{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:WSHPZ7BUZDFL6DMQB5M4PGLGO2","short_pith_number":"pith:WSHPZ7BU","canonical_record":{"source":{"id":"1412.4654","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-15T16:09:48Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"d7b3e3a568cada46368920cfd52732c377bb410a8175fdd7b93b052591562584","abstract_canon_sha256":"b0db5e00bca5af8169fc761ca379d4f784b495e0faf307d7d08b2900fea1c884"},"schema_version":"1.0"},"canonical_sha256":"b48efcfc34c8cabf0d900f59c7996676bb61ba82aae08908c0c84b345940a1c9","source":{"kind":"arxiv","id":"1412.4654","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.4654","created_at":"2026-05-18T01:31:21Z"},{"alias_kind":"arxiv_version","alias_value":"1412.4654v1","created_at":"2026-05-18T01:31:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.4654","created_at":"2026-05-18T01:31:21Z"},{"alias_kind":"pith_short_12","alias_value":"WSHPZ7BUZDFL","created_at":"2026-05-18T12:28:54Z"},{"alias_kind":"pith_short_16","alias_value":"WSHPZ7BUZDFL6DMQ","created_at":"2026-05-18T12:28:54Z"},{"alias_kind":"pith_short_8","alias_value":"WSHPZ7BU","created_at":"2026-05-18T12:28:54Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:WSHPZ7BUZDFL6DMQB5M4PGLGO2","target":"record","payload":{"canonical_record":{"source":{"id":"1412.4654","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-15T16:09:48Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"d7b3e3a568cada46368920cfd52732c377bb410a8175fdd7b93b052591562584","abstract_canon_sha256":"b0db5e00bca5af8169fc761ca379d4f784b495e0faf307d7d08b2900fea1c884"},"schema_version":"1.0"},"canonical_sha256":"b48efcfc34c8cabf0d900f59c7996676bb61ba82aae08908c0c84b345940a1c9","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:31:21.363563Z","signature_b64":"xjTgcVhAIQAbwFI1H/R0T/KjrM9cmayBhgaYG3aMxni1eEhpN2rf7xI8Hi5xqEvk6aZFU7B9/OkNCkQ41NadAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b48efcfc34c8cabf0d900f59c7996676bb61ba82aae08908c0c84b345940a1c9","last_reissued_at":"2026-05-18T01:31:21.363100Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:31:21.363100Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1412.4654","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":"2026-05-18T01:31:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ebAcSqaxJfL2yFo22CbKyQSSMzGi70Hsq5Pela4zpQB60ZnV1gUnlHo+t+DoDzVwgPqhvN0ttE72GEMqt+sfCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T15:09:16.260499Z"},"content_sha256":"f02d570200490437a5ed11b582f4a98940037b102aab1219e31d75c2622d00b2","schema_version":"1.0","event_id":"sha256:f02d570200490437a5ed11b582f4a98940037b102aab1219e31d75c2622d00b2"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:WSHPZ7BUZDFL6DMQB5M4PGLGO2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Electrically charged finite energy solutions of an $SO(5)$ and an $SU(3)$ Higgs-Chern-Simons--Yang-Mills-Higgs systems in $3+1$ dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"D. H. Tchrakian, Francisco Navarro-Lerida","submitted_at":"2014-12-15T16:09:48Z","abstract_excerpt":"We study spherically symmetric finite energy solutions of two Higgs-Chern-Simons--Yang-Mills-Higgs (HCS-YMH) models in $3+1$ dimensions, one with gauge group $SO(5)$ and the other with $SU(3)$. The Chern-Simons (CS) densities are defined in terms of both the Yang-Mills (YM) and Higgs fields and the choice of the two gauge groups is made so they do not vanish. The solutions of the $SO(5)$ model carry only electric charge and zero magnetic charge, while the solutions of the $SU(3)$ model are dyons carrying both electric and magnetic charges like the Julia-Zee (JZ) dyon. Unlike the latter however"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.4654","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":"2026-05-18T01:31:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XcrERe8C2vU93bX52vBRF6qKU4Nngf5ysD5kfgFnxfke3v008CF8wplgrDwvNNLRxEjYTX5cO6Iv64VP3dlwCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T15:09:16.261128Z"},"content_sha256":"846380d76bc797132c36cc0e259e027d800db4ad380607ff0467aac8b493aac3","schema_version":"1.0","event_id":"sha256:846380d76bc797132c36cc0e259e027d800db4ad380607ff0467aac8b493aac3"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/WSHPZ7BUZDFL6DMQB5M4PGLGO2/bundle.json","state_url":"https://pith.science/pith/WSHPZ7BUZDFL6DMQB5M4PGLGO2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/WSHPZ7BUZDFL6DMQB5M4PGLGO2/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":"2026-05-25T15:09:16Z","links":{"resolver":"https://pith.science/pith/WSHPZ7BUZDFL6DMQB5M4PGLGO2","bundle":"https://pith.science/pith/WSHPZ7BUZDFL6DMQB5M4PGLGO2/bundle.json","state":"https://pith.science/pith/WSHPZ7BUZDFL6DMQB5M4PGLGO2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/WSHPZ7BUZDFL6DMQB5M4PGLGO2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:WSHPZ7BUZDFL6DMQB5M4PGLGO2","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":"b0db5e00bca5af8169fc761ca379d4f784b495e0faf307d7d08b2900fea1c884","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-15T16:09:48Z","title_canon_sha256":"d7b3e3a568cada46368920cfd52732c377bb410a8175fdd7b93b052591562584"},"schema_version":"1.0","source":{"id":"1412.4654","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.4654","created_at":"2026-05-18T01:31:21Z"},{"alias_kind":"arxiv_version","alias_value":"1412.4654v1","created_at":"2026-05-18T01:31:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.4654","created_at":"2026-05-18T01:31:21Z"},{"alias_kind":"pith_short_12","alias_value":"WSHPZ7BUZDFL","created_at":"2026-05-18T12:28:54Z"},{"alias_kind":"pith_short_16","alias_value":"WSHPZ7BUZDFL6DMQ","created_at":"2026-05-18T12:28:54Z"},{"alias_kind":"pith_short_8","alias_value":"WSHPZ7BU","created_at":"2026-05-18T12:28:54Z"}],"graph_snapshots":[{"event_id":"sha256:846380d76bc797132c36cc0e259e027d800db4ad380607ff0467aac8b493aac3","target":"graph","created_at":"2026-05-18T01:31:21Z","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":"We study spherically symmetric finite energy solutions of two Higgs-Chern-Simons--Yang-Mills-Higgs (HCS-YMH) models in $3+1$ dimensions, one with gauge group $SO(5)$ and the other with $SU(3)$. The Chern-Simons (CS) densities are defined in terms of both the Yang-Mills (YM) and Higgs fields and the choice of the two gauge groups is made so they do not vanish. The solutions of the $SO(5)$ model carry only electric charge and zero magnetic charge, while the solutions of the $SU(3)$ model are dyons carrying both electric and magnetic charges like the Julia-Zee (JZ) dyon. Unlike the latter however","authors_text":"D. H. Tchrakian, Francisco Navarro-Lerida","cross_cats":["gr-qc"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-15T16:09:48Z","title":"Electrically charged finite energy solutions of an $SO(5)$ and an $SU(3)$ Higgs-Chern-Simons--Yang-Mills-Higgs systems in $3+1$ dimensions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.4654","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:f02d570200490437a5ed11b582f4a98940037b102aab1219e31d75c2622d00b2","target":"record","created_at":"2026-05-18T01:31:21Z","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":"b0db5e00bca5af8169fc761ca379d4f784b495e0faf307d7d08b2900fea1c884","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-15T16:09:48Z","title_canon_sha256":"d7b3e3a568cada46368920cfd52732c377bb410a8175fdd7b93b052591562584"},"schema_version":"1.0","source":{"id":"1412.4654","kind":"arxiv","version":1}},"canonical_sha256":"b48efcfc34c8cabf0d900f59c7996676bb61ba82aae08908c0c84b345940a1c9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b48efcfc34c8cabf0d900f59c7996676bb61ba82aae08908c0c84b345940a1c9","first_computed_at":"2026-05-18T01:31:21.363100Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:31:21.363100Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"xjTgcVhAIQAbwFI1H/R0T/KjrM9cmayBhgaYG3aMxni1eEhpN2rf7xI8Hi5xqEvk6aZFU7B9/OkNCkQ41NadAg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:31:21.363563Z","signed_message":"canonical_sha256_bytes"},"source_id":"1412.4654","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f02d570200490437a5ed11b582f4a98940037b102aab1219e31d75c2622d00b2","sha256:846380d76bc797132c36cc0e259e027d800db4ad380607ff0467aac8b493aac3"],"state_sha256":"68f95a91e828c42e759efbeadcd21c48c1c803a558fe00e63a5377a0ecf17ba4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"k7cLm+sIivsIHmtvEAkDj/kJZC8euYHzk4RY9Z3nA+6FuBasM+orNdKyacHT26cmCZdsdwlc41NFFM9VvWUdDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T15:09:16.264411Z","bundle_sha256":"9e0c1b44d913704d04728361ad16abf36624afe3c3283fbf91ad9a71eaa7e16a"}}