{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:ZYUA6K2ZXR2JIBJZPEZ3GPZ7NR","short_pith_number":"pith:ZYUA6K2Z","canonical_record":{"source":{"id":"2410.06532","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2024-10-09T04:11:05Z","cross_cats_sorted":["physics.acc-ph","physics.app-ph"],"title_canon_sha256":"da4316dce3b258a553e875406db6a0ba01cbd19df706e0378aebe976d7a0fd82","abstract_canon_sha256":"5fb6cfd8ba4c3ffd596f39246274c3adbb9722c3d580eee63d0f5b3669afc877"},"schema_version":"1.0"},"canonical_sha256":"ce280f2b59bc749405397933b33f3f6c4b1eed40b72a635088453cb1162bff25","source":{"kind":"arxiv","id":"2410.06532","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2410.06532","created_at":"2026-07-05T09:24:39Z"},{"alias_kind":"arxiv_version","alias_value":"2410.06532v2","created_at":"2026-07-05T09:24:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2410.06532","created_at":"2026-07-05T09:24:39Z"},{"alias_kind":"pith_short_12","alias_value":"ZYUA6K2ZXR2J","created_at":"2026-07-05T09:24:39Z"},{"alias_kind":"pith_short_16","alias_value":"ZYUA6K2ZXR2JIBJZ","created_at":"2026-07-05T09:24:39Z"},{"alias_kind":"pith_short_8","alias_value":"ZYUA6K2Z","created_at":"2026-07-05T09:24:39Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:ZYUA6K2ZXR2JIBJZPEZ3GPZ7NR","target":"record","payload":{"canonical_record":{"source":{"id":"2410.06532","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2024-10-09T04:11:05Z","cross_cats_sorted":["physics.acc-ph","physics.app-ph"],"title_canon_sha256":"da4316dce3b258a553e875406db6a0ba01cbd19df706e0378aebe976d7a0fd82","abstract_canon_sha256":"5fb6cfd8ba4c3ffd596f39246274c3adbb9722c3d580eee63d0f5b3669afc877"},"schema_version":"1.0"},"canonical_sha256":"ce280f2b59bc749405397933b33f3f6c4b1eed40b72a635088453cb1162bff25","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:24:39.017088Z","signature_b64":"dGrpYxwTh7dBJ4zTrJAmndLPJOVHbjBlzkfCdVr/YZSftZse1KSdojnTTTtoK10n+QrJR3gXHAT0c7YjHKe7Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ce280f2b59bc749405397933b33f3f6c4b1eed40b72a635088453cb1162bff25","last_reissued_at":"2026-07-05T09:24:39.016564Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:24:39.016564Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2410.06532","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":"2026-07-05T09:24:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Wond1u04BxKvIgoYvjH7lwhNuzJXpyHzxn/2e7RjM8nBiGDUqZdYHgSPXyYihCL43/x+Zd30G9phmKvENs7zBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-19T18:53:09.515044Z"},"content_sha256":"308104e160549366a334efcfd959c6dae41e50519ed68bf044e03be1fa6ebbcb","schema_version":"1.0","event_id":"sha256:308104e160549366a334efcfd959c6dae41e50519ed68bf044e03be1fa6ebbcb"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:ZYUA6K2ZXR2JIBJZPEZ3GPZ7NR","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Analytic model of stable shock-like structures in laser interaction with underdense plasma for identifying of phase and polarization dependent regime of laser wakefield accelerators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.acc-ph","physics.app-ph"],"primary_cat":"physics.plasm-ph","authors_text":"Gennady Shvets, Jihoon Kim, Junjue Liao","submitted_at":"2024-10-09T04:11:05Z","abstract_excerpt":"We present an analytical model describing a stable shock-like structure that is formed when an ultra-intense laser propagates through an underdense plasma. It is shown that such structures exist in a wide range of laser-plasma parameters, with a unique sub-luminal shock front velocity for each parameter. Numerical methods to accurately describe such shock-front is developed. The formalism is applied to describe the parameter space in which the Carrier-Envelope-Phase (CEP) effect under which phase and polarization dependent super-ponderomotive effects becomes significant. The developed formalis"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2410.06532","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/2410.06532/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":"2026-07-05T09:24:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cdKFMWV931CuJo0ArqfgJqzPhbTagIS/8GQfiy7MRLSZJEiqQOqBA+P+tNyaMrF6aP0V48bKFGTk8Hga6dZqCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-19T18:53:09.516402Z"},"content_sha256":"e95309a3e133bc706495359b362a8ec3f8508c33e3b599ec27a2dd3d71f10963","schema_version":"1.0","event_id":"sha256:e95309a3e133bc706495359b362a8ec3f8508c33e3b599ec27a2dd3d71f10963"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZYUA6K2ZXR2JIBJZPEZ3GPZ7NR/bundle.json","state_url":"https://pith.science/pith/