{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:5JI22Y5KPJS37QCSUHNP3ZVQNX","short_pith_number":"pith:5JI22Y5K","canonical_record":{"source":{"id":"1004.1144","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2010-04-07T17:49:29Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"ef643809f2cd8851dcdd7fe2282f027cbe02dbba833009cbffaf9da52c34c690","abstract_canon_sha256":"e42bf5d237206bdbafa59bb5fe7c97984c26fb27c498eb47e7f2f5001caa689e"},"schema_version":"1.0"},"canonical_sha256":"ea51ad63aa7a65bfc052a1dafde6b06dfdc3977591d2acf5a68f0a39cdde27d7","source":{"kind":"arxiv","id":"1004.1144","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1004.1144","created_at":"2026-05-18T02:08:08Z"},{"alias_kind":"arxiv_version","alias_value":"1004.1144v1","created_at":"2026-05-18T02:08:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1004.1144","created_at":"2026-05-18T02:08:08Z"},{"alias_kind":"pith_short_12","alias_value":"5JI22Y5KPJS3","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_16","alias_value":"5JI22Y5KPJS37QCS","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_8","alias_value":"5JI22Y5K","created_at":"2026-05-18T12:26:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:5JI22Y5KPJS37QCSUHNP3ZVQNX","target":"record","payload":{"canonical_record":{"source":{"id":"1004.1144","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2010-04-07T17:49:29Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"ef643809f2cd8851dcdd7fe2282f027cbe02dbba833009cbffaf9da52c34c690","abstract_canon_sha256":"e42bf5d237206bdbafa59bb5fe7c97984c26fb27c498eb47e7f2f5001caa689e"},"schema_version":"1.0"},"canonical_sha256":"ea51ad63aa7a65bfc052a1dafde6b06dfdc3977591d2acf5a68f0a39cdde27d7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:08:08.336023Z","signature_b64":"m0QYJnEt0slPVlYoJot/2OI6tKJ5IMl4ByzjAOXOs93NJIH5b+TsKQIoCaCa7QzNWRGy6gN7NHRGZHHTpJauDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ea51ad63aa7a65bfc052a1dafde6b06dfdc3977591d2acf5a68f0a39cdde27d7","last_reissued_at":"2026-05-18T02:08:08.335360Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:08:08.335360Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1004.1144","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:08:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HnCTTZbC1RIZmRm8XxVdHF8RWtxo2rL6rOTvNE3Gbg94jDELhgtfsKnHfFgnsO0+1HelqlelyC/3gHxv2DG7DA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T15:07:18.446019Z"},"content_sha256":"0f9c080fa1c52c1c9ed09d2c8869ce935665379cdd98753e4c68b8a686c6c33d","schema_version":"1.0","event_id":"sha256:0f9c080fa1c52c1c9ed09d2c8869ce935665379cdd98753e4c68b8a686c6c33d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:5JI22Y5KPJS37QCSUHNP3ZVQNX","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Ballistic transport, chiral anomaly and emergence of the neutral electron - hole plasma in graphene","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat.mes-hall","authors_text":"B. Rosenstein, H.C. Kao, M. Lewkowicz","submitted_at":"2010-04-07T17:49:29Z","abstract_excerpt":"The process of coherent creation of particle - hole excitations by an electric field in graphene is quantitatively described using a dynamic \"first quantized\" approach. We calculate the evolution of current density, number of pairs and energy in ballistic regime using the tight binding model. The series in electric field strength $E$ up to third order in both DC and AC are calculated. We show how the physics far from the two Dirac points enters various physical quantities in linear response and how it is related to the chiral anomaly. The third harmonic generation and the imaginary part of con"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1004.1144","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:08:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"k9+nuxjR1/E9i4QIvBIJBEiWMGUVu7oKJT567JBfpBRdgrPD6HZn1OQO2cVDfz4PX6jQQ1SRR+oXKBi1SNfFBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T15:07:18.446647Z"},"content_sha256":"ebcad29d29756881a9092e3420899763544db5ea99f97924b9914f0c1ce93437","schema_version":"1.0","event_id":"sha256:ebcad29d29756881a9092e3420899763544db5ea99f97924b9914f0c1ce93437"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5JI22Y5KPJS37QCSUHNP3ZVQNX/bundle.json","state_url":"https://pith.science/pith/5JI22Y5KPJS37QCSUHNP3ZVQNX/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5JI22Y5KPJS37QCSUHNP3ZVQNX/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":"2026-05-29T15:07:18Z","links":{"resolver":"https://pith.science/pith/5JI22Y5KPJS37QCSUHNP3ZVQNX","bundle":"https://pith.science/pith/5JI22Y5KPJS37QCSUHNP3ZVQNX/bundle.json","state":"https://pith.science/pith/5JI22Y5KPJS37QCSUHNP3ZVQNX/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5JI22Y5KPJS37QCSUHNP3ZVQNX/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:5JI22Y5KPJS37QCSUHNP3ZVQNX","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":"e42bf5d237206bdbafa59bb5fe7c97984c26fb27c498eb47e7f2f5001caa689e","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2010-04-07T17:49:29Z","title_canon_sha256":"ef643809f2cd8851dcdd7fe2282f027cbe02dbba833009cbffaf9da52c34c690"},"schema_version":"1.0","source":{"id":"1004.1144","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1004.1144","created_at":"2026-05-18T02:08:08Z"},{"alias_kind":"arxiv_version","alias_value":"1004.1144v1","created_at":"2026-05-18T02:08:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1004.1144","created_at":"2026-05-18T02:08:08Z"},{"alias_kind":"pith_short_12","alias_value":"5JI22Y5KPJS3","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_16","alias_value":"5JI22Y5KPJS37QCS","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_8","alias_value":"5JI22Y5K","created_at":"2026-05-18T12:26:04Z"}],"graph_snapshots":[{"event_id":"sha256:ebcad29d29756881a9092e3420899763544db5ea99f97924b9914f0c1ce93437","target":"graph","created_at":"2026-05-18T02:08:08Z","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"},"paper":{"abstract_excerpt":"The process of coherent creation of particle - hole excitations by an electric field in graphene is quantitatively described using a dynamic \"first quantized\" approach. We calculate the evolution of current density, number of pairs and energy in ballistic regime using the tight binding model. The series in electric field strength $E$ up to third order in both DC and AC are calculated. We show how the physics far from the two Dirac points enters various physical quantities in linear response and how it is related to the chiral anomaly. The third harmonic generation and the imaginary part of con","authors_text":"B. Rosenstein, H.C. Kao, M. Lewkowicz","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2010-04-07T17:49:29Z","title":"Ballistic transport, chiral anomaly and emergence of the neutral electron - hole plasma in graphene"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1004.1144","kind":"arxiv","version":1},"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":"sha256:0f9c080fa1c52c1c9ed09d2c8869ce935665379cdd98753e4c68b8a686c6c33d","target":"record","created_at":"2026-05-18T02:08:08Z","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":"e42bf5d237206bdbafa59bb5fe7c97984c26fb27c498eb47e7f2f5001caa689e","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2010-04-07T17:49:29Z","title_canon_sha256":"ef643809f2cd8851dcdd7fe2282f027cbe02dbba833009cbffaf9da52c34c690"},"schema_version":"1.0","source":{"id":"1004.1144","kind":"arxiv","version":1}},"canonical_sha256":"ea51ad63aa7a65bfc052a1dafde6b06dfdc3977591d2acf5a68f0a39cdde27d7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ea51ad63aa7a65bfc052a1dafde6b06dfdc3977591d2acf5a68f0a39cdde27d7","first_computed_at":"2026-05-18T02:08:08.335360Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:08:08.335360Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"m0QYJnEt0slPVlYoJot/2OI6tKJ5IMl4ByzjAOXOs93NJIH5b+TsKQIoCaCa7QzNWRGy6gN7NHRGZHHTpJauDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:08:08.336023Z","signed_message":"canonical_sha256_bytes"},"source_id":"1004.1144","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0f9c080fa1c52c1c9ed09d2c8869ce935665379cdd98753e4c68b8a686c6c33d","sha256:ebcad29d29756881a9092e3420899763544db5ea99f97924b9914f0c1ce93437"],"state_sha256":"59bd502a0c8493d152624130a569b5f4eb40a9cded51148f4bfe3a2c618396cf"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DTQen9kEQq7zQTldcVnAdXrAvYFddGRH+u9PG7tyfhwVj04x6bsaF0kpEZcpgDCOxlr/onW9oRV4eDY+lw8iAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-29T15:07:18.450019Z","bundle_sha256":"06f110cf952586755b65a7fc7d699944ee4e67b4e12750f43387fd89bdbe7745"}}