{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:JCXZD4TCCQJCFXK26ZJFWWYEA4","short_pith_number":"pith:JCXZD4TC","canonical_record":{"source":{"id":"2408.10835","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-08-20T13:31:10Z","cross_cats_sorted":[],"title_canon_sha256":"2834e70b5a672e982e3917e81f9b39d8d9fafcfbfa2432617c685d2e84cac225","abstract_canon_sha256":"1004bdc43119fa6de6ca526dfa5549a071462dabf5e661ee5d2f8bf649991928"},"schema_version":"1.0"},"canonical_sha256":"48af91f262141222dd5af6525b5b04072b91256fbbe946b675f6c69d5989d718","source":{"kind":"arxiv","id":"2408.10835","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2408.10835","created_at":"2026-07-05T10:46:38Z"},{"alias_kind":"arxiv_version","alias_value":"2408.10835v2","created_at":"2026-07-05T10:46:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2408.10835","created_at":"2026-07-05T10:46:38Z"},{"alias_kind":"pith_short_12","alias_value":"JCXZD4TCCQJC","created_at":"2026-07-05T10:46:38Z"},{"alias_kind":"pith_short_16","alias_value":"JCXZD4TCCQJCFXK2","created_at":"2026-07-05T10:46:38Z"},{"alias_kind":"pith_short_8","alias_value":"JCXZD4TC","created_at":"2026-07-05T10:46:38Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:JCXZD4TCCQJCFXK26ZJFWWYEA4","target":"record","payload":{"canonical_record":{"source":{"id":"2408.10835","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-08-20T13:31:10Z","cross_cats_sorted":[],"title_canon_sha256":"2834e70b5a672e982e3917e81f9b39d8d9fafcfbfa2432617c685d2e84cac225","abstract_canon_sha256":"1004bdc43119fa6de6ca526dfa5549a071462dabf5e661ee5d2f8bf649991928"},"schema_version":"1.0"},"canonical_sha256":"48af91f262141222dd5af6525b5b04072b91256fbbe946b675f6c69d5989d718","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:46:38.117897Z","signature_b64":"uBkJXCrTOEHxVMEj5PHL+HBXmco2ca4aKhQZg+SMkIQunptwxaoZb9XPb8WE+wBviGTzfDYL3TPvHXDXWd4BAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"48af91f262141222dd5af6525b5b04072b91256fbbe946b675f6c69d5989d718","last_reissued_at":"2026-07-05T10:46:38.117431Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:46:38.117431Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2408.10835","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":"2026-07-05T10:46:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WIsxv60dLOlRrvjg8rHUm/qksqHPbIFHRplb82xSoWWF/smwdgKFUPqWVUWcTe7eoCucCAoa0maGrs95QE+QBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T16:33:27.213754Z"},"content_sha256":"cbd0ec727504526d51695800ce5d735b8f397270a4b042c126304cd5b533104b","schema_version":"1.0","event_id":"sha256:cbd0ec727504526d51695800ce5d735b8f397270a4b042c126304cd5b533104b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:JCXZD4TCCQJCFXK26ZJFWWYEA4","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Designer bubble walls in a holographic Weyl semi-metal with magnetic field","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Nick Evans, Wanxiang Fan","submitted_at":"2024-08-20T13:31:10Z","abstract_excerpt":"We study bubble walls in the holographic D3/probe D7 system that is dual to strongly coupled quark dynamics. We work to construct holographic descriptions of bubble wall junctions where we can tune the bubble wall height and pressure difference in a theory at zero temperature and density. We study the system in the presence of a background axial vector field b (associated with the z direction) that induces a Weyl semi-metal, massless phase and a perpendicular background magnetic field Bx which favours mass generation. We find a first order transition line in the mass-Bx plane, at fixed b, endi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2408.10835","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2408.10835/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-05T10:46:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"MyktVHK8X/7a6Za7N94dL+7tTyQcrCQOZwboGfse1njo9Y/IXjOd2dSUYG8ZLpYCnEkH5mp1sUWXGkbTYzbRBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T16:33:27.214324Z"},"content_sha256":"8b1f1c8d717d45d77e399d2f934bff06b3e5b941363d435c3bd9ff8b361f9c60","schema_version":"1.0","event_id":"sha256:8b1f1c8d717d45d77e399d2f934bff06b3e5b941363d435c3bd9ff8b361f9c60"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/JCXZD4TCCQJCFXK26ZJFWWYEA4/bundle.json","state_url":"https://pith.science/pith/JCXZD4