{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:UDMZF5O3MN5NM4AV7J5QE5OXHQ","short_pith_number":"pith:UDMZF5O3","canonical_record":{"source":{"id":"1108.5263","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2011-08-26T09:13:44Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"029888af5e8aa2a42dca55f5d46bda9f50faa3982a2fcf72261a916596e9f0a0","abstract_canon_sha256":"4e770075489eed1fdb5e34d5063d7cf91b21ddf246c4d321dd8ef967fbd1f4ad"},"schema_version":"1.0"},"canonical_sha256":"a0d992f5db637ad67015fa7b0275d73c30bfde63b185a7f42fd2d3e2da122eec","source":{"kind":"arxiv","id":"1108.5263","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1108.5263","created_at":"2026-05-18T04:05:38Z"},{"alias_kind":"arxiv_version","alias_value":"1108.5263v1","created_at":"2026-05-18T04:05:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1108.5263","created_at":"2026-05-18T04:05:38Z"},{"alias_kind":"pith_short_12","alias_value":"UDMZF5O3MN5N","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_16","alias_value":"UDMZF5O3MN5NM4AV","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_8","alias_value":"UDMZF5O3","created_at":"2026-05-18T12:26:42Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:UDMZF5O3MN5NM4AV7J5QE5OXHQ","target":"record","payload":{"canonical_record":{"source":{"id":"1108.5263","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2011-08-26T09:13:44Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"029888af5e8aa2a42dca55f5d46bda9f50faa3982a2fcf72261a916596e9f0a0","abstract_canon_sha256":"4e770075489eed1fdb5e34d5063d7cf91b21ddf246c4d321dd8ef967fbd1f4ad"},"schema_version":"1.0"},"canonical_sha256":"a0d992f5db637ad67015fa7b0275d73c30bfde63b185a7f42fd2d3e2da122eec","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:05:38.382784Z","signature_b64":"Hn0iUQ/Ldusa0UxHcwAy9xm7jLrfVg3AdenDS8DFRUomtvBT0CXcQvF5ndarKhUpTQ8hRhpR61unRqNUnXg+BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a0d992f5db637ad67015fa7b0275d73c30bfde63b185a7f42fd2d3e2da122eec","last_reissued_at":"2026-05-18T04:05:38.382426Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:05:38.382426Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1108.5263","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":"2026-05-18T04:05:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tQakWVrJbCTEuczD1QWXdBVYiL6xwr/Ym6cCZorHvj12hxKO5BR7Fxpbd2T+ndLBUTZ1dsHL7sCN+XcPMwNODg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T03:20:17.350796Z"},"content_sha256":"baaad3c7680c60fd0f8f5495b82b928f461d35f4fd9d501bdc1cdbd2f333393c","schema_version":"1.0","event_id":"sha256:baaad3c7680c60fd0f8f5495b82b928f461d35f4fd9d501bdc1cdbd2f333393c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:UDMZF5O3MN5NM4AV7J5QE5OXHQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Electronic transport within a quasi two-dimensional model for rubrene single-crystal field effect transistors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.str-el","authors_text":"C. A. Perroni, F. Gargiulo, V. Cataudella, V. Marigliano Ramaglia","submitted_at":"2011-08-26T09:13:44Z","abstract_excerpt":"Spectral and transport properties of the quasi two-dimensional adiabatic Su-Schrieffer-Heeger model are studied adjusting the parameters in order to model rubrene single-crystal field effect transistors with small but finite density of injected charge carriers. We show that, with increasing temperature $T$, the chemical potential moves into the tail of the density of states corresponding to localized states, but this is not enough to drive the system into an insulating state. The mobility along different crystallographic directions is calculated including vertex corrections which give rise to "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1108.5263","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":"2026-05-18T04:05:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CnY7Olm//JsOxF3cBPmk3x8TAd7mn6WB0YvO+Lbu/ploG1UhJUb+c11qi2oeD8W8y/fO2joy/zUL5Mcv/2kCBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T03:20:17.351631Z"},"content_sha256":"7049d778347ba0c4efaa14b9865d32516be2b47b736b357b995a1aecf14ac692","schema_version":"1.0","event_id":"sha256:7049d778347ba0c4efaa14b9865d32516be2b47b736b357b995a1aecf14ac692"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UDMZF5O3MN5NM4AV7J5QE5OXHQ/bundle.json","state_url":"https://pith.science