{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:Q2MHDJ3XNGINW4TFHZ2EWY6I77","short_pith_number":"pith:Q2MHDJ3X","canonical_record":{"source":{"id":"2607.15622","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2026-07-17T04:45:13Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"091f40c851ef63ea4c2ae110aab1cb14a6d76f5432d455ebccb833c3ace032b1","abstract_canon_sha256":"03238b8e47f4fb24f47a4f9c66fac276b97ce65283354dae34eb5a08956848f1"},"schema_version":"1.0"},"canonical_sha256":"869871a7776990db72653e744b63c8ffe75f08c7515e8af08bc3609a8bb89e0d","source":{"kind":"arxiv","id":"2607.15622","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2607.15622","created_at":"2026-07-20T01:19:00Z"},{"alias_kind":"arxiv_version","alias_value":"2607.15622v1","created_at":"2026-07-20T01:19:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.15622","created_at":"2026-07-20T01:19:00Z"},{"alias_kind":"pith_short_12","alias_value":"Q2MHDJ3XNGIN","created_at":"2026-07-20T01:19:00Z"},{"alias_kind":"pith_short_16","alias_value":"Q2MHDJ3XNGINW4TF","created_at":"2026-07-20T01:19:00Z"},{"alias_kind":"pith_short_8","alias_value":"Q2MHDJ3X","created_at":"2026-07-20T01:19:00Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:Q2MHDJ3XNGINW4TFHZ2EWY6I77","target":"record","payload":{"canonical_record":{"source":{"id":"2607.15622","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2026-07-17T04:45:13Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"091f40c851ef63ea4c2ae110aab1cb14a6d76f5432d455ebccb833c3ace032b1","abstract_canon_sha256":"03238b8e47f4fb24f47a4f9c66fac276b97ce65283354dae34eb5a08956848f1"},"schema_version":"1.0"},"canonical_sha256":"869871a7776990db72653e744b63c8ffe75f08c7515e8af08bc3609a8bb89e0d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-20T01:19:00.823312Z","signature_b64":"tubfPJKz8mp6APM7mTeKNdP5J3SINtptHI+qMpTzK4nRww1+0d074mAqb/B+oSm66K7QcEL49ieQrAq14WJECQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"869871a7776990db72653e744b63c8ffe75f08c7515e8af08bc3609a8bb89e0d","last_reissued_at":"2026-07-20T01:19:00.822434Z","signature_status":"signed_v1","first_computed_at":"2026-07-20T01:19:00.822434Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2607.15622","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":"2026-07-20T01:19:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lqOw60kAUtOgieo3w1Fk0XCwBKq4lLha7rWGyOwRpBxPcWai14+JkNWpSvIKH/TdFtpEYANSj/hR88FfcHCTBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T23:05:37.132982Z"},"content_sha256":"b6fce34b5d89d6bb47076f38b9611ad672ed75065b9f41a5b68dcadd2c993f50","schema_version":"1.0","event_id":"sha256:b6fce34b5d89d6bb47076f38b9611ad672ed75065b9f41a5b68dcadd2c993f50"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:Q2MHDJ3XNGINW4TFHZ2EWY6I77","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Near-field Dressing of Thermal Emission","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"physics.optics","authors_text":"Philippe Ben-Abdallah, Raphael Mol, Riccardo Messina, Valentina Krachmalnicoff, Victor Guillemot, Wilfrid Poirier, Yannick De Wilde","submitted_at":"2026-07-17T04:45:13Z","abstract_excerpt":"Radiative heat transfer at subwavelength distances is generally understood as enhanced energy exchange mediated by photon tunnelling between neighboring bodies. While near-field interactions can dramatically increase mutual heat transfer, whether they also