{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:TLBN3KODUNY5DSZLJKPVOCPHAV","short_pith_number":"pith:TLBN3KOD","schema_version":"1.0","canonical_sha256":"9ac2dda9c3a371d1cb2b4a9f5709e70562680434eefd7ad573ab8dc1b0bf65c7","source":{"kind":"arxiv","id":"2607.07602","version":1},"attestation_state":"computed","paper":{"title":"When the Environment Speaks: Quantum Signatures in Non-Attractor Inflation","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["gr-qc","hep-th"],"primary_cat":"astro-ph.CO","authors_text":"Gianpiero Mangano, Mattia Cielo, Ofelia Pisanti, Simone Scarlatella","submitted_at":"2026-07-08T16:20:44Z","abstract_excerpt":"We study the open quantum dynamics of the adiabatic curvature perturbation interacting with a massive entropic scalar environment during an inflationary scenario featuring a transient Ultra-Slow-Roll phase. Working within a Gaussian two-field effective Lagrangian, we employ the exact Transport Equations Method to track the full non-unitary, non-Markovian evolution of the system's covariance matrix across the SR-USR-SR transition. We find that the efficiency of decoherence is sensitive to the background kinematics at horizon crossing. Most importantly, the interaction with the environment leave"},"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":"2607.07602","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"astro-ph.CO","submitted_at":"2026-07-08T16:20:44Z","cross_cats_sorted":["gr-qc","hep-th"],"title_canon_sha256":"b1b9de77b50832084ad8b5eedae8d556a78d7e3501764d2691ff74ddc8ce55c5","abstract_canon_sha256":"935ae2b7627ca31d9de006f0694f9928b9239e4988037f19dc48fcaf2a1ace16"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-09T01:20:30.598369Z","signature_b64":"UD2IRRmb7KUuabMlbfN20K9VwHzNT1ofHn5UG3TuzEMUG6xn1UAOTP1fZUaG4en2lEwuEnE7GLIsn/nOfNbaDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9ac2dda9c3a371d1cb2b4a9f5709e70562680434eefd7ad573ab8dc1b0bf65c7","last_reissued_at":"2026-07-09T01:20:30.597955Z","signature_status":"signed_v1","first_computed_at":"2026-07-09T01:20:30.597955Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"When the Environment Speaks: Quantum Signatures in Non-Attractor Inflation","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["gr-qc","hep-th"],"primary_cat":"astro-ph.CO","authors_text":"Gianpiero Mangano, Mattia Cielo, Ofelia Pisanti, Simone Scarlatella","submitted_at":"2026-07-08T16:20:44Z","abstract_excerpt":"We study the open quantum dynamics of the adiabatic curvature perturbation interacting with a massive entropic scalar environment during an inflationary scenario featuring a transient Ultra-Slow-Roll phase. Working within a Gaussian two-field effective Lagrangian, we employ the exact Transport Equations Method to track the full non-unitary, non-Markovian evolution of the system's covariance matrix across the SR-USR-SR transition. We find that the efficiency of decoherence is sensitive to the background kinematics at horizon crossing. Most importantly, the interaction with the environment leave"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.07602","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2607.07602/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2607.07602","created_at":"2026-07-09T01:20:30.598013+00:00"},{"alias_kind":"arxiv_version","alias_value":"2607.07602v1","created_at":"2026-07-09T01:20:30.598013+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.07602","created_at":"2026-07-09T01:20:30.598013+00:00"},{"alias_kind":"pith_short_12","alias_value":"TLBN3KODUNY5","created_at":"2026-07-09T01:20:30.598013+00:00"},{"alias_kind":"pith_short_16","alias_value":"TLBN3KODUNY5DSZL","created_at":"2026-07-09T01:20:30.598013+00:00"},{"alias_kind":"pith_short_8","alias_value":"TLBN3KOD","created_at":"2026-07-09T01:20:30.598013+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.22914","citing_title":"Tensor Catalyzed Decoherence of Primordial Scalar Fluctuations","ref_index":21,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TLBN3KODUNY5DSZLJKPVOCPHAV","json":"https://pith.science/pith/TLBN3KODUNY5DSZLJKPVOCPHAV.json","graph_json":"https://pith.science/api/pith-number/TLBN3KODUNY5DSZLJKPVOCPHAV/graph.json","events_json":"https://pith.science/api/pith-number/TLBN3KODUNY5DSZLJKPVOCPHAV/events.json","paper":"https://pith.science/paper/TLBN3KOD"},"agent_actions":{"view_html":"https://pith.science/pith/TLBN3KODUNY5DSZLJKPVOCPHAV","download_json":"https://pith.science/pith/TLBN3KODUNY5DSZLJKPVOCPHAV.json","view_paper":"https://pith.science/paper/TLBN3KOD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2607.07602&json=true","fetch_graph":"https://pith.science/api/pith-number/TLBN3KODUNY5DSZLJKPVOCPHAV/graph.json","fetch_events":"https://pith.science/api/pith-number/TLBN3KODUNY5DSZLJKPVOCPHAV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TLBN3KODUNY5DSZLJKPVOCPHAV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TLBN3KODUNY5DSZLJKPVOCPHAV/action/storage_attestation","attest_author":"https://pith.science/pith/TLBN3KODUNY5DSZLJKPVOCPHAV/action/author_attestation","sign_citation":"https://pith.science/pith/TLBN3KODUNY5DSZLJKPVOCPHAV/action/citation_signature","submit_replication":"https://pith.science/pith/TLBN3KODUNY5DSZLJKPVOCPHAV/action/replication_record"}},"created_at":"2026-07-09T01:20:30.598013+00:00","updated_at":"2026-07-09T01:20:30.598013+00:00"}