{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:2G5FEVLSNNLOOLL3UCVM4GY4KV","short_pith_number":"pith:2G5FEVLS","canonical_record":{"source":{"id":"1501.05509","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-01-22T14:28:42Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"a1b6c636d1e426d9edb827d704ccaf6bc0a344cfc3d49a228a09bc0f688bbb74","abstract_canon_sha256":"cec5f89ad012455b360e870f59bcd07574229e45a41c4f30ddc4884c9bee90bf"},"schema_version":"1.0"},"canonical_sha256":"d1ba5255726b56e72d7ba0aace1b1c55629641018c149aa222af7d94e713f46b","source":{"kind":"arxiv","id":"1501.05509","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1501.05509","created_at":"2026-05-18T02:27:56Z"},{"alias_kind":"arxiv_version","alias_value":"1501.05509v1","created_at":"2026-05-18T02:27:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1501.05509","created_at":"2026-05-18T02:27:56Z"},{"alias_kind":"pith_short_12","alias_value":"2G5FEVLSNNLO","created_at":"2026-05-18T12:28:59Z"},{"alias_kind":"pith_short_16","alias_value":"2G5FEVLSNNLOOLL3","created_at":"2026-05-18T12:28:59Z"},{"alias_kind":"pith_short_8","alias_value":"2G5FEVLS","created_at":"2026-05-18T12:28:59Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:2G5FEVLSNNLOOLL3UCVM4GY4KV","target":"record","payload":{"canonical_record":{"source":{"id":"1501.05509","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-01-22T14:28:42Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"a1b6c636d1e426d9edb827d704ccaf6bc0a344cfc3d49a228a09bc0f688bbb74","abstract_canon_sha256":"cec5f89ad012455b360e870f59bcd07574229e45a41c4f30ddc4884c9bee90bf"},"schema_version":"1.0"},"canonical_sha256":"d1ba5255726b56e72d7ba0aace1b1c55629641018c149aa222af7d94e713f46b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:27:56.755205Z","signature_b64":"GbURTIdfk0X4FBUcQIOiG0CN0her5cjQT7ymRZSqobrSRbPLdGC4MV3LObS5EmqUObcYaeFvMkpI1xBhAkzbBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d1ba5255726b56e72d7ba0aace1b1c55629641018c149aa222af7d94e713f46b","last_reissued_at":"2026-05-18T02:27:56.754791Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:27:56.754791Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1501.05509","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":"2026-05-18T02:27:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4DQ4e9zEhfwk03aLBxpzu/R3IfrhkDNGlH6oMc5FdLZh5NXnWXShOw2Jvtaaa758vAOFl7Onsh++ym3fCg5KCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T11:49:48.941738Z"},"content_sha256":"09d1fdb6a419e62ff20499a21e54100f8cd4e92ca0a9fefa106540cebbe07f66","schema_version":"1.0","event_id":"sha256:09d1fdb6a419e62ff20499a21e54100f8cd4e92ca0a9fefa106540cebbe07f66"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:2G5FEVLSNNLOOLL3UCVM4GY4KV","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Relativistic dynamical spin excitations of magnetic adatoms","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mes-hall","authors_text":"Benedikt Schweflinghaus, Manuel dos Santos Dias, Samir Lounis, Stefan Bl\\\"ugel","submitted_at":"2015-01-22T14:28:42Z","abstract_excerpt":"We present a first-principles theory of dynamical spin excitations in the presence of spin-orbit coupling. The broken global spin rotational invariance leads to a new sum rule. We explore the competition between the magnetic anisotropy energy and the external magnetic field, as well as the role of electron-hole excitations, through calculations for 3$d$-metal adatoms on the Cu(111) surface. The spin excitation resonance energy and lifetime display non-trivial behavior, establishing the strong impact of relativistic effects. We legitimate the use of the Landau-Lifshitz-Gilbert equation down to "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1501.05509","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":"2026-05-18T02:27:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VXvYHq79WCe2s0MxMLPNshhpLMh/T3zatLoXWb71uydu5/lDynrRo2H7+r+8iPYVIidK3Rbktd+tlEI05SHAAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T11:49:48.942194Z"},"content_sha256":"9624fb1cf62482beddc800262c443783bebb7f5440c03e706916fc9e11f722e8","schema_version":"1.0","event_id":"sha256:9624fb1cf62482beddc800262c443783bebb7f5440c03e706916fc9e11f722e8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2G5FEVLSNNLOOLL3UCVM4GY4KV/bundle.json","state_url":"https://pith.science/pith/2G5FEVLSNNLOOLL3UCVM4GY4KV/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2G5FEVLSNNLOOLL3UCVM4GY4KV/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":"2026-05-27T11:49:48Z","links":{"resolver":"https://pith.science/pith/2G5FEVLSNNLOOLL3UCVM4GY4KV","bundle":"https://pith.science/pith/2G5FEVLSNNLOOLL3UCVM4GY4KV/bundle.json","state":"https://pith.science/pith/2G5FEVLSNNLOOLL3UCVM4GY4KV/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2G5FEVLSNNLOOLL3UCVM4GY4KV/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:2G5FEVLSNNLOOLL3UCVM4GY4KV","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":"cec5f89ad012455b360e870f59bcd07574229e45a41c4f30ddc4884c9bee90bf","cross_cats_sorted":["cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-01-22T14:28:42Z","title_canon_sha256":"a1b6c636d1e426d9edb827d704ccaf6bc0a344cfc3d49a228a09bc0f688bbb74"},"schema_version":"1.0","source":{"id":"1501.05509","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1501.05509","created_at":"2026-05-18T02:27:56Z"},{"alias_kind":"arxiv_version","alias_value":"1501.05509v1","created_at":"2026-05-18T02:27:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1501.05509","created_at":"2026-05-18T02:27:56Z"},{"alias_kind":"pith_short_12","alias_value":"2G5FEVLSNNLO","created_at":"2026-05-18T12:28:59Z"},{"alias_kind":"pith_short_16","alias_value":"2G5FEVLSNNLOOLL3","created_at":"2026-05-18T12:28:59Z"},{"alias_kind":"pith_short_8","alias_value":"2G5FEVLS","created_at":"2026-05-18T12:28:59Z"}],"graph_snapshots":[{"event_id":"sha256:9624fb1cf62482beddc800262c443783bebb7f5440c03e706916fc9e11f722e8","target":"graph","created_at":"2026-05-18T02:27:56Z","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 present a first-principles theory of dynamical spin excitations in the presence of spin-orbit coupling. The broken global spin rotational invariance leads to a new sum rule. We explore the competition between the magnetic anisotropy energy and the external magnetic field, as well as the role of electron-hole excitations, through calculations for 3$d$-metal adatoms on the Cu(111) surface. The spin excitation resonance energy and lifetime display non-trivial behavior, establishing the strong impact of relativistic effects. We legitimate the use of the Landau-Lifshitz-Gilbert equation down to ","authors_text":"Benedikt Schweflinghaus, Manuel dos Santos Dias, Samir Lounis, Stefan Bl\\\"ugel","cross_cats":["cond-mat.str-el"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-01-22T14:28:42Z","title":"Relativistic dynamical spin excitations of magnetic adatoms"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1501.05509","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":"sha256:09d1fdb6a419e62ff20499a21e54100f8cd4e92ca0a9fefa106540cebbe07f66","target":"record","created_at":"2026-05-18T02:27:56Z","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":"cec5f89ad012455b360e870f59bcd07574229e45a41c4f30ddc4884c9bee90bf","cross_cats_sorted":["cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-01-22T14:28:42Z","title_canon_sha256":"a1b6c636d1e426d9edb827d704ccaf6bc0a344cfc3d49a228a09bc0f688bbb74"},"schema_version":"1.0","source":{"id":"1501.05509","kind":"arxiv","version":1}},"canonical_sha256":"d1ba5255726b56e72d7ba0aace1b1c55629641018c149aa222af7d94e713f46b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d1ba5255726b56e72d7ba0aace1b1c55629641018c149aa222af7d94e713f46b","first_computed_at":"2026-05-18T02:27:56.754791Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:27:56.754791Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"GbURTIdfk0X4FBUcQIOiG0CN0her5cjQT7ymRZSqobrSRbPLdGC4MV3LObS5EmqUObcYaeFvMkpI1xBhAkzbBg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:27:56.755205Z","signed_message":"canonical_sha256_bytes"},"source_id":"1501.05509","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:09d1fdb6a419e62ff20499a21e54100f8cd4e92ca0a9fefa106540cebbe07f66","sha256:9624fb1cf62482beddc800262c443783bebb7f5440c03e706916fc9e11f722e8"],"state_sha256":"4c2b12ac86f694ae493574942428075727787ca41001442afbcc1085cd92e105"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ws2jZqDmc8+ZZIgBQQMq0gpEao+AYkG6kg7UNOgnRJpKG8tmCXn+/299tOQe2/k764CBavQlEAwIDzj0Nq7cCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T11:49:48.946329Z","bundle_sha256":"92b36e15c90221068425d2c34c82cc9328b279368616c5e5126ce4f2ac249134"}}