{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:2FMEVN5N2EKW27JN55KYHPGW5K","short_pith_number":"pith:2FMEVN5N","canonical_record":{"source":{"id":"1610.03886","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2016-10-12T21:24:13Z","cross_cats_sorted":["nucl-ex","physics.ins-det"],"title_canon_sha256":"2a0dded4823b4f0abba87d5aae3e85767a96aae997a9af6a9ef88b2e50779bfd","abstract_canon_sha256":"f5715691dcedeea702e07f67504756d953d9a57a5ce880c1c0a81c3432198996"},"schema_version":"1.0"},"canonical_sha256":"d1584ab7add1156d7d2def5583bcd6eab9feb0731f66fce11dd6934b90472278","source":{"kind":"arxiv","id":"1610.03886","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1610.03886","created_at":"2026-05-18T00:51:22Z"},{"alias_kind":"arxiv_version","alias_value":"1610.03886v2","created_at":"2026-05-18T00:51:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.03886","created_at":"2026-05-18T00:51:22Z"},{"alias_kind":"pith_short_12","alias_value":"2FMEVN5N2EKW","created_at":"2026-05-18T12:29:55Z"},{"alias_kind":"pith_short_16","alias_value":"2FMEVN5N2EKW27JN","created_at":"2026-05-18T12:29:55Z"},{"alias_kind":"pith_short_8","alias_value":"2FMEVN5N","created_at":"2026-05-18T12:29:55Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:2FMEVN5N2EKW27JN55KYHPGW5K","target":"record","payload":{"canonical_record":{"source":{"id":"1610.03886","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2016-10-12T21:24:13Z","cross_cats_sorted":["nucl-ex","physics.ins-det"],"title_canon_sha256":"2a0dded4823b4f0abba87d5aae3e85767a96aae997a9af6a9ef88b2e50779bfd","abstract_canon_sha256":"f5715691dcedeea702e07f67504756d953d9a57a5ce880c1c0a81c3432198996"},"schema_version":"1.0"},"canonical_sha256":"d1584ab7add1156d7d2def5583bcd6eab9feb0731f66fce11dd6934b90472278","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:51:22.447308Z","signature_b64":"4jr68uQ44/ejSsoM3F1BEZvBBoHJzCmFkkAXFIt6oX2SVdseKG/t5B94yacLZ15o3hHNsOdnVzLba7tdq5zfAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d1584ab7add1156d7d2def5583bcd6eab9feb0731f66fce11dd6934b90472278","last_reissued_at":"2026-05-18T00:51:22.446522Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:51:22.446522Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1610.03886","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":"2026-05-18T00:51:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xoMnlQrV5xaqYbG2sN7RTdGwZJiQ/obqHIaxADnisr/YZXzUPrxPEdF5yp8PZC89zW5PoYjQLP1hEu5lGYcXAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T05:14:50.208094Z"},"content_sha256":"b3bccc0e5163929c34e5ff9796e0f239fb301e6a78b8954e82dfc2af47b94556","schema_version":"1.0","event_id":"sha256:b3bccc0e5163929c34e5ff9796e0f239fb301e6a78b8954e82dfc2af47b94556"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:2FMEVN5N2EKW27JN55KYHPGW5K","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Solar Axion Search Technique with Correlated Signals from Multiple Detectors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex","physics.ins-det"],"primary_cat":"hep-ex","authors_text":"Steven R. Elliott, Wenqin Xu","submitted_at":"2016-10-12T21:24:13Z","abstract_excerpt":"The coherent Bragg scattering of photons converted from solar axions inside crystals would boost the signal for axion-photon coupling enhancing experimental sensitivity for these hypothetical particles. Knowledge of the scattering angle of solar axions with respect to the crystal lattice is required to make theoretical predications of signal strength. Hence, both the lattice axis angle within a crystal and the absolute angle between the crystal and the Sun must be known. In this paper, we examine how the experimental sensitivity changes with respect to various experimental parameters. We also "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.03886","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":""},"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":"2026-05-18T00:51:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OamcZ3TVR3bgng91rzYoQvuqdP+jl5O/sezTxtzK07almYrDT+G+UCHF+sD4rFQpTBqUGUb0rrCamY4Dia82DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T05:14:50.208757Z"},"content_sha256":"7f11e6d546208b92ad4e600e8f071aae2920ce393bbf3fe048bfa92b176c400c","schema_version":"1.0","event_id":"sha256:7f11e6d546208b92ad4e600e8f071aae2920ce393bbf3fe048bfa92b176c400c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2FMEVN5N2EKW27JN55KYHPGW5K/bundle.json","state_url