{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:HDHHJHGXSTHWSGJKQP4KEGXA2F","short_pith_number":"pith:HDHHJHGX","canonical_record":{"source":{"id":"2405.06040","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-05-09T18:19:36Z","cross_cats_sorted":["hep-ex","physics.comp-ph"],"title_canon_sha256":"677c0ee9761994cc1b939580615d571021b5a5f6c0f42b4668934bd860555e32","abstract_canon_sha256":"bd1b61958c9ce6f5b0e460117721c5fa8a5db0c60b40ed76c10de525b10ec37c"},"schema_version":"1.0"},"canonical_sha256":"38ce749cd794cf69192a83f8a21ae0d14acc0431fa686ded918909c7e2261bcf","source":{"kind":"arxiv","id":"2405.06040","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2405.06040","created_at":"2026-07-05T11:40:48Z"},{"alias_kind":"arxiv_version","alias_value":"2405.06040v2","created_at":"2026-07-05T11:40:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2405.06040","created_at":"2026-07-05T11:40:48Z"},{"alias_kind":"pith_short_12","alias_value":"HDHHJHGXSTHW","created_at":"2026-07-05T11:40:48Z"},{"alias_kind":"pith_short_16","alias_value":"HDHHJHGXSTHWSGJK","created_at":"2026-07-05T11:40:48Z"},{"alias_kind":"pith_short_8","alias_value":"HDHHJHGX","created_at":"2026-07-05T11:40:48Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:HDHHJHGXSTHWSGJKQP4KEGXA2F","target":"record","payload":{"canonical_record":{"source":{"id":"2405.06040","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-05-09T18:19:36Z","cross_cats_sorted":["hep-ex","physics.comp-ph"],"title_canon_sha256":"677c0ee9761994cc1b939580615d571021b5a5f6c0f42b4668934bd860555e32","abstract_canon_sha256":"bd1b61958c9ce6f5b0e460117721c5fa8a5db0c60b40ed76c10de525b10ec37c"},"schema_version":"1.0"},"canonical_sha256":"38ce749cd794cf69192a83f8a21ae0d14acc0431fa686ded918909c7e2261bcf","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:40:48.294869Z","signature_b64":"lScvrLGtGxoJz6Qfffduypt2Gf5wwV3shKLnikqJnL/lENvxzA1xErwwP9f52iUroa0QG1WlTCDsYHqf45lfAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"38ce749cd794cf69192a83f8a21ae0d14acc0431fa686ded918909c7e2261bcf","last_reissued_at":"2026-07-05T11:40:48.294354Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:40:48.294354Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2405.06040","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":"2026-07-05T11:40:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"k4SlLINM22KEL8uhJBNNCxgpuYK5ZVtpnyxkZGmNqgQvdoRO/DuYA/89Nuz0zYo9Van2pEZb8uqpeIG7/+O7Bw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-08T16:15:19.470688Z"},"content_sha256":"4fd314c5a11f724a09110eed7f46338c370635348df1bedc133cee89c9f3bde8","schema_version":"1.0","event_id":"sha256:4fd314c5a11f724a09110eed7f46338c370635348df1bedc133cee89c9f3bde8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:HDHHJHGXSTHWSGJKQP4KEGXA2F","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Searches for the BSM scenarios at the LHC using decision tree based machine learning algorithms: A comparative study and review of Random Forest, Adaboost, XGboost and LightGBM frameworks","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex","physics.comp-ph"],"primary_cat":"hep-ph","authors_text":"Arghya Choudhury, Arpita Mondal, Subhadeep Sarkar","submitted_at":"2024-05-09T18:19:36Z","abstract_excerpt":"Machine learning algorithms are now being extensively used in our daily lives, spanning across diverse industries as well as academia. In the field of high energy physics (HEP), the most common and challenging task is separating a rare signal from a much larger background. The boosted decision tree (BDT) algorithm has been a cornerstone of the high energy physics for analyzing event triggering, particle identification, jet tagging, object reconstruction, event classification, and other related tasks for quite some time. This article presents a comprehensive overview of research conducted by bo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2405.06040","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/2405.06040/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":"2026-07-05T11:40:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NVtgdl9pUm48zXZqSSy6HA6Lg8J/GnqyTl3ePiJ5rdDKn394VmkErybqJu39bncHpeQweKMyr9d8wEFa9rnEBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-08T16:15:19.471327Z"},"content_sha256":"1c25b1d2c138b720b84391d2900073cb0c0d5caac82352961cad3299370548af","schema_version":"1.0","event_id":"sha256:1c25b1d2c138b720b84391d2900073cb0c0d5caac82352961cad3299370548af"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HDHHJHGXSTHWSGJKQP4KEGXA2F/bundle.json","state_url":"https://pith.science/pith