{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:YECK7NGWBPWMTV3UP54K65CI7W","short_pith_number":"pith:YECK7NGW","canonical_record":{"source":{"id":"1704.01758","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2017-04-06T09:41:14Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"59f75c4ef3a7f545ebecf653eca11bfb82770407346b03dc30dfac415ddfd221","abstract_canon_sha256":"96446e9940777cd1e52ae3b4cfd508e58d80ffc46f2906b4722372e39f6ca1ac"},"schema_version":"1.0"},"canonical_sha256":"c104afb4d60becc9d7747f78af7448fd8da09450503f09964bb6fe6ff06a4686","source":{"kind":"arxiv","id":"1704.01758","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1704.01758","created_at":"2026-05-18T00:25:20Z"},{"alias_kind":"arxiv_version","alias_value":"1704.01758v2","created_at":"2026-05-18T00:25:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.01758","created_at":"2026-05-18T00:25:20Z"},{"alias_kind":"pith_short_12","alias_value":"YECK7NGWBPWM","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_16","alias_value":"YECK7NGWBPWMTV3U","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_8","alias_value":"YECK7NGW","created_at":"2026-05-18T12:31:56Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:YECK7NGWBPWMTV3UP54K65CI7W","target":"record","payload":{"canonical_record":{"source":{"id":"1704.01758","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2017-04-06T09:41:14Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"59f75c4ef3a7f545ebecf653eca11bfb82770407346b03dc30dfac415ddfd221","abstract_canon_sha256":"96446e9940777cd1e52ae3b4cfd508e58d80ffc46f2906b4722372e39f6ca1ac"},"schema_version":"1.0"},"canonical_sha256":"c104afb4d60becc9d7747f78af7448fd8da09450503f09964bb6fe6ff06a4686","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:25:20.805688Z","signature_b64":"St7oNtwPYIiTcKS6Tb8+YyGeB+4CsgrKkTP4NA51QBzgiXS32kIO18NcUiSGJ6kB51TChZZyKpweijP7HtAqCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c104afb4d60becc9d7747f78af7448fd8da09450503f09964bb6fe6ff06a4686","last_reissued_at":"2026-05-18T00:25:20.805079Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:25:20.805079Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1704.01758","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:25:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1airEpnXnRGo//8jgPQSwSV29YHIASIW6Zgt3/LvEQNJ0sw8noUNdGj5FWMync12OQV/wbUdmdsz2FKL2JvDBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T18:22:09.510839Z"},"content_sha256":"43b7573e302b5e13cbb16fa58957d391f017d1ae73a4a2a6294be0755e4f4a21","schema_version":"1.0","event_id":"sha256:43b7573e302b5e13cbb16fa58957d391f017d1ae73a4a2a6294be0755e4f4a21"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:YECK7NGWBPWMTV3UP54K65CI7W","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Development of $^{100}$Mo-containing scintillating bolometers for a high-sensitivity neutrinoless double-beta decay search","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"physics.ins-det","authors_text":"A. Beno\\^it, A. Broniatowski, A. Cazes, A. Fleischmann, A. Giuliani, A. Juillard, A.S. Barabash, A.S. Zolotarova, B. Paul, B. Siebenborn, C. Augier, C. Enss, C. Marrache-Kikuchi, C. Nones, C. Rusconi, C. Tomei, D.M. Chernyak, D. Tcherniakhovski, D.V. Poda, E. Armengaud, E. Olivieri, E.P. Makarov, E. Queguiner, E. Yakushev, F.A. Danevich, F. Bellini, F. Charlieux, F. Ferroni, F. Koskas, G. Pessina, G. Piperno, H. Kraus, H. le Sueur, I. Dafinei, I.M. Ivanov, J. Billard, J. Gascon, J.W. Beeman, K. Eitel, K. Sch\\\"affner, L. Berg\\'e, L. Cardani, L. Devoyon, L. Dumoulin, L. Gastaldo, L. Gironi, L. Hehn, L. Pagnanini, L. Pattavina, L. Vagneron, M. Chapellier, M. de Combarieu, M. De Jesus, M. Gros, M. Kleifges, M. Laubenstein, M. Loidl, M. Mancuso, M.O. Nikolaichuk, M. Pavan, M. Rodrigues, M. Velazquez, M. Vignati, M. Weber, N. Casali, N. Coron, N. Foerster, N.V. Ivannikova, O. Plantevin, O. Strazzer, P. Camus, P. de