":"https://pith.science/pith/2FMEVN5N2EKW27JN55KYHPGW5K/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2FMEVN5N2EKW27JN55KYHPGW5K/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":"2026-06-02T05:14:50Z","links":{"resolver":"https://pith.science/pith/2FMEVN5N2EKW27JN55KYHPGW5K","bundle":"https://pith.science/pith/2FMEVN5N2EKW27JN55KYHPGW5K/bundle.json","state":"https://pith.science/pith/2FMEVN5N2EKW27JN55KYHPGW5K/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2FMEVN5N2EKW27JN55KYHPGW5K/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:2FMEVN5N2EKW27JN55KYHPGW5K","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":"f5715691dcedeea702e07f67504756d953d9a57a5ce880c1c0a81c3432198996","cross_cats_sorted":["nucl-ex","physics.ins-det"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2016-10-12T21:24:13Z","title_canon_sha256":"2a0dded4823b4f0abba87d5aae3e85767a96aae997a9af6a9ef88b2e50779bfd"},"schema_version":"1.0","source":{"id":"1610.03886","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1610.03886","created_at":"2026-05-18T00:51:22Z"},{"alias_kind":"arxiv_version","alias_value":"1610.03886v2","created_at":"2026-05-18T00:51:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.03886","created_at":"2026-05-18T00:51:22Z"},{"alias_kind":"pith_short_12","alias_value":"2FMEVN5N2EKW","created_at":"2026-05-18T12:29:55Z"},{"alias_kind":"pith_short_16","alias_value":"2FMEVN5N2EKW27JN","created_at":"2026-05-18T12:29:55Z"},{"alias_kind":"pith_short_8","alias_value":"2FMEVN5N","created_at":"2026-05-18T12:29:55Z"}],"graph_snapshots":[{"event_id":"sha256:7f11e6d546208b92ad4e600e8f071aae2920ce393bbf3fe048bfa92b176c400c","target":"graph","created_at":"2026-05-18T00:51:22Z","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":"The coherent Bragg scattering of photons converted from solar axions inside crystals would boost the signal for axion-photon coupling enhancing experimental sensitivity for these hypothetical particles. Knowledge of the scattering angle of solar axions with respect to the crystal lattice is required to make theoretical predications of signal strength. Hence, both the lattice axis angle within a crystal and the absolute angle between the crystal and the Sun must be known. In this paper, we examine how the experimental sensitivity changes with respect to various experimental parameters. We also ","authors_text":"Steven R. Elliott, Wenqin Xu","cross_cats":["nucl-ex","physics.ins-det"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2016-10-12T21:24:13Z","title":"Solar Axion Search Technique with Correlated Signals from Multiple Detectors"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.03886","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:b3bccc0e5163929c34e5ff9796e0f239fb301e6a78b8954e82dfc2af47b94556","target":"record","created_at":"2026-05-18T00:51:22Z","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":"f5715691dcedeea702e07f67504756d953d9a57a5ce880c1c0a81c3432198996","cross_cats_sorted":["nucl-ex","physics.ins-det"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2016-10-12T21:24:13Z","title_canon_sha256":"2a0dded4823b4f0abba87d5aae3e85767a96aae997a9af6a9ef88b2e50779bfd"},"schema_version":"1.0","source":{"id":"1610.03886","kind":"arxiv","version":2}},"canonical_sha256":"d1584ab7add1156d7d2def5583bcd6eab9feb0731f66fce11dd6934b90472278","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d1584ab7add1156d7d2def5583bcd6eab9feb0731f66fce11dd6934b90472278","first_computed_at":"2026-05-18T00:51:22.446522Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:51:22.446522Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"4jr68uQ44/ejSsoM3F1BEZvBBoHJzCmFkkAXFIt6oX2SVdseKG/t5B94yacLZ15o3hHNsOdnVzLba7tdq5zfAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:51:22.447308Z","signed_message":"canonical_sha256_bytes"},"source_id":"1610.03886","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b3bccc0e5163929c34e5ff9796e0f239fb301e6a78b8954e82dfc2af47b94556","sha256:7f11e6d546208b92ad4e600e8f071aae2920ce393bbf3fe048bfa92b176c400c"],"state_sha256":"604a59fd750fecceedec0eed5669b09aba2f7087ec106fa32eb687791aa24a9e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KJ2m9pDLrsZ+YksWUvDZH0tvqUARrChdsr86UXLOhBkGeOihA1cD59MMw5sAfDkTLh+RuJDcror8iUeo6IFRBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T05:14:50.212035Z","bundle_sha256":"c1eab8fce093a966e45b817931dafeb275a921e1d5728e8fc30de3df5def9343"}}