{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:7EQE3XAY6L6Q2P3ISPBMRACHIC","short_pith_number":"pith:7EQE3XAY","canonical_record":{"source":{"id":"2411.13448","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2024-11-20T16:42:21Z","cross_cats_sorted":[],"title_canon_sha256":"979e2850329db752e25cab52629877e48d93475288777d1e34945a3a16e54c6b","abstract_canon_sha256":"6eb943ea1637fa71e807721aa6701da8c6f52fb5e4375fdb470f8e0428a4e427"},"schema_version":"1.0"},"canonical_sha256":"f9204ddc18f2fd0d3f6893c2c8804740a7c1c2c457b129bc324de7557dcfade8","source":{"kind":"arxiv","id":"2411.13448","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2411.13448","created_at":"2026-07-05T10:30:26Z"},{"alias_kind":"arxiv_version","alias_value":"2411.13448v1","created_at":"2026-07-05T10:30:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.13448","created_at":"2026-07-05T10:30:26Z"},{"alias_kind":"pith_short_12","alias_value":"7EQE3XAY6L6Q","created_at":"2026-07-05T10:30:26Z"},{"alias_kind":"pith_short_16","alias_value":"7EQE3XAY6L6Q2P3I","created_at":"2026-07-05T10:30:26Z"},{"alias_kind":"pith_short_8","alias_value":"7EQE3XAY","created_at":"2026-07-05T10:30:26Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:7EQE3XAY6L6Q2P3ISPBMRACHIC","target":"record","payload":{"canonical_record":{"source":{"id":"2411.13448","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2024-11-20T16:42:21Z","cross_cats_sorted":[],"title_canon_sha256":"979e2850329db752e25cab52629877e48d93475288777d1e34945a3a16e54c6b","abstract_canon_sha256":"6eb943ea1637fa71e807721aa6701da8c6f52fb5e4375fdb470f8e0428a4e427"},"schema_version":"1.0"},"canonical_sha256":"f9204ddc18f2fd0d3f6893c2c8804740a7c1c2c457b129bc324de7557dcfade8","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:30:26.980290Z","signature_b64":"pMn0KOzYWtqs2UyhcuA/SsgmdKDM8vbg6CCAPivNeaIJCh9rNRxNeEgu/2r8gYFK+emuxyRoZ3kBKtbClovgAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f9204ddc18f2fd0d3f6893c2c8804740a7c1c2c457b129bc324de7557dcfade8","last_reissued_at":"2026-07-05T10:30:26.979264Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:30:26.979264Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2411.13448","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":"2026-07-05T10:30:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sPEARnrXVivwpRGNz2OkwGqiN42WpPpcCLobUIpFCbg6mJdooX3Ri6Bb+l8tLpr9ib0DwaOSqoos733rPcpwCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-13T01:42:41.632395Z"},"content_sha256":"4b925d9c08dbb17e861228fbf443204276d8f6a37f0761b0018b162fdd518a44","schema_version":"1.0","event_id":"sha256:4b925d9c08dbb17e861228fbf443204276d8f6a37f0761b0018b162fdd518a44"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:7EQE3XAY6L6Q2P3ISPBMRACHIC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Taylor Modeling and Comparative Research Containing Aspect-Ratio Dependent Optimization of Three-Dimensional Hk Superjunction MOSFETs","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.app-ph","authors_text":"Chenxing Wang, Haimeng Huang, Zhentao Xiao, Zonghao Zhang","submitted_at":"2024-11-20T16:42:21Z","abstract_excerpt":"This paper presents a comprehensive study on aspect-ratio dependent optimization for specific on-resistance of three-dimensional high-k superjunction MOSFETs. The research introduces a Taylor modeling method, overcoming the computational limitations of the Bessel method. It also employs the Chynoweth model for more accurate breakdown voltage determination. The study provides a comparative analysis of four different superjunction structures, across five aspects: electric field, impact ionization integral, aspect ratio dependent optimization, charge imbalance effect and temperature. The findings"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.13448","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2411.13448/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":"2026-07-05T10:30:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ngUwb6WQE/DqTKfHWJx6AIb/XglhDHbUzSK25iMBt+T10Xtr1o9SYv5L8fBzRQFzBkght9zZyigoEC+1G1PKAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-13T01:42:41.632939Z"},"content_sha256":"ced07e7d696f1875ec80bdc2e538d0bcc2b361d329edab6de04e238fbfa14bfe","schema_version":"1.0","event_id":"sha256:ced07e7d696f1875ec80bdc2e538d0bcc2b361d329edab6de04e238fbfa14bfe"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/7EQE3XAY6L6Q2P3ISPBMRACHIC/bundle.json","state_url":"https://pith