{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:VVVLEI2654HYD4UPA2L6BWFAWS","short_pith_number":"pith:VVVLEI26","canonical_record":{"source":{"id":"2409.05147","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2024-09-08T16:24:43Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"4854a03b21a96236c73acfe007f7e149dceeb9c6c672c39d4acaa60b47f7c818","abstract_canon_sha256":"983c3323130bab683e0163efc2f85168dd4f9ac9e51202ca57121222e6245355"},"schema_version":"1.0"},"canonical_sha256":"ad6ab2235eef0f81f28f0697e0d8a0b4a6ad9b85e24098ccbdbba06dcde25f7a","source":{"kind":"arxiv","id":"2409.05147","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2409.05147","created_at":"2026-07-05T11:46:35Z"},{"alias_kind":"arxiv_version","alias_value":"2409.05147v2","created_at":"2026-07-05T11:46:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2409.05147","created_at":"2026-07-05T11:46:35Z"},{"alias_kind":"pith_short_12","alias_value":"VVVLEI2654HY","created_at":"2026-07-05T11:46:35Z"},{"alias_kind":"pith_short_16","alias_value":"VVVLEI2654HYD4UP","created_at":"2026-07-05T11:46:35Z"},{"alias_kind":"pith_short_8","alias_value":"VVVLEI26","created_at":"2026-07-05T11:46:35Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:VVVLEI2654HYD4UPA2L6BWFAWS","target":"record","payload":{"canonical_record":{"source":{"id":"2409.05147","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2024-09-08T16:24:43Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"4854a03b21a96236c73acfe007f7e149dceeb9c6c672c39d4acaa60b47f7c818","abstract_canon_sha256":"983c3323130bab683e0163efc2f85168dd4f9ac9e51202ca57121222e6245355"},"schema_version":"1.0"},"canonical_sha256":"ad6ab2235eef0f81f28f0697e0d8a0b4a6ad9b85e24098ccbdbba06dcde25f7a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:46:35.793110Z","signature_b64":"LXE+2WFxJac/SbXZE4hPavPAJO8XPSjztWm5OFbFgpisc6ud7dhCLH7btpl2oqdqvgvLHGTk9RT5pOpNIbhRCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ad6ab2235eef0f81f28f0697e0d8a0b4a6ad9b85e24098ccbdbba06dcde25f7a","last_reissued_at":"2026-07-05T11:46:35.792574Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:46:35.792574Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2409.05147","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T11:46:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6Q9ix/CCFN9jAzA8TO1gVcDYfIbKr+76jIbffnd9YwUzYNxsiai+B1Jl72orMihSyFggPTe22jwcRn6BmbvKAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-15T22:16:05.420879Z"},"content_sha256":"6ea43e34765c8ecf8fb0f5409fb2292e63a43ed33c0811291bc994d547bf7e0e","schema_version":"1.0","event_id":"sha256:6ea43e34765c8ecf8fb0f5409fb2292e63a43ed33c0811291bc994d547bf7e0e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:VVVLEI2654HYD4UPA2L6BWFAWS","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Testing the tomographic Fermi liquid hypothesis with high-order cyclotron resonance","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"cond-mat.str-el","authors_text":"Denis Bandurin, Dmitry Svintsov, Erwin M\\\"onch, Ilia Moiseenko, Kirill Kapralov, Sergey Ganichev","submitted_at":"2024-09-08T16:24:43Z","abstract_excerpt":"Recent theoretical studies of carrier-carrier scattering in degenerate two-dimensional systems have revealed radically different relaxation times for odd and even angular harmonics of distribution function. This theoretical concept, dubbed as 'tomographic Fermi liquid', is yet challenging to test with dc electrical measurements as electron scattering weakly affects the electrical resistivity. Here, we show that linewidth and amplitude of electromagnetic absorption at the multiple harmonics of the cyclotron resonance carries all necessary information to test the tomographic Fermi liquid hypothe"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2409.05147","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/2409.05147/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T11:46:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DEGDCxFrIHC1EJLDyu4lZJ/etSFKRV6x8ZdDUqhYAU2/KgdfjF/xDKPVdNKkKcGXSdopkHtNsNWFO8OxdoDPDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-15T22:16:05.421417Z"},"content_sha256":"f7520ab393f76dd378788425423739ca4e9e9a241892a850b5d33ecafac13432","schema_version":"1.0","event_id":"sha256:f7520ab393f76dd378788425423739ca4e9e9a241892a850b5d33ecafac13432"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/VVVLEI2654HYD4UPA2L6BWFAWS/bundle.json","state_url":"https://pith.science/pith/VVVLEI2654HYD