{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:J2GFEADSBNUT4G22MDRAQVYWHU","short_pith_number":"pith:J2GFEADS","schema_version":"1.0","canonical_sha256":"4e8c5200720b693e1b5a60e20857163d11433d6d8386cfda5766f6a843a43776","source":{"kind":"arxiv","id":"1211.4474","version":1},"attestation_state":"computed","paper":{"title":"Near-Intrinsic Energy Resolution for 30 to 662 keV Gamma Rays in a High Pressure Xenon Electroluminescent TPC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex"],"primary_cat":"physics.ins-det","authors_text":"A. Cervera, A. Gil, A. Goldschmidt, A. Laing, A. L. Ferreira, A. Mar\\'i, A. Mart\\'inez, A. Moiseenko, A. Rodr\\'iguez, A. Sim\\'on, A. Tom\\'as, C. A. B. Oliveira, C. A. N. Conde, C. M. B. Monteiro, C. Sofka, D. C. Herrera, D. Gonz\\'alez-D\\'iaz, D. Lorca, D. Nygren, D. Shuman, D. V\\'azquez, E. D. C. Freitas, F. I. G. M. Borges, F. J. Iguaz, F. J. Mora, F. Monrabal, F. P. Santos, G. Luz\\'on, G. Navarro, H. G\\'omez, H. Natal da Luz, I. G. Irastorza, I. Liubarsky, J. A. Hernando Morata, J. A. M. Lopes, J. A. Villar, J. Castel, J. D\\'iaz, J. F. C. A. Veloso, J. F. Toledo, J. Hauptman, J. J. G\\'omez-Cadenas, J. L. P\\'erez Aparicio, J. Mart\\'in-Albo, J. M. F. dos Santos, J. Mu\\~noz Vidal, J. P\\'erez, J. Renner, J. Rodr\\'iguez, J. Torrent, J. T White, L. Labarga, L. M. Moutinho, L. M. P. Fernandes, L. Ripoll, L. Segui, L. Serra, M. A. Jinete, M. Egorov, M. Losada, M. Nebot, M. Sorel, NEXT Collaboration: V. \\'Alvarez, N. Yahlali, P. Evtoukhovitch, P. Ferrario, R. Esteve, R. M. Guti\\'errez, R. Palma, R. Webb, S. C\\'arcel, S. Cebri\\'an, T. Dafni, T. H. V. T. Dias, T. Miller, V. M. Gehman, Z. Tsamalaidze","submitted_at":"2012-11-19T16:00:12Z","abstract_excerpt":"We present the design, data and results from the NEXT prototype for Double Beta and Dark Matter (NEXT-DBDM) detector, a high-pressure gaseous natural xenon electroluminescent time projection chamber (TPC) that was built at the Lawrence Berkeley National Laboratory. It is a prototype of the planned NEXT-100 $^{136}$Xe neutrino-less double beta decay ($0\\nu\\beta\\beta$) experiment with the main objectives of demonstrating near-intrinsic energy resolution at energies up to 662 keV and of optimizing the NEXT-100 detector design and operating parameters. Energy resolutions of $\\sim$1% FWHM for 662 k"},"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":"1211.4474","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2012-11-19T16:00:12Z","cross_cats_sorted":["hep-ex","nucl-ex"],"title_canon_sha256":"a55a8a029cad5d88ab2fa68aba1837fcdda9b1ddd5e35813b4eec923c9b74e37","abstract_canon_sha256":"37b31f25ec0796cac43a8b5cb526cf580259128860bdc8a12c76315d585f146f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:40:26.786608Z","signature_b64":"BTqDHD+PannWX22mXnHIMNGZs5whyRpcqeYPZeis8wIpkPLp6M3qBs78IOww+CUors1Z6vfi7+ZmBw/tHFGwDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4e8c5200720b693e1b5a60e20857163d11433d6d8386cfda5766f6a843a43776","last_reissued_at":"2026-05-18T03:40:26.785936Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:40:26.785936Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Near-Intrinsic Energy Resolution for 30 to 662 keV Gamma Rays in a High Pressure Xenon Electroluminescent TPC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex"],"primary_cat":"physics.ins-det","authors_text":"A. Cervera, A. Gil, A. Goldschmidt, A. Laing, A. L. Ferreira, A. Mar\\'i, A. Mart\\'inez, A. Moiseenko, A. Rodr\\'iguez, A. Sim\\'on, A. Tom\\'as, C. A. B. Oliveira, C. A. N. Conde, C. M. B. Monteiro, C. Sofka, D. C. Herrera, D. Gonz\\'alez-D\\'iaz, D. Lorca, D. Nygren, D. Shuman, D. V\\'azquez, E. D. C. Freitas, F. I. G. M. Borges, F. J. Iguaz, F. J. Mora, F. Monrabal, F. P. Santos, G. Luz\\'on, G. Navarro, H. G\\'omez, H. Natal