c0208a3a2a9f3aabb09dec15fbe0704dc03190a89731c132148df","schema_version":"1.0","event_id":"sha256:26f4ebcb475c0208a3a2a9f3aabb09dec15fbe0704dc03190a89731c132148df"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:S6NZQZ3SUNPPWIVM25DFTHGRS6","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Anomaly and long-range forces","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A.V. Sadofyev, V.I. Zakharov, V.P. Kirilin","submitted_at":"2013-12-03T18:19:43Z","abstract_excerpt":"We consider infrared dependences of chiral effects, like chiral magnetic effect, in chiral media. The main observation is that there exist competing infrared-sensitive parameters, sometimes not apparent. The value of the chiral effects depends in fact on the actual hierarchy of the parameters. Some examples have been already given in the literature. We argue that magnetostatics of chiral media with a non-vanishing chiral chemical potential $\\mu_5\\neq 0$ is also infrared sensitive. In particular, the system turns to be unstable if the volume is large enough. The instability is with respect to t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.0895","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:37:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3WSbMShoddEFQ1krrRrlLGN/reRrMaRMsjU71cLPFgfC/LIo4S/NVhC9Kaop6CgUQcqQwfGktgeksigCCjDIBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T12:38:31.394410Z"},"content_sha256":"43cd01eb708ec1ec0b2d88147963b0f80b4a2d8dade62bf1226d181e508e8347","schema_version":"1.0","event_id":"sha256:43cd01eb708ec1ec0b2d88147963b0f80b4a2d8dade62bf1226d181e508e8347"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/S6NZQZ3SUNPPWIVM25DFTHGRS6/bundle.json","state_url":"https://pith.science/pith/S6NZQZ3SUNPPWIVM25DFTHGRS6/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/S6NZQZ3SUNPPWIVM25DFTHGRS6/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":"2026-05-31T12:38:31Z","links":{"resolver":"https://pith.science/pith/S6NZQZ3SUNPPWIVM25DFTHGRS6","bundle":"https://pith.science/pith/S6NZQZ3SUNPPWIVM25DFTHGRS6/bundle.json","state":"https://pith.science/pith/S6NZQZ3SUNPPWIVM25DFTHGRS6/state.json","well_known_bundle":"https://pith.science/.well-known/pith/S6NZQZ3SUNPPWIVM25DFTHGRS6/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:S6NZQZ3SUNPPWIVM25DFTHGRS6","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":"39cefeb63484e10b2c3b114677a35aa00dae51adee364f096d319fe45b536356","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-12-03T18:19:43Z","title_canon_sha256":"f50892492da4c630c40bffd349d31c28cddf183589a3d3d146b468cdd1bec9ef"},"schema_version":"1.0","source":{"id":"1312.0895","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1312.0895","created_at":"2026-05-18T00:37:02Z"},{"alias_kind":"arxiv_version","alias_value":"1312.0895v1","created_at":"2026-05-18T00:37:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.0895","created_at":"2026-05-18T00:37:02Z"},{"alias_kind":"pith_short_12","alias_value":"S6NZQZ3SUNPP","created_at":"2026-05-18T12:27:59Z"},{"alias_kind":"pith_short_16","alias_value":"S6NZQZ3SUNPPWIVM","created_at":"2026-05-18T12:27:59Z"},{"alias_kind":"pith_short_8","alias_value":"S6NZQZ3S","created_at":"2026-05-18T12:27:59Z"}],"graph_snapshots":[{"event_id":"sha256:43cd01eb708ec1ec0b2d88147963b0f80b4a2d8dade62bf1226d181e508e8347","target":"graph","created_at":"2026-05-18T00:37:02Z","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 consider infrared dependences of chiral effects, like chiral magnetic effect, in chiral media. The main observation is that there exist competing infrared-sensitive parameters, sometimes not apparent. The value of the chiral effects depends in fact on the actual hierarchy of the parameters. Some examples have been already given in the literature. We argue that magnetostatics of chiral media with a non-vanishing chiral chemical potential $\\mu_5\\neq 0$ is also infrared sensitive. In particular, the system turns to be unstable if the volume is large enough. The instability is with respect to t","authors_text":"A.V. Sadofyev, V.I. Zakharov, V.P. Kirilin","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-12-03T18:19:43Z","title":"Anomaly and long-range forces"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.0895","kind":"arxiv","version":1},"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":"sha256:26f4ebcb475c0208a3a2a9f3aabb09dec15fbe0704dc03190a89731c132148df","target":"record","created_at":"2026-05-18T00:37:02Z","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":"39cefeb63484e10b2c3b114677a35aa00dae51adee364f096d319fe45b536356","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-12-03T18:19:43Z","title_canon_sha256":"f50892492da4c630c40bffd349d31c28cddf183589a3d3d146b468cdd1bec9ef"},"schema_version":"1.0","source":{"id":"1312.0895","kind":"arxiv","version":1}},"canonical_sha256":"979b986772a35efb22acd746599cd197b1b856cfe01e52c4551c9777bee133a9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"979b986772a35efb22acd746599cd197b1b856cfe01e52c4551c9777bee133a9","first_computed_at":"2026-05-18T00:37:02.131112Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:37:02.131112Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"+z4UpjfcAKX/Oz/c2dxwnaT6hNV0+p32E066bMZ+kGfQkQwnmD/hZu4GB0fJnLln0iPqDKG8+Hxr66wyn0fTBw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:37:02.131847Z","signed_message":"canonical_sha256_bytes"},"source_id":"1312.0895","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:26f4ebcb475c0208a3a2a9f3aabb09dec15fbe0704dc03190a89731c132148df","sha256:43cd01eb708ec1ec0b2d88147963b0f80b4a2d8dade62bf1226d181e508e8347"],"state_sha256":"1dcde56407afd7006977cdf59193e685d1736cff0366383eb0a3bfe3ee3731c4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Q1WRKcTa5ZLvNrGls3lFy7KwRP8NRej5nz44+bitoZu6Q2r7896eV9x0CqnNNHOYmvy64wNonKDYuk0jOHH+Bg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T12:38:31.397818Z","bundle_sha256":"b569846606008ceda8de4079a6adcdfd9f7cc44c8996c59bc970cc09b0ea5c9f"}}