{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:RIQ7QHNLEJN3TCQSCQZ2V3EHMZ","short_pith_number":"pith:RIQ7QHNL","schema_version":"1.0","canonical_sha256":"8a21f81dab225bb98a121433aaec876667be473129102b15016f7d8e4a568cca","source":{"kind":"arxiv","id":"1706.05478","version":2},"attestation_state":"computed","paper":{"title":"Magnon-phonon coupling effects on the indirect K-edge resonant inelastic X-ray scattering spectrum of a 2D Heisenberg antiferromagnet","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Dao-Xin Yao, Kenneth Stiwinter, Trinanjan Datta, Zijian Xiong","submitted_at":"2017-06-17T05:46:58Z","abstract_excerpt":"We compute the effects of magnon-phonon coupling on the indirect K-edge bimagnon resonant inelastic x-ray scattering (RIXS) intensity spectrum of a square lattice Heisenberg antiferromagnet. We analyze the effects of competing nearest and next--nearest magnetic and magnon-phonon coupling interaction in the RIXS spectrum, for both the antiferromagnetic (AF) and the collinear antiferromagnetic (CAF) phases of the model. Utilizing the Dyson-Maleev representation of spin operators, the Bethe-Salpeter ladder approximation scheme for the bimagnon interacting channel, and considering the lowest order"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1706.05478","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-06-17T05:46:58Z","cross_cats_sorted":[],"title_canon_sha256":"8ed7f264d1476b2d6c03a0facabe4e955351738db2b3a1276f3217efd1fac85d","abstract_canon_sha256":"594409b94ead706bcca27677f4ca661df0a78bba222f44593787c0a2aba9537e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:31:35.842430Z","signature_b64":"dOmnu/BL1V3wKSZLJ5DcG+N25EStQH2DiM01MnknT51v6nTeh0jbtjbMbhXb/t+5Yn5SRRub8VKrFRuh4gL7BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8a21f81dab225bb98a121433aaec876667be473129102b15016f7d8e4a568cca","last_reissued_at":"2026-05-18T00:31:35.841927Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:31:35.841927Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Magnon-phonon coupling effects on the indirect K-edge resonant inelastic X-ray scattering spectrum of a 2D Heisenberg antiferromagnet","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Dao-Xin Yao, Kenneth Stiwinter, Trinanjan Datta, Zijian Xiong","submitted_at":"2017-06-17T05:46:58Z","abstract_excerpt":"We compute the effects of magnon-phonon coupling on the indirect K-edge bimagnon resonant inelastic x-ray scattering (RIXS) intensity spectrum of a square lattice Heisenberg antiferromagnet. We analyze the effects of competing nearest and next--nearest magnetic and magnon-phonon coupling interaction in the RIXS spectrum, for both the antiferromagnetic (AF) and the collinear antiferromagnetic (CAF) phases of the model. Utilizing the Dyson-Maleev representation of spin operators, the Bethe-Salpeter ladder approximation scheme for the bimagnon interacting channel, and considering the lowest order"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.05478","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1706.05478","created_at":"2026-05-18T00:31:35.842002+00:00"},{"alias_kind":"arxiv_version","alias_value":"1706.05478v2","created_at":"2026-05-18T00:31:35.842002+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.05478","created_at":"2026-05-18T00:31:35.842002+00:00"},{"alias_kind":"pith_short_12","alias_value":"RIQ7QHNLEJN3","created_at":"2026-05-18T12:31:39.905425+00:00"},{"alias_kind":"pith_short_16","alias_value":"RIQ7QHNLEJN3TCQS","created_at":"2026-05-18T12:31:39.905425+00:00"},{"alias_kind":"pith_short_8","alias_value":"RIQ7QHNL","created_at":"2026-05-18T12:31:39.905425+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RIQ7QHNLEJN3TCQSCQZ2V3EHMZ","json":"https://pith.science/pith/RIQ7QHNLEJN3TCQSCQZ2V3EHMZ.json","graph_json":"https://pith.science/api/pith-number/RIQ7QHNLEJN3TCQSCQZ2V3EHMZ/graph.json","events_json":"https://pith.science/api/pith-number/RIQ7QHNLEJN3TCQSCQZ2V3EHMZ/events.json","paper":"https://pith.science/paper/RIQ7QHNL"},"agent_actions":{"view_html":"https://pith.science/pith/RIQ7QHNLEJN3TCQSCQZ2V3EHMZ","download_json":"https://pith.science/pith/RIQ7QHNLEJN3TCQSCQZ2V3EHMZ.json","view_paper":"https://pith.science/paper/RIQ7QHNL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1706.05478&json=true","fetch_graph":"https://pith.science/api/pith-number/RIQ7QHNLEJN3TCQSCQZ2V3EHMZ/graph.json","fetch_events":"https://pith.science/api/pith-number/RIQ7QHNLEJN3TCQSCQZ2V3EHMZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RIQ7QHNLEJN3TCQSCQZ2V3EHMZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RIQ7QHNLEJN3TCQSCQZ2V3EHMZ/action/storage_attestation","attest_author":"https://pith.science/pith/RIQ7QHNLEJN3TCQSCQZ2V3EHMZ/action/author_attestation","sign_citation":"https://pith.science/pith/RIQ7QHNLEJN3TCQSCQZ2V3EHMZ/action/citation_signature","submit_replication":"https://pith.science/pith/RIQ7QHNLEJN3TCQSCQZ2V3EHMZ/action/replication_record"}},"created_at":"2026-05-18T00:31:35.842002+00:00","updated_at":"2026-05-18T00:31:35.842002+00:00"}