da Luz, I. G. Irastorza, I. Liubarsky, J. A. Hernando Morata, J. A. M. Lopes, J. A. Villar, J. Castel, J. D\\'iaz, J. F. C. A. Veloso, J. F. Toledo, J. Hauptman, J. J. G\\'omez-Cadenas, J. L. P\\'erez Aparicio, J. Mart\\'in-Albo, J. M. F. dos Santos, J. Mu\\~noz Vidal, J. P\\'erez, J. Renner, J. Rodr\\'iguez, J. Torrent, J. T White, L. Labarga, L. M. Moutinho, L. M. P. Fernandes, L. Ripoll, L. Segui, L. Serra, M. A. Jinete, M. Egorov, M. Losada, M. Nebot, M. Sorel, NEXT Collaboration: V. \\'Alvarez, N. Yahlali, P. Evtoukhovitch, P. Ferrario, R. Esteve, R. M. Guti\\'errez, R. Palma, R. Webb, S. C\\'arcel, S. Cebri\\'an, T. Dafni, T. H. V. T. Dias, T. Miller, V. M. Gehman, Z. Tsamalaidze","submitted_at":"2012-11-19T16:00:12Z","abstract_excerpt":"We present the design, data and results from the NEXT prototype for Double Beta and Dark Matter (NEXT-DBDM) detector, a high-pressure gaseous natural xenon electroluminescent time projection chamber (TPC) that was built at the Lawrence Berkeley National Laboratory. It is a prototype of the planned NEXT-100 $^{136}$Xe neutrino-less double beta decay ($0\\nu\\beta\\beta$) experiment with the main objectives of demonstrating near-intrinsic energy resolution at energies up to 662 keV and of optimizing the NEXT-100 detector design and operating parameters. Energy resolutions of $\\sim$1% FWHM for 662 k"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1211.4474","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1211.4474","created_at":"2026-05-18T03:40:26.786041+00:00"},{"alias_kind":"arxiv_version","alias_value":"1211.4474v1","created_at":"2026-05-18T03:40:26.786041+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1211.4474","created_at":"2026-05-18T03:40:26.786041+00:00"},{"alias_kind":"pith_short_12","alias_value":"J2GFEADSBNUT","created_at":"2026-05-18T12:27:09.501522+00:00"},{"alias_kind":"pith_short_16","alias_value":"J2GFEADSBNUT4G22","created_at":"2026-05-18T12:27:09.501522+00:00"},{"alias_kind":"pith_short_8","alias_value":"J2GFEADS","created_at":"2026-05-18T12:27:09.501522+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/J2GFEADSBNUT4G22MDRAQVYWHU","json":"https://pith.science/pith/J2GFEADSBNUT4G22MDRAQVYWHU.json","graph_json":"https://pith.science/api/pith-number/J2GFEADSBNUT4G22MDRAQVYWHU/graph.json","events_json":"https://pith.science/api/pith-number/J2GFEADSBNUT4G22MDRAQVYWHU/events.json","paper":"https://pith.science/paper/J2GFEADS"},"agent_actions":{"view_html":"https://pith.science/pith/J2GFEADSBNUT4G22MDRAQVYWHU","download_json":"https://pith.science/pith/J2GFEADSBNUT4G22MDRAQVYWHU.json","view_paper":"https://pith.science/paper/J2GFEADS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1211.4474&json=true","fetch_graph":"https://pith.science/api/pith-number/J2GFEADSBNUT4G22MDRAQVYWHU/graph.json","fetch_events":"https://pith.science/api/pith-number/J2GFEADSBNUT4G22MDRAQVYWHU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/J2GFEADSBNUT4G22MDRAQVYWHU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/J2GFEADSBNUT4G22MDRAQVYWHU/action/storage_attestation","attest_author":"https://pith.science/pith/J2GFEADSBNUT4G22MDRAQVYWHU/action/author_attestation","sign_citation":"https://pith.science/pith/J2GFEADSBNUT4G22MDRAQVYWHU/action/citation_signature","submit_replication":"https://pith.science/pith/J2GFEADSBNUT4G22MDRAQVYWHU/action/replication_record"}},"created_at":"2026-05-18T03:40:26.786041+00:00","updated_at":"2026-05-18T03:40:26.786041+00:00"}