{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:I7O72XNQCCBXTBDJRN4Q7FGLPD","short_pith_number":"pith:I7O72XNQ","canonical_record":{"source":{"id":"1606.02969","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-06-09T14:07:29Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"c154a0bf68069dee2284cb2ff7d66d4e02c1708556e9762f9b32adedb100c2c8","abstract_canon_sha256":"5018ebad310fa4b777507013e3176a6a38aade7b8214f459f2613874a8b45afd"},"schema_version":"1.0"},"canonical_sha256":"47ddfd5db010837984698b790f94cb78fb322ec33a6e04cf9216ff7d26203475","source":{"kind":"arxiv","id":"1606.02969","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1606.02969","created_at":"2026-05-18T01:04:12Z"},{"alias_kind":"arxiv_version","alias_value":"1606.02969v2","created_at":"2026-05-18T01:04:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1606.02969","created_at":"2026-05-18T01:04:12Z"},{"alias_kind":"pith_short_12","alias_value":"I7O72XNQCCBX","created_at":"2026-05-18T12:30:22Z"},{"alias_kind":"pith_short_16","alias_value":"I7O72XNQCCBXTBDJ","created_at":"2026-05-18T12:30:22Z"},{"alias_kind":"pith_short_8","alias_value":"I7O72XNQ","created_at":"2026-05-18T12:30:22Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:I7O72XNQCCBXTBDJRN4Q7FGLPD","target":"record","payload":{"canonical_record":{"source":{"id":"1606.02969","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-06-09T14:07:29Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"c154a0bf68069dee2284cb2ff7d66d4e02c1708556e9762f9b32adedb100c2c8","abstract_canon_sha256":"5018ebad310fa4b777507013e3176a6a38aade7b8214f459f2613874a8b45afd"},"schema_version":"1.0"},"canonical_sha256":"47ddfd5db010837984698b790f94cb78fb322ec33a6e04cf9216ff7d26203475","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:04:12.492461Z","signature_b64":"91T+mUjKuegf1PY//f8bYSogVmN8HBXuXibMImitNkuc/oXDcV7rm2gNT+t3IvcYrv2grabAe5FOgtnhQflDAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"47ddfd5db010837984698b790f94cb78fb322ec33a6e04cf9216ff7d26203475","last_reissued_at":"2026-05-18T01:04:12.491867Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:04:12.491867Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1606.02969","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":"2026-05-18T01:04:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"S+dOKIJCly/3gMP0jeDW2n0gPz5LJsycOXEjIz9jfEkN1OM6f7hWqCRZIMfaRdHLzVjwCRhHbdHSrOOVv/95Cg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T05:03:45.986823Z"},"content_sha256":"d561e9b39366438d9a982aae7f2e012d1fc1a41af267092f1523c88f02625c3c","schema_version":"1.0","event_id":"sha256:d561e9b39366438d9a982aae7f2e012d1fc1a41af267092f1523c88f02625c3c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:I7O72XNQCCBXTBDJRN4Q7FGLPD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"AdS/QCD approach to the scale-invariant extension of the standard model with a strongly interacting hidden sector","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Dong-Won Jung, Hisaki Hatanaka, Pyungwon Ko","submitted_at":"2016-06-09T14:07:29Z","abstract_excerpt":"In this paper, we revisit a scale-invariant extension of the standard model (SM) with a strongly interacting hidden sector within AdS/QCD approach. Using the AdS/QCD, we reduce the number of input parameters to three, {\\it i.e.} hidden pion decay constant, hidden pion mass and $\\tan\\beta$ that is defined as the ratio of the vacuum expectation values (VEV) of the singlet scalar field and the SM Higgs boson. As a result, our model has sharp predictability. We perform the phenomenological analysis of the hidden pions which is one of the dark matter (DM) candidates in this model. With various theo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1606.02969","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":"2026-05-18T01:04:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/1Pq86CeiyWc+weKqR/LAKKCcEdCeVOxyUByMDe2+8tkf6X/VFTcM4xr25jS8NIbck1LCh73UzU2Fp+4Eq9BBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T05:03:45.987493Z"},"content_sha256":"c028402e8145745d7bf429170786e6c732efb09ee72bc1db35953e307ca79f70","schema_version":"1.0","event_id":"sha256:c028402e8145745d7bf429170786e6c732efb09ee72bc1db35953e307ca79f70"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/I7O72XNQCCBXTBDJRN4Q7FGLPD/bundle.json","state_url":"https