{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:JHSS6PKPVJN3K3SR5DQEZDWLMZ","short_pith_number":"pith:JHSS6PKP","schema_version":"1.0","canonical_sha256":"49e52f3d4faa5bb56e51e8e04c8ecb6663e415c0a92abdff98e06abb24b11917","source":{"kind":"arxiv","id":"1008.3132","version":2},"attestation_state":"computed","paper":{"title":"Generating particle-like scattering states in wave transport","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn","physics.optics"],"primary_cat":"cond-mat.mes-hall","authors_text":"Florian Libisch, Philipp Ambichl, Stefan Rotter","submitted_at":"2010-08-18T16:51:56Z","abstract_excerpt":"We introduce a procedure to generate scattering states which display trajectory-like wave function patterns in wave transport through complex scatterers. These deterministic scattering states feature the dual property of being eigenstates to the Wigner-Smith time-delay matrix and to the transmission matrix with classical (noiseless) transmission eigenvalues close to 0 or 1. Our procedure to create such beam-like states is based solely on the scattering matrix and successfully tested numerically for regular, chaotic and disordered cavities. These results pave the way for the experimental realiz"},"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":"1008.3132","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2010-08-18T16:51:56Z","cross_cats_sorted":["cond-mat.dis-nn","physics.optics"],"title_canon_sha256":"bbc9ae5797eb7b876aa425964565091a296a2bdcf79dcba06bc0461d826ce4e2","abstract_canon_sha256":"b6a11b181454126d886c63cfa6b974a3f42a7e2847af9e4c0ec37bd93528a53e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:22:41.492096Z","signature_b64":"VI0rnRcKg7szNxgTz7tvcEYoM9nWgivq+BCKc31eiDOgUJ9z6yueRfQSsE79/QVfVlbxKtSLuuUKl50iyHYMCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"49e52f3d4faa5bb56e51e8e04c8ecb6663e415c0a92abdff98e06abb24b11917","last_reissued_at":"2026-05-18T04:22:41.491645Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:22:41.491645Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Generating particle-like scattering states in wave transport","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn","physics.optics"],"primary_cat":"cond-mat.mes-hall","authors_text":"Florian Libisch, Philipp Ambichl, Stefan Rotter","submitted_at":"2010-08-18T16:51:56Z","abstract_excerpt":"We introduce a procedure to generate scattering states which display trajectory-like wave function patterns in wave transport through complex scatterers. These deterministic scattering states feature the dual property of being eigenstates to the Wigner-Smith time-delay matrix and to the transmission matrix with classical (noiseless) transmission eigenvalues close to 0 or 1. Our procedure to create such beam-like states is based solely on the scattering matrix and successfully tested numerically for regular, chaotic and disordered cavities. These results pave the way for the experimental realiz"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1008.3132","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":"1008.3132","created_at":"2026-05-18T04:22:41.491720+00:00"},{"alias_kind":"arxiv_version","alias_value":"1008.3132v2","created_at":"2026-05-18T04:22:41.491720+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1008.3132","created_at":"2026-05-18T04:22:41.491720+00:00"},{"alias_kind":"pith_short_12","alias_value":"JHSS6PKPVJN3","created_at":"2026-05-18T12:26:09.077623+00:00"},{"alias_kind":"pith_short_16","alias_value":"JHSS6PKPVJN3K3SR","created_at":"2026-05-18T12:26:09.077623+00:00"},{"alias_kind":"pith_short_8","alias_value":"JHSS6PKP","created_at":"2026-05-18T12:26:09.077623+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/JHSS6PKPVJN3K3SR5DQEZDWLMZ","json":"https://pith.science/pith/JHSS6PKPVJN3K3SR5DQEZDWLMZ.json","graph_json":"https://pith.science/api/pith-number/JHSS6PKPVJN3K3SR5DQEZDWLMZ/graph.json","events_json":"https://pith.science/api/pith-number/JHSS6PKPVJN3K3SR5DQEZDWLMZ/events.json","paper":"https://pith.science/paper/JHSS6PKP"},"agent_actions":{"view_html":"https://pith.science/pith/JHSS6PKPVJN3K3SR5DQEZDWLMZ","download_json":"https://pith.science/pith/JHSS6PKPVJN3K3SR5DQEZDWLMZ.json","view_paper":"https://pith.science/paper/JHSS6PKP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1008.3132&json=true","fetch_graph":"https://pith.science/api/pith-number/JHSS6PKPVJN3K3SR5DQEZDWLMZ/graph.json","fetch_events":"https://pith.science/api/pith-number/JHSS6PKPVJN3K3SR5DQEZDWLMZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JHSS6PKPVJN3K3SR5DQEZDWLMZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JHSS6PKPVJN3K3SR5DQEZDWLMZ/action/storage_attestation","attest_author":"https://pith.science/pith/JHSS6PKPVJN3K3SR5DQEZDWLMZ/action/author_attestation","sign_citation":"https://pith.science/pith/JHSS6PKPVJN3K3SR5DQEZDWLMZ/action/citation_signature","submit_replication":"https://pith.science/pith/JHSS6PKPVJN3K3SR5DQEZDWLMZ/action/replication_record"}},"created_at":"2026-05-18T04:22:41.491720+00:00","updated_at":"2026-05-18T04:22:41.491720+00:00"}