{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:QF72GWSUTFX2NILHSDXV7G7KMB","short_pith_number":"pith:QF72GWSU","canonical_record":{"source":{"id":"1508.06081","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2015-08-25T09:19:03Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"a3605b631707e5ac16da29972ca1800eec6568c30b279a02039d4cc8d2e55491","abstract_canon_sha256":"261246bfda4aaa9934a6587f88a7ea957ab80c3defe8b47777c67e0419e6b347"},"schema_version":"1.0"},"canonical_sha256":"817fa35a54996fa6a16790ef5f9bea607f32d74f4efcc603052b475dcc05f5d1","source":{"kind":"arxiv","id":"1508.06081","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1508.06081","created_at":"2026-05-18T01:34:46Z"},{"alias_kind":"arxiv_version","alias_value":"1508.06081v1","created_at":"2026-05-18T01:34:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1508.06081","created_at":"2026-05-18T01:34:46Z"},{"alias_kind":"pith_short_12","alias_value":"QF72GWSUTFX2","created_at":"2026-05-18T12:29:37Z"},{"alias_kind":"pith_short_16","alias_value":"QF72GWSUTFX2NILH","created_at":"2026-05-18T12:29:37Z"},{"alias_kind":"pith_short_8","alias_value":"QF72GWSU","created_at":"2026-05-18T12:29:37Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:QF72GWSUTFX2NILHSDXV7G7KMB","target":"record","payload":{"canonical_record":{"source":{"id":"1508.06081","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2015-08-25T09:19:03Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"a3605b631707e5ac16da29972ca1800eec6568c30b279a02039d4cc8d2e55491","abstract_canon_sha256":"261246bfda4aaa9934a6587f88a7ea957ab80c3defe8b47777c67e0419e6b347"},"schema_version":"1.0"},"canonical_sha256":"817fa35a54996fa6a16790ef5f9bea607f32d74f4efcc603052b475dcc05f5d1","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:34:46.940890Z","signature_b64":"V/iypqLroiMVW9UxEYf/4SRD1xgPJOEkuyYSnEudC0vxGBgguHg74tKGKFn6xTXU9F8gAU8wU7bYzRuXnT4VCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"817fa35a54996fa6a16790ef5f9bea607f32d74f4efcc603052b475dcc05f5d1","last_reissued_at":"2026-05-18T01:34:46.940279Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:34:46.940279Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1508.06081","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":"2026-05-18T01:34:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"owIM6UUc0q0Ba+23Ii9SliENlIWBqIKU0Crlp5BLa+YWenrXVxqIeYylQIrRf+onZIKoYxeWxLmG2KqK4dLNCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T11:59:37.949184Z"},"content_sha256":"a23d909edfdc2bd38e14197390d6000bb091994e97137dbd67f7acb14211c77d","schema_version":"1.0","event_id":"sha256:a23d909edfdc2bd38e14197390d6000bb091994e97137dbd67f7acb14211c77d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:QF72GWSUTFX2NILHSDXV7G7KMB","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Polarizability Tensor Calculation: Induced Local Charge and Current Distributions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"physics.class-ph","authors_text":"Constantin Simovski, Mohammad Albooyeh, Mohammad Yazdi, Nader Komjani","submitted_at":"2015-08-25T09:19:03Z","abstract_excerpt":"We develop a semi-analytical approach to calculate the polarizability tensors of an arbitrary individual scatterer. The approach is based on the calculation of induced electric and/or magnetic dipole moments on the scatterer. By taking the advantages of the present approach, we calculate the individual polarizability tensors of an isolated scatterer in a homogeneous isotropic medium. Moreover, we obtain the polarizability tensors of scatterers located between two different isotropic media. Furthermore, due to the nature of the proposed method, we may determine the effective polarizability of a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1508.06081","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":"2026-05-18T01:34:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Etm4kNCWR2KYpe2rIDZ73ntzQuf2WySIIv/nhYUHKN8rtRmFhXo0dQZvoTMwnnWXw7fxSqXeUNRf6WsqvxtoAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T11:59:37.949560Z"},"content_sha256":"db2dc113b9de06cd00c881b26850698a55a0790dc37797a7c13bbc0a3ca9deac","schema_version":"1.0","event_id":"sha256:db2dc113b9de06cd00c881b26850698a55a0790dc37797a7c13bbc0a3ca9deac"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/QF72GWSUTFX2NILHSDXV7G7KMB/bundle.json","state_url":"https://