{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:4PRCFRLG52VM4K5MPTQLMJM4VE","short_pith_number":"pith:4PRCFRLG","canonical_record":{"source":{"id":"1805.05351","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-05-14T18:00:14Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"ad024112850590ae7d5d04f2c6cfa27c45aa0928f4444723153cad23847c8030","abstract_canon_sha256":"cad2c9d2ad7c43fa04553365f188905f1e1fa586cc270ec78a28076be974db4c"},"schema_version":"1.0"},"canonical_sha256":"e3e222c566eeaace2bac7ce0b6259ca9226e78d5f6957d9910c2fdd897a5e33d","source":{"kind":"arxiv","id":"1805.05351","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1805.05351","created_at":"2026-05-18T00:04:44Z"},{"alias_kind":"arxiv_version","alias_value":"1805.05351v2","created_at":"2026-05-18T00:04:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.05351","created_at":"2026-05-18T00:04:44Z"},{"alias_kind":"pith_short_12","alias_value":"4PRCFRLG52VM","created_at":"2026-05-18T12:32:05Z"},{"alias_kind":"pith_short_16","alias_value":"4PRCFRLG52VM4K5M","created_at":"2026-05-18T12:32:05Z"},{"alias_kind":"pith_short_8","alias_value":"4PRCFRLG","created_at":"2026-05-18T12:32:05Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:4PRCFRLG52VM4K5MPTQLMJM4VE","target":"record","payload":{"canonical_record":{"source":{"id":"1805.05351","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-05-14T18:00:14Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"ad024112850590ae7d5d04f2c6cfa27c45aa0928f4444723153cad23847c8030","abstract_canon_sha256":"cad2c9d2ad7c43fa04553365f188905f1e1fa586cc270ec78a28076be974db4c"},"schema_version":"1.0"},"canonical_sha256":"e3e222c566eeaace2bac7ce0b6259ca9226e78d5f6957d9910c2fdd897a5e33d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:04:44.784887Z","signature_b64":"SrnjMQnrxeULFcc35gGHQoFriR2BYHqxykXU6JKb05xVQ4v7HMmbAECmAHaY0H1rOtYrUBB/765iukMulEyvCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e3e222c566eeaace2bac7ce0b6259ca9226e78d5f6957d9910c2fdd897a5e33d","last_reissued_at":"2026-05-18T00:04:44.784162Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:04:44.784162Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1805.05351","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":"2026-05-18T00:04:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"O+NnwJvNikjfgpNMH6i/Zw65ygqWyKEJ9e+a/BsnC99/9u6EHe/bb39Z35UPHDvQDNwuvwavcYbM87yqLG/oAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T07:55:09.517850Z"},"content_sha256":"b9934d52a2a5ebd198caa9be340ce27dd4e349abe3864b479a6866a94d5499a2","schema_version":"1.0","event_id":"sha256:b9934d52a2a5ebd198caa9be340ce27dd4e349abe3864b479a6866a94d5499a2"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:4PRCFRLG52VM4K5MPTQLMJM4VE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Chaos, Diffusivity, and Spreading of Entanglement in Magnetic Branes, and the Strengthening of the Internal Interaction","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Daniel \\'Avila, Leonardo Pati\\~no, Viktor Jahnke","submitted_at":"2018-05-14T18:00:14Z","abstract_excerpt":"We use holographic methods to study several chaotic properties of a super Yang-Mills theory at temperature $T$ in the presence of a background magnetic field of constant strength $\\mathcal{B}$. The field theory we work on has a renormalization flow between a fixed point in the ultraviolet and another in the infrared, occurring in such a way that the energy at which the crossover takes place is a monotonically increasing function of the dimensionless ratio $\\mathcal{B}/T^2$. By considering shock waves in the bulk of the dual gravitational theory, and varying $\\mathcal{B}/T^2$, we study how seve"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.05351","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":"2026-05-18T00:04:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Mkn5GFxjb26/sr4Z5OlCiL0OyJodAdS/q7L7nPmPKaI5J8/jpvuZU39NSAIDfbTR8VkIQfb3fNoUTY3igq0BBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T07:55:09.518554Z"},"content_sha256":"6d5c91cbc23e43eb96f3451e8bcc37b837dfd6856672f988824c85869992a57d","schema_version":"1.0","event_id":"sha256:6d5c91cbc23e43eb96f3451e8bcc37b837dfd6856672f988824c85869992a57d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4PRCFRLG52VM4K5MPTQLMJM4VE/bundle.json","state_url":"https://pith.science