{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2022:QHWBTO3FJXP2U3JAZ2VJJQFHPQ","short_pith_number":"pith:QHWBTO3F","canonical_record":{"source":{"id":"2209.03794","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2022-09-08T13:07:06Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"26c43101c978edc8c47ae919e18ee72a4341ff560f9b3b1234c3429f0f621a64","abstract_canon_sha256":"911683954c8fd457638d4404aa12c941b22422edd7541189d2bebdda3760f92b"},"schema_version":"1.0"},"canonical_sha256":"81ec19bb654ddfaa6d20ceaa94c0a77c39855ddc6bfa98a47bcb62b8f2247a17","source":{"kind":"arxiv","id":"2209.03794","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2209.03794","created_at":"2026-07-05T04:55:45Z"},{"alias_kind":"arxiv_version","alias_value":"2209.03794v1","created_at":"2026-07-05T04:55:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2209.03794","created_at":"2026-07-05T04:55:45Z"},{"alias_kind":"pith_short_12","alias_value":"QHWBTO3FJXP2","created_at":"2026-07-05T04:55:45Z"},{"alias_kind":"pith_short_16","alias_value":"QHWBTO3FJXP2U3JA","created_at":"2026-07-05T04:55:45Z"},{"alias_kind":"pith_short_8","alias_value":"QHWBTO3F","created_at":"2026-07-05T04:55:45Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2022:QHWBTO3FJXP2U3JAZ2VJJQFHPQ","target":"record","payload":{"canonical_record":{"source":{"id":"2209.03794","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2022-09-08T13:07:06Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"26c43101c978edc8c47ae919e18ee72a4341ff560f9b3b1234c3429f0f621a64","abstract_canon_sha256":"911683954c8fd457638d4404aa12c941b22422edd7541189d2bebdda3760f92b"},"schema_version":"1.0"},"canonical_sha256":"81ec19bb654ddfaa6d20ceaa94c0a77c39855ddc6bfa98a47bcb62b8f2247a17","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:55:45.920367Z","signature_b64":"rO4qtSBYFI8yS2bNCmHGDeey9/FgIt5Eh0IRKO1lU8wFOasuWcyxqEmFTP8B8JlusBEzM7F5MO8axQf9BpJMDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"81ec19bb654ddfaa6d20ceaa94c0a77c39855ddc6bfa98a47bcb62b8f2247a17","last_reissued_at":"2026-07-05T04:55:45.920015Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:55:45.920015Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2209.03794","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":"2026-07-05T04:55:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nCKB24DHESgHqJKwq7m/Qbw1OcFNe5QW+M9y9WBUPxmZa0bnz72Ovk5rMaJmjBEMVkcII4M37fYnsf9bTMQgDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T16:29:39.226367Z"},"content_sha256":"dc028741271a4f40026bb3c59df7314cfbfeef8b00e41c189d961583f8469032","schema_version":"1.0","event_id":"sha256:dc028741271a4f40026bb3c59df7314cfbfeef8b00e41c189d961583f8469032"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2022:QHWBTO3FJXP2U3JAZ2VJJQFHPQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Snowmass Topical Group Summary Report: IF04 -- Trigger and Data Acquisition Systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"physics.ins-det","authors_text":"Allison Deiana, Darin Acosta, Wesley Ketchum","submitted_at":"2022-09-08T13:07:06Z","abstract_excerpt":"A trend for future high energy physics experiments is an increase in the data bandwidth produced from the detectors. Datasets of the Petabyte scale have already become the norm, and the requirements of future experiments -- greater in size, exposure, and complexity -- will further push the limits of data acquisition technologies to data rates of exabytes per seconds. The challenge for these future data-intensive physics facilities lies in the reduction of the flow of data through a combination of sophisticated event selection in the form of high-performance triggers and improved data represent"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2209.03794","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2209.03794/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":"2026-07-05T04:55:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0gumkSWRLH7p4gtGzEIZPHEJ0o6aTr6EC9HmKMvNhCP+Df8b4AsDKOWNCZu6fNTLjx+dE0YQGqyN646a1iPwCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T16:29:39.228915Z"},"content_sha256":"38b1d36d624d6872f5cba877dc41c6a2a4cbfb0a1a944f46375eca9ffe481ea0","schema_version":"1.0","event_id":"sha256:38b1d36d624d6872f5cba877dc41c6a2a4cbfb0a1a944f46375eca9ffe481ea0"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/QHWBTO3FJXP2U3JAZ2VJJQFHPQ/bundle.json","state_url":"https://