{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:CRBYZJKTQNMOF32KW7JEUVNIUU","short_pith_number":"pith:CRBYZJKT","canonical_record":{"source":{"id":"1403.2799","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2014-03-12T03:08:17Z","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"title_canon_sha256":"8e7153508aa39430f18ca45b24169899305549d275d6997e1aa83eb58ac83fdb","abstract_canon_sha256":"c1846e08bbeffda00549d5d8d45fb970985a61a24a86499af902d1cbecccd393"},"schema_version":"1.0"},"canonical_sha256":"14438ca5538358e2ef4ab7d24a55a8a502a1d7bf36125a126ff04393e649c41a","source":{"kind":"arxiv","id":"1403.2799","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1403.2799","created_at":"2026-05-18T02:56:34Z"},{"alias_kind":"arxiv_version","alias_value":"1403.2799v1","created_at":"2026-05-18T02:56:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.2799","created_at":"2026-05-18T02:56:34Z"},{"alias_kind":"pith_short_12","alias_value":"CRBYZJKTQNMO","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_16","alias_value":"CRBYZJKTQNMOF32K","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_8","alias_value":"CRBYZJKT","created_at":"2026-05-18T12:28:22Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:CRBYZJKTQNMOF32KW7JEUVNIUU","target":"record","payload":{"canonical_record":{"source":{"id":"1403.2799","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2014-03-12T03:08:17Z","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"title_canon_sha256":"8e7153508aa39430f18ca45b24169899305549d275d6997e1aa83eb58ac83fdb","abstract_canon_sha256":"c1846e08bbeffda00549d5d8d45fb970985a61a24a86499af902d1cbecccd393"},"schema_version":"1.0"},"canonical_sha256":"14438ca5538358e2ef4ab7d24a55a8a502a1d7bf36125a126ff04393e649c41a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:56:34.089386Z","signature_b64":"oTkb2JmYklchjXKKi5lZAr5vBYxLW8/5t1kYFpwjA94XSc+raTbOZjtl/x4OBFTIX5iGC7/0UvsBURHg9NQwCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"14438ca5538358e2ef4ab7d24a55a8a502a1d7bf36125a126ff04393e649c41a","last_reissued_at":"2026-05-18T02:56:34.088539Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:56:34.088539Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1403.2799","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":"2026-05-18T02:56:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"N5xFtt4oBCf7IF4I1EPMdm5IMt4Ix8effvzzrvknnAEymqQ/nz9KQWHahibt85EnFFEoe3eclAx0QXWMHKRyCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-19T20:53:38.446987Z"},"content_sha256":"1af50550bfe6fc6ddfab17ffecfcb76fbf6de4d01c650820ed3f82f7e2e21514","schema_version":"1.0","event_id":"sha256:1af50550bfe6fc6ddfab17ffecfcb76fbf6de4d01c650820ed3f82f7e2e21514"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:CRBYZJKTQNMOF32KW7JEUVNIUU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Graphene Plasmonics for Terahertz to Mid-Infrared Applications","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","physics.optics"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Phaedon Avouris, Tony Low","submitted_at":"2014-03-12T03:08:17Z","abstract_excerpt":"In recent years, we have seen a rapid progress in the field of graphene plasmonics, motivated by graphene's unique electrical and optical properties, tunabilty, long-lived collective excitation and their extreme light confinement. Here, we review the basic properties of graphene plasmons; their energy dispersion, localization and propagation, plasmon-phonon hybridization, lifetimes and damping pathways. The application space of graphene plasmonics lies in the technologically significant, but relatively unexploited terahertz to mid-infrared regime. We discuss emerging and potential