://pith.science/pith/I7O72XNQCCBXTBDJRN4Q7FGLPD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/I7O72XNQCCBXTBDJRN4Q7FGLPD/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":"2026-05-26T05:03:45Z","links":{"resolver":"https://pith.science/pith/I7O72XNQCCBXTBDJRN4Q7FGLPD","bundle":"https://pith.science/pith/I7O72XNQCCBXTBDJRN4Q7FGLPD/bundle.json","state":"https://pith.science/pith/I7O72XNQCCBXTBDJRN4Q7FGLPD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/I7O72XNQCCBXTBDJRN4Q7FGLPD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:I7O72XNQCCBXTBDJRN4Q7FGLPD","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":"5018ebad310fa4b777507013e3176a6a38aade7b8214f459f2613874a8b45afd","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-06-09T14:07:29Z","title_canon_sha256":"c154a0bf68069dee2284cb2ff7d66d4e02c1708556e9762f9b32adedb100c2c8"},"schema_version":"1.0","source":{"id":"1606.02969","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1606.02969","created_at":"2026-05-18T01:04:12Z"},{"alias_kind":"arxiv_version","alias_value":"1606.02969v2","created_at":"2026-05-18T01:04:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1606.02969","created_at":"2026-05-18T01:04:12Z"},{"alias_kind":"pith_short_12","alias_value":"I7O72XNQCCBX","created_at":"2026-05-18T12:30:22Z"},{"alias_kind":"pith_short_16","alias_value":"I7O72XNQCCBXTBDJ","created_at":"2026-05-18T12:30:22Z"},{"alias_kind":"pith_short_8","alias_value":"I7O72XNQ","created_at":"2026-05-18T12:30:22Z"}],"graph_snapshots":[{"event_id":"sha256:c028402e8145745d7bf429170786e6c732efb09ee72bc1db35953e307ca79f70","target":"graph","created_at":"2026-05-18T01:04:12Z","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 paper, we revisit a scale-invariant extension of the standard model (SM) with a strongly interacting hidden sector within AdS/QCD approach. Using the AdS/QCD, we reduce the number of input parameters to three, {\\it i.e.} hidden pion decay constant, hidden pion mass and $\\tan\\beta$ that is defined as the ratio of the vacuum expectation values (VEV) of the singlet scalar field and the SM Higgs boson. As a result, our model has sharp predictability. We perform the phenomenological analysis of the hidden pions which is one of the dark matter (DM) candidates in this model. With various theo","authors_text":"Dong-Won Jung, Hisaki Hatanaka, Pyungwon Ko","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-06-09T14:07:29Z","title":"AdS/QCD approach to the scale-invariant extension of the standard model with a strongly interacting hidden sector"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1606.02969","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:d561e9b39366438d9a982aae7f2e012d1fc1a41af267092f1523c88f02625c3c","target":"record","created_at":"2026-05-18T01:04:12Z","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":"5018ebad310fa4b777507013e3176a6a38aade7b8214f459f2613874a8b45afd","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-06-09T14:07:29Z","title_canon_sha256":"c154a0bf68069dee2284cb2ff7d66d4e02c1708556e9762f9b32adedb100c2c8"},"schema_version":"1.0","source":{"id":"1606.02969","kind":"arxiv","version":2}},"canonical_sha256":"47ddfd5db010837984698b790f94cb78fb322ec33a6e04cf9216ff7d26203475","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"47ddfd5db010837984698b790f94cb78fb322ec33a6e04cf9216ff7d26203475","first_computed_at":"2026-05-18T01:04:12.491867Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:04:12.491867Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"91T+mUjKuegf1PY//f8bYSogVmN8HBXuXibMImitNkuc/oXDcV7rm2gNT+t3IvcYrv2grabAe5FOgtnhQflDAg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:04:12.492461Z","signed_message":"canonical_sha256_bytes"},"source_id":"1606.02969","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d561e9b39366438d9a982aae7f2e012d1fc1a41af267092f1523c88f02625c3c","sha256:c028402e8145745d7bf429170786e6c732efb09ee72bc1db35953e307ca79f70"],"state_sha256":"7520c8941efb9cd84245176e094c5b83ede33fae06b7274afbd52e343f096672"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1Vvg+4zSg36OFdKeHPTLyyDIDCxJnTWVrZ7SZltXx1Q+vQ747PAuxALl9vpA5Qf/O8dCocT3+hn02t3O73GuDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T05:03:45.990903Z","bundle_sha256":"022706ccf4fda5777ef0369b2344b2b9901d2dd69090563a05ec1bccbc733142"}}