{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:ZRDTGES2SSOAYHH3VGVLU7DSAY","short_pith_number":"pith:ZRDTGES2","schema_version":"1.0","canonical_sha256":"cc4733125a949c0c1cfba9aaba7c7206013ef22274fc5d47c75b9c6e940e776f","source":{"kind":"arxiv","id":"1705.07634","version":3},"attestation_state":"computed","paper":{"title":"Resonant transport and near-field effects in photonic glasses","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mes-hall","physics.optics"],"primary_cat":"cond-mat.dis-nn","authors_text":"Christof M. Aegerter, Geoffroy J. Aubry, Georg Maret, Helmut C\\\"olfen, Henrik Weyer, Lukas Schertel, Mengdi Chen, Sebastian Polarz","submitted_at":"2017-05-22T09:50:44Z","abstract_excerpt":"A fundamental quantity in multiple scattering is the transport mean free path the inverse of which describes the scattering strength of a sample. In this paper, we emphasize the importance of an appropriate description of the effective refractive index $n_{\\mathrm{eff}}$ in multiple light scattering to accurately describe the light transport in dense photonic glasses. Using $n_{\\mathrm{eff}}$ as calculated by the energy-density coherent potential approximation we are able to predict the transport mean free path of monodisperse photonic glasses. This model without any fit parameter is in qualit"},"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":"1705.07634","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2017-05-22T09:50:44Z","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"title_canon_sha256":"1f5e856443ac0b872bca55eb22ee0c179fc1e3916b3485cc66b4477790f3356f","abstract_canon_sha256":"c5c926ba481a792fd0900eeb4340e7eed82095c98569ab14b7d676b8f949558a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:31:35.958762Z","signature_b64":"ED0V3NUTo2qbdX56jjVcMaWw2V79RmkUzA7fxKG6NPwxmtdL4lGknhSmqcgnGF1l7c33VTOD4Omr7P688gufBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cc4733125a949c0c1cfba9aaba7c7206013ef22274fc5d47c75b9c6e940e776f","last_reissued_at":"2026-05-18T00:31:35.958246Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:31:35.958246Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Resonant transport and near-field effects in photonic glasses","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mes-hall","physics.optics"],"primary_cat":"cond-mat.dis-nn","authors_text":"Christof M. Aegerter, Geoffroy J. Aubry, Georg Maret, Helmut C\\\"olfen, Henrik Weyer, Lukas Schertel, Mengdi Chen, Sebastian Polarz","submitted_at":"2017-05-22T09:50:44Z","abstract_excerpt":"A fundamental quantity in multiple scattering is the transport mean free path the inverse of which describes the scattering strength of a sample. In this paper, we emphasize the importance of an appropriate description of the effective refractive index $n_{\\mathrm{eff}}$ in multiple light scattering to accurately describe the light transport in dense photonic glasses. Using $n_{\\mathrm{eff}}$ as calculated by the energy-density coherent potential approximation we are able to predict the transport mean free path of monodisperse photonic glasses. This model without any fit parameter is in qualit"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.07634","kind":"arxiv","version":3},"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":"1705.07634","created_at":"2026-05-18T00:31:35.958328+00:00"},{"alias_kind":"arxiv_version","alias_value":"1705.07634v3","created_at":"2026-05-18T00:31:35.958328+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.07634","created_at":"2026-05-18T00:31:35.958328+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZRDTGES2SSOA","created_at":"2026-05-18T12:31:59.375834+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZRDTGES2SSOAYHH3","created_at":"2026-05-18T12:31:59.375834+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZRDTGES2","created_at":"2026-05-18T12:31:59.375834+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/ZRDTGES2SSOAYHH3VGVLU7DSAY","json":"https://pith.science/pith/ZRDTGES2SSOAYHH3VGVLU7DSAY.json","graph_json":"https://pith.science/api/pith-number/ZRDTGES2SSOAYHH3VGVLU7DSAY/graph.json","events_json":"https://pith.science/api/pith-number/ZRDTGES2SSOAYHH3VGVLU7DSAY/events.json","paper":"https://pith.science/paper/ZRDTGES2"},"agent_actions":{"view_html":"https://pith.science/pith/ZRDTGES2SSOAYHH3VGVLU7DSAY","download_json":"https://pith.science/pith/ZRDTGES2SSOAYHH3VGVLU7DSAY.json","view_paper":"https://pith.science/paper/ZRDTGES2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1705.07634&json=true","fetch_graph":"https://pith.science/api/pith-number/ZRDTGES2SSOAYHH3VGVLU7DSAY/graph.json","fetch_events":"https://pith.science/api/pith-number/ZRDTGES2SSOAYHH3VGVLU7DSAY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZRDTGES2SSOAYHH3VGVLU7DSAY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZRDTGES2SSOAYHH3VGVLU7DSAY/action/storage_attestation","attest_author":"https://pith.science/pith/ZRDTGES2SSOAYHH3VGVLU7DSAY/action/author_attestation","sign_citation":"https://pith.science/pith/ZRDTGES2SSOAYHH3VGVLU7DSAY/action/citation_signature","submit_replication":"https://pith.science/pith/ZRDTGES2SSOAYHH3VGVLU7DSAY/action/replication_record"}},"created_at":"2026-05-18T00:31:35.958328+00:00","updated_at":"2026-05-18T00:31:35.958328+00:00"}