{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:ZFOKZW35UZ3PEKJMNNXW3PMOJZ","short_pith_number":"pith:ZFOKZW35","canonical_record":{"source":{"id":"1612.02918","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-12-09T05:14:18Z","cross_cats_sorted":[],"title_canon_sha256":"a151f2e46e9ccdfc71e45dcdf08957799abd74238e9269f358a1bd0686e31ff7","abstract_canon_sha256":"20f7b4504d9f8f81915c52e43abee5220b6118efbaf0b8a6bf526f0bfb429518"},"schema_version":"1.0"},"canonical_sha256":"c95cacdb7da676f2292c6b6f6dbd8e4e75b0c503cebe35a028022fcbd20a63d1","source":{"kind":"arxiv","id":"1612.02918","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1612.02918","created_at":"2026-05-18T00:49:10Z"},{"alias_kind":"arxiv_version","alias_value":"1612.02918v1","created_at":"2026-05-18T00:49:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1612.02918","created_at":"2026-05-18T00:49:10Z"},{"alias_kind":"pith_short_12","alias_value":"ZFOKZW35UZ3P","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_16","alias_value":"ZFOKZW35UZ3PEKJM","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_8","alias_value":"ZFOKZW35","created_at":"2026-05-18T12:30:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:ZFOKZW35UZ3PEKJMNNXW3PMOJZ","target":"record","payload":{"canonical_record":{"source":{"id":"1612.02918","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-12-09T05:14:18Z","cross_cats_sorted":[],"title_canon_sha256":"a151f2e46e9ccdfc71e45dcdf08957799abd74238e9269f358a1bd0686e31ff7","abstract_canon_sha256":"20f7b4504d9f8f81915c52e43abee5220b6118efbaf0b8a6bf526f0bfb429518"},"schema_version":"1.0"},"canonical_sha256":"c95cacdb7da676f2292c6b6f6dbd8e4e75b0c503cebe35a028022fcbd20a63d1","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:49:10.850201Z","signature_b64":"kGqdzPuehiEvsLasC56hLNZB9Ex7eD13F3bwBefVtWAAjsfFceYuyAMsbk7Atxo26JXbrGTsrkJnEeWOls7bAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c95cacdb7da676f2292c6b6f6dbd8e4e75b0c503cebe35a028022fcbd20a63d1","last_reissued_at":"2026-05-18T00:49:10.849520Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:49:10.849520Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1612.02918","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":"2026-05-18T00:49:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"r0EQlI3jTQTLqygWc13qaT2jfNpm3nyb2hiBEjjB4SYPIH8yQ4fknLIlpr4iBVWRp5v2IkMXTnD6pvoOspnoCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T22:09:27.072418Z"},"content_sha256":"6506fbda52a2c55cf26dbc06ac3865055d4dd45d692cc4b1ab4ffb2eb35fa365","schema_version":"1.0","event_id":"sha256:6506fbda52a2c55cf26dbc06ac3865055d4dd45d692cc4b1ab4ffb2eb35fa365"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:ZFOKZW35UZ3PEKJMNNXW3PMOJZ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"New Tl2LaBr5: Ce3+ Crystal Scintillator for {\\gamma}-Rays Detection","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.ins-det","authors_text":"Arshad Khan, Gul Rooh, H. J. Kim, Sunghwan Kim","submitted_at":"2016-12-09T05:14:18Z","abstract_excerpt":"In this study we present our preliminary report on the scintillation properties of new Ce-doped Tl2LaBr5 single crystal. Two zones vertical Bridgman technique is used for the growth of this compound. Pure and Ce-doped samples showed maximum emission peaks at 435 nm and 415 nm, respectively. Best light yield of 43,000+-4300 ph/MeV with 6.3% (FWHM) energy resolution is obtained for 5% Ce-doped sample under {\\gamma}-ray excitation. Single exponential decay time constant of 25 ns is observed for 5% Ce doped sample. Effective Z-number is found to be 67, therefore efficient detection of X- and {\\gam"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1612.02918","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":"2026-05-18T00:49:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"T6aC8pZjMZxKazV7QQrLMZK3gXOfYYM6UsQNTB5qtczARlU8oTlaL57+f+n2LG6BVfCRMjPyiOzXJP+u3qcUCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T22:09:27.073075Z"},"content_sha256":"99b80c70369133a9ba1cd83a9ec5ccf29d3485ea7d59d5fabcc6364d05bf3b7c","schema_version":"1.0","event_id":"sha256:99b80c70369133a9ba1cd83a9ec5ccf29d3485ea7d59d5fabcc6364d05bf3b7c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZFOKZW35UZ3PEKJMNNXW3PMOJZ/bundle.json","state_url":"https