TCCQJCFXK26ZJFWWYEA4/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/JCXZD4TCCQJCFXK26ZJFWWYEA4/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":"2026-08-12T16:33:27Z","links":{"resolver":"https://pith.science/pith/JCXZD4TCCQJCFXK26ZJFWWYEA4","bundle":"https://pith.science/pith/JCXZD4TCCQJCFXK26ZJFWWYEA4/bundle.json","state":"https://pith.science/pith/JCXZD4TCCQJCFXK26ZJFWWYEA4/state.json","well_known_bundle":"https://pith.science/.well-known/pith/JCXZD4TCCQJCFXK26ZJFWWYEA4/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:JCXZD4TCCQJCFXK26ZJFWWYEA4","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":"1004bdc43119fa6de6ca526dfa5549a071462dabf5e661ee5d2f8bf649991928","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-08-20T13:31:10Z","title_canon_sha256":"2834e70b5a672e982e3917e81f9b39d8d9fafcfbfa2432617c685d2e84cac225"},"schema_version":"1.0","source":{"id":"2408.10835","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2408.10835","created_at":"2026-07-05T10:46:38Z"},{"alias_kind":"arxiv_version","alias_value":"2408.10835v2","created_at":"2026-07-05T10:46:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2408.10835","created_at":"2026-07-05T10:46:38Z"},{"alias_kind":"pith_short_12","alias_value":"JCXZD4TCCQJC","created_at":"2026-07-05T10:46:38Z"},{"alias_kind":"pith_short_16","alias_value":"JCXZD4TCCQJCFXK2","created_at":"2026-07-05T10:46:38Z"},{"alias_kind":"pith_short_8","alias_value":"JCXZD4TC","created_at":"2026-07-05T10:46:38Z"}],"graph_snapshots":[{"event_id":"sha256:8b1f1c8d717d45d77e399d2f934bff06b3e5b941363d435c3bd9ff8b361f9c60","target":"graph","created_at":"2026-07-05T10:46:38Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2408.10835/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We study bubble walls in the holographic D3/probe D7 system that is dual to strongly coupled quark dynamics. We work to construct holographic descriptions of bubble wall junctions where we can tune the bubble wall height and pressure difference in a theory at zero temperature and density. We study the system in the presence of a background axial vector field b (associated with the z direction) that induces a Weyl semi-metal, massless phase and a perpendicular background magnetic field Bx which favours mass generation. We find a first order transition line in the mass-Bx plane, at fixed b, endi","authors_text":"Nick Evans, Wanxiang Fan","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-08-20T13:31:10Z","title":"Designer bubble walls in a holographic Weyl semi-metal with magnetic field"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2408.10835","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:cbd0ec727504526d51695800ce5d735b8f397270a4b042c126304cd5b533104b","target":"record","created_at":"2026-07-05T10:46:38Z","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":"1004bdc43119fa6de6ca526dfa5549a071462dabf5e661ee5d2f8bf649991928","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-08-20T13:31:10Z","title_canon_sha256":"2834e70b5a672e982e3917e81f9b39d8d9fafcfbfa2432617c685d2e84cac225"},"schema_version":"1.0","source":{"id":"2408.10835","kind":"arxiv","version":2}},"canonical_sha256":"48af91f262141222dd5af6525b5b04072b91256fbbe946b675f6c69d5989d718","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"48af91f262141222dd5af6525b5b04072b91256fbbe946b675f6c69d5989d718","first_computed_at":"2026-07-05T10:46:38.117431Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:46:38.117431Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"uBkJXCrTOEHxVMEj5PHL+HBXmco2ca4aKhQZg+SMkIQunptwxaoZb9XPb8WE+wBviGTzfDYL3TPvHXDXWd4BAA==","signature_status":"signed_v1","signed_at":"2026-07-05T10:46:38.117897Z","signed_message":"canonical_sha256_bytes"},"source_id":"2408.10835","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cbd0ec727504526d51695800ce5d735b8f397270a4b042c126304cd5b533104b","sha256:8b1f1c8d717d45d77e399d2f934bff06b3e5b941363d435c3bd9ff8b361f9c60"],"state_sha256":"ab1e782611b1aa381cecae9b4219067a934e35e349d50dad3ff45ca11644aaa9"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WTpbXmj/u+lbejok9ktKZdhqDZgoyJKCKZXW2lHEGc1UDY4MVTZT/eETXP5SDMKV6qSI+3/+zoW4OaiveVXEBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-12T16:33:27.219422Z","bundle_sha256":"5f818e40bcebab187d7add39887daaee27b8f59363e6875a303a01e9708a52fc"}}