{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2023:ZTE6IUPIT3VYYI46I3QEQSUYBO","short_pith_number":"pith:ZTE6IUPI","canonical_record":{"source":{"id":"2311.07756","kind":"arxiv","version":4},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.comp-ph","submitted_at":"2023-11-13T21:15:13Z","cross_cats_sorted":["physics.plasm-ph","quant-ph"],"title_canon_sha256":"3f0c0672aff83bd84b1c28d2c0dffa74cdce28b32dbd3c962095eaa17113d2e5","abstract_canon_sha256":"e2bd65227c322bf573adf1d73faf19a728031b87464a2dd6c0f4de1f6a6bee62"},"schema_version":"1.0"},"canonical_sha256":"ccc9e451e89eeb8c239e46e0484a980ba782f998098a3d6e56c0f7e2d652e2ab","source":{"kind":"arxiv","id":"2311.07756","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2311.07756","created_at":"2026-05-18T03:09:47Z"},{"alias_kind":"arxiv_version","alias_value":"2311.07756v4","created_at":"2026-05-18T03:09:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2311.07756","created_at":"2026-05-18T03:09:47Z"},{"alias_kind":"pith_short_12","alias_value":"ZTE6IUPIT3VY","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_16","alias_value":"ZTE6IUPIT3VYYI46","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_8","alias_value":"ZTE6IUPI","created_at":"2026-05-18T12:33:37Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2023:ZTE6IUPIT3VYYI46I3QEQSUYBO","target":"record","payload":{"canonical_record":{"source":{"id":"2311.07756","kind":"arxiv","version":4},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.comp-ph","submitted_at":"2023-11-13T21:15:13Z","cross_cats_sorted":["physics.plasm-ph","quant-ph"],"title_canon_sha256":"3f0c0672aff83bd84b1c28d2c0dffa74cdce28b32dbd3c962095eaa17113d2e5","abstract_canon_sha256":"e2bd65227c322bf573adf1d73faf19a728031b87464a2dd6c0f4de1f6a6bee62"},"schema_version":"1.0"},"canonical_sha256":"ccc9e451e89eeb8c239e46e0484a980ba782f998098a3d6e56c0f7e2d652e2ab","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:09:47.271975Z","signature_b64":"ZC0dP3sEFIzyuCRYd+iHxyZZ0upEh7yIrctailwrhpY5EL3JSbc4iV23useF9MLJ7QPwgfneZAcCqbHkNQNbBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ccc9e451e89eeb8c239e46e0484a980ba782f998098a3d6e56c0f7e2d652e2ab","last_reissued_at":"2026-05-18T03:09:47.271101Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:09:47.271101Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2311.07756","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:09:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XUsQKoGpw5RbMDBD5YzIwFbpDnuGgXn7feRm9AZ/J1nnsSrG0knIR90ASujYS7z2HQ7AltDTZyamC2QrjycJBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T03:23:50.412226Z"},"content_sha256":"7eb7f266fe96836d7ea5623f28d3b0b7434b4af9e3bf15f0717557244cd7b3f5","schema_version":"1.0","event_id":"sha256:7eb7f266fe96836d7ea5623f28d3b0b7434b4af9e3bf15f0717557244cd7b3f5"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2023:ZTE6IUPIT3VYYI46I3QEQSUYBO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quantized tensor networks for solving the Vlasov-Maxwell equations","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["physics.plasm-ph","quant-ph"],"primary_cat":"physics.comp-ph","authors_text":"Erika Ye, Nuno Loureiro","submitted_at":"2023-11-13T21:15:13Z","abstract_excerpt":"The Vlasov-Maxwell equations provide an \\textit{ab-initio} description of collisionless plasmas, but solving them is often impractical because of the wide range of spatial and temporal scales that must be resolved and the high dimensionality of the problem. In this work, we present a quantum-inspired semi-implicit Vlasov-Maxwell solver that utilizes the quantized tensor network (QTN) framework. With this QTN solver, the cost of grid-based numerical simulation of size $N$ is reduced from $\\mathcal{O}(N)$ to $\\mathcal{O}(\\text{poly}(D))$, where $D$ is the ``rank'' or ``bond dimension'' of the QT"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2311.07756","kind":"arxiv","version":4},"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":"2026-05-18T03:09:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5oQISDPOUtdgp6wSQf6ODDPyUqs0RuI556OJLHthzw/D9Bhjz7qwbumrRmWpmLGUrXlkhlggd5rQO8yznuohAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T03:23:50.412945Z"},"content_sha256":"7b0e1acb0bf037b62cdb91d2e8a144790d1067998503bf650f753fa0b3101273","schema_version":"1.0","event_id":"sha256:7b0e1acb0bf037b62cdb91d2e8a144790d1067998503bf650f753fa0b3101273"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZTE6IUPIT3VYYI46I3QEQSUYBO/bundle.json","state_url":"https