{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:7JKT7TWE4YDH3WL7R52PPEKMPN","short_pith_number":"pith:7JKT7TWE","schema_version":"1.0","canonical_sha256":"fa553fcec4e6067dd97f8f74f7914c7b4dab76514897199605596f04815a37e8","source":{"kind":"arxiv","id":"1912.13442","version":1},"attestation_state":"computed","paper":{"title":"Hybrid Exciton-Plasmon-Polaritons in van der Waals Semiconductor Gratings","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci","physics.app-ph","physics.optics"],"primary_cat":"cond-mat.mes-hall","authors_text":"Artur R. Davoyan, Bhaskar Abhiraman, Deep Jariwala, Huiqin Zhang, Jinshui Miao, Kiyoung Jo, Mark W. Knight, Qing Zhang, Stefano Roccasecca","submitted_at":"2019-12-31T17:20:59Z","abstract_excerpt":"Van der Waals materials and heterostructures manifesting strongly bound room temperature exciton states exhibit emergent physical phenomena and are of a great promise for optoelectronic applications. Here, we demonstrate that nanostructured multilayer transition metal dichalcogenides by themselves provide an ideal platform for excitation and control of excitonic modes, paving the way to exciton-photonics. Hence, we show that by patterning the TMDCs into nanoresonators, strong dispersion and avoided crossing of excitons and hybrid polaritons with interaction potentials exceeding 410 meV may be "},"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":"1912.13442","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2019-12-31T17:20:59Z","cross_cats_sorted":["cond-mat.mtrl-sci","physics.app-ph","physics.optics"],"title_canon_sha256":"91c8b583953b8430470f20b345a75eac5e1941bb962505365dfccfc36c5f2947","abstract_canon_sha256":"382f76351716e01c4df02b477d872e3d17b1210bcaed32dd3e38d66551fe910b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:33:34.897756Z","signature_b64":"fDsgYeyTlISlgb2HOz3IEW3uPjtkyOjm2TTQk92c/m+kflynnfO/cJw8lDxdDqQQAQjruH0tXEVUuRoGJt+BDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fa553fcec4e6067dd97f8f74f7914c7b4dab76514897199605596f04815a37e8","last_reissued_at":"2026-07-05T01:33:34.897199Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:33:34.897199Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hybrid Exciton-Plasmon-Polaritons in van der Waals Semiconductor Gratings","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci","physics.app-ph","physics.optics"],"primary_cat":"cond-mat.mes-hall","authors_text":"Artur R. Davoyan, Bhaskar Abhiraman, Deep Jariwala, Huiqin Zhang, Jinshui Miao, Kiyoung Jo, Mark W. Knight, Qing Zhang, Stefano Roccasecca","submitted_at":"2019-12-31T17:20:59Z","abstract_excerpt":"Van der Waals materials and heterostructures manifesting strongly bound room temperature exciton states exhibit emergent physical phenomena and are of a great promise for optoelectronic applications. Here, we demonstrate that nanostructured multilayer transition metal dichalcogenides by themselves provide an ideal platform for excitation and control of excitonic modes, paving the way to exciton-photonics. Hence, we show that by patterning the TMDCs into nanoresonators, strong dispersion and avoided crossing of excitons and hybrid polaritons with interaction potentials exceeding 410 meV may be "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1912.13442","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1912.13442/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"1912.13442","created_at":"2026-07-05T01:33:34.897258+00:00"},{"alias_kind":"arxiv_version","alias_value":"1912.13442v1","created_at":"2026-07-05T01:33:34.897258+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1912.13442","created_at":"2026-07-05T01:33:34.897258+00:00"},{"alias_kind":"pith_short_12","alias_value":"7JKT7TWE4YDH","created_at":"2026-07-05T01:33:34.897258+00:00"},{"alias_kind":"pith_short_16","alias_value":"7JKT7TWE4YDH3WL7","created_at":"2026-07-05T01:33:34.897258+00:00"},{"alias_kind":"pith_short_8","alias_value":"7JKT7TWE","created_at":"2026-07-05T01:33:34.897258+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/7JKT7TWE4YDH3WL7R52PPEKMPN","json":"https://pith.science/pith/7JKT7TWE4YDH3WL7R52PPEKMPN.json","graph_json":"https://pith.science/api/pith-number/7JKT7TWE4YDH3WL7R52PPEKMPN/graph.json","events_json":"https://pith.science/api/pith-number/7JKT7TWE4YDH3WL7R52PPEKMPN/events.json","paper":"https://pith.science/paper/7JKT7TWE"},"agent_actions":{"view_html":"https://pith.science/pith/7JKT7TWE4YDH3WL7R52PPEKMPN","download_json":"https://pith.science/pith/7JKT7TWE4YDH3WL7R52PPEKMPN.json","view_paper":"https://pith.science/paper/7JKT7TWE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1912.13442&json=true","fetch_graph":"https://pith.science/api/pith-number/7JKT7TWE4YDH3WL7R52PPEKMPN/graph.json","fetch_events":"https://pith.science/api/pith-number/7JKT7TWE4YDH3WL7R52PPEKMPN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7JKT7TWE4YDH3WL7R52PPEKMPN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7JKT7TWE4YDH3WL7R52PPEKMPN/action/storage_attestation","attest_author":"https://pith.science/pith/7JKT7TWE4YDH3WL7R52PPEKMPN/action/author_attestation","sign_citation":"https://pith.science/pith/7JKT7TWE4YDH3WL7R52PPEKMPN/action/citation_signature","submit_replication":"https://pith.science/pith/7JKT7TWE4YDH3WL7R52PPEKMPN/action/replication_record"}},"created_at":"2026-07-05T01:33:34.897258+00:00","updated_at":"2026-07-05T01:33:34.897258+00:00"}