{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:67QKHLOK6AHPCWLD4DS33WD6IN","short_pith_number":"pith:67QKHLOK","canonical_record":{"source":{"id":"1702.05337","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-02-17T13:37:14Z","cross_cats_sorted":["hep-ex","hep-lat","nucl-ex","nucl-th"],"title_canon_sha256":"d505598573c058e8ce27e90d1f0f31c1f9372fefafb68e4facb4e6c721e6dfce","abstract_canon_sha256":"d675044cfa68975e4e2709308edc149c0760b6d8648d56581986ce27a126eb0d"},"schema_version":"1.0"},"canonical_sha256":"f7e0a3adcaf00ef15963e0e5bdd87e43653f019d317a1dbf8ab443c874837bd8","source":{"kind":"arxiv","id":"1702.05337","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1702.05337","created_at":"2026-05-18T00:43:54Z"},{"alias_kind":"arxiv_version","alias_value":"1702.05337v3","created_at":"2026-05-18T00:43:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.05337","created_at":"2026-05-18T00:43:54Z"},{"alias_kind":"pith_short_12","alias_value":"67QKHLOK6AHP","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_16","alias_value":"67QKHLOK6AHPCWLD","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_8","alias_value":"67QKHLOK","created_at":"2026-05-18T12:31:03Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:67QKHLOK6AHPCWLD4DS33WD6IN","target":"record","payload":{"canonical_record":{"source":{"id":"1702.05337","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-02-17T13:37:14Z","cross_cats_sorted":["hep-ex","hep-lat","nucl-ex","nucl-th"],"title_canon_sha256":"d505598573c058e8ce27e90d1f0f31c1f9372fefafb68e4facb4e6c721e6dfce","abstract_canon_sha256":"d675044cfa68975e4e2709308edc149c0760b6d8648d56581986ce27a126eb0d"},"schema_version":"1.0"},"canonical_sha256":"f7e0a3adcaf00ef15963e0e5bdd87e43653f019d317a1dbf8ab443c874837bd8","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:43:54.465481Z","signature_b64":"V9jNqDg0/ovx6Thc/TB08ZJiEv5Vwq9lWoBbFiw9KxZdWbDS7AVjsLpTcpk0cBRR7P0tilMBV3aB7SOXZ+BsBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f7e0a3adcaf00ef15963e0e5bdd87e43653f019d317a1dbf8ab443c874837bd8","last_reissued_at":"2026-05-18T00:43:54.464759Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:43:54.464759Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1702.05337","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:43:54Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ox3TFgf0/lp3GSP9EhLSrpYcKMxM0JUJPojr5bKFbfRRj3hLFm5iph73jlfafmFNJ8MC0X7xK/Wf7N/9Xn7YDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-05T02:56:47.853391Z"},"content_sha256":"93fbb971cc959553dd80515f249c2e0072a91bf12e2fa5ef58140649e0b585a7","schema_version":"1.0","event_id":"sha256:93fbb971cc959553dd80515f249c2e0072a91bf12e2fa5ef58140649e0b585a7"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:67QKHLOK6AHPCWLD4DS33WD6IN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Tensor-polarized structure function $b_1$ in the standard convolution description of the deuteron","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"M. Sargsian, S. Kumano, W. Cosyn, Yu-bing Dong","submitted_at":"2017-02-17T13:37:14Z","abstract_excerpt":"Tensor-polarized structure functions of a spin-1 hadron are additional observables which do not exist for the spin-1/2 nucleon. They could probe novel aspects of the internal hadron structure. Twist-2 tensor-polarized structure functions are $b_1$ and $b_2$, and they are related by the Callan-Gross-like relation in the Bjorken scaling limit. In this work, we theoretically calculate $b_1$ in the standard convolution description for the deuteron. Two different theoretical models, a basic convolution description and a virtual nucleon approximation, are used for calculating $b_1$ and their results"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.05337","kind":"arxiv","version":3},"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":"2026-05-18T00:43:54Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bPBqairUcOJzJIqJ9qxaIzJnMeWx6TOr/4R+Vmspt+kP+E5wBrW4E13bcxnFZH49g9KG3yWkARPVcYrM9ksGAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-05T02:56:47.853746Z"},"content_sha256":"6cbbe79b734a76d043993d7ed77f108151636790a884d28d0de486b0de0476b2","schema_version":"1.0","event_id":"sha256:6cbbe79b734a76d043993d7ed77f108151636790a884d28d0de486b0de0476b2"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/67QKHLOK6AHPCWLD4DS33WD6IN/bundle.json","state_url":"https://pith.science/pith/67QKHLOK6AHPCWLD4DS33WD6IN