.science/pith/7EQE3XAY6L6Q2P3ISPBMRACHIC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/7EQE3XAY6L6Q2P3ISPBMRACHIC/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":"2026-08-13T01:42:41Z","links":{"resolver":"https://pith.science/pith/7EQE3XAY6L6Q2P3ISPBMRACHIC","bundle":"https://pith.science/pith/7EQE3XAY6L6Q2P3ISPBMRACHIC/bundle.json","state":"https://pith.science/pith/7EQE3XAY6L6Q2P3ISPBMRACHIC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/7EQE3XAY6L6Q2P3ISPBMRACHIC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:7EQE3XAY6L6Q2P3ISPBMRACHIC","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":"6eb943ea1637fa71e807721aa6701da8c6f52fb5e4375fdb470f8e0428a4e427","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2024-11-20T16:42:21Z","title_canon_sha256":"979e2850329db752e25cab52629877e48d93475288777d1e34945a3a16e54c6b"},"schema_version":"1.0","source":{"id":"2411.13448","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2411.13448","created_at":"2026-07-05T10:30:26Z"},{"alias_kind":"arxiv_version","alias_value":"2411.13448v1","created_at":"2026-07-05T10:30:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.13448","created_at":"2026-07-05T10:30:26Z"},{"alias_kind":"pith_short_12","alias_value":"7EQE3XAY6L6Q","created_at":"2026-07-05T10:30:26Z"},{"alias_kind":"pith_short_16","alias_value":"7EQE3XAY6L6Q2P3I","created_at":"2026-07-05T10:30:26Z"},{"alias_kind":"pith_short_8","alias_value":"7EQE3XAY","created_at":"2026-07-05T10:30:26Z"}],"graph_snapshots":[{"event_id":"sha256:ced07e7d696f1875ec80bdc2e538d0bcc2b361d329edab6de04e238fbfa14bfe","target":"graph","created_at":"2026-07-05T10:30:26Z","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/2411.13448/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"This paper presents a comprehensive study on aspect-ratio dependent optimization for specific on-resistance of three-dimensional high-k superjunction MOSFETs. The research introduces a Taylor modeling method, overcoming the computational limitations of the Bessel method. It also employs the Chynoweth model for more accurate breakdown voltage determination. The study provides a comparative analysis of four different superjunction structures, across five aspects: electric field, impact ionization integral, aspect ratio dependent optimization, charge imbalance effect and temperature. The findings","authors_text":"Chenxing Wang, Haimeng Huang, Zhentao Xiao, Zonghao Zhang","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2024-11-20T16:42:21Z","title":"Taylor Modeling and Comparative Research Containing Aspect-Ratio Dependent Optimization of Three-Dimensional Hk Superjunction MOSFETs"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.13448","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":"sha256:4b925d9c08dbb17e861228fbf443204276d8f6a37f0761b0018b162fdd518a44","target":"record","created_at":"2026-07-05T10:30:26Z","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":"6eb943ea1637fa71e807721aa6701da8c6f52fb5e4375fdb470f8e0428a4e427","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2024-11-20T16:42:21Z","title_canon_sha256":"979e2850329db752e25cab52629877e48d93475288777d1e34945a3a16e54c6b"},"schema_version":"1.0","source":{"id":"2411.13448","kind":"arxiv","version":1}},"canonical_sha256":"f9204ddc18f2fd0d3f6893c2c8804740a7c1c2c457b129bc324de7557dcfade8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f9204ddc18f2fd0d3f6893c2c8804740a7c1c2c457b129bc324de7557dcfade8","first_computed_at":"2026-07-05T10:30:26.979264Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:30:26.979264Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"pMn0KOzYWtqs2UyhcuA/SsgmdKDM8vbg6CCAPivNeaIJCh9rNRxNeEgu/2r8gYFK+emuxyRoZ3kBKtbClovgAA==","signature_status":"signed_v1","signed_at":"2026-07-05T10:30:26.980290Z","signed_message":"canonical_sha256_bytes"},"source_id":"2411.13448","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4b925d9c08dbb17e861228fbf443204276d8f6a37f0761b0018b162fdd518a44","sha256:ced07e7d696f1875ec80bdc2e538d0bcc2b361d329edab6de04e238fbfa14bfe"],"state_sha256":"e46489a0ba248d5e673839c90c2bd4877cdb4287ac25db655e41afb9660b74bd"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/U+waxtydJcoyFQlJ7qRKlSgyIjHgEY+rj2HNY3fM0tANFU6QIYv6HtR+gnzpuP3UAWj3jkWTvzYrAtjQWNtCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-13T01:42:41.637029Z","bundle_sha256":"82826a6658ff56e851b2c418e6bbda08b2777f7366fee1ca9f8c5f4c870fd21e"}}