/pith/4PRCFRLG52VM4K5MPTQLMJM4VE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4PRCFRLG52VM4K5MPTQLMJM4VE/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":"2026-05-25T07:55:09Z","links":{"resolver":"https://pith.science/pith/4PRCFRLG52VM4K5MPTQLMJM4VE","bundle":"https://pith.science/pith/4PRCFRLG52VM4K5MPTQLMJM4VE/bundle.json","state":"https://pith.science/pith/4PRCFRLG52VM4K5MPTQLMJM4VE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4PRCFRLG52VM4K5MPTQLMJM4VE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:4PRCFRLG52VM4K5MPTQLMJM4VE","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":"cad2c9d2ad7c43fa04553365f188905f1e1fa586cc270ec78a28076be974db4c","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-05-14T18:00:14Z","title_canon_sha256":"ad024112850590ae7d5d04f2c6cfa27c45aa0928f4444723153cad23847c8030"},"schema_version":"1.0","source":{"id":"1805.05351","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1805.05351","created_at":"2026-05-18T00:04:44Z"},{"alias_kind":"arxiv_version","alias_value":"1805.05351v2","created_at":"2026-05-18T00:04:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.05351","created_at":"2026-05-18T00:04:44Z"},{"alias_kind":"pith_short_12","alias_value":"4PRCFRLG52VM","created_at":"2026-05-18T12:32:05Z"},{"alias_kind":"pith_short_16","alias_value":"4PRCFRLG52VM4K5M","created_at":"2026-05-18T12:32:05Z"},{"alias_kind":"pith_short_8","alias_value":"4PRCFRLG","created_at":"2026-05-18T12:32:05Z"}],"graph_snapshots":[{"event_id":"sha256:6d5c91cbc23e43eb96f3451e8bcc37b837dfd6856672f988824c85869992a57d","target":"graph","created_at":"2026-05-18T00:04:44Z","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 use holographic methods to study several chaotic properties of a super Yang-Mills theory at temperature $T$ in the presence of a background magnetic field of constant strength $\\mathcal{B}$. The field theory we work on has a renormalization flow between a fixed point in the ultraviolet and another in the infrared, occurring in such a way that the energy at which the crossover takes place is a monotonically increasing function of the dimensionless ratio $\\mathcal{B}/T^2$. By considering shock waves in the bulk of the dual gravitational theory, and varying $\\mathcal{B}/T^2$, we study how seve","authors_text":"Daniel \\'Avila, Leonardo Pati\\~no, Viktor Jahnke","cross_cats":["gr-qc"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-05-14T18:00:14Z","title":"Chaos, Diffusivity, and Spreading of Entanglement in Magnetic Branes, and the Strengthening of the Internal Interaction"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.05351","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:b9934d52a2a5ebd198caa9be340ce27dd4e349abe3864b479a6866a94d5499a2","target":"record","created_at":"2026-05-18T00:04:44Z","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":"cad2c9d2ad7c43fa04553365f188905f1e1fa586cc270ec78a28076be974db4c","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-05-14T18:00:14Z","title_canon_sha256":"ad024112850590ae7d5d04f2c6cfa27c45aa0928f4444723153cad23847c8030"},"schema_version":"1.0","source":{"id":"1805.05351","kind":"arxiv","version":2}},"canonical_sha256":"e3e222c566eeaace2bac7ce0b6259ca9226e78d5f6957d9910c2fdd897a5e33d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e3e222c566eeaace2bac7ce0b6259ca9226e78d5f6957d9910c2fdd897a5e33d","first_computed_at":"2026-05-18T00:04:44.784162Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:04:44.784162Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"SrnjMQnrxeULFcc35gGHQoFriR2BYHqxykXU6JKb05xVQ4v7HMmbAECmAHaY0H1rOtYrUBB/765iukMulEyvCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:04:44.784887Z","signed_message":"canonical_sha256_bytes"},"source_id":"1805.05351","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b9934d52a2a5ebd198caa9be340ce27dd4e349abe3864b479a6866a94d5499a2","sha256:6d5c91cbc23e43eb96f3451e8bcc37b837dfd6856672f988824c85869992a57d"],"state_sha256":"94c2f585eb2f2471b1ebadc515f5be254a3cbe2e3975fb0e8ef8c72b312358c1"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XVZPtJX1QoxSUhiViiRhLX2LEssSqBcT55W/YTegMqLOVunb7VeHqQ7QpqHE3iG8W6C0mK8Y4zO7K9JOndCBDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T07:55:09.523185Z","bundle_sha256":"cfcd66479d1ce356dcdec133958a275eff03db8abbb76b3ac773978db277defd"}}