{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:TCJ6TF2DZIBMIVQPCVKPE5IXKY","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":"4e10bdcae6cd294a0d8dd82637be615287945795a52eede6bbeb0c1b074d51f2","cross_cats_sorted":["hep-ph","physics.ins-det"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2014-10-23T09:38:57Z","title_canon_sha256":"9d7bc249ffe122baf7a8312f5dbaf0db201188f35933963fd5f0889067dc5ba5"},"schema_version":"1.0","source":{"id":"1410.6302","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1410.6302","created_at":"2026-05-18T02:39:31Z"},{"alias_kind":"arxiv_version","alias_value":"1410.6302v1","created_at":"2026-05-18T02:39:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.6302","created_at":"2026-05-18T02:39:31Z"},{"alias_kind":"pith_short_12","alias_value":"TCJ6TF2DZIBM","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_16","alias_value":"TCJ6TF2DZIBMIVQP","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_8","alias_value":"TCJ6TF2D","created_at":"2026-05-18T12:28:49Z"}],"graph_snapshots":[{"event_id":"sha256:7715a9dc6269e5ce8cb363f2d35e8fd56468f3b55636acfa799cf7528c1f5c3c","target":"graph","created_at":"2026-05-18T02:39:31Z","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":"Light cold dark matter consisting of weakly interacting slim (or sub-eV) particles (WISPs) has been in the focus of a large number of studies made over the past two decades. The QCD axion and axion-like particles with masses in the $0.1\\,\\mu$eV--$100\\,$meV are strong candidates for the dark matter particle, together with hidden photons with masses below $\\lesssim 100\\,$meV. This motivates several new initiatives in the field, including the WISP Dark Matter eXperiment (WISPDMX) and novel conceptual approaches for broad-band WISP searches using radiometry measurements in large volume chambers. F","authors_text":"1) Andreas Ringwald (2) ((1) Institut f\\\"ur Experimentalphysik, (2) Deutsches Elektronen-Synchrotron, (3) Max-Planck-Institut f\\\"ur Radioastronomie, Andrei Lobanov (3, Axel Lindner (2), Bonn, Dieter Horns (1), Germany, Germany), Hamburg, Universit\\\"at Hamburg","cross_cats":["hep-ph","physics.ins-det"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2014-10-23T09:38:57Z","title":"WISP Dark Matter eXperiment and Prospects for Broadband Dark Matter Searches in the $1\\,\\mu$eV--$10\\,$meV Mass Range"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.6302","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":"sha256:685f452d7ff531313cf4e9bdc8a258e0f02165f4c1eea29fb3bb09cdad04f254","target":"record","created_at":"2026-05-18T02:39:31Z","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":"4e10bdcae6cd294a0d8dd82637be615287945795a52eede6bbeb0c1b074d51f2","cross_cats_sorted":["hep-ph","physics.ins-det"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2014-10-23T09:38:57Z","title_canon_sha256":"9d7bc249ffe122baf7a8312f5dbaf0db201188f35933963fd5f0889067dc5ba5"},"schema_version":"1.0","source":{"id":"1410.6302","kind":"arxiv","version":1}},"canonical_sha256":"9893e99743ca02c4560f1554f2751756026c42b0395bba06a156d0abad607b4d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9893e99743ca02c4560f1554f2751756026c42b0395bba06a156d0abad607b4d","first_computed_at":"2026-05-18T02:39:31.148756Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:39:31.148756Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"y0USzmF5izIenyQ7tSuD+mXfFoT+HFRRjc1SM0bBO93mxUNrx5WvbMuaGFfUMVeXAl8f7MD2/QnogrqzwRTCCg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:39:31.149384Z","signed_message":"canonical_sha256_bytes"},"source_id":"1410.6302","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:685f452d7ff531313cf4e9bdc8a258e0f02165f4c1eea29fb3bb09cdad04f254","sha256:7715a9dc6269e5ce8cb363f2d35e8fd56468f3b55636acfa799cf7528c1f5c3c"],"state_sha256":"b86a7c8817200165c0038be0ad0fddac53548880cc2ec7fb90127a959803b733"}