{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:SAJUBEA5CCE677B6LVRCCMCA5V","short_pith_number":"pith:SAJUBEA5","canonical_record":{"source":{"id":"1207.7170","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-07-31T05:44:46Z","cross_cats_sorted":[],"title_canon_sha256":"4178feacacc1386b5098b86378e83104b393719bfa805232b46d198538c00a9c","abstract_canon_sha256":"c2944d5f0455a76f5af865d942799e734349a868809cb782d8d89d8c2f714c98"},"schema_version":"1.0"},"canonical_sha256":"901340901d1089effc3e5d62213040ed639408f1f9f6679db3677f25e779cf53","source":{"kind":"arxiv","id":"1207.7170","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1207.7170","created_at":"2026-05-18T03:49:46Z"},{"alias_kind":"arxiv_version","alias_value":"1207.7170v1","created_at":"2026-05-18T03:49:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1207.7170","created_at":"2026-05-18T03:49:46Z"},{"alias_kind":"pith_short_12","alias_value":"SAJUBEA5CCE6","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_16","alias_value":"SAJUBEA5CCE677B6","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_8","alias_value":"SAJUBEA5","created_at":"2026-05-18T12:27:20Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:SAJUBEA5CCE677B6LVRCCMCA5V","target":"record","payload":{"canonical_record":{"source":{"id":"1207.7170","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-07-31T05:44:46Z","cross_cats_sorted":[],"title_canon_sha256":"4178feacacc1386b5098b86378e83104b393719bfa805232b46d198538c00a9c","abstract_canon_sha256":"c2944d5f0455a76f5af865d942799e734349a868809cb782d8d89d8c2f714c98"},"schema_version":"1.0"},"canonical_sha256":"901340901d1089effc3e5d62213040ed639408f1f9f6679db3677f25e779cf53","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:49:46.579269Z","signature_b64":"Ynm6/UmhMhXdK/uzhB2WU7tWIpEJQ6evHKqQOBkGgEi7j2rTRU+NInaHaIBwKBogvHS+k4CFyLsNyqaEf2kZBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"901340901d1089effc3e5d62213040ed639408f1f9f6679db3677f25e779cf53","last_reissued_at":"2026-05-18T03:49:46.578753Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:49:46.578753Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1207.7170","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":"2026-05-18T03:49:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sGKX4KEQKe+ZsvMspKvY8+1xttcDsczy0bKEGApwv4VVVbHNTmdZFoCk6uBuNvErbfKMN0/RSgTuTahuq/DHBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T22:07:34.451527Z"},"content_sha256":"20ab0452e4b24c3b48eb309003190e51eb8fd3cd189987d4cce6a7696a97b73b","schema_version":"1.0","event_id":"sha256:20ab0452e4b24c3b48eb309003190e51eb8fd3cd189987d4cce6a7696a97b73b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:SAJUBEA5CCE677B6LVRCCMCA5V","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Formulation of an Electrostatic Field with a Charge Density in the Presence of a Minimal Length Based on the Kempf Algebra","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"H. Moayeri, M. R. Setare, S. K. Moayedi","submitted_at":"2012-07-31T05:44:46Z","abstract_excerpt":"In a series of papers, Kempf and co-workers (J. Phys. A: Math. Gen. {\\bf 30}, 2093, (1997); Phys. Rev. D {\\bf52}, 1108, (1995); Phys. Rev. D {\\bf55}, 7909, (1997)) introduced a D-dimensional $(\\beta,\\beta')$-two-parameter deformed Heisenberg algebra which leads to a nonzero minimal observable length. In this work, the Lagrangian formulation of an electrostatic field in three spatial dimensions described by Kempf algebra is studied in the case where $\\beta'=2\\beta$ up to first order over deformation parameter $\\beta$. It is shown that there is a similarity between electrostatics in the presence"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1207.7170","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":"2026-05-18T03:49:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ezl28Ld4FTr5kG0QZuOqAH+Ts8sQb1/z6aJd+1WxjqesNebwrkPqhizJddc96jBMDG/bXIXi3UYlO0DSR1WZAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T22:07:34.451922Z"},"content_sha256":"943be8d09ebcae50efd411ceb06faf8fc3fc6741b53a3969c2b30b7908c4b6fb","schema_version":"1.0","event_id":"sha256:943be8d09ebcae50efd411ceb06faf8fc3fc6741b53a3969c2b30b7908c4b6fb"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/SAJUBEA5CCE677B6LVRCCMCA5V/bundle.json","state_url":"https://pith.science/pith/SAJUBEA5CCE677B6LVRCCMCA5V/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/SAJUBEA5CCE677B6LVRCCMCA5V/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":"2026-06-05T22:07:34Z","links":{"resolver":"https://pith.science/pith/SAJUBEA5CCE677B6LVRCCMCA5V","bundle":"https://pith.science/pith/SAJUBEA5CCE677B6LVRCCMCA5V/bundle.json","state":"https://pith.science/pith/SAJUBEA5CCE677B6LVRCCMCA5V/state.json","well_known_bundle":"https://pith.science/.well-known/pith/SAJUBEA5CCE677B6LVRCCMCA5V/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:SAJUBEA5CCE677B6LVRCCMCA5V","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":"c2944d5f0455a76f5af865d942799e734349a868809cb782d8d89d8c2f714c98","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-07-31T05:44:46Z","title_canon_sha256":"4178feacacc1386b5098b86378e83104b393719bfa805232b46d198538c00a9c"},"schema_version":"1.0","source":{"id":"1207.7170","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1207.7170","created_at":"2026-05-18T03:49:46Z"},{"alias_kind":"arxiv_version","alias_value":"1207.7170v1","created_at":"2026-05-18T03:49:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1207.7170","created_at":"2026-05-18T03:49:46Z"},{"alias_kind":"pith_short_12","alias_value":"SAJUBEA5CCE6","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_16","alias_value":"SAJUBEA5CCE677B6","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_8","alias_value":"SAJUBEA5","created_at":"2026-05-18T12:27:20Z"}],"graph_snapshots":[{"event_id":"sha256:943be8d09ebcae50efd411ceb06faf8fc3fc6741b53a3969c2b30b7908c4b6fb","target":"graph","created_at":"2026-05-18T03:49:46Z","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":"In a series of papers, Kempf and co-workers (J. Phys. A: Math. Gen. {\\bf 30}, 2093, (1997); Phys. Rev. D {\\bf52}, 1108, (1995); Phys. Rev. D {\\bf55}, 7909, (1997)) introduced a D-dimensional $(\\beta,\\beta')$-two-parameter deformed Heisenberg algebra which leads to a nonzero minimal observable length. In this work, the Lagrangian formulation of an electrostatic field in three spatial dimensions described by Kempf algebra is studied in the case where $\\beta'=2\\beta$ up to first order over deformation parameter $\\beta$. It is shown that there is a similarity between electrostatics in the presence","authors_text":"H. Moayeri, M. R. Setare, S. K. Moayedi","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-07-31T05:44:46Z","title":"Formulation of an Electrostatic Field with a Charge Density in the Presence of a Minimal Length Based on the Kempf Algebra"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1207.7170","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":"sha256:20ab0452e4b24c3b48eb309003190e51eb8fd3cd189987d4cce6a7696a97b73b","target":"record","created_at":"2026-05-18T03:49:46Z","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":"c2944d5f0455a76f5af865d942799e734349a868809cb782d8d89d8c2f714c98","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-07-31T05:44:46Z","title_canon_sha256":"4178feacacc1386b5098b86378e83104b393719bfa805232b46d198538c00a9c"},"schema_version":"1.0","source":{"id":"1207.7170","kind":"arxiv","version":1}},"canonical_sha256":"901340901d1089effc3e5d62213040ed639408f1f9f6679db3677f25e779cf53","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"901340901d1089effc3e5d62213040ed639408f1f9f6679db3677f25e779cf53","first_computed_at":"2026-05-18T03:49:46.578753Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:49:46.578753Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Ynm6/UmhMhXdK/uzhB2WU7tWIpEJQ6evHKqQOBkGgEi7j2rTRU+NInaHaIBwKBogvHS+k4CFyLsNyqaEf2kZBw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:49:46.579269Z","signed_message":"canonical_sha256_bytes"},"source_id":"1207.7170","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:20ab0452e4b24c3b48eb309003190e51eb8fd3cd189987d4cce6a7696a97b73b","sha256:943be8d09ebcae50efd411ceb06faf8fc3fc6741b53a3969c2b30b7908c4b6fb"],"state_sha256":"573b97cf0d96e8c8d9aad0eb884575a003922af6a9fc5d909d5d8f5304ff2cac"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1E1Ds2WFitKR6Yx644m+chxawW8hRRKyYk2iN+7bpqPlW9Uvc4lKWx7QOHzCKsCQWJvdVM1I4wEIH1+l4Fq4Dg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-05T22:07:34.455029Z","bundle_sha256":"659717de087beacc88abcab19e0aa4ea39f800b491ac4d9c51cdb78fd836bebf"}}