Marcillac, P. Magnier, P. Pari, R.S. Boiko, S. Capelli, S. Di Domizio, S. Herv\\'e, S.I. Konovalov, S. Marnieros, S. Nagorny, S. Pirro, S. Rozov, S. Scorza, T.B. Bekker, T. Bergmann, T. Redon, V.A. Kudryavtsev, V. Brudanin, V.D. Grigorieva, V. Humbert, V.I. Tretyak, V.I. Umatov, V. Kozlov, V. Novati, V.N. Shlegel, V. Sanglard, V.V. Kobychev, X-F. Navick, Ya.V. Vasiliev, Y. Jin, Y. Penichot","submitted_at":"2017-04-06T09:41:14Z","abstract_excerpt":"This paper reports on the development of a technology involving $^{100}$Mo-enriched scintillating bolometers, compatible with the goals of CUPID, a proposed next-generation bolometric experiment to search for neutrinoless double-beta decay. Large mass ($\\sim$1~kg), high optical quality, radiopure $^{100}$Mo-containing zinc and lithium molybdate crystals have been produced and used to develop high performance single detector modules based on 0.2--0.4~kg scintillating bolometers. In particular, the energy resolution of the lithium molybdate detectors near the $Q$-value of the double-beta transit"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.01758","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":""},"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":"2026-05-18T00:25:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ohF75/gPv9bqn+cIgURCodja6XM2+VrG+qfq2uzp2u6pwqTQpnkaM7KkkNa7Uxqnk+tyvRoSR187CeIsqDUwBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T18:22:09.511544Z"},"content_sha256":"a9fe8568c19b49dec2e9f3f522c0fcd7c3660b15400146541b98778cd313155e","schema_version":"1.0","event_id":"sha256:a9fe8568c19b49dec2e9f3f522c0fcd7c3660b15400146541b98778cd313155e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YECK7NGWBPWMTV3UP54K65CI7W/bundle.json","state_url":"https://pith.science/pith/YECK7NGWBPWMTV3UP54K65CI7W/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YECK7NGWBPWMTV3UP54K65CI7W/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":"2026-05-25T18:22:09Z","links":{"resolver":"https://pith.science/pith/YECK7NGWBPWMTV3UP54K65CI7W","bundle":"https://pith.science/pith/YECK7NGWBPWMTV3UP54K65CI7W/bundle.json","state":"https://pith.science/pith/YECK7NGWBPWMTV3UP54K65CI7W/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YECK7NGWBPWMTV3UP54K65CI7W/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:YECK7NGWBPWMTV3UP54K65CI7W","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":"96446e9940777cd1e52ae3b4cfd508e58d80ffc46f2906b4722372e39f6ca1ac","cross_cats_sorted":["nucl-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2017-04-06T09:41:14Z","title_canon_sha256":"59f75c4ef3a7f545ebecf653eca11bfb82770407346b03dc30dfac415ddfd221"},"schema_version":"1.0","source":{"id":"1704.01758","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1704.01758","created_at":"2026-05-18T00:25:20Z"},{"alias_kind":"arxiv_version","alias_value":"1704.01758v2","created_at":"2026-05-18T00:25:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.01758","created_at":"2026-05-18T00:25:20Z"},{"alias_kind":"pith_short_12","alias_value":"YECK7NGWBPWM","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_16","alias_value":"YECK7NGWBPWMTV3U","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_8","alias_value":"YECK7NGW","created_at":"2026-05-18T12:31:56Z"}],"graph_snapshots":[{"event_id":"sha256:a9fe8568c19b49dec2e9f3f522c0fcd7c3660b15400146541b98778cd313155e","target":"graph","created_at":"2026-05-18T00:25:20Z","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":"This paper reports on the development of a technology involving $^{100}$Mo-enriched scintillating bolometers, compatible with the goals of CUPID, a proposed next-generation bolometric experiment to