pith.science/pith/QHWBTO3FJXP2U3JAZ2VJJQFHPQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/QHWBTO3FJXP2U3JAZ2VJJQFHPQ/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":"2026-08-03T16:29:39Z","links":{"resolver":"https://pith.science/pith/QHWBTO3FJXP2U3JAZ2VJJQFHPQ","bundle":"https://pith.science/pith/QHWBTO3FJXP2U3JAZ2VJJQFHPQ/bundle.json","state":"https://pith.science/pith/QHWBTO3FJXP2U3JAZ2VJJQFHPQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/QHWBTO3FJXP2U3JAZ2VJJQFHPQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:QHWBTO3FJXP2U3JAZ2VJJQFHPQ","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":"911683954c8fd457638d4404aa12c941b22422edd7541189d2bebdda3760f92b","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2022-09-08T13:07:06Z","title_canon_sha256":"26c43101c978edc8c47ae919e18ee72a4341ff560f9b3b1234c3429f0f621a64"},"schema_version":"1.0","source":{"id":"2209.03794","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2209.03794","created_at":"2026-07-05T04:55:45Z"},{"alias_kind":"arxiv_version","alias_value":"2209.03794v1","created_at":"2026-07-05T04:55:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2209.03794","created_at":"2026-07-05T04:55:45Z"},{"alias_kind":"pith_short_12","alias_value":"QHWBTO3FJXP2","created_at":"2026-07-05T04:55:45Z"},{"alias_kind":"pith_short_16","alias_value":"QHWBTO3FJXP2U3JA","created_at":"2026-07-05T04:55:45Z"},{"alias_kind":"pith_short_8","alias_value":"QHWBTO3F","created_at":"2026-07-05T04:55:45Z"}],"graph_snapshots":[{"event_id":"sha256:38b1d36d624d6872f5cba877dc41c6a2a4cbfb0a1a944f46375eca9ffe481ea0","target":"graph","created_at":"2026-07-05T04:55:45Z","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/2209.03794/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"A trend for future high energy physics experiments is an increase in the data bandwidth produced from the detectors. Datasets of the Petabyte scale have already become the norm, and the requirements of future experiments -- greater in size, exposure, and complexity -- will further push the limits of data acquisition technologies to data rates of exabytes per seconds. The challenge for these future data-intensive physics facilities lies in the reduction of the flow of data through a combination of sophisticated event selection in the form of high-performance triggers and improved data represent","authors_text":"Allison Deiana, Darin Acosta, Wesley Ketchum","cross_cats":["hep-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2022-09-08T13:07:06Z","title":"Snowmass Topical Group Summary Report: IF04 -- Trigger and Data Acquisition Systems"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2209.03794","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:dc028741271a4f40026bb3c59df7314cfbfeef8b00e41c189d961583f8469032","target":"record","created_at":"2026-07-05T04:55:45Z","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":"911683954c8fd457638d4404aa12c941b22422edd7541189d2bebdda3760f92b","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2022-09-08T13:07:06Z","title_canon_sha256":"26c43101c978edc8c47ae919e18ee72a4341ff560f9b3b1234c3429f0f621a64"},"schema_version":"1.0","source":{"id":"2209.03794","kind":"arxiv","version":1}},"canonical_sha256":"81ec19bb654ddfaa6d20ceaa94c0a77c39855ddc6bfa98a47bcb62b8f2247a17","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"81ec19bb654ddfaa6d20ceaa94c0a77c39855ddc6bfa98a47bcb62b8f2247a17","first_computed_at":"2026-07-05T04:55:45.920015Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:55:45.920015Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"rO4qtSBYFI8yS2bNCmHGDeey9/FgIt5Eh0IRKO1lU8wFOasuWcyxqEmFTP8B8JlusBEzM7F5MO8axQf9BpJMDA==","signature_status":"signed_v1","signed_at":"2026-07-05T04:55:45.920367Z","signed_message":"canonical_sha256_bytes"},"source_id":"2209.03794","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:dc028741271a4f40026bb3c59df7314cfbfeef8b00e41c189d961583f8469032","sha256:38b1d36d624d6872f5cba877dc41c6a2a4cbfb0a1a944f46375eca9ffe481ea0"],"state_sha256":"2a120c5aacc84b8629b73966546f88c769d8056f737777a9fe5c6cbf33e7bc70"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7LJS1WwcmDqnbDj27iQlZFebkuhS5COohSaSv4Kr/uwk9ZCD7tYnkmMwjBc+dHLtXTXFunLpqbVfobcnDmRQDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-03T16:29:39.253266Z","bundle_sha256":"25c26041c8163b7fbe9acb318a9d1d072c46083c277bd575fc4405d2ffef5e78"}}