applications"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.2799","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":"2026-05-18T02:56:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/rQnmuZHp2gInAjSr+cF9Tfj0ZdSfD6dWs96EY6PB7Jao6p3I+198usc3w+8Ogjy1C1oZ0VTnm/14fEQOoK8CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-19T20:53:38.447511Z"},"content_sha256":"f8fa03f80ee5f19e37f819dedf5f01b321c2131e029455767f70c41d7aeab307","schema_version":"1.0","event_id":"sha256:f8fa03f80ee5f19e37f819dedf5f01b321c2131e029455767f70c41d7aeab307"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/CRBYZJKTQNMOF32KW7JEUVNIUU/bundle.json","state_url":"https://pith.science/pith/CRBYZJKTQNMOF32KW7JEUVNIUU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/CRBYZJKTQNMOF32KW7JEUVNIUU/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":"2026-08-19T20:53:38Z","links":{"resolver":"https://pith.science/pith/CRBYZJKTQNMOF32KW7JEUVNIUU","bundle":"https://pith.science/pith/CRBYZJKTQNMOF32KW7JEUVNIUU/bundle.json","state":"https://pith.science/pith/CRBYZJKTQNMOF32KW7JEUVNIUU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/CRBYZJKTQNMOF32KW7JEUVNIUU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:CRBYZJKTQNMOF32KW7JEUVNIUU","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":"c1846e08bbeffda00549d5d8d45fb970985a61a24a86499af902d1cbecccd393","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2014-03-12T03:08:17Z","title_canon_sha256":"8e7153508aa39430f18ca45b24169899305549d275d6997e1aa83eb58ac83fdb"},"schema_version":"1.0","source":{"id":"1403.2799","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1403.2799","created_at":"2026-05-18T02:56:34Z"},{"alias_kind":"arxiv_version","alias_value":"1403.2799v1","created_at":"2026-05-18T02:56:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.2799","created_at":"2026-05-18T02:56:34Z"},{"alias_kind":"pith_short_12","alias_value":"CRBYZJKTQNMO","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_16","alias_value":"CRBYZJKTQNMOF32K","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_8","alias_value":"CRBYZJKT","created_at":"2026-05-18T12:28:22Z"}],"graph_snapshots":[{"event_id":"sha256:f8fa03f80ee5f19e37f819dedf5f01b321c2131e029455767f70c41d7aeab307","target":"graph","created_at":"2026-05-18T02:56:34Z","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":"In recent years, we have seen a rapid progress in the field of graphene plasmonics, motivated by graphene's unique electrical and optical properties, tunabilty, long-lived collective excitation and their extreme light confinement. Here, we review the basic properties of graphene plasmons; their energy dispersion, localization and propagation, plasmon-phonon hybridization, lifetimes and damping pathways. The application space of graphene plasmonics lies in the technologically significant, but relatively unexploited terahertz to mid-infrared regime. We discuss emerging and potential applications","authors_text":"Phaedon Avouris, Tony Low","cross_cats":["cond-mat.mes-hall","physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2014-03-12T03:08:17Z","title":"Graphene Plasmonics for Terahertz to Mid-Infrared Applications"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.2799","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":"sha256:1af50550bfe6fc6ddfab17ffecfcb76fbf6de4d01c650820ed3f82f7e2e21514","target":"record","created_at":"2026-05-18T02:56:34Z","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":"c1846e08bbeffda00549d5d8d45fb970985a61a24a86499af902d1cbecccd393","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2014-03-12T03:08:17Z","title_canon_sha256":"8e7153508aa39430f18ca45b24169899305549d275d6997e1aa83eb58ac83fdb"},"schema_version":"1.0","source":{"id":"1403.2799","kind":"arxiv","version":1}},"canonical_sha256":"14438ca5538358e2ef4ab7d24a55a8a502a1d7bf36125a126ff04393e649c41a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"14438ca5538358e2ef4ab7d24a55a8a502a1d7bf36125a126ff04393e649c41a","first_computed_at":"2026-05-18T02:56:34.088539Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:56:34.088539Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"oTkb2JmYklchjXKKi5lZAr5vBYxLW8/5t1kYFpwjA94XSc+raTbOZjtl/x4OBFTIX5iGC7/0UvsBURHg9NQwCw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:56:34.089386Z","signed_message":"canonical_sha256_bytes"},"source_id":"1403.2799","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1af50550bfe6fc6ddfab17ffecfcb76fbf6de4d01c650820ed3f82f7e2e21514","sha256:f8fa03f80ee5f19e37f819dedf5f01b321c2131e029455767f70c41d7aeab307"],"state_sha256":"39585c4b6c5f4b435fd6bdec6ec614b99104269f1c3ea25aa2b74e001f2ac42d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zDdUyqPLDtSm+CsxtcabSE5Ic8V8Nf2E7DIixjCti29nvXTw0mUm+ulyDfNcCgF+bLBb/hwZbhfLwa9erdynAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-19T20:53:38.452804Z","bundle_sha256":"749caf02734bcb2e121879dab66cc6c88911c3ffc71d84906f682113fa64e473"}}