://pith.science/pith/ZTE6IUPIT3VYYI46I3QEQSUYBO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZTE6IUPIT3VYYI46I3QEQSUYBO/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":"2026-06-11T03:23:50Z","links":{"resolver":"https://pith.science/pith/ZTE6IUPIT3VYYI46I3QEQSUYBO","bundle":"https://pith.science/pith/ZTE6IUPIT3VYYI46I3QEQSUYBO/bundle.json","state":"https://pith.science/pith/ZTE6IUPIT3VYYI46I3QEQSUYBO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZTE6IUPIT3VYYI46I3QEQSUYBO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:ZTE6IUPIT3VYYI46I3QEQSUYBO","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":"e2bd65227c322bf573adf1d73faf19a728031b87464a2dd6c0f4de1f6a6bee62","cross_cats_sorted":["physics.plasm-ph","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.comp-ph","submitted_at":"2023-11-13T21:15:13Z","title_canon_sha256":"3f0c0672aff83bd84b1c28d2c0dffa74cdce28b32dbd3c962095eaa17113d2e5"},"schema_version":"1.0","source":{"id":"2311.07756","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2311.07756","created_at":"2026-05-18T03:09:47Z"},{"alias_kind":"arxiv_version","alias_value":"2311.07756v4","created_at":"2026-05-18T03:09:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2311.07756","created_at":"2026-05-18T03:09:47Z"},{"alias_kind":"pith_short_12","alias_value":"ZTE6IUPIT3VY","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_16","alias_value":"ZTE6IUPIT3VYYI46","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_8","alias_value":"ZTE6IUPI","created_at":"2026-05-18T12:33:37Z"}],"graph_snapshots":[{"event_id":"sha256:7b0e1acb0bf037b62cdb91d2e8a144790d1067998503bf650f753fa0b3101273","target":"graph","created_at":"2026-05-18T03:09:47Z","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":"The Vlasov-Maxwell equations provide an \\textit{ab-initio} description of collisionless plasmas, but solving them is often impractical because of the wide range of spatial and temporal scales that must be resolved and the high dimensionality of the problem. In this work, we present a quantum-inspired semi-implicit Vlasov-Maxwell solver that utilizes the quantized tensor network (QTN) framework. With this QTN solver, the cost of grid-based numerical simulation of size $N$ is reduced from $\\mathcal{O}(N)$ to $\\mathcal{O}(\\text{poly}(D))$, where $D$ is the ``rank'' or ``bond dimension'' of the QT","authors_text":"Erika Ye, Nuno Loureiro","cross_cats":["physics.plasm-ph","quant-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.comp-ph","submitted_at":"2023-11-13T21:15:13Z","title":"Quantized tensor networks for solving the Vlasov-Maxwell equations"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2311.07756","kind":"arxiv","version":4},"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":"sha256:7eb7f266fe96836d7ea5623f28d3b0b7434b4af9e3bf15f0717557244cd7b3f5","target":"record","created_at":"2026-05-18T03:09:47Z","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":"e2bd65227c322bf573adf1d73faf19a728031b87464a2dd6c0f4de1f6a6bee62","cross_cats_sorted":["physics.plasm-ph","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.comp-ph","submitted_at":"2023-11-13T21:15:13Z","title_canon_sha256":"3f0c0672aff83bd84b1c28d2c0dffa74cdce28b32dbd3c962095eaa17113d2e5"},"schema_version":"1.0","source":{"id":"2311.07756","kind":"arxiv","version":4}},"canonical_sha256":"ccc9e451e89eeb8c239e46e0484a980ba782f998098a3d6e56c0f7e2d652e2ab","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ccc9e451e89eeb8c239e46e0484a980ba782f998098a3d6e56c0f7e2d652e2ab","first_computed_at":"2026-05-18T03:09:47.271101Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:09:47.271101Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ZC0dP3sEFIzyuCRYd+iHxyZZ0upEh7yIrctailwrhpY5EL3JSbc4iV23useF9MLJ7QPwgfneZAcCqbHkNQNbBA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:09:47.271975Z","signed_message":"canonical_sha256_bytes"},"source_id":"2311.07756","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7eb7f266fe96836d7ea5623f28d3b0b7434b4af9e3bf15f0717557244cd7b3f5","sha256:7b0e1acb0bf037b62cdb91d2e8a144790d1067998503bf650f753fa0b3101273"],"state_sha256":"db22e39c0e00df8d042e58cdf3756427b68b824f6a5d201ea01680493b1b5fa9"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AtMFXBYoRtpfhhYl5fyzcCauvX86D8sTQxKFdGS/hRbPZCQehZBXcFaetkqe8AZ8R1wnCdevVJB4ULWM20tgDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-11T03:23:50.417095Z","bundle_sha256":"df25a795f4f9f22a4718aa4b12775b872716efa0b82a2dd8268fafee49688034"}}