://pith.science/pith/ZFOKZW35UZ3PEKJMNNXW3PMOJZ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZFOKZW35UZ3PEKJMNNXW3PMOJZ/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":"2026-06-07T22:09:27Z","links":{"resolver":"https://pith.science/pith/ZFOKZW35UZ3PEKJMNNXW3PMOJZ","bundle":"https://pith.science/pith/ZFOKZW35UZ3PEKJMNNXW3PMOJZ/bundle.json","state":"https://pith.science/pith/ZFOKZW35UZ3PEKJMNNXW3PMOJZ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZFOKZW35UZ3PEKJMNNXW3PMOJZ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:ZFOKZW35UZ3PEKJMNNXW3PMOJZ","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":"20f7b4504d9f8f81915c52e43abee5220b6118efbaf0b8a6bf526f0bfb429518","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-12-09T05:14:18Z","title_canon_sha256":"a151f2e46e9ccdfc71e45dcdf08957799abd74238e9269f358a1bd0686e31ff7"},"schema_version":"1.0","source":{"id":"1612.02918","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1612.02918","created_at":"2026-05-18T00:49:10Z"},{"alias_kind":"arxiv_version","alias_value":"1612.02918v1","created_at":"2026-05-18T00:49:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1612.02918","created_at":"2026-05-18T00:49:10Z"},{"alias_kind":"pith_short_12","alias_value":"ZFOKZW35UZ3P","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_16","alias_value":"ZFOKZW35UZ3PEKJM","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_8","alias_value":"ZFOKZW35","created_at":"2026-05-18T12:30:53Z"}],"graph_snapshots":[{"event_id":"sha256:99b80c70369133a9ba1cd83a9ec5ccf29d3485ea7d59d5fabcc6364d05bf3b7c","target":"graph","created_at":"2026-05-18T00:49:10Z","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 this study we present our preliminary report on the scintillation properties of new Ce-doped Tl2LaBr5 single crystal. Two zones vertical Bridgman technique is used for the growth of this compound. Pure and Ce-doped samples showed maximum emission peaks at 435 nm and 415 nm, respectively. Best light yield of 43,000+-4300 ph/MeV with 6.3% (FWHM) energy resolution is obtained for 5% Ce-doped sample under {\\gamma}-ray excitation. Single exponential decay time constant of 25 ns is observed for 5% Ce doped sample. Effective Z-number is found to be 67, therefore efficient detection of X- and {\\gam","authors_text":"Arshad Khan, Gul Rooh, H. J. Kim, Sunghwan Kim","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-12-09T05:14:18Z","title":"New Tl2LaBr5: Ce3+ Crystal Scintillator for {\\gamma}-Rays Detection"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1612.02918","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":"sha256:6506fbda52a2c55cf26dbc06ac3865055d4dd45d692cc4b1ab4ffb2eb35fa365","target":"record","created_at":"2026-05-18T00:49:10Z","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":"20f7b4504d9f8f81915c52e43abee5220b6118efbaf0b8a6bf526f0bfb429518","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-12-09T05:14:18Z","title_canon_sha256":"a151f2e46e9ccdfc71e45dcdf08957799abd74238e9269f358a1bd0686e31ff7"},"schema_version":"1.0","source":{"id":"1612.02918","kind":"arxiv","version":1}},"canonical_sha256":"c95cacdb7da676f2292c6b6f6dbd8e4e75b0c503cebe35a028022fcbd20a63d1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c95cacdb7da676f2292c6b6f6dbd8e4e75b0c503cebe35a028022fcbd20a63d1","first_computed_at":"2026-05-18T00:49:10.849520Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:49:10.849520Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"kGqdzPuehiEvsLasC56hLNZB9Ex7eD13F3bwBefVtWAAjsfFceYuyAMsbk7Atxo26JXbrGTsrkJnEeWOls7bAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:49:10.850201Z","signed_message":"canonical_sha256_bytes"},"source_id":"1612.02918","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6506fbda52a2c55cf26dbc06ac3865055d4dd45d692cc4b1ab4ffb2eb35fa365","sha256:99b80c70369133a9ba1cd83a9ec5ccf29d3485ea7d59d5fabcc6364d05bf3b7c"],"state_sha256":"57c88b4d9d716f242085cd6af50ec6ad16adeebc58ac00e156522542aad8ba96"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"z/1CChDcJ5s0gAQMQB92I4UkkTIgBaw0eT9eZzCFUuPqa/tNA4QaFoH/FzAVVh6/EJ8W56KFmffI3+Wq4oirDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-07T22:09:27.077463Z","bundle_sha256":"786fdacf1bda33f5e9355b8f236d44373176e9c2ea591fed15f088ad75493665"}}