modify the thermal radiation emitted by the bodies themselves remains an open question. Here we experimentally show that near-field electromagnetic coupling reshapes far-field thermal emission through a distance-dependent dressed emissivity. Using a dual-probe calorimetric platform, we independently monitor the radiative balance of two boros"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.15622","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/2607.15622/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-20T01:19:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zUciogxw0VlBeOS6uFizZLHt2B1ED9HZMZX8u+gj/lESIYIxO/zp3g9UQEirt4WsfIOu4iGjj6GsDfE+3ENbDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T23:05:37.133849Z"},"content_sha256":"94745023fd1c6a02a7d61024be383007cbf3a027b84130e42454f0d8e814fde2","schema_version":"1.0","event_id":"sha256:94745023fd1c6a02a7d61024be383007cbf3a027b84130e42454f0d8e814fde2"},{"event_type":"integrity_finding","subject_pith_number":"pith:2026:Q2MHDJ3XNGINW4TFHZ2EWY6I77","target":"integrity","payload":{"note":"DOI is split by whitespace or line breaks in the printed bibliography. Reconstructed DOI 10.1103/PhysRevB.95.085413 resolves to 'Many-body heat radiation and heat transfer in the presence of a nonabsorbing background medium'. A reader following the printed text alone cannot reach it.","snippet":"M¨ uller, B., Incardone, R., Antezza, M., Emig, T., Kr¨ uger, M.: Many-body heat radiation and heat transfer in the presence of a nonabsorbing background medium. Physical Review B95(8), 085413 https://doi.org/10.1103/PhysRevB. 95.085413","arxiv_id":"2607.15622","detector":"doi_compliance","evidence":{"ref_index":19,"verdict_class":"incontrovertible","resolved_title":"Many-body heat radiation and heat transfer in the presence of a nonabsorbing background medium","printed_excerpt":"10.1103/physrevb","reconstructed_doi":"10.1103/PhysRevB.95.085413"},"severity":"advisory","ref_index":19,"audited_at":"2026-08-01T22:58:56.090473Z","event_type":"pith.integrity.v1","detected_doi":"10.1103/PhysRevB.95.085413","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"recoverable_identifier","evidence_hash":"bc7f7693702e68c76b0b1f5d34a6b210dd371ee6cff9745369905f02b89f8c27","paper_version":1,"verdict_class":"incontrovertible","resolved_title":"Many-body heat radiation and heat transfer in the presence of a nonabsorbing background medium","detector_version":"1.1.0","detected_arxiv_id":null,"integrity_event_id":16805,"payload_sha256":"b7d9e89dc85d93a5da3b5f6e77645f74db75e0f51cd34d3be7e3f98b4a23db1c","signature_b64":"HyOyI2SXQdg5oai+V+lPtq8EK2Q5tm9+cRKcOK6fPHlTXRZwNhvUE6bTsI/KdI3NlLz2Pn07coJQW2jpDIeiDw==","signing_key_id":"pith-v1-2026-05"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-08-01T23:03:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"efVpP3gFreZ/hosLcysSIGfyEXuWUxF88ZnT53YWJ/zp8Lamdylk9zmKkeMJkV+hgXq/4UWbm7HbHPctntLHCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T23:05:37.138290Z"},"content_sha256":"58cdd41bc36880f34c14f69b863f8ff7d920c45e40ad61898f650cfe663be52d","schema_version":"1.0","event_id":"sha256:58cdd41bc36880f34c14f69b863f8ff7d920c45e40ad61898f650cfe663be52d"},{"event_type":"integrity_finding","subject_pith_number":"pith:2026:Q2MHDJ3XNGINW4TFHZ2EWY6I77","target":"integrity","payload":{"note":"DOI is split by whitespace or line breaks in the printed bibliography. Reconstructed DOI 10.1016/j.surfrep.2014.11.001 resolves to 'Electromagnetic density of states in complex plasmonic systems'. A reader following the printed text alone cannot reach it.","snippet":"Carminati, R., Caz´ e, A., Cao, D., Peragut, F., Krachmalnicoff, V., Pierrat, R., De Wilde, Y.: Electromagnetic density of states in complex plasmonic systems. Surface Science Reports70(1), 1–41 https://doi.org/10.1016/j.surfrep.2014.11. 00","arxiv_id":"2607.15622","detector":"doi_compliance","evidence":{"ref_index":17,"verdict_class":"incontrovertible","resolved_title":"Electromagnetic density of states in complex plasmonic systems","printed_excerpt":"10.1016/j.surfrep.2014.11","reconstructed_doi":"10.1016/j.surfrep.2014.11.001"},"severity":"advisory","ref_index":17,"audited_at":"2026-08-01T22:58:56.090473Z","event_type":"pith.integrity.v1","detected_doi":"10.1016/j.surfrep.2014.11.001","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"recoverable_identifier","evidence_hash":"cfce3c9900307198eea11cd54782f8422eb2dbaea75c96ee5f4cc59665280e0a","paper_version":1,"verdict_class":"incontrovertible","resolved_title":"Electromagnetic density of states in complex plasmonic systems","detector_version":"1.1.0","detected_arxiv_id":null,"integrity_event_id":16804,"payload_sha256":"98f8312b12a6f9013a48ef274414429710b23c05fa7b2fe5ccc4b34b4dfe899c","signature_b64":"figXx5vxM0VcPgrmxxGxux1inaR1nGQJYZcHWsQxNfGLvBZlj7hdiXI/aUMeestEUUN+70W3wyQyzKRJs24qBg==","signing_key_id":"pith-v1-2026-05"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-08-01T23:03:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yES3ka0Fgz+3iboSV4Ruh7GIq/6dOQM5BHz8gEwFfxrZkZmoVouHK/lN2hOyT51cSEfQQXilqOyE2DjcS/FoDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T23:05:37.138960Z"},"content_sha256":"0545f8c4152e616db0d776f1ddfb769b28f054052a3aaf749b1ccdf31f6ad68d","schema_version":"1.0","event_id":"sha256:0545f8c4152e616db0d776f1ddfb769b28f054052a3aaf749b1ccdf31f6ad68d"},{"event_type":"integrity_finding","subject_pith_number":"pith:2026:Q2MHDJ3XNGINW4TFHZ2EWY6I77","target":"integrity","payload":{"note":"Identifier '10.1016/0022-2313(70' is syntactically valid but the DOI registry (doi.org) returned 404, and Crossref / OpenAlex / internal corpus also have no record. The cited work could not be located through any authoritative source.","snippet":"Drexhage, K.H.: Influence of a dielectric interface on fluorescence decay time. Journal of Luminescence1-2, 693–701 https://doi.org/10.1016/0022-2313(70) 90082-7","arxiv_id":"2607.15622","detector":"doi_compliance","evidence":{"doi":"10.1016/0022-2313(70","arxiv_id":null,"ref_index":15,"raw_excerpt":"Drexhage, K.H.: Influence of a dielectric interface on fluorescence decay time. Journal of Luminescence1-2, 693–701 https://doi.org/10.1016/0022-2313(70) 90082-7","parse_status":"well_formed","verdict_class":"cross_source","checked_sources":["crossref_by_doi","openalex_by_doi","doi_org_head"],"resolution_status":"hard_miss"},"severity":"critical","ref_index":15,"audited_at":"2026-08-01T22:58:56.090473Z","event_type":"pith.integrity.v1","detected_doi":"10.1016/0022-2313(70","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"unresolvable_identifier","evidence_hash":"2099c3fc2ff40a9070f1ce10cbb7d96a09c3d1695cdcffc60d51f3d96ee20334","paper_version":1,"verdict_class":"cross_source","resolved_title":null,"detector_version":"1.1.0","detected_arxiv_id":null,"integrity_event_id":16