/HDHHJHGXSTHWSGJKQP4KEGXA2F/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HDHHJHGXSTHWSGJKQP4KEGXA2F/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":"2026-08-08T16:15:19Z","links":{"resolver":"https://pith.science/pith/HDHHJHGXSTHWSGJKQP4KEGXA2F","bundle":"https://pith.science/pith/HDHHJHGXSTHWSGJKQP4KEGXA2F/bundle.json","state":"https://pith.science/pith/HDHHJHGXSTHWSGJKQP4KEGXA2F/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HDHHJHGXSTHWSGJKQP4KEGXA2F/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:HDHHJHGXSTHWSGJKQP4KEGXA2F","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":"bd1b61958c9ce6f5b0e460117721c5fa8a5db0c60b40ed76c10de525b10ec37c","cross_cats_sorted":["hep-ex","physics.comp-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-05-09T18:19:36Z","title_canon_sha256":"677c0ee9761994cc1b939580615d571021b5a5f6c0f42b4668934bd860555e32"},"schema_version":"1.0","source":{"id":"2405.06040","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2405.06040","created_at":"2026-07-05T11:40:48Z"},{"alias_kind":"arxiv_version","alias_value":"2405.06040v2","created_at":"2026-07-05T11:40:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2405.06040","created_at":"2026-07-05T11:40:48Z"},{"alias_kind":"pith_short_12","alias_value":"HDHHJHGXSTHW","created_at":"2026-07-05T11:40:48Z"},{"alias_kind":"pith_short_16","alias_value":"HDHHJHGXSTHWSGJK","created_at":"2026-07-05T11:40:48Z"},{"alias_kind":"pith_short_8","alias_value":"HDHHJHGX","created_at":"2026-07-05T11:40:48Z"}],"graph_snapshots":[{"event_id":"sha256:1c25b1d2c138b720b84391d2900073cb0c0d5caac82352961cad3299370548af","target":"graph","created_at":"2026-07-05T11:40:48Z","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/2405.06040/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Machine learning algorithms are now being extensively used in our daily lives, spanning across diverse industries as well as academia. In the field of high energy physics (HEP), the most common and challenging task is separating a rare signal from a much larger background. The boosted decision tree (BDT) algorithm has been a cornerstone of the high energy physics for analyzing event triggering, particle identification, jet tagging, object reconstruction, event classification, and other related tasks for quite some time. This article presents a comprehensive overview of research conducted by bo","authors_text":"Arghya Choudhury, Arpita Mondal, Subhadeep Sarkar","cross_cats":["hep-ex","physics.comp-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-05-09T18:19:36Z","title":"Searches for the BSM scenarios at the LHC using decision tree based machine learning algorithms: A comparative study and review of Random Forest, Adaboost, XGboost and LightGBM frameworks"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2405.06040","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":"sha256:4fd314c5a11f724a09110eed7f46338c370635348df1bedc133cee89c9f3bde8","target":"record","created_at":"2026-07-05T11:40:48Z","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":"bd1b61958c9ce6f5b0e460117721c5fa8a5db0c60b40ed76c10de525b10ec37c","cross_cats_sorted":["hep-ex","physics.comp-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-05-09T18:19:36Z","title_canon_sha256":"677c0ee9761994cc1b939580615d571021b5a5f6c0f42b4668934bd860555e32"},"schema_version":"1.0","source":{"id":"2405.06040","kind":"arxiv","version":2}},"canonical_sha256":"38ce749cd794cf69192a83f8a21ae0d14acc0431fa686ded918909c7e2261bcf","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"38ce749cd794cf69192a83f8a21ae0d14acc0431fa686ded918909c7e2261bcf","first_computed_at":"2026-07-05T11:40:48.294354Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:40:48.294354Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"lScvrLGtGxoJz6Qfffduypt2Gf5wwV3shKLnikqJnL/lENvxzA1xErwwP9f52iUroa0QG1WlTCDsYHqf45lfAg==","signature_status":"signed_v1","signed_at":"2026-07-05T11:40:48.294869Z","signed_message":"canonical_sha256_bytes"},"source_id":"2405.06040","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4fd314c5a11f724a09110eed7f46338c370635348df1bedc133cee89c9f3bde8","sha256:1c25b1d2c138b720b84391d2900073cb0c0d5caac82352961cad3299370548af"],"state_sha256":"a1a632e278645b92515911ad6c73ab9adc4e6777f67ee7a15d828b9e542b9df4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"w80riiLZmJsac7jObshrohXleFMOcMcfWr7oYZb7bqBV6JWaM/grNF/gBKJiiEgfM+K44Bjt+TnkbKgyqG62Cg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-08T16:15:19.476969Z","bundle_sha256":"78602b37f9985e0cabe7ce03c22bb71eeddbbf4808e6171bcb738109ccf5cc1f"}}