{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:XROCL52UTXAT6SUQA5S4CHO5HB","short_pith_number":"pith:XROCL52U","canonical_record":{"source":{"id":"1305.7356","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-05-31T11:10:27Z","cross_cats_sorted":[],"title_canon_sha256":"aefea70f7d221e1d79727c173c97cdaa8827214982097ac0c89a69347e595e13","abstract_canon_sha256":"75f1889092b68ea9881583e951d18ec22df7293338746c69acc1520847fe6e28"},"schema_version":"1.0"},"canonical_sha256":"bc5c25f7549dc13f4a900765c11ddd387e57cdaef8fcaae167f3aad530e3a3c3","source":{"kind":"arxiv","id":"1305.7356","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1305.7356","created_at":"2026-05-18T03:22:07Z"},{"alias_kind":"arxiv_version","alias_value":"1305.7356v1","created_at":"2026-05-18T03:22:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1305.7356","created_at":"2026-05-18T03:22:07Z"},{"alias_kind":"pith_short_12","alias_value":"XROCL52UTXAT","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_16","alias_value":"XROCL52UTXAT6SUQ","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_8","alias_value":"XROCL52U","created_at":"2026-05-18T12:28:06Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:XROCL52UTXAT6SUQA5S4CHO5HB","target":"record","payload":{"canonical_record":{"source":{"id":"1305.7356","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-05-31T11:10:27Z","cross_cats_sorted":[],"title_canon_sha256":"aefea70f7d221e1d79727c173c97cdaa8827214982097ac0c89a69347e595e13","abstract_canon_sha256":"75f1889092b68ea9881583e951d18ec22df7293338746c69acc1520847fe6e28"},"schema_version":"1.0"},"canonical_sha256":"bc5c25f7549dc13f4a900765c11ddd387e57cdaef8fcaae167f3aad530e3a3c3","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:22:07.112500Z","signature_b64":"OaO8trwcwMqZ3WqBYdY9wj5wFr+JOLPA7nKn8Q0yv4Zr2j4+Ltp/oPQH9epehdpbZ+JOloipau6TFDeTYQ4qAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bc5c25f7549dc13f4a900765c11ddd387e57cdaef8fcaae167f3aad530e3a3c3","last_reissued_at":"2026-05-18T03:22:07.111975Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:22:07.111975Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1305.7356","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":"2026-05-18T03:22:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GE5/8sf9L+C7SssIovfUYssyp/iNXsw3ivAVECN1w5LRKKKIVn9Lyzs9WFq6TrH6K3Kf3hlO7UXoyoBMniEwCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T01:36:29.791195Z"},"content_sha256":"cd1ca42997baef1cd5997a5d1e88dabac019587b81a652ac4716c8a3c93fcc0b","schema_version":"1.0","event_id":"sha256:cd1ca42997baef1cd5997a5d1e88dabac019587b81a652ac4716c8a3c93fcc0b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:XROCL52UTXAT6SUQA5S4CHO5HB","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"2-photon decay rate of the scalar boson in the Inert Doublet Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Bogumila Swiezewska, Maria Krawczyk","submitted_at":"2013-05-31T11:10:27Z","abstract_excerpt":"Motivated by experimental hints on the possibility of deviating from the SM predictions for the 2-photon decay rate of the 125 GeV SM-like scalar boson h, an analysis of this rate in the framework of the Inert Doublet Model is presented. Regions in the parameter space where the 2-photon decay rate is enhanced were found. The resulting regions are confronted with the allowed values of the Dark Matter (DM) particle's mass. Constraints on the masses of the charged scalar and the DM particle, and scalar couplings are presented."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1305.7356","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":"2026-05-18T03:22:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nNetoynfKQtyHU4s69hdCmgZwV9cITxnqch2863/KW/vxPqUurPn1ff0z8msx/53o4L0V8MJDzQsqk1mkHQUDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T01:36:29.791992Z"},"content_sha256":"ebbaf3f7e327b9ef004addabd1cd0efc0f62fad6185abaee54c751e6937521a8","schema_version":"1.0","event_id":"sha256:ebbaf3f7e327b9ef004addabd1cd0efc0f62fad6185abaee54c751e6937521a8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/XROCL52UTXAT6SUQA5S4CHO5HB/bundle.json","state_url":"https://pith.science