4UPA2L6BWFAWS/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/VVVLEI2654HYD4UPA2L6BWFAWS/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-08-15T22:16:05Z","links":{"resolver":"https://pith.science/pith/VVVLEI2654HYD4UPA2L6BWFAWS","bundle":"https://pith.science/pith/VVVLEI2654HYD4UPA2L6BWFAWS/bundle.json","state":"https://pith.science/pith/VVVLEI2654HYD4UPA2L6BWFAWS/state.json","well_known_bundle":"https://pith.science/.well-known/pith/VVVLEI2654HYD4UPA2L6BWFAWS/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:VVVLEI2654HYD4UPA2L6BWFAWS","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":"983c3323130bab683e0163efc2f85168dd4f9ac9e51202ca57121222e6245355","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2024-09-08T16:24:43Z","title_canon_sha256":"4854a03b21a96236c73acfe007f7e149dceeb9c6c672c39d4acaa60b47f7c818"},"schema_version":"1.0","source":{"id":"2409.05147","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2409.05147","created_at":"2026-07-05T11:46:35Z"},{"alias_kind":"arxiv_version","alias_value":"2409.05147v2","created_at":"2026-07-05T11:46:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2409.05147","created_at":"2026-07-05T11:46:35Z"},{"alias_kind":"pith_short_12","alias_value":"VVVLEI2654HY","created_at":"2026-07-05T11:46:35Z"},{"alias_kind":"pith_short_16","alias_value":"VVVLEI2654HYD4UP","created_at":"2026-07-05T11:46:35Z"},{"alias_kind":"pith_short_8","alias_value":"VVVLEI26","created_at":"2026-07-05T11:46:35Z"}],"graph_snapshots":[{"event_id":"sha256:f7520ab393f76dd378788425423739ca4e9e9a241892a850b5d33ecafac13432","target":"graph","created_at":"2026-07-05T11:46:35Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2409.05147/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Recent theoretical studies of carrier-carrier scattering in degenerate two-dimensional systems have revealed radically different relaxation times for odd and even angular harmonics of distribution function. This theoretical concept, dubbed as 'tomographic Fermi liquid', is yet challenging to test with dc electrical measurements as electron scattering weakly affects the electrical resistivity. Here, we show that linewidth and amplitude of electromagnetic absorption at the multiple harmonics of the cyclotron resonance carries all necessary information to test the tomographic Fermi liquid hypothe","authors_text":"Denis Bandurin, Dmitry Svintsov, Erwin M\\\"onch, Ilia Moiseenko, Kirill Kapralov, Sergey Ganichev","cross_cats":["physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2024-09-08T16:24:43Z","title":"Testing the tomographic Fermi liquid hypothesis with high-order cyclotron resonance"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2409.05147","kind":"arxiv","version":2},"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":"sha256:6ea43e34765c8ecf8fb0f5409fb2292e63a43ed33c0811291bc994d547bf7e0e","target":"record","created_at":"2026-07-05T11:46:35Z","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":"983c3323130bab683e0163efc2f85168dd4f9ac9e51202ca57121222e6245355","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2024-09-08T16:24:43Z","title_canon_sha256":"4854a03b21a96236c73acfe007f7e149dceeb9c6c672c39d4acaa60b47f7c818"},"schema_version":"1.0","source":{"id":"2409.05147","kind":"arxiv","version":2}},"canonical_sha256":"ad6ab2235eef0f81f28f0697e0d8a0b4a6ad9b85e24098ccbdbba06dcde25f7a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ad6ab2235eef0f81f28f0697e0d8a0b4a6ad9b85e24098ccbdbba06dcde25f7a","first_computed_at":"2026-07-05T11:46:35.792574Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:46:35.792574Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"LXE+2WFxJac/SbXZE4hPavPAJO8XPSjztWm5OFbFgpisc6ud7dhCLH7btpl2oqdqvgvLHGTk9RT5pOpNIbhRCQ==","signature_status":"signed_v1","signed_at":"2026-07-05T11:46:35.793110Z","signed_message":"canonical_sha256_bytes"},"source_id":"2409.05147","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6ea43e34765c8ecf8fb0f5409fb2292e63a43ed33c0811291bc994d547bf7e0e","sha256:f7520ab393f76dd378788425423739ca4e9e9a241892a850b5d33ecafac13432"],"state_sha256":"73f986ecea3eccba83635c078f6c34dff9d3aa68870c7772eed4d742eec19eaa"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wEBtu1rbPyKZv4NZvaLT/2iEul30ZA3G+r8nRWCFd7ah1VZl5OOwUJjvtgvzI/TG5wi5gOMW4yFuAhM8gZUFBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-15T22:16:05.425752Z","bundle_sha256":"72edec19e5a109c87a0024253add3fb445b8bc97ea0804351cd7a8705112d044"}}