search for neutrinoless double-beta decay. Large mass ($\\sim$1~kg), high optical quality, radiopure $^{100}$Mo-containing zinc and lithium molybdate crystals have been produced and used to develop high performance single detector modules based on 0.2--0.4~kg scintillating bolometers. In particular, the energy resolution of the lithium molybdate detectors near the $Q$-value of the double-beta transit","authors_text":"A. Beno\\^it, A. Broniatowski, A. Cazes, A. Fleischmann, A. Giuliani, A. Juillard, A.S. Barabash, A.S. Zolotarova, B. Paul, B. Siebenborn, C. Augier, C. Enss, C. Marrache-Kikuchi, C. Nones, C. Rusconi, C. Tomei, D.M. Chernyak, D. Tcherniakhovski, D.V. Poda, E. Armengaud, E. Olivieri, E.P. Makarov, E. Queguiner, E. Yakushev, F.A. Danevich, F. Bellini, F. Charlieux, F. Ferroni, F. Koskas, G. Pessina, G. Piperno, H. Kraus, H. le Sueur, I. Dafinei, I.M. Ivanov, J. Billard, J. Gascon, J.W. Beeman, K. Eitel, K. Sch\\\"affner, L. Berg\\'e, L. Cardani, L. Devoyon, L. Dumoulin, L. Gastaldo, L. Gironi, L. Hehn, L. Pagnanini, L. Pattavina, L. Vagneron, M. Chapellier, M. de Combarieu, M. De Jesus, M. Gros, M. Kleifges, M. Laubenstein, M. Loidl, M. Mancuso, M.O. Nikolaichuk, M. Pavan, M. Rodrigues, M. Velazquez, M. Vignati, M. Weber, N. Casali, N. Coron, N. Foerster, N.V. Ivannikova, O. Plantevin, O. Strazzer, P. Camus, P. de Marcillac, P. Magnier, P. Pari, R.S. Boiko, S. Capelli, S. Di Domizio, S. Herv\\'e, S.I. Konovalov, S. Marnieros, S. Nagorny, S. Pirro, S. Rozov, S. Scorza, T.B. Bekker, T. Bergmann, T. Redon, V.A. Kudryavtsev, V. Brudanin, V.D. Grigorieva, V. Humbert, V.I. Tretyak, V.I. Umatov, V. Kozlov, V. Novati, V.N. Shlegel, V. Sanglard, V.V. Kobychev, X-F. Navick, Ya.V. Vasiliev, Y. Jin, Y. Penichot","cross_cats":["nucl-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2017-04-06T09:41:14Z","title":"Development of $^{100}$Mo-containing scintillating bolometers for a high-sensitivity neutrinoless double-beta decay search"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.01758","kind":"arxiv","version":2},"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":"sha256:43b7573e302b5e13cbb16fa58957d391f017d1ae73a4a2a6294be0755e4f4a21","target":"record","created_at":"2026-05-18T00:25:20Z","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":"96446e9940777cd1e52ae3b4cfd508e58d80ffc46f2906b4722372e39f6ca1ac","cross_cats_sorted":["nucl-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2017-04-06T09:41:14Z","title_canon_sha256":"59f75c4ef3a7f545ebecf653eca11bfb82770407346b03dc30dfac415ddfd221"},"schema_version":"1.0","source":{"id":"1704.01758","kind":"arxiv","version":2}},"canonical_sha256":"c104afb4d60becc9d7747f78af7448fd8da09450503f09964bb6fe6ff06a4686","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c104afb4d60becc9d7747f78af7448fd8da09450503f09964bb6fe6ff06a4686","first_computed_at":"2026-05-18T00:25:20.805079Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:25:20.805079Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"St7oNtwPYIiTcKS6Tb8+YyGeB+4CsgrKkTP4NA51QBzgiXS32kIO18NcUiSGJ6kB51TChZZyKpweijP7HtAqCw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:25:20.805688Z","signed_message":"canonical_sha256_bytes"},"source_id":"1704.01758","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:43b7573e302b5e13cbb16fa58957d391f017d1ae73a4a2a6294be0755e4f4a21","sha256:a9fe8568c19b49dec2e9f3f522c0fcd7c3660b15400146541b98778cd313155e"],"state_sha256":"ced69c94c116418b60a0eddc0739d65b5a63bc5ca53071f0ac654a6844d45a31"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"br1DmrlmXnP+ImMnFihLb9aZFlL0Cl/ramSMlj++LVkpMzMga2/03fT/JAUSY/65H/PZeORi7ovzGppcR2F9DA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T18:22:09.515486Z","bundle_sha256":"4070f4b482ef31c129f06ef07f72b445ea8386edffc433136deb980b72717c43"}}