{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:WWJ2B6SES4U6MQC3TRJ7XCM2ZV","short_pith_number":"pith:WWJ2B6SE","canonical_record":{"source":{"id":"1210.0677","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2012-10-02T07:35:47Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"e6d29d014fc8bfc692b7a20c4243431cb1c220ef012241c3aa89ccfab274b978","abstract_canon_sha256":"7d4c6ef37602b3f66eb0de656510a45b324b748e865957b9a7401bcaab9c8a97"},"schema_version":"1.0"},"canonical_sha256":"b593a0fa449729e6405b9c53fb899acd76bd9dd00e85f337d6238f4e8a028390","source":{"kind":"arxiv","id":"1210.0677","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1210.0677","created_at":"2026-05-18T03:44:14Z"},{"alias_kind":"arxiv_version","alias_value":"1210.0677v1","created_at":"2026-05-18T03:44:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.0677","created_at":"2026-05-18T03:44:14Z"},{"alias_kind":"pith_short_12","alias_value":"WWJ2B6SES4U6","created_at":"2026-05-18T12:27:27Z"},{"alias_kind":"pith_short_16","alias_value":"WWJ2B6SES4U6MQC3","created_at":"2026-05-18T12:27:27Z"},{"alias_kind":"pith_short_8","alias_value":"WWJ2B6SE","created_at":"2026-05-18T12:27:27Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:WWJ2B6SES4U6MQC3TRJ7XCM2ZV","target":"record","payload":{"canonical_record":{"source":{"id":"1210.0677","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2012-10-02T07:35:47Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"e6d29d014fc8bfc692b7a20c4243431cb1c220ef012241c3aa89ccfab274b978","abstract_canon_sha256":"7d4c6ef37602b3f66eb0de656510a45b324b748e865957b9a7401bcaab9c8a97"},"schema_version":"1.0"},"canonical_sha256":"b593a0fa449729e6405b9c53fb899acd76bd9dd00e85f337d6238f4e8a028390","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:44:14.531482Z","signature_b64":"47NjBsqvPdUbk/yKNrP90MOEqU+9yB1FZSUlgPDGRXEhMOQjH0cH8uTEk1+W8mjnk7NmYDLpt2uFuSC6+NnWAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b593a0fa449729e6405b9c53fb899acd76bd9dd00e85f337d6238f4e8a028390","last_reissued_at":"2026-05-18T03:44:14.531048Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:44:14.531048Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1210.0677","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":"2026-05-18T03:44:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2LO4R7ccOuFOzzQr48rLLMJibp0vyOYgPyrPVx0dIbeVsl171KxGu5/iDnQs9kie5e3JgQrXZSIIDLlMtQaKAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T21:56:53.774188Z"},"content_sha256":"70da11891a7224c673600414a6d974b62b8bc36603632742d9cf5a4d6f2778ee","schema_version":"1.0","event_id":"sha256:70da11891a7224c673600414a6d974b62b8bc36603632742d9cf5a4d6f2778ee"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:WWJ2B6SES4U6MQC3TRJ7XCM2ZV","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Resonant x-ray scattering from chiral materials, $\\alpha$-quartz and $\\alpha$-berlinite","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Jun-ichi Igarashi, Manabu Takahashi","submitted_at":"2012-10-02T07:35:47Z","abstract_excerpt":"We study the resonant x-ray scattering at Si and Al K-edges from chiral materials, $\\alpha$-quartz and $\\alpha$-berlinite. We derive the general form of the scattering matrix for the dipole transition by summing up the local scattering matrices which satisfy the symmetry requirement. The oscillation term is obtained in the spectral intensity as a function of azimuthal angle with an expression of possible phase shift. We evaluate the parameters undetermined by the symmetry argument alone on the basis of underlying electronic structures given by the bond-orbital model. The spectra are calculated"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.0677","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":""},"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":"2026-05-18T03:44:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/k0KEsyyGCRM1yd1JNl3zjcJoi47zfRZ6Y7cY9JSm0po4wef/0dNSgLL4K8oB1HQYr6vUzppOFDvgtTGfYmhDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T21:56:53.774560Z"},"content_sha256":"9ccc089f9aefe1c9afff4f681e70953ec89659880a1bdf0befb68aba625d28c7","schema_version":"1.0","event_id":"sha256:9ccc089f9aefe1c9afff4f681e70953ec89659880a1bdf0befb68aba625d28c7"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/WWJ2B6SES4U6MQC3TRJ7XCM2ZV/bundle.json","state_url":"https://pith.science/pith/WWJ2B6SES4U6MQC3TRJ7XCM2ZV/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/WWJ2B6SES4U6MQC3TRJ7XCM2ZV/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":"2026-06-02T21:56:53Z","links":{"resolver":"https://pith.science/pith/WWJ2B6SES4U6MQC3TRJ7XCM2ZV","bundle":"https://pith.science/pith/WWJ2B6SES4U6MQC3TRJ7XCM2ZV/bundle.json","state":"https://pith.science/pith/WWJ2B6SES4U6MQC3TRJ7XCM2ZV/state.json","well_known_bundle":"https://pith.science/.well-known/pith/WWJ2B6SES4U6MQC3TRJ7XCM2ZV/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:WWJ2B6SES4U6MQC3TRJ7XCM2ZV","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":"7d4c6ef37602b3f66eb0de656510a45b324b748e865957b9a7401bcaab9c8a97","cross_cats_sorted":["cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2012-10-02T07:35:47Z","title_canon_sha256":"e6d29d014fc8bfc692b7a20c4243431cb1c220ef012241c3aa89ccfab274b978"},"schema_version":"1.0","source":{"id":"1210.0677","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1210.0677","created_at":"2026-05-18T03:44:14Z"},{"alias_kind":"arxiv_version","alias_value":"1210.0677v1","created_at":"2026-05-18T03:44:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.0677","created_at":"2026-05-18T03:44:14Z"},{"alias_kind":"pith_short_12","alias_value":"WWJ2B6SES4U6","created_at":"2026-05-18T12:27:27Z"},{"alias_kind":"pith_short_16","alias_value":"WWJ2B6SES4U6MQC3","created_at":"2026-05-18T12:27:27Z"},{"alias_kind":"pith_short_8","alias_value":"WWJ2B6SE","created_at":"2026-05-18T12:27:27Z"}],"graph_snapshots":[{"event_id":"sha256:9ccc089f9aefe1c9afff4f681e70953ec89659880a1bdf0befb68aba625d28c7","target":"graph","created_at":"2026-05-18T03:44:14Z","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":"We study the resonant x-ray scattering at Si and Al K-edges from chiral materials, $\\alpha$-quartz and $\\alpha$-berlinite. We derive the general form of the scattering matrix for the dipole transition by summing up the local scattering matrices which satisfy the symmetry requirement. The oscillation term is obtained in the spectral intensity as a function of azimuthal angle with an expression of possible phase shift. We evaluate the parameters undetermined by the symmetry argument alone on the basis of underlying electronic structures given by the bond-orbital model. The spectra are calculated","authors_text":"Jun-ichi Igarashi, Manabu Takahashi","cross_cats":["cond-mat.str-el"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2012-10-02T07:35:47Z","title":"Resonant x-ray scattering from chiral materials, $\\alpha$-quartz and $\\alpha$-berlinite"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.0677","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":"sha256:70da11891a7224c673600414a6d974b62b8bc36603632742d9cf5a4d6f2778ee","target":"record","created_at":"2026-05-18T03:44:14Z","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":"7d4c6ef37602b3f66eb0de656510a45b324b748e865957b9a7401bcaab9c8a97","cross_cats_sorted":["cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2012-10-02T07:35:47Z","title_canon_sha256":"e6d29d014fc8bfc692b7a20c4243431cb1c220ef012241c3aa89ccfab274b978"},"schema_version":"1.0","source":{"id":"1210.0677","kind":"arxiv","version":1}},"canonical_sha256":"b593a0fa449729e6405b9c53fb899acd76bd9dd00e85f337d6238f4e8a028390","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b593a0fa449729e6405b9c53fb899acd76bd9dd00e85f337d6238f4e8a028390","first_computed_at":"2026-05-18T03:44:14.531048Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:44:14.531048Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"47NjBsqvPdUbk/yKNrP90MOEqU+9yB1FZSUlgPDGRXEhMOQjH0cH8uTEk1+W8mjnk7NmYDLpt2uFuSC6+NnWAA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:44:14.531482Z","signed_message":"canonical_sha256_bytes"},"source_id":"1210.0677","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:70da11891a7224c673600414a6d974b62b8bc36603632742d9cf5a4d6f2778ee","sha256:9ccc089f9aefe1c9afff4f681e70953ec89659880a1bdf0befb68aba625d28c7"],"state_sha256":"86fbfdf4459e4210ada8da3f69a8717f40a8ce85948bb7dde9d0aa0e3afb7824"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"J8mjDY0wWD3m9c4x2telU0EZ/glWX16E3VRnwSZ7v/Q3OZqDv5Gn7uzughIwRqrs2lX9iePqkMXcns4HL1wwBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T21:56:53.776467Z","bundle_sha256":"ac9f0ef264c6f31e91d2b45df87ac8157a28228706a5a979003fd5a8dabfa54f"}}