ZYUA6K2ZXR2JIBJZPEZ3GPZ7NR/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZYUA6K2ZXR2JIBJZPEZ3GPZ7NR/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":"2026-08-19T18:53:09Z","links":{"resolver":"https://pith.science/pith/ZYUA6K2ZXR2JIBJZPEZ3GPZ7NR","bundle":"https://pith.science/pith/ZYUA6K2ZXR2JIBJZPEZ3GPZ7NR/bundle.json","state":"https://pith.science/pith/ZYUA6K2ZXR2JIBJZPEZ3GPZ7NR/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZYUA6K2ZXR2JIBJZPEZ3GPZ7NR/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:ZYUA6K2ZXR2JIBJZPEZ3GPZ7NR","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":"5fb6cfd8ba4c3ffd596f39246274c3adbb9722c3d580eee63d0f5b3669afc877","cross_cats_sorted":["physics.acc-ph","physics.app-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2024-10-09T04:11:05Z","title_canon_sha256":"da4316dce3b258a553e875406db6a0ba01cbd19df706e0378aebe976d7a0fd82"},"schema_version":"1.0","source":{"id":"2410.06532","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2410.06532","created_at":"2026-07-05T09:24:39Z"},{"alias_kind":"arxiv_version","alias_value":"2410.06532v2","created_at":"2026-07-05T09:24:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2410.06532","created_at":"2026-07-05T09:24:39Z"},{"alias_kind":"pith_short_12","alias_value":"ZYUA6K2ZXR2J","created_at":"2026-07-05T09:24:39Z"},{"alias_kind":"pith_short_16","alias_value":"ZYUA6K2ZXR2JIBJZ","created_at":"2026-07-05T09:24:39Z"},{"alias_kind":"pith_short_8","alias_value":"ZYUA6K2Z","created_at":"2026-07-05T09:24:39Z"}],"graph_snapshots":[{"event_id":"sha256:e95309a3e133bc706495359b362a8ec3f8508c33e3b599ec27a2dd3d71f10963","target":"graph","created_at":"2026-07-05T09:24:39Z","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/2410.06532/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present an analytical model describing a stable shock-like structure that is formed when an ultra-intense laser propagates through an underdense plasma. It is shown that such structures exist in a wide range of laser-plasma parameters, with a unique sub-luminal shock front velocity for each parameter. Numerical methods to accurately describe such shock-front is developed. The formalism is applied to describe the parameter space in which the Carrier-Envelope-Phase (CEP) effect under which phase and polarization dependent super-ponderomotive effects becomes significant. The developed formalis","authors_text":"Gennady Shvets, Jihoon Kim, Junjue Liao","cross_cats":["physics.acc-ph","physics.app-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2024-10-09T04:11:05Z","title":"Analytic model of stable shock-like structures in laser interaction with underdense plasma for identifying of phase and polarization dependent regime of laser wakefield accelerators"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2410.06532","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":"sha256:308104e160549366a334efcfd959c6dae41e50519ed68bf044e03be1fa6ebbcb","target":"record","created_at":"2026-07-05T09:24:39Z","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":"5fb6cfd8ba4c3ffd596f39246274c3adbb9722c3d580eee63d0f5b3669afc877","cross_cats_sorted":["physics.acc-ph","physics.app-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2024-10-09T04:11:05Z","title_canon_sha256":"da4316dce3b258a553e875406db6a0ba01cbd19df706e0378aebe976d7a0fd82"},"schema_version":"1.0","source":{"id":"2410.06532","kind":"arxiv","version":2}},"canonical_sha256":"ce280f2b59bc749405397933b33f3f6c4b1eed40b72a635088453cb1162bff25","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ce280f2b59bc749405397933b33f3f6c4b1eed40b72a635088453cb1162bff25","first_computed_at":"2026-07-05T09:24:39.016564Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T09:24:39.016564Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"dGrpYxwTh7dBJ4zTrJAmndLPJOVHbjBlzkfCdVr/YZSftZse1KSdojnTTTtoK10n+QrJR3gXHAT0c7YjHKe7Dg==","signature_status":"signed_v1","signed_at":"2026-07-05T09:24:39.017088Z","signed_message":"canonical_sha256_bytes"},"source_id":"2410.06532","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:308104e160549366a334efcfd959c6dae41e50519ed68bf044e03be1fa6ebbcb","sha256:e95309a3e133bc706495359b362a8ec3f8508c33e3b599ec27a2dd3d71f10963"],"state_sha256":"3e8f0cd8bf77c3a95d35ba7be62c5d485764310faaf1b632b6fcab40736d0a84"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UXgQwPu7oE67ms/7RQfqka1QL5Hca+7ZfWfceVAAEpcA5XnAbjWHuksUoTrO1AFiQjmNNncFTh6xlEFDcR/5DQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-19T18:53:09.559047Z","bundle_sha256":"92f25141ec891e4b2db8d1bc849a5f58c01f446fbaac4f226a4d7df3790d55fb"}}