803,"payload_sha256":"50641f36a330903bc57e048d3e965820ff8d55afbe26bded4a13fa28714db313","signature_b64":"pG9gWm03Gj/L6kSaCMil7816Bd7MlyD2s47wItVenL6tFYkbcJ1ztsH3esR35E6PyEGn6bottIR2lHZVK3RfDw==","signing_key_id":"pith-v1-2026-05"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-08-01T23:03:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dG/53XnXilU9CUaZ4DVNNsUJDY2p3/HqKzf5K5VvBaaRLHxJbm+AzXSDJVFOAyjCPfpuhlpbM9sAJeAHp2NiDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T23:05:37.139748Z"},"content_sha256":"576f5e7af0d73f0433061d15bc6fd02323cb0e33fadef9acfdd237f39ce9ed98","schema_version":"1.0","event_id":"sha256:576f5e7af0d73f0433061d15bc6fd02323cb0e33fadef9acfdd237f39ce9ed98"},{"event_type":"integrity_finding","subject_pith_number":"pith:2026:Q2MHDJ3XNGINW4TFHZ2EWY6I77","target":"integrity","payload":{"note":"DOI is split by whitespace or line breaks in the printed bibliography. Reconstructed DOI 10.1021/acs.nanolett.2c04735 resolves to 'Probing the Limits to Near-Field Heat Transfer Enhancements in Phonon-Polaritonic Materials'. A reader following the printed text alone cannot reach it.","snippet":"Mittapally, R., Lim, J.W., Zhang, L., Miller, O.D., Reddy, P., Meyhofer, E.: Probing the limits to near-field heat transfer enhancements in phonon-polaritonic materials. Nano Letters23(6), 2187–2194 https://doi.org/10.1021/acs.nanolett. 2c0","arxiv_id":"2607.15622","detector":"doi_compliance","evidence":{"ref_index":9,"verdict_class":"incontrovertible","resolved_title":"Probing the Limits to Near-Field Heat Transfer Enhancements in Phonon-Polaritonic Materials","printed_excerpt":"10.1021/acs.nanolett","reconstructed_doi":"10.1021/acs.nanolett.2c04735"},"severity":"advisory","ref_index":9,"audited_at":"2026-08-01T22:58:56.090473Z","event_type":"pith.integrity.v1","detected_doi":"10.1021/acs.nanolett.2c04735","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"recoverable_identifier","evidence_hash":"d94f42bc368f33040dc4ba08dd67562e71330f534a7977b1a5780a51f90c82df","paper_version":1,"verdict_class":"incontrovertible","resolved_title":"Probing the Limits to Near-Field Heat Transfer Enhancements in Phonon-Polaritonic Materials","detector_version":"1.1.0","detected_arxiv_id":null,"integrity_event_id":16802,"payload_sha256":"316e57529a61036f5e199af566981a223459f3dda9c16acece02d709d9ec93fb","signature_b64":"Z2W2aMjl/1Ae/h0GdZveoE642i/aTuJM2vVKSzPpFwLOIc1p4dBWL7e2UuTZNcUs00/PRJOfH9PPa5DEfHejBw==","signing_key_id":"pith-v1-2026-05"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-08-01T23:03:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Y/xYrqEPGqBjteK4h+NW8sxysTXiUy7f/dLUdhXlgb/hHi6qUiml76GyAeiQqfQr+e3klk/9M2H6uSQ4+gHYDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T23:05:37.140441Z"},"content_sha256":"52386f9077196e5ebcd6593494e2f91ee192e524101d9337fbff5bcb9c8e6f8c","schema_version":"1.0","event_id":"sha256:52386f9077196e5ebcd6593494e2f91ee192e524101d9337fbff5bcb9c8e6f8c"},{"event_type":"integrity_finding","subject_pith_number":"pith:2026:Q2MHDJ3XNGINW4TFHZ2EWY6I77","target":"integrity","payload":{"note":"DOI is split by whitespace or line breaks in the printed bibliography. Reconstructed DOI 10.1103/PhysRevLett.123.264301 resolves to 'Multitip Near-Field Scanning Thermal Microscopy'. A reader following the printed text alone cannot reach it.","snippet":"Ben-Abdallah, P.: Multitip near-field scanning thermal microscopy. Physi- cal Review Letters123(26), 264301 https://doi.org/10.1103/PhysRevLett.123. 