{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:QLFOJBK5C3I4VI6PCMLW54XR2Q","short_pith_number":"pith:QLFOJBK5","schema_version":"1.0","canonical_sha256":"82cae4855d16d1caa3cf13176ef2f1d43a2880cdd625140cfc4eaef5c1e7e8ef","source":{"kind":"arxiv","id":"1602.01216","version":2},"attestation_state":"computed","paper":{"title":"Inflation and the Measurement Problem","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","hep-th","quant-ph"],"primary_cat":"gr-qc","authors_text":"Dhrubo Jyoti, Joao Magueijo, Stephon Alexander","submitted_at":"2016-02-03T07:40:25Z","abstract_excerpt":"We propose a solution to the quantum measurement problem in Inflation. Our model treats Fourier modes of cosmological perturbations as analogous to particles in a weakly-interacting Bose gas. We generalize the idea of a macroscopic wavefunction to cosmological fields, and construct a self-interaction Hamiltonian that focuses that wavefunction. By appropriately setting the coupling between modes, we obtain the standard adiabatic, scale-invariant power spectrum. Because of Central Limit Theorem (CLT), we recover a Gaussian Random Field, consistent with observations."},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1602.01216","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2016-02-03T07:40:25Z","cross_cats_sorted":["astro-ph.CO","hep-th","quant-ph"],"title_canon_sha256":"b37c4d54cb1f46cfbd58c86990d459d8bd4b79665d96b653b0362f0362b58e26","abstract_canon_sha256":"16cfe009be799ada5a7abca1ff793e70cdb1cfb43f4aa83a03b82a4b01e014f7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:09:36.102925Z","signature_b64":"ydtYBggsJfbgYnVCd0NPrkZ56+9Ifxm31wPBW9cAVTw+fHC4JkiRDAdRQqNEkzEQVimSTAiQMa9z3kJMb5LfDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"82cae4855d16d1caa3cf13176ef2f1d43a2880cdd625140cfc4eaef5c1e7e8ef","last_reissued_at":"2026-05-18T01:09:36.102484Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:09:36.102484Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Inflation and the Measurement Problem","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","hep-th","quant-ph"],"primary_cat":"gr-qc","authors_text":"Dhrubo Jyoti, Joao Magueijo, Stephon Alexander","submitted_at":"2016-02-03T07:40:25Z","abstract_excerpt":"We propose a solution to the quantum measurement problem in Inflation. Our model treats Fourier modes of cosmological perturbations as analogous to particles in a weakly-interacting Bose gas. We generalize the idea of a macroscopic wavefunction to cosmological fields, and construct a self-interaction Hamiltonian that focuses that wavefunction. By appropriately setting the coupling between modes, we obtain the standard adiabatic, scale-invariant power spectrum. Because of Central Limit Theorem (CLT), we recover a Gaussian Random Field, consistent with observations."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1602.01216","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1602.01216","created_at":"2026-05-18T01:09:36.102550+00:00"},{"alias_kind":"arxiv_version","alias_value":"1602.01216v2","created_at":"2026-05-18T01:09:36.102550+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1602.01216","created_at":"2026-05-18T01:09:36.102550+00:00"},{"alias_kind":"pith_short_12","alias_value":"QLFOJBK5C3I4","created_at":"2026-05-18T12:30:39.010887+00:00"},{"alias_kind":"pith_short_16","alias_value":"QLFOJBK5C3I4VI6P","created_at":"2026-05-18T12:30:39.010887+00:00"},{"alias_kind":"pith_short_8","alias_value":"QLFOJBK5","created_at":"2026-05-18T12:30:39.010887+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QLFOJBK5C3I4VI6PCMLW54XR2Q","json":"https://pith.science/pith/QLFOJBK5C3I4VI6PCMLW54XR2Q.json","graph_json":"https://pith.science/api/pith-number/QLFOJBK5C3I4VI6PCMLW54XR2Q/graph.json","events_json":"https://pith.science/api/pith-number/QLFOJBK5C3I4VI6PCMLW54XR2Q/events.json","paper":"https://pith.science/paper/QLFOJBK5"},"agent_actions":{"view_html":"https://pith.science/pith/QLFOJBK5C3I4VI6PCMLW54XR2Q","download_json":"https://pith.science/pith/QLFOJBK5C3I4VI6PCMLW54XR2Q.json","view_paper":"https://pith.science/paper/QLFOJBK5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1602.01216&json=true","fetch_graph":"https://pith.science/api/pith-number/QLFOJBK5C3I4VI6PCMLW54XR2Q/graph.json","fetch_events":"https://pith.science/api/pith-number/QLFOJBK5C3I4VI6PCMLW54XR2Q/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QLFOJBK5C3I4VI6PCMLW54XR2Q/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QLFOJBK5C3I4VI6PCMLW54XR2Q/action/storage_attestation","attest_author":"https://pith.science/pith/QLFOJBK5C3I4VI6PCMLW54XR2Q/action/author_attestation","sign_citation":"https://pith.science/pith/QLFOJBK5C3I4VI6PCMLW54XR2Q/action/citation_signature","submit_replication":"https://pith.science/pith/QLFOJBK5C3I4VI6PCMLW54XR2Q/action/replication_record"}},"created_at":"2026-05-18T01:09:36.102550+00:00","updated_at":"2026-05-18T01:09:36.102550+00:00"}