pith.science/pith/QF72GWSUTFX2NILHSDXV7G7KMB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/QF72GWSUTFX2NILHSDXV7G7KMB/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":"2026-06-11T11:59:37Z","links":{"resolver":"https://pith.science/pith/QF72GWSUTFX2NILHSDXV7G7KMB","bundle":"https://pith.science/pith/QF72GWSUTFX2NILHSDXV7G7KMB/bundle.json","state":"https://pith.science/pith/QF72GWSUTFX2NILHSDXV7G7KMB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/QF72GWSUTFX2NILHSDXV7G7KMB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:QF72GWSUTFX2NILHSDXV7G7KMB","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":"261246bfda4aaa9934a6587f88a7ea957ab80c3defe8b47777c67e0419e6b347","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2015-08-25T09:19:03Z","title_canon_sha256":"a3605b631707e5ac16da29972ca1800eec6568c30b279a02039d4cc8d2e55491"},"schema_version":"1.0","source":{"id":"1508.06081","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1508.06081","created_at":"2026-05-18T01:34:46Z"},{"alias_kind":"arxiv_version","alias_value":"1508.06081v1","created_at":"2026-05-18T01:34:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1508.06081","created_at":"2026-05-18T01:34:46Z"},{"alias_kind":"pith_short_12","alias_value":"QF72GWSUTFX2","created_at":"2026-05-18T12:29:37Z"},{"alias_kind":"pith_short_16","alias_value":"QF72GWSUTFX2NILH","created_at":"2026-05-18T12:29:37Z"},{"alias_kind":"pith_short_8","alias_value":"QF72GWSU","created_at":"2026-05-18T12:29:37Z"}],"graph_snapshots":[{"event_id":"sha256:db2dc113b9de06cd00c881b26850698a55a0790dc37797a7c13bbc0a3ca9deac","target":"graph","created_at":"2026-05-18T01:34:46Z","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 develop a semi-analytical approach to calculate the polarizability tensors of an arbitrary individual scatterer. The approach is based on the calculation of induced electric and/or magnetic dipole moments on the scatterer. By taking the advantages of the present approach, we calculate the individual polarizability tensors of an isolated scatterer in a homogeneous isotropic medium. Moreover, we obtain the polarizability tensors of scatterers located between two different isotropic media. Furthermore, due to the nature of the proposed method, we may determine the effective polarizability of a","authors_text":"Constantin Simovski, Mohammad Albooyeh, Mohammad Yazdi, Nader Komjani","cross_cats":["cond-mat.mtrl-sci"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2015-08-25T09:19:03Z","title":"Polarizability Tensor Calculation: Induced Local Charge and Current Distributions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1508.06081","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:a23d909edfdc2bd38e14197390d6000bb091994e97137dbd67f7acb14211c77d","target":"record","created_at":"2026-05-18T01:34:46Z","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":"261246bfda4aaa9934a6587f88a7ea957ab80c3defe8b47777c67e0419e6b347","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2015-08-25T09:19:03Z","title_canon_sha256":"a3605b631707e5ac16da29972ca1800eec6568c30b279a02039d4cc8d2e55491"},"schema_version":"1.0","source":{"id":"1508.06081","kind":"arxiv","version":1}},"canonical_sha256":"817fa35a54996fa6a16790ef5f9bea607f32d74f4efcc603052b475dcc05f5d1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"817fa35a54996fa6a16790ef5f9bea607f32d74f4efcc603052b475dcc05f5d1","first_computed_at":"2026-05-18T01:34:46.940279Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:34:46.940279Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"V/iypqLroiMVW9UxEYf/4SRD1xgPJOEkuyYSnEudC0vxGBgguHg74tKGKFn6xTXU9F8gAU8wU7bYzRuXnT4VCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:34:46.940890Z","signed_message":"canonical_sha256_bytes"},"source_id":"1508.06081","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a23d909edfdc2bd38e14197390d6000bb091994e97137dbd67f7acb14211c77d","sha256:db2dc113b9de06cd00c881b26850698a55a0790dc37797a7c13bbc0a3ca9deac"],"state_sha256":"d92cfd759dd91a4978bfe4e342a7c2da5eb5d95a238b2a0ee89a9d6c3f07bbf1"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PaSSyHgokSaAm18f8bdg92y0BVSwESGZ6FPqgU3W2zdoGNKCDvna0vLyn4+hTkyqN1lIUd1CVreCW2WKuEgBAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-11T11:59:37.951585Z","bundle_sha256":"88a3946b38c881cd54fa38d13f0fdca95d3a821909eb4198f485c86f2eaa81dc"}}