{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:AGPJTZWFDEOWE4X6EOMQBF4NWC","short_pith_number":"pith:AGPJTZWF","canonical_record":{"source":{"id":"1804.04453","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-04-12T12:05:40Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"a23e217e702c9405fc559cdbae1e0f6edf165c57ab86f5f559a338c08fc04399","abstract_canon_sha256":"b4f25f082900c2616c2e670e2f0d9542569a37d50a692a38704bb75401008226"},"schema_version":"1.0"},"canonical_sha256":"019e99e6c5191d6272fe239900978db0a844a550d3b7d824fcf96fff2c2f05f5","source":{"kind":"arxiv","id":"1804.04453","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1804.04453","created_at":"2026-05-18T00:06:16Z"},{"alias_kind":"arxiv_version","alias_value":"1804.04453v2","created_at":"2026-05-18T00:06:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1804.04453","created_at":"2026-05-18T00:06:16Z"},{"alias_kind":"pith_short_12","alias_value":"AGPJTZWFDEOW","created_at":"2026-05-18T12:32:13Z"},{"alias_kind":"pith_short_16","alias_value":"AGPJTZWFDEOWE4X6","created_at":"2026-05-18T12:32:13Z"},{"alias_kind":"pith_short_8","alias_value":"AGPJTZWF","created_at":"2026-05-18T12:32:13Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:AGPJTZWFDEOWE4X6EOMQBF4NWC","target":"record","payload":{"canonical_record":{"source":{"id":"1804.04453","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-04-12T12:05:40Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"a23e217e702c9405fc559cdbae1e0f6edf165c57ab86f5f559a338c08fc04399","abstract_canon_sha256":"b4f25f082900c2616c2e670e2f0d9542569a37d50a692a38704bb75401008226"},"schema_version":"1.0"},"canonical_sha256":"019e99e6c5191d6272fe239900978db0a844a550d3b7d824fcf96fff2c2f05f5","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:06:16.079193Z","signature_b64":"tHlXaAiCA3E0hx+2EA9GkZlcF3XbJ17eVL8hBlmJ8dkO/a0Swf5JZ1kCR0GY/e19pl//LD7D+ANc9Gqb/5GZAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"019e99e6c5191d6272fe239900978db0a844a550d3b7d824fcf96fff2c2f05f5","last_reissued_at":"2026-05-18T00:06:16.078537Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:06:16.078537Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1804.04453","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:06:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pIbXY0xeqQwXTmg+mCXQlvSpdnUAT+yNn55ytycE7KMMMDDRO6rPv0g30WoTvFz3WV4wcwZwA6k1yJAUslQjCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T09:41:47.350067Z"},"content_sha256":"d89e523bd6cc8049ef8b3c21eea3ecef1d6a7bb4354a1172af52215fbe80e241","schema_version":"1.0","event_id":"sha256:d89e523bd6cc8049ef8b3c21eea3ecef1d6a7bb4354a1172af52215fbe80e241"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:AGPJTZWFDEOWE4X6EOMQBF4NWC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The spectrum of an SU(3) gauge theory with a fundamental Higgs field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Axel Maas, Pascal T\\\"orek","submitted_at":"2018-04-12T12:05:40Z","abstract_excerpt":"In gauge theories, the physical, experimentally observable spectrum consists only of gauge-invariant states. This spectrum can be different from the elementary spectrum even at weak coupling and in the presence of the Brout-Englert-Higgs effect. We demonstrate this for an SU(3) gauge theory with a single fundamental Higgs, a toy theory for grand-unified theories. The manifestly gauge-invariant approach of lattice gauge theory is used to determine the spectrum in four different channels. It is found to be qualitatively different from the elementary one, and especially from the one predicted by "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1804.04453","kind":"arxiv","version":2},"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":"2026-05-18T00:06:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tfRkH0fqrAGrgol7I6Vxc0SbqWapz1xYcbHEXCZqVjPkv/M5hMNmG2Etya5IZrgxpMvR08dUPzGdwOjoSh30DA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T09:41:47.350676Z"},"content_sha256":"ab0070893926358cb5e1224bf0f560d8dc74168f509c61c8a814e944ca88df38","schema_version":"1.0","event_id":"sha256:ab0070893926358cb5e1224bf0f560d8dc74168f509c61c8a814e944ca88df38"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/AGPJTZWFDEOWE4X6EOMQBF4NWC/bundle.json","state_url":"https://pith.science/pith