264301","arxiv_id":"2607.15622","detector":"doi_compliance","evidence":{"ref_index":22,"verdict_class":"incontrovertible","resolved_title":"Multitip Near-Field Scanning Thermal Microscopy","printed_excerpt":"10.1103/physrevlett.123","reconstructed_doi":"10.1103/PhysRevLett.123.264301"},"severity":"advisory","ref_index":22,"audited_at":"2026-08-01T22:58:56.090473Z","event_type":"pith.integrity.v1","detected_doi":"10.1103/PhysRevLett.123.264301","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"recoverable_identifier","evidence_hash":"b782b59d0731e1fd4203b7bd33252a00d7d2bb5648ed0ad9d2870bb5dbe9e7c7","paper_version":1,"verdict_class":"incontrovertible","resolved_title":"Multitip Near-Field Scanning Thermal Microscopy","detector_version":"1.1.0","detected_arxiv_id":null,"integrity_event_id":16801,"payload_sha256":"d8c727c710929f3bb3128a4acf155b384704a813354b9e2051333cb8abc7aceb","signature_b64":"3fJFJgvxkBHGBUcveYiyLZ9RVTPd1XPFMuPpjaIFNOBCyTXQjKNZYYEx+1+zgsXBHjEqUyRORemrPENwyjtXAQ==","signing_key_id":"pith-v1-2026-05"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-08-01T23:03:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"muBUFi/Ee1ds7BTO7iRsIJYV5//gaVoFoIb7dIbePtA8kZSbw4xl0iP6J4bHUvkuoQQTTxSUxHwgYRdUzMMrCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T23:05:37.141063Z"},"content_sha256":"a3be95672f63ec869481c723aedc02dd777413f5323243664617dbfa58a31be3","schema_version":"1.0","event_id":"sha256:a3be95672f63ec869481c723aedc02dd777413f5323243664617dbfa58a31be3"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/Q2MHDJ3XNGINW4TFHZ2EWY6I77/bundle.json","state_url":"https://pith.science/pith/Q2MHDJ3XNGINW4TFHZ2EWY6I77/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/Q2MHDJ3XNGINW4TFHZ2EWY6I77/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":"2026-08-04T23:05:37Z","links":{"resolver":"https://pith.science/pith/Q2MHDJ3XNGINW4TFHZ2EWY6I77","bundle":"https://pith.science/pith/Q2MHDJ3XNGINW4TFHZ2EWY6I77/bundle.json","state":"https://pith.science/pith/Q2MHDJ3XNGINW4TFHZ2EWY6I77/state.json","well_known_bundle":"https://pith.science/.well-known/pith/Q2MHDJ3XNGINW4TFHZ2EWY6I77/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:Q2MHDJ3XNGINW4TFHZ2EWY6I77","merge_version":"pith-open-graph-merge-v1","event_count":7,"valid_event_count":7,"invalid_event_count":0,"equivocation_count":1,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"03238b8e47f4fb24f47a4f9c66fac276b97ce65283354dae34eb5a08956848f1","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2026-07-17T04:45:13Z","title_canon_sha256":"091f40c851ef63ea4c2ae110aab1cb14a6d76f5432d455ebccb833c3ace032b1"},"schema_version":"1.0","source":{"id":"2607.15622","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2607.15622","created_at":"2026-07-20T01:19:00Z"},{"alias_kind":"arxiv_version","alias_value":"2607.15622v1","created_at":"2026-07-20T01:19:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.15622","created_at":"2026-07-20T01:19:00Z"},{"alias_kind":"pith_short_12","alias_value":"Q2MHDJ3XNGIN","created_at":"2026-07-20T01:19:00Z"},{"alias_kind":"pith_short_16","alias_value":"Q2MHDJ3XNGINW4TF","created_at":"2026-07-20T01:19:00Z"},{"alias_kind":"pith_short_8","alias_value":"Q2MHDJ3X","created_at":"2026-07-20T01:19:00Z"}],"graph_snapshots":[{"event_id":"sha256:94745023fd1c6a02a7d61024be383007cbf3a027b84130e42454f0d8e814fde2","target":"graph","created_at":"2026-07-20T01:19:00Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2607.15622/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Radiative