/pith/XROCL52UTXAT6SUQA5S4CHO5HB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/XROCL52UTXAT6SUQA5S4CHO5HB/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":"2026-06-01T01:36:29Z","links":{"resolver":"https://pith.science/pith/XROCL52UTXAT6SUQA5S4CHO5HB","bundle":"https://pith.science/pith/XROCL52UTXAT6SUQA5S4CHO5HB/bundle.json","state":"https://pith.science/pith/XROCL52UTXAT6SUQA5S4CHO5HB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/XROCL52UTXAT6SUQA5S4CHO5HB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:XROCL52UTXAT6SUQA5S4CHO5HB","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":"75f1889092b68ea9881583e951d18ec22df7293338746c69acc1520847fe6e28","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-05-31T11:10:27Z","title_canon_sha256":"aefea70f7d221e1d79727c173c97cdaa8827214982097ac0c89a69347e595e13"},"schema_version":"1.0","source":{"id":"1305.7356","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1305.7356","created_at":"2026-05-18T03:22:07Z"},{"alias_kind":"arxiv_version","alias_value":"1305.7356v1","created_at":"2026-05-18T03:22:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1305.7356","created_at":"2026-05-18T03:22:07Z"},{"alias_kind":"pith_short_12","alias_value":"XROCL52UTXAT","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_16","alias_value":"XROCL52UTXAT6SUQ","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_8","alias_value":"XROCL52U","created_at":"2026-05-18T12:28:06Z"}],"graph_snapshots":[{"event_id":"sha256:ebbaf3f7e327b9ef004addabd1cd0efc0f62fad6185abaee54c751e6937521a8","target":"graph","created_at":"2026-05-18T03:22:07Z","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":"Motivated by experimental hints on the possibility of deviating from the SM predictions for the 2-photon decay rate of the 125 GeV SM-like scalar boson h, an analysis of this rate in the framework of the Inert Doublet Model is presented. Regions in the parameter space where the 2-photon decay rate is enhanced were found. The resulting regions are confronted with the allowed values of the Dark Matter (DM) particle's mass. Constraints on the masses of the charged scalar and the DM particle, and scalar couplings are presented.","authors_text":"Bogumila Swiezewska, Maria Krawczyk","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-05-31T11:10:27Z","title":"2-photon decay rate of the scalar boson in the Inert Doublet Model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1305.7356","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:cd1ca42997baef1cd5997a5d1e88dabac019587b81a652ac4716c8a3c93fcc0b","target":"record","created_at":"2026-05-18T03:22:07Z","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":"75f1889092b68ea9881583e951d18ec22df7293338746c69acc1520847fe6e28","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-05-31T11:10:27Z","title_canon_sha256":"aefea70f7d221e1d79727c173c97cdaa8827214982097ac0c89a69347e595e13"},"schema_version":"1.0","source":{"id":"1305.7356","kind":"arxiv","version":1}},"canonical_sha256":"bc5c25f7549dc13f4a900765c11ddd387e57cdaef8fcaae167f3aad530e3a3c3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"bc5c25f7549dc13f4a900765c11ddd387e57cdaef8fcaae167f3aad530e3a3c3","first_computed_at":"2026-05-18T03:22:07.111975Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:22:07.111975Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"OaO8trwcwMqZ3WqBYdY9wj5wFr+JOLPA7nKn8Q0yv4Zr2j4+Ltp/oPQH9epehdpbZ+JOloipau6TFDeTYQ4qAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:22:07.112500Z","signed_message":"canonical_sha256_bytes"},"source_id":"1305.7356","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cd1ca42997baef1cd5997a5d1e88dabac019587b81a652ac4716c8a3c93fcc0b","sha256:ebbaf3f7e327b9ef004addabd1cd0efc0f62fad6185abaee54c751e6937521a8"],"state_sha256":"d67dab4835d5e3ed6d2dc4a90f84b3f7e0e7b657c7206da284a0d7aadf06bb5e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"TGXD987yXsp2asftOpfhNkcgCRaKn4SEQC43+RZx4oaB9e6BYjljT6lOrxOJk1oqfCwtnMyIBO5rLO09FaU/Cg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T01:36:29.795492Z","bundle_sha256":"c8085521318705f3821493d25ee2924b67b9536ba77c2ed838cd972edcff80f4"}}