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/67QKHLOK6AHPCWLD4DS33WD6IN/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":"2026-07-05T02:56:47Z","links":{"resolver":"https://pith.science/pith/67QKHLOK6AHPCWLD4DS33WD6IN","bundle":"https://pith.science/pith/67QKHLOK6AHPCWLD4DS33WD6IN/bundle.json","state":"https://pith.science/pith/67QKHLOK6AHPCWLD4DS33WD6IN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/67QKHLOK6AHPCWLD4DS33WD6IN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:67QKHLOK6AHPCWLD4DS33WD6IN","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":"d675044cfa68975e4e2709308edc149c0760b6d8648d56581986ce27a126eb0d","cross_cats_sorted":["hep-ex","hep-lat","nucl-ex","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-02-17T13:37:14Z","title_canon_sha256":"d505598573c058e8ce27e90d1f0f31c1f9372fefafb68e4facb4e6c721e6dfce"},"schema_version":"1.0","source":{"id":"1702.05337","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1702.05337","created_at":"2026-05-18T00:43:54Z"},{"alias_kind":"arxiv_version","alias_value":"1702.05337v3","created_at":"2026-05-18T00:43:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.05337","created_at":"2026-05-18T00:43:54Z"},{"alias_kind":"pith_short_12","alias_value":"67QKHLOK6AHP","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_16","alias_value":"67QKHLOK6AHPCWLD","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_8","alias_value":"67QKHLOK","created_at":"2026-05-18T12:31:03Z"}],"graph_snapshots":[{"event_id":"sha256:6cbbe79b734a76d043993d7ed77f108151636790a884d28d0de486b0de0476b2","target":"graph","created_at":"2026-05-18T00:43:54Z","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":"Tensor-polarized structure functions of a spin-1 hadron are additional observables which do not exist for the spin-1/2 nucleon. They could probe novel aspects of the internal hadron structure. Twist-2 tensor-polarized structure functions are $b_1$ and $b_2$, and they are related by the Callan-Gross-like relation in the Bjorken scaling limit. In this work, we theoretically calculate $b_1$ in the standard convolution description for the deuteron. Two different theoretical models, a basic convolution description and a virtual nucleon approximation, are used for calculating $b_1$ and their results","authors_text":"M. Sargsian, S. Kumano, W. Cosyn, Yu-bing Dong","cross_cats":["hep-ex","hep-lat","nucl-ex","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-02-17T13:37:14Z","title":"Tensor-polarized structure function $b_1$ in the standard convolution description of the deuteron"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.05337","kind":"arxiv","version":3},"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":"sha256:93fbb971cc959553dd80515f249c2e0072a91bf12e2fa5ef58140649e0b585a7","target":"record","created_at":"2026-05-18T00:43:54Z","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":"d675044cfa68975e4e2709308edc149c0760b6d8648d56581986ce27a126eb0d","cross_cats_sorted":["hep-ex","hep-lat","nucl-ex","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-02-17T13:37:14Z","title_canon_sha256":"d505598573c058e8ce27e90d1f0f31c1f9372fefafb68e4facb4e6c721e6dfce"},"schema_version":"1.0","source":{"id":"1702.05337","kind":"arxiv","version":3}},"canonical_sha256":"f7e0a3adcaf00ef15963e0e5bdd87e43653f019d317a1dbf8ab443c874837bd8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f7e0a3adcaf00ef15963e0e5bdd87e43653f019d317a1dbf8ab443c874837bd8","first_computed_at":"2026-05-18T00:43:54.464759Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:43:54.464759Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"V9jNqDg0/ovx6Thc/TB08ZJiEv5Vwq9lWoBbFiw9KxZdWbDS7AVjsLpTcpk0cBRR7P0tilMBV3aB7SOXZ+BsBA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:43:54.465481Z","signed_message":"canonical_sha256_bytes"},"source_id":"1702.05337","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:93fbb971cc959553dd80515f249c2e0072a91bf12e2fa5ef58140649e0b585a7","sha256:6cbbe79b734a76d043993d7ed77f108151636790a884d28d0de486b0de0476b2"],"state_sha256":"c81cfc607171ae792d5aead41d76c670f589a51657dd6b0ea520771b4d13f3f1"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"inwg84LDPbtbAJaIAmQDT/uZ1qvXqyUng92ARKtNKvumOqbxV/3d5B9gD2TnR+61Z7utReA+lGuVajmfytkwBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-05T02:56:47.855724Z","bundle_sha256":"6cb1986d89974ea95974a6babb9555b8c12cdfe2c313b4c40a2adbf5bebb5411"}}