heat transfer at subwavelength distances is generally understood as enhanced energy exchange mediated by photon tunnelling between neighboring bodies. While near-field interactions can dramatically increase mutual heat transfer, whether they also modify the thermal radiation emitted by the bodies themselves remains an open question. Here we experimentally show that near-field electromagnetic coupling reshapes far-field thermal emission through a distance-dependent dressed emissivity. Using a dual-probe calorimetric platform, we independently monitor the radiative balance of two boros","authors_text":"Philippe Ben-Abdallah, Raphael Mol, Riccardo Messina, Valentina Krachmalnicoff, Victor Guillemot, Wilfrid Poirier, Yannick De Wilde","cross_cats":["cond-mat.mes-hall"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2026-07-17T04:45:13Z","title":"Near-field Dressing of Thermal Emission"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.15622","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:b6fce34b5d89d6bb47076f38b9611ad672ed75065b9f41a5b68dcadd2c993f50","target":"record","created_at":"2026-07-20T01:19:00Z","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":"03238b8e47f4fb24f47a4f9c66fac276b97ce65283354dae34eb5a08956848f1","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2026-07-17T04:45:13Z","title_canon_sha256":"091f40c851ef63ea4c2ae110aab1cb14a6d76f5432d455ebccb833c3ace032b1"},"schema_version":"1.0","source":{"id":"2607.15622","kind":"arxiv","version":1}},"canonical_sha256":"869871a7776990db72653e744b63c8ffe75f08c7515e8af08bc3609a8bb89e0d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"869871a7776990db72653e744b63c8ffe75f08c7515e8af08bc3609a8bb89e0d","first_computed_at":"2026-07-20T01:19:00.822434Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-20T01:19:00.822434Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"tubfPJKz8mp6APM7mTeKNdP5J3SINtptHI+qMpTzK4nRww1+0d074mAqb/B+oSm66K7QcEL49ieQrAq14WJECQ==","signature_status":"signed_v1","signed_at":"2026-07-20T01:19:00.823312Z","signed_message":"canonical_sha256_bytes"},"source_id":"2607.15622","source_kind":"arxiv","source_version":1}}},"equivocations":[{"signer_id":"pith.science","event_type":"integrity_finding","target":"integrity","event_ids":["sha256:0545f8c4152e616db0d776f1ddfb769b28f054052a3aaf749b1ccdf31f6ad68d","sha256:52386f9077196e5ebcd6593494e2f91ee192e524101d9337fbff5bcb9c8e6f8c","sha256:576f5e7af0d73f0433061d15bc6fd02323cb0e33fadef9acfdd237f39ce9ed98","sha256:58cdd41bc36880f34c14f69b863f8ff7d920c45e40ad61898f650cfe663be52d","sha256:a3be95672f63ec869481c723aedc02dd777413f5323243664617dbfa58a31be3"]}],"invalid_events":[],"applied_event_ids":["sha256:b6fce34b5d89d6bb47076f38b9611ad672ed75065b9f41a5b68dcadd2c993f50","sha256:94745023fd1c6a02a7d61024be383007cbf3a027b84130e42454f0d8e814fde2"],"state_sha256":"dff1eaf6db7d070e2a1c7f121776b0ee7a0f0360db263f68472b99d81d48e179"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"15UlEx9LMIauz7iLqCZBLMEo8oQI80e9ZDQiqBZWW2VC8JE1scDWns42uhLrXSxRUnXDqNsWv2t0+zaN0a8fBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-04T23:05:37.147152Z","bundle_sha256":"c0e679d9118c3ef7533508ab68f6a41b55cd5306eb4a8e6c40900f04d46927fd"}}