{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:VLASYBOYEN7PYM2I6NCUUOZKUF","short_pith_number":"pith:VLASYBOY","canonical_record":{"source":{"id":"1605.05632","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-05-18T15:53:03Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"416ef68de14f7b0c86d9663d3e9e25ce6dd194a690552a5bc11c0ee4b28fa956","abstract_canon_sha256":"5ab7dd7fc1eaedff900e51cd913581e6220b335c75cd6d60416b6fdc941a6158"},"schema_version":"1.0"},"canonical_sha256":"aac12c05d8237efc3348f3454a3b2aa15c9ae31b5aac4c15298881de98805801","source":{"kind":"arxiv","id":"1605.05632","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1605.05632","created_at":"2026-05-18T01:14:30Z"},{"alias_kind":"arxiv_version","alias_value":"1605.05632v1","created_at":"2026-05-18T01:14:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1605.05632","created_at":"2026-05-18T01:14:30Z"},{"alias_kind":"pith_short_12","alias_value":"VLASYBOYEN7P","created_at":"2026-05-18T12:30:48Z"},{"alias_kind":"pith_short_16","alias_value":"VLASYBOYEN7PYM2I","created_at":"2026-05-18T12:30:48Z"},{"alias_kind":"pith_short_8","alias_value":"VLASYBOY","created_at":"2026-05-18T12:30:48Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:VLASYBOYEN7PYM2I6NCUUOZKUF","target":"record","payload":{"canonical_record":{"source":{"id":"1605.05632","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-05-18T15:53:03Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"416ef68de14f7b0c86d9663d3e9e25ce6dd194a690552a5bc11c0ee4b28fa956","abstract_canon_sha256":"5ab7dd7fc1eaedff900e51cd913581e6220b335c75cd6d60416b6fdc941a6158"},"schema_version":"1.0"},"canonical_sha256":"aac12c05d8237efc3348f3454a3b2aa15c9ae31b5aac4c15298881de98805801","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:14:30.171982Z","signature_b64":"7XiZsvk5+PBJB5FEFeqo7zoIL1urhD7fNZxLqFcfXh8mu4AvXP2UV69O1YmcjbUVu4/x0CQxsN+AzLbqTlg2Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"aac12c05d8237efc3348f3454a3b2aa15c9ae31b5aac4c15298881de98805801","last_reissued_at":"2026-05-18T01:14:30.171482Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:14:30.171482Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1605.05632","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":"2026-05-18T01:14:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LZqlY/NWsjaRp8CHXkOyQ9O4KnnG8wbAqmTEV4mH/kbNCQX+yfoOq52R7PDSuZt4WxhOExZR3QPSL3qFE2RYCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-27T16:51:03.832419Z"},"content_sha256":"5a242e1abf623a831be2fe11a1b32e1da9c74b103c0237e77f1bb2b214aab929","schema_version":"1.0","event_id":"sha256:5a242e1abf623a831be2fe11a1b32e1da9c74b103c0237e77f1bb2b214aab929"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:VLASYBOYEN7PYM2I6NCUUOZKUF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"One-loop potential with scale invariance and effective operators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"D. M. Ghilencea","submitted_at":"2016-05-18T15:53:03Z","abstract_excerpt":"We study quantum corrections to the scalar potential in classically scale invariant theories, using a manifestly scale invariant regularization. To this purpose, the subtraction scale $\\mu$ of the dimensional regularization is generated after spontaneous scale symmetry breaking, from a subtraction function of the fields, $\\mu(\\phi,\\sigma)$. This function is then uniquely determined from general principles showing that it depends on the dilaton only, with $\\mu(\\sigma)\\sim \\sigma$. The result is a scale invariant one-loop potential $U$ for a higgs field $\\phi$ and dilaton $\\sigma$ that contains "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1605.05632","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":"2026-05-18T01:14:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zVOeIgEed1uMGmgDn/T296xPW5qBeZlXixH5byBo74pgAcyJOP9MUV6iSM4vr7ibzcZm3Joqmko3UGEnfmKtCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-27T16:51:03.832768Z"},"content_sha256":"ed2db7bb3e4ad5f5d6a90b7c53ad5efd6ad3e6ed8b727b4390c438b2658838f8","schema_version":"1.0","event_id":"sha256:ed2db7bb3e4ad5f5d6a90b7c53ad5efd6ad3e6ed8b727b4390c438b2658838f8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/VLASYBOYEN7PYM2I6NCUUOZKUF/bundle.json","state_url":"https://pith.science/pith/VLASYBOYEN7PYM2I6NCUUOZKUF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/VLASYBOYEN7PYM2I6NCUUOZKUF/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":"2026-06-27T16:51:03Z","links":{"resolver":"https://pith.science/pith/VLASYBOYEN7PYM2I6NCUUOZKUF","bundle":"https://pith.science/pith/VLASYBOYEN7PYM2I6NCUUOZKUF/bundle.json","state":"https://pith.science/pith/VLASYBOYEN7PYM2I6NCUUOZKUF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/VLASYBOYEN7PYM2I6NCUUOZKUF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:VLASYBOYEN7PYM2I6NCUUOZKUF","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":"5ab7dd7fc1eaedff900e51cd913581e6220b335c75cd6d60416b6fdc941a6158","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-05-18T15:53:03Z","title_canon_sha256":"416ef68de14f7b0c86d9663d3e9e25ce6dd194a690552a5bc11c0ee4b28fa956"},"schema_version":"1.0","source":{"id":"1605.05632","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1605.05632","created_at":"2026-05-18T01:14:30Z"},{"alias_kind":"arxiv_version","alias_value":"1605.05632v1","created_at":"2026-05-18T01:14:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1605.05632","created_at":"2026-05-18T01:14:30Z"},{"alias_kind":"pith_short_12","alias_value":"VLASYBOYEN7P","created_at":"2026-05-18T12:30:48Z"},{"alias_kind":"pith_short_16","alias_value":"VLASYBOYEN7PYM2I","created_at":"2026-05-18T12:30:48Z"},{"alias_kind":"pith_short_8","alias_value":"VLASYBOY","created_at":"2026-05-18T12:30:48Z"}],"graph_snapshots":[{"event_id":"sha256:ed2db7bb3e4ad5f5d6a90b7c53ad5efd6ad3e6ed8b727b4390c438b2658838f8","target":"graph","created_at":"2026-05-18T01:14:30Z","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 quantum corrections to the scalar potential in classically scale invariant theories, using a manifestly scale invariant regularization. To this purpose, the subtraction scale $\\mu$ of the dimensional regularization is generated after spontaneous scale symmetry breaking, from a subtraction function of the fields, $\\mu(\\phi,\\sigma)$. This function is then uniquely determined from general principles showing that it depends on the dilaton only, with $\\mu(\\sigma)\\sim \\sigma$. The result is a scale invariant one-loop potential $U$ for a higgs field $\\phi$ and dilaton $\\sigma$ that contains ","authors_text":"D. M. Ghilencea","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-05-18T15:53:03Z","title":"One-loop potential with scale invariance and effective operators"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1605.05632","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":"sha256:5a242e1abf623a831be2fe11a1b32e1da9c74b103c0237e77f1bb2b214aab929","target":"record","created_at":"2026-05-18T01:14:30Z","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":"5ab7dd7fc1eaedff900e51cd913581e6220b335c75cd6d60416b6fdc941a6158","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-05-18T15:53:03Z","title_canon_sha256":"416ef68de14f7b0c86d9663d3e9e25ce6dd194a690552a5bc11c0ee4b28fa956"},"schema_version":"1.0","source":{"id":"1605.05632","kind":"arxiv","version":1}},"canonical_sha256":"aac12c05d8237efc3348f3454a3b2aa15c9ae31b5aac4c15298881de98805801","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"aac12c05d8237efc3348f3454a3b2aa15c9ae31b5aac4c15298881de98805801","first_computed_at":"2026-05-18T01:14:30.171482Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:14:30.171482Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"7XiZsvk5+PBJB5FEFeqo7zoIL1urhD7fNZxLqFcfXh8mu4AvXP2UV69O1YmcjbUVu4/x0CQxsN+AzLbqTlg2Aw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:14:30.171982Z","signed_message":"canonical_sha256_bytes"},"source_id":"1605.05632","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5a242e1abf623a831be2fe11a1b32e1da9c74b103c0237e77f1bb2b214aab929","sha256:ed2db7bb3e4ad5f5d6a90b7c53ad5efd6ad3e6ed8b727b4390c438b2658838f8"],"state_sha256":"69803e1220627706be351151cf8298f84d8cfebbafa1593b0b85eee8b39c7a36"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jNyoLWjM1Nt8JNF196KJNKLzBp9Wwzj/C5+sNcmJ5EkFasYJQvMpcFOjpBRtf87ObKMbibeTUt/QLBc7LTU0Dg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-27T16:51:03.835774Z","bundle_sha256":"cdf06edc33c271be546aa655bd74e6a3909c79f825e5187ec7618a862c5f21fe"}}