{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:2YTGX3ZKOILCIRQSQJKOSXVXF4","short_pith_number":"pith:2YTGX3ZK","schema_version":"1.0","canonical_sha256":"d6266bef2a72162446128254e95eb72f0db1d05a4f09fdc8ce10e8bbe460b397","source":{"kind":"arxiv","id":"2412.17608","version":2},"attestation_state":"computed","paper":{"title":"Interplay between dressed and strong-axial-field states in Nitrogen-Vacancy centers for quantum sensing and computation","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"E. Bernardi, E. Losero, E. Moreva, G. Zanelli, I. P. Degiovanni, J. Forneris, M. Genovese, P. Traina, S. Ditalia Tchernij, \\v{Z}. Pastuovi\\'c","submitted_at":"2024-12-23T14:28:19Z","abstract_excerpt":"The Nitrogen-Vacancy (NV) center in diamond is an intriguing electronic spin system with applications in quantum radiometry, sensing and computation. In those experiments, a bias magnetic field is commonly applied along the NV symmetry axis to eliminate the triplet ground state manifold's degeneracy (S=1). In this configuration, the eigenvectors of the NV spin's projection along its axis are called strong-axial field states. Conversely, in some experiments a weak magnetic field is applied orthogonal to the NV symmetry axis, leading to eigenstates that are balanced linear superpositions of stro"},"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":"2412.17608","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2024-12-23T14:28:19Z","cross_cats_sorted":[],"title_canon_sha256":"21f61d8c80b3560518c6f7554aaabcfc929661e2cc50c07338cefacd29ad5e82","abstract_canon_sha256":"eb5fba3e42036b9d4db92ad97d2786a133c3a23f519965627a000083a1663c9b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:17:52.450894Z","signature_b64":"qfOqcAWH2UrOSUKycDknZlvPSsRY71VQubbAU5c8mbfionFNclXabdx/IU4bQM88DtPzNsNfxkfagroMUM+iAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d6266bef2a72162446128254e95eb72f0db1d05a4f09fdc8ce10e8bbe460b397","last_reissued_at":"2026-07-05T10:17:52.450405Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:17:52.450405Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Interplay between dressed and strong-axial-field states in Nitrogen-Vacancy centers for quantum sensing and computation","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"E. Bernardi, E. Losero, E. Moreva, G. Zanelli, I. P. Degiovanni, J. Forneris, M. Genovese, P. Traina, S. Ditalia Tchernij, \\v{Z}. Pastuovi\\'c","submitted_at":"2024-12-23T14:28:19Z","abstract_excerpt":"The Nitrogen-Vacancy (NV) center in diamond is an intriguing electronic spin system with applications in quantum radiometry, sensing and computation. In those experiments, a bias magnetic field is commonly applied along the NV symmetry axis to eliminate the triplet ground state manifold's degeneracy (S=1). In this configuration, the eigenvectors of the NV spin's projection along its axis are called strong-axial field states. Conversely, in some experiments a weak magnetic field is applied orthogonal to the NV symmetry axis, leading to eigenstates that are balanced linear superpositions of stro"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2412.17608","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2412.17608/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":"2412.17608","created_at":"2026-07-05T10:17:52.450470+00:00"},{"alias_kind":"arxiv_version","alias_value":"2412.17608v2","created_at":"2026-07-05T10:17:52.450470+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2412.17608","created_at":"2026-07-05T10:17:52.450470+00:00"},{"alias_kind":"pith_short_12","alias_value":"2YTGX3ZKOILC","created_at":"2026-07-05T10:17:52.450470+00:00"},{"alias_kind":"pith_short_16","alias_value":"2YTGX3ZKOILCIRQS","created_at":"2026-07-05T10:17:52.450470+00:00"},{"alias_kind":"pith_short_8","alias_value":"2YTGX3ZK","created_at":"2026-07-05T10:17:52.450470+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/2YTGX3ZKOILCIRQSQJKOSXVXF4","json":"https://pith.science/pith/2YTGX3ZKOILCIRQSQJKOSXVXF4.json","graph_json":"https://pith.science/api/pith-number/2YTGX3ZKOILCIRQSQJKOSXVXF4/graph.json","events_json":"https://pith.science/api/pith-number/2YTGX3ZKOILCIRQSQJKOSXVXF4/events.json","paper":"https://pith.science/paper/2YTGX3ZK"},"agent_actions":{"view_html":"https://pith.science/pith/2YTGX3ZKOILCIRQSQJKOSXVXF4","download_json":"https://pith.science/pith/2YTGX3ZKOILCIRQSQJKOSXVXF4.json","view_paper":"https://pith.science/paper/2YTGX3ZK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2412.17608&json=true","fetch_graph":"https://pith.science/api/pith-number/2YTGX3ZKOILCIRQSQJKOSXVXF4/graph.json","fetch_events":"https://pith.science/api/pith-number/2YTGX3ZKOILCIRQSQJKOSXVXF4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2YTGX3ZKOILCIRQSQJKOSXVXF4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2YTGX3ZKOILCIRQSQJKOSXVXF4/action/storage_attestation","attest_author":"https://pith.science/pith/2YTGX3ZKOILCIRQSQJKOSXVXF4/action/author_attestation","sign_citation":"https://pith.science/pith/2YTGX3ZKOILCIRQSQJKOSXVXF4/action/citation_signature","submit_replication":"https://pith.science/pith/2YTGX3ZKOILCIRQSQJKOSXVXF4/action/replication_record"}},"created_at":"2026-07-05T10:17:52.450470+00:00","updated_at":"2026-07-05T10:17:52.450470+00:00"}