{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:JGTGYHZI66ILJM7UIORBGICCVO","short_pith_number":"pith:JGTGYHZI","schema_version":"1.0","canonical_sha256":"49a66c1f28f790b4b3f443a2132042aba37d54fae24a3019d325595259f74c11","source":{"kind":"arxiv","id":"1107.0766","version":1},"attestation_state":"computed","paper":{"title":"A nonlinear scalar model of extreme mass ratio inspirals in effective field theory II. Scalar perturbations and a master source","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"Chad R. Galley","submitted_at":"2011-07-05T02:04:06Z","abstract_excerpt":"The motion of a small compact object (SCO) in a background spacetime is investigated further in a class of model nonlinear scalar field theories having a perturbative structure analogous to the General Relativistic description of extreme mass ratio inspirals (EMRIs). We derive regular expressions for the scalar perturbations generated by the SCO's motion valid through third order in $\\epsilon$, the size of the SCO to the background curvature length scale. Our expressions are compared to those calculated through second order in $\\epsilon$ by Rosenthal in [E. Rosenthal, CQG 22, S859 (2005)] and "},"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":"1107.0766","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2011-07-05T02:04:06Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"80889a79bbfd5a2910e3d994677dedba852f4b5a4fad4b53cf281ca952f44548","abstract_canon_sha256":"95eacc76248c6f522a2c4bd927153771a921916d7439191045166499e50d5d70"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:01:24.882838Z","signature_b64":"UoqJNuFcvvikVk6E7l1zlrI+egtmvkwATOHj9xRWFlNUcqHFiA4JO5DBI6lomK0ONWl6ZDPQ0iDji8/WtgYtAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"49a66c1f28f790b4b3f443a2132042aba37d54fae24a3019d325595259f74c11","last_reissued_at":"2026-05-18T02:01:24.882448Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:01:24.882448Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A nonlinear scalar model of extreme mass ratio inspirals in effective field theory II. Scalar perturbations and a master source","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"Chad R. Galley","submitted_at":"2011-07-05T02:04:06Z","abstract_excerpt":"The motion of a small compact object (SCO) in a background spacetime is investigated further in a class of model nonlinear scalar field theories having a perturbative structure analogous to the General Relativistic description of extreme mass ratio inspirals (EMRIs). We derive regular expressions for the scalar perturbations generated by the SCO's motion valid through third order in $\\epsilon$, the size of the SCO to the background curvature length scale. Our expressions are compared to those calculated through second order in $\\epsilon$ by Rosenthal in [E. Rosenthal, CQG 22, S859 (2005)] and "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1107.0766","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1107.0766","created_at":"2026-05-18T02:01:24.882513+00:00"},{"alias_kind":"arxiv_version","alias_value":"1107.0766v1","created_at":"2026-05-18T02:01:24.882513+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1107.0766","created_at":"2026-05-18T02:01:24.882513+00:00"},{"alias_kind":"pith_short_12","alias_value":"JGTGYHZI66IL","created_at":"2026-05-18T12:26:32.869790+00:00"},{"alias_kind":"pith_short_16","alias_value":"JGTGYHZI66ILJM7U","created_at":"2026-05-18T12:26:32.869790+00:00"},{"alias_kind":"pith_short_8","alias_value":"JGTGYHZI","created_at":"2026-05-18T12:26:32.869790+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/JGTGYHZI66ILJM7UIORBGICCVO","json":"https://pith.science/pith/JGTGYHZI66ILJM7UIORBGICCVO.json","graph_json":"https://pith.science/api/pith-number/JGTGYHZI66ILJM7UIORBGICCVO/graph.json","events_json":"https://pith.science/api/pith-number/JGTGYHZI66ILJM7UIORBGICCVO/events.json","paper":"https://pith.science/paper/JGTGYHZI"},"agent_actions":{"view_html":"https://pith.science/pith/JGTGYHZI66ILJM7UIORBGICCVO","download_json":"https://pith.science/pith/JGTGYHZI66ILJM7UIORBGICCVO.json","view_paper":"https://pith.science/paper/JGTGYHZI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1107.0766&json=true","fetch_graph":"https://pith.science/api/pith-number/JGTGYHZI66ILJM7UIORBGICCVO/graph.json","fetch_events":"https://pith.science/api/pith-number/JGTGYHZI66ILJM7UIORBGICCVO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JGTGYHZI66ILJM7UIORBGICCVO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JGTGYHZI66ILJM7UIORBGICCVO/action/storage_attestation","attest_author":"https://pith.science/pith/JGTGYHZI66ILJM7UIORBGICCVO/action/author_attestation","sign_citation":"https://pith.science/pith/JGTGYHZI66ILJM7UIORBGICCVO/action/citation_signature","submit_replication":"https://pith.science/pith/JGTGYHZI66ILJM7UIORBGICCVO/action/replication_record"}},"created_at":"2026-05-18T02:01:24.882513+00:00","updated_at":"2026-05-18T02:01:24.882513+00:00"}