/AGPJTZWFDEOWE4X6EOMQBF4NWC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/AGPJTZWFDEOWE4X6EOMQBF4NWC/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":"2026-06-08T09:41:47Z","links":{"resolver":"https://pith.science/pith/AGPJTZWFDEOWE4X6EOMQBF4NWC","bundle":"https://pith.science/pith/AGPJTZWFDEOWE4X6EOMQBF4NWC/bundle.json","state":"https://pith.science/pith/AGPJTZWFDEOWE4X6EOMQBF4NWC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/AGPJTZWFDEOWE4X6EOMQBF4NWC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:AGPJTZWFDEOWE4X6EOMQBF4NWC","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":"b4f25f082900c2616c2e670e2f0d9542569a37d50a692a38704bb75401008226","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-04-12T12:05:40Z","title_canon_sha256":"a23e217e702c9405fc559cdbae1e0f6edf165c57ab86f5f559a338c08fc04399"},"schema_version":"1.0","source":{"id":"1804.04453","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1804.04453","created_at":"2026-05-18T00:06:16Z"},{"alias_kind":"arxiv_version","alias_value":"1804.04453v2","created_at":"2026-05-18T00:06:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1804.04453","created_at":"2026-05-18T00:06:16Z"},{"alias_kind":"pith_short_12","alias_value":"AGPJTZWFDEOW","created_at":"2026-05-18T12:32:13Z"},{"alias_kind":"pith_short_16","alias_value":"AGPJTZWFDEOWE4X6","created_at":"2026-05-18T12:32:13Z"},{"alias_kind":"pith_short_8","alias_value":"AGPJTZWF","created_at":"2026-05-18T12:32:13Z"}],"graph_snapshots":[{"event_id":"sha256:ab0070893926358cb5e1224bf0f560d8dc74168f509c61c8a814e944ca88df38","target":"graph","created_at":"2026-05-18T00:06:16Z","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 gauge theories, the physical, experimentally observable spectrum consists only of gauge-invariant states. This spectrum can be different from the elementary spectrum even at weak coupling and in the presence of the Brout-Englert-Higgs effect. We demonstrate this for an SU(3) gauge theory with a single fundamental Higgs, a toy theory for grand-unified theories. The manifestly gauge-invariant approach of lattice gauge theory is used to determine the spectrum in four different channels. It is found to be qualitatively different from the elementary one, and especially from the one predicted by ","authors_text":"Axel Maas, Pascal T\\\"orek","cross_cats":["hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-04-12T12:05:40Z","title":"The spectrum of an SU(3) gauge theory with a fundamental Higgs field"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1804.04453","kind":"arxiv","version":2},"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:d89e523bd6cc8049ef8b3c21eea3ecef1d6a7bb4354a1172af52215fbe80e241","target":"record","created_at":"2026-05-18T00:06:16Z","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":"b4f25f082900c2616c2e670e2f0d9542569a37d50a692a38704bb75401008226","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-04-12T12:05:40Z","title_canon_sha256":"a23e217e702c9405fc559cdbae1e0f6edf165c57ab86f5f559a338c08fc04399"},"schema_version":"1.0","source":{"id":"1804.04453","kind":"arxiv","version":2}},"canonical_sha256":"019e99e6c5191d6272fe239900978db0a844a550d3b7d824fcf96fff2c2f05f5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"019e99e6c5191d6272fe239900978db0a844a550d3b7d824fcf96fff2c2f05f5","first_computed_at":"2026-05-18T00:06:16.078537Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:06:16.078537Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"tHlXaAiCA3E0hx+2EA9GkZlcF3XbJ17eVL8hBlmJ8dkO/a0Swf5JZ1kCR0GY/e19pl//LD7D+ANc9Gqb/5GZAA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:06:16.079193Z","signed_message":"canonical_sha256_bytes"},"source_id":"1804.04453","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d89e523bd6cc8049ef8b3c21eea3ecef1d6a7bb4354a1172af52215fbe80e241","sha256:ab0070893926358cb5e1224bf0f560d8dc74168f509c61c8a814e944ca88df38"],"state_sha256":"0764bbae987cb1300440c6fb71b2be23b350e9484ea62bd2fdc841534f05bbf4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bDTda+ap81hvao7qmnoONbddYJLcjyEkPtQUPouisVRSiXwwE4rzCd4EZKmG7II37Ysh/X+CUCG8G0yI3Pb8Bw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-08T09:41:47.353994Z","bundle_sha256":"cbb9abb557a91ebf49242ffe56f60b94947e1784e9a47659d8a0ad404427ced8"}}