{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:HFSCXJVGBYYL7HA3OX3JFZ3H2Y","short_pith_number":"pith:HFSCXJVG","schema_version":"1.0","canonical_sha256":"39642ba6a60e30bf9c1b75f692e767d608c5339cedcf187b2a23a1f3e942947d","source":{"kind":"arxiv","id":"1905.07414","version":2},"attestation_state":"computed","paper":{"title":"On the Spectrum of Electrons Accelerated in Supernova Remnants","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"astro-ph.HE","authors_text":"Damiano Caprioli, Rebecca Diesing","submitted_at":"2019-05-17T18:00:04Z","abstract_excerpt":"Using a semi-analytic model of non-linear diffusive shock acceleration, we model the spectrum of cosmic ray (CR) electrons accelerated by supernova remnants (SNRs). Because electrons experience synchrotron losses in the amplified magnetic fields characteristic of SNRs, they exhibit substantially steeper spectra than protons. In particular, we find that the difference between the electron and proton spectral index (power law slope) ranges from 0.1 to 0.4. Our findings must be reckoned with theories of Galactic CR transport, which often assume that electrons and protons are injected with the sam"},"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":"1905.07414","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.HE","submitted_at":"2019-05-17T18:00:04Z","cross_cats_sorted":[],"title_canon_sha256":"4141e6301a9d0d8b054973ab07c34474ff05fef932f64791fd05005c7225264f","abstract_canon_sha256":"29996bdc742e87dd2d84bb1eda63d5565e7510f60a5b19566461bd6126444b84"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T23:58:50.318870Z","signature_b64":"dw2k8wdlo/EyhrXUMNGtEhuQy+s/YLAtyiYfJPooRMSWGyQ8Pf/FpSsYy5niDkFxTcUagUGn8HCBXnQF+vNEBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"39642ba6a60e30bf9c1b75f692e767d608c5339cedcf187b2a23a1f3e942947d","last_reissued_at":"2026-07-04T23:58:50.318467Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T23:58:50.318467Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On the Spectrum of Electrons Accelerated in Supernova Remnants","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"astro-ph.HE","authors_text":"Damiano Caprioli, Rebecca Diesing","submitted_at":"2019-05-17T18:00:04Z","abstract_excerpt":"Using a semi-analytic model of non-linear diffusive shock acceleration, we model the spectrum of cosmic ray (CR) electrons accelerated by supernova remnants (SNRs). Because electrons experience synchrotron losses in the amplified magnetic fields characteristic of SNRs, they exhibit substantially steeper spectra than protons. In particular, we find that the difference between the electron and proton spectral index (power law slope) ranges from 0.1 to 0.4. Our findings must be reckoned with theories of Galactic CR transport, which often assume that electrons and protons are injected with the sam"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1905.07414","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1905.07414/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":"1905.07414","created_at":"2026-07-04T23:58:50.318526+00:00"},{"alias_kind":"arxiv_version","alias_value":"1905.07414v2","created_at":"2026-07-04T23:58:50.318526+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1905.07414","created_at":"2026-07-04T23:58:50.318526+00:00"},{"alias_kind":"pith_short_12","alias_value":"HFSCXJVGBYYL","created_at":"2026-07-04T23:58:50.318526+00:00"},{"alias_kind":"pith_short_16","alias_value":"HFSCXJVGBYYL7HA3","created_at":"2026-07-04T23:58:50.318526+00:00"},{"alias_kind":"pith_short_8","alias_value":"HFSCXJVG","created_at":"2026-07-04T23:58:50.318526+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.06011","citing_title":"SECRET: Stochasticity Emulator for Cosmic Ray Electrons","ref_index":25,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HFSCXJVGBYYL7HA3OX3JFZ3H2Y","json":"https://pith.science/pith/HFSCXJVGBYYL7HA3OX3JFZ3H2Y.json","graph_json":"https://pith.science/api/pith-number/HFSCXJVGBYYL7HA3OX3JFZ3H2Y/graph.json","events_json":"https://pith.science/api/pith-number/HFSCXJVGBYYL7HA3OX3JFZ3H2Y/events.json","paper":"https://pith.science/paper/HFSCXJVG"},"agent_actions":{"view_html":"https://pith.science/pith/HFSCXJVGBYYL7HA3OX3JFZ3H2Y","download_json":"https://pith.science/pith/HFSCXJVGBYYL7HA3OX3JFZ3H2Y.json","view_paper":"https://pith.science/paper/HFSCXJVG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1905.07414&json=true","fetch_graph":"https://pith.science/api/pith-number/HFSCXJVGBYYL7HA3OX3JFZ3H2Y/graph.json","fetch_events":"https://pith.science/api/pith-number/HFSCXJVGBYYL7HA3OX3JFZ3H2Y/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HFSCXJVGBYYL7HA3OX3JFZ3H2Y/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HFSCXJVGBYYL7HA3OX3JFZ3H2Y/action/storage_attestation","attest_author":"https://pith.science/pith/HFSCXJVGBYYL7HA3OX3JFZ3H2Y/action/author_attestation","sign_citation":"https://pith.science/pith/HFSCXJVGBYYL7HA3OX3JFZ3H2Y/action/citation_signature","submit_replication":"https://pith.science/pith/HFSCXJVGBYYL7HA3OX3JFZ3H2Y/action/replication_record"}},"created_at":"2026-07-04T23:58:50.318526+00:00","updated_at":"2026-07-04T23:58:50.318526+00:00"}