/pith/UDMZF5O3MN5NM4AV7J5QE5OXHQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UDMZF5O3MN5NM4AV7J5QE5OXHQ/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":"2026-05-31T03:20:17Z","links":{"resolver":"https://pith.science/pith/UDMZF5O3MN5NM4AV7J5QE5OXHQ","bundle":"https://pith.science/pith/UDMZF5O3MN5NM4AV7J5QE5OXHQ/bundle.json","state":"https://pith.science/pith/UDMZF5O3MN5NM4AV7J5QE5OXHQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UDMZF5O3MN5NM4AV7J5QE5OXHQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:UDMZF5O3MN5NM4AV7J5QE5OXHQ","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":"4e770075489eed1fdb5e34d5063d7cf91b21ddf246c4d321dd8ef967fbd1f4ad","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2011-08-26T09:13:44Z","title_canon_sha256":"029888af5e8aa2a42dca55f5d46bda9f50faa3982a2fcf72261a916596e9f0a0"},"schema_version":"1.0","source":{"id":"1108.5263","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1108.5263","created_at":"2026-05-18T04:05:38Z"},{"alias_kind":"arxiv_version","alias_value":"1108.5263v1","created_at":"2026-05-18T04:05:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1108.5263","created_at":"2026-05-18T04:05:38Z"},{"alias_kind":"pith_short_12","alias_value":"UDMZF5O3MN5N","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_16","alias_value":"UDMZF5O3MN5NM4AV","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_8","alias_value":"UDMZF5O3","created_at":"2026-05-18T12:26:42Z"}],"graph_snapshots":[{"event_id":"sha256:7049d778347ba0c4efaa14b9865d32516be2b47b736b357b995a1aecf14ac692","target":"graph","created_at":"2026-05-18T04:05:38Z","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":"Spectral and transport properties of the quasi two-dimensional adiabatic Su-Schrieffer-Heeger model are studied adjusting the parameters in order to model rubrene single-crystal field effect transistors with small but finite density of injected charge carriers. We show that, with increasing temperature $T$, the chemical potential moves into the tail of the density of states corresponding to localized states, but this is not enough to drive the system into an insulating state. The mobility along different crystallographic directions is calculated including vertex corrections which give rise to ","authors_text":"C. A. Perroni, F. Gargiulo, V. Cataudella, V. Marigliano Ramaglia","cross_cats":["cond-mat.mtrl-sci"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2011-08-26T09:13:44Z","title":"Electronic transport within a quasi two-dimensional model for rubrene single-crystal field effect transistors"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1108.5263","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:baaad3c7680c60fd0f8f5495b82b928f461d35f4fd9d501bdc1cdbd2f333393c","target":"record","created_at":"2026-05-18T04:05:38Z","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":"4e770075489eed1fdb5e34d5063d7cf91b21ddf246c4d321dd8ef967fbd1f4ad","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2011-08-26T09:13:44Z","title_canon_sha256":"029888af5e8aa2a42dca55f5d46bda9f50faa3982a2fcf72261a916596e9f0a0"},"schema_version":"1.0","source":{"id":"1108.5263","kind":"arxiv","version":1}},"canonical_sha256":"a0d992f5db637ad67015fa7b0275d73c30bfde63b185a7f42fd2d3e2da122eec","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a0d992f5db637ad67015fa7b0275d73c30bfde63b185a7f42fd2d3e2da122eec","first_computed_at":"2026-05-18T04:05:38.382426Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:05:38.382426Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Hn0iUQ/Ldusa0UxHcwAy9xm7jLrfVg3AdenDS8DFRUomtvBT0CXcQvF5ndarKhUpTQ8hRhpR61unRqNUnXg+BA==","signature_status":"signed_v1","signed_at":"2026-05-18T04:05:38.382784Z","signed_message":"canonical_sha256_bytes"},"source_id":"1108.5263","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:baaad3c7680c60fd0f8f5495b82b928f461d35f4fd9d501bdc1cdbd2f333393c","sha256:7049d778347ba0c4efaa14b9865d32516be2b47b736b357b995a1aecf14ac692"],"state_sha256":"23e30f55e7ca659b1802d7796918e8caf83f2dd61ce28ce7a8aa4ad3f5740a41"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ADDVPod1o8KbYxCR7JQQwEKo9DDIIOR1Du+Ga25izFTlQyh7D/CIqfldL4JtAbFd3edZR/Vl0pWzs0NnjfNTCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T03:20:17.355698Z","bundle_sha256":"e227d564e302a135f2f0eac80cacf7b435db2a687d069652854ec27632bc1ed9"}}