{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2006:SCOKNIFY56TYKD6CVMBRNOTINA","short_pith_number":"pith:SCOKNIFY","canonical_record":{"source":{"id":"nucl-th/0608036","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2006-08-13T23:35:51Z","cross_cats_sorted":["hep-ph","nucl-ex"],"title_canon_sha256":"12277c0ce2d56a9a9eb11580df8baa5de05f49599e715b8568bd9334ec0dd447","abstract_canon_sha256":"4e1d966e93e60e2f67d9864b4e8bc99450296e6b0174c00e7e5a86c4b16392c4"},"schema_version":"1.0"},"canonical_sha256":"909ca6a0b8efa7850fc2ab0316ba686828be6bafe5b984818537470a7ce258d6","source":{"kind":"arxiv","id":"nucl-th/0608036","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/0608036","created_at":"2026-07-04T15:22:47Z"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0608036v1","created_at":"2026-07-04T15:22:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0608036","created_at":"2026-07-04T15:22:47Z"},{"alias_kind":"pith_short_12","alias_value":"SCOKNIFY56TY","created_at":"2026-07-04T15:22:47Z"},{"alias_kind":"pith_short_16","alias_value":"SCOKNIFY56TYKD6C","created_at":"2026-07-04T15:22:47Z"},{"alias_kind":"pith_short_8","alias_value":"SCOKNIFY","created_at":"2026-07-04T15:22:47Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2006:SCOKNIFY56TYKD6CVMBRNOTINA","target":"record","payload":{"canonical_record":{"source":{"id":"nucl-th/0608036","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2006-08-13T23:35:51Z","cross_cats_sorted":["hep-ph","nucl-ex"],"title_canon_sha256":"12277c0ce2d56a9a9eb11580df8baa5de05f49599e715b8568bd9334ec0dd447","abstract_canon_sha256":"4e1d966e93e60e2f67d9864b4e8bc99450296e6b0174c00e7e5a86c4b16392c4"},"schema_version":"1.0"},"canonical_sha256":"909ca6a0b8efa7850fc2ab0316ba686828be6bafe5b984818537470a7ce258d6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:22:47.388453Z","signature_b64":"CaS8qCgS67fDldxod6Uywvpua14dDrfcEmPSPo5Bzyj9I+P7WUMrP6qQv5U3oHqVTJkjb7TR+74WmXQu2JCXAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"909ca6a0b8efa7850fc2ab0316ba686828be6bafe5b984818537470a7ce258d6","last_reissued_at":"2026-07-04T15:22:47.388044Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:22:47.388044Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"nucl-th/0608036","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":"2026-07-04T15:22:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nRCnehMlovxoD6IG6lhxD45d6t5cJjnCGVEO05XwsSlhsGthDpuQqSUhKbkUInoGQxY+hHPFH7Qj5/8vSqrJBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-13T20:36:29.766531Z"},"content_sha256":"26734d40996627e82a70b99b33af6d8f2b9b54d7abb77a3d04c2b0ada0b73eff","schema_version":"1.0","event_id":"sha256:26734d40996627e82a70b99b33af6d8f2b9b54d7abb77a3d04c2b0ada0b73eff"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2006:SCOKNIFY56TYKD6CVMBRNOTINA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Chiral effective theory predictions for deuteron form factor ratios at low Q^2","license":"","headline":"","cross_cats":["hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"Chubu University), Daniel R. Phillips (Ohio University","submitted_at":"2006-08-13T23:35:51Z","abstract_excerpt":"We use chiral effective theory to predict the deuteron form factor ratio G_C/G_Q as well as ratios of deuteron to nucleon form factors. These ratios are calculated to next-to-next-to-leading order. At this order the chiral expansion for the NN isoscalar charge operator (including consistently calculated 1/M corrections) is a parameter-free prediction of the effective theory. Use of this operator in conjunction with NLO and NNLO chiral effective theory wave functions produces results that are consistent with extant experimental data for Q^2 < 0.35 GeV^2. These wave functions predict a deuteron "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0608036","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/nucl-th/0608036/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":"2026-07-04T15:22:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VTVahv2J2pFEsixYtWSu1q1GHF92t8T0wx7JIjhnqBT8ZAnxTel+KZUWQsRF04i1PB7DHRJTq/ETF7+AT/z5CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-13T20:36:29.767062Z"},"content_sha256":"938b1330ece315cf6f5628d905f5551d0bf4159625cea570a7671653f633bf30","schema_version":"1.0","event_id":"sha256:938b1330ece315cf6f5628d905f5551d0bf4159625cea570a7671653f633bf30"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/SCOKNIFY56TYKD6CVMBRNOTINA/bundle.json","state_url":"https://pith.science/pith/SCOKNIFY56TYKD6CVMBRNOTINA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/SCOKNIFY56TYKD6CVMBRNOTINA/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":"2026-08-13T20:36:29Z","links":{"resolver":"https://pith.science/pith/SCOKNIFY56TYKD6CVMBRNOTINA","bundle":"https://pith.science/pith/SCOKNIFY56TYKD6CVMBRNOTINA/bundle.json","state":"https://pith.science/pith/SCOKNIFY56TYKD6CVMBRNOTINA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/SCOKNIFY56TYKD6CVMBRNOTINA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2006:SCOKNIFY56TYKD6CVMBRNOTINA","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":"4e1d966e93e60e2f67d9864b4e8bc99450296e6b0174c00e7e5a86c4b16392c4","cross_cats_sorted":["hep-ph","nucl-ex"],"license":"","primary_cat":"nucl-th","submitted_at":"2006-08-13T23:35:51Z","title_canon_sha256":"12277c0ce2d56a9a9eb11580df8baa5de05f49599e715b8568bd9334ec0dd447"},"schema_version":"1.0","source":{"id":"nucl-th/0608036","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/0608036","created_at":"2026-07-04T15:22:47Z"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0608036v1","created_at":"2026-07-04T15:22:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0608036","created_at":"2026-07-04T15:22:47Z"},{"alias_kind":"pith_short_12","alias_value":"SCOKNIFY56TY","created_at":"2026-07-04T15:22:47Z"},{"alias_kind":"pith_short_16","alias_value":"SCOKNIFY56TYKD6C","created_at":"2026-07-04T15:22:47Z"},{"alias_kind":"pith_short_8","alias_value":"SCOKNIFY","created_at":"2026-07-04T15:22:47Z"}],"graph_snapshots":[{"event_id":"sha256:938b1330ece315cf6f5628d905f5551d0bf4159625cea570a7671653f633bf30","target":"graph","created_at":"2026-07-04T15:22:47Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/nucl-th/0608036/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We use chiral effective theory to predict the deuteron form factor ratio G_C/G_Q as well as ratios of deuteron to nucleon form factors. These ratios are calculated to next-to-next-to-leading order. At this order the chiral expansion for the NN isoscalar charge operator (including consistently calculated 1/M corrections) is a parameter-free prediction of the effective theory. Use of this operator in conjunction with NLO and NNLO chiral effective theory wave functions produces results that are consistent with extant experimental data for Q^2 < 0.35 GeV^2. These wave functions predict a deuteron ","authors_text":"Chubu University), Daniel R. Phillips (Ohio University","cross_cats":["hep-ph","nucl-ex"],"headline":"","license":"","primary_cat":"nucl-th","submitted_at":"2006-08-13T23:35:51Z","title":"Chiral effective theory predictions for deuteron form factor ratios at low Q^2"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0608036","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":"sha256:26734d40996627e82a70b99b33af6d8f2b9b54d7abb77a3d04c2b0ada0b73eff","target":"record","created_at":"2026-07-04T15:22:47Z","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":"4e1d966e93e60e2f67d9864b4e8bc99450296e6b0174c00e7e5a86c4b16392c4","cross_cats_sorted":["hep-ph","nucl-ex"],"license":"","primary_cat":"nucl-th","submitted_at":"2006-08-13T23:35:51Z","title_canon_sha256":"12277c0ce2d56a9a9eb11580df8baa5de05f49599e715b8568bd9334ec0dd447"},"schema_version":"1.0","source":{"id":"nucl-th/0608036","kind":"arxiv","version":1}},"canonical_sha256":"909ca6a0b8efa7850fc2ab0316ba686828be6bafe5b984818537470a7ce258d6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"909ca6a0b8efa7850fc2ab0316ba686828be6bafe5b984818537470a7ce258d6","first_computed_at":"2026-07-04T15:22:47.388044Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:22:47.388044Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"CaS8qCgS67fDldxod6Uywvpua14dDrfcEmPSPo5Bzyj9I+P7WUMrP6qQv5U3oHqVTJkjb7TR+74WmXQu2JCXAA==","signature_status":"signed_v1","signed_at":"2026-07-04T15:22:47.388453Z","signed_message":"canonical_sha256_bytes"},"source_id":"nucl-th/0608036","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:26734d40996627e82a70b99b33af6d8f2b9b54d7abb77a3d04c2b0ada0b73eff","sha256:938b1330ece315cf6f5628d905f5551d0bf4159625cea570a7671653f633bf30"],"state_sha256":"1b23708a6724eb4e05ead621456586c2ee48386fd59745934d588a34bdb7ea25"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3RR3H58Csd3yd4fwWPUlrFdrytTZnu4j8Z1jPW9ilpBIsvQvV2+C+ZzrbTEjLBXx3GvRSNW/hzh/so46jNYEDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-13T20:36:29.782378Z","bundle_sha256":"41434974c82e6bf779055d2afb5cd7b1442d608ce119697a4a6a1beb5d99574c"}}