{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2022:P3JTP5M5GQNI3YVM7WOUQVQFVI","short_pith_number":"pith:P3JTP5M5","canonical_record":{"source":{"id":"2202.11102","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-02-22T19:00:00Z","cross_cats_sorted":[],"title_canon_sha256":"94f3fa722980db2a42b1ffdc844bf8e96fe1b9dee589c1dbeb822c93909894ba","abstract_canon_sha256":"cd29294af84c4b963abb4d65b9a5538f38453c665b316b8ddd6811181580c3dd"},"schema_version":"1.0"},"canonical_sha256":"7ed337f59d341a8de2acfd9d485605aa13a3e69599fa08e3536133a67230afe1","source":{"kind":"arxiv","id":"2202.11102","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2202.11102","created_at":"2026-07-05T04:54:52Z"},{"alias_kind":"arxiv_version","alias_value":"2202.11102v3","created_at":"2026-07-05T04:54:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2202.11102","created_at":"2026-07-05T04:54:52Z"},{"alias_kind":"pith_short_12","alias_value":"P3JTP5M5GQNI","created_at":"2026-07-05T04:54:52Z"},{"alias_kind":"pith_short_16","alias_value":"P3JTP5M5GQNI3YVM","created_at":"2026-07-05T04:54:52Z"},{"alias_kind":"pith_short_8","alias_value":"P3JTP5M5","created_at":"2026-07-05T04:54:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2022:P3JTP5M5GQNI3YVM7WOUQVQFVI","target":"record","payload":{"canonical_record":{"source":{"id":"2202.11102","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-02-22T19:00:00Z","cross_cats_sorted":[],"title_canon_sha256":"94f3fa722980db2a42b1ffdc844bf8e96fe1b9dee589c1dbeb822c93909894ba","abstract_canon_sha256":"cd29294af84c4b963abb4d65b9a5538f38453c665b316b8ddd6811181580c3dd"},"schema_version":"1.0"},"canonical_sha256":"7ed337f59d341a8de2acfd9d485605aa13a3e69599fa08e3536133a67230afe1","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:54:52.925882Z","signature_b64":"h32i5b8xl3H2cSUY06MHui71iKPr7Uo0h8kci3heHQ+hJGDPR5QlF/J9CCy/cHBj1gePwtI11+uMFxR2M2V/AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7ed337f59d341a8de2acfd9d485605aa13a3e69599fa08e3536133a67230afe1","last_reissued_at":"2026-07-05T04:54:52.925461Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:54:52.925461Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2202.11102","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T04:54:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2E9UL/hiYM/kMpWFd8KFUKQdhHqrpwph5aYehZiAUs4dDRGlcQ9SFH7q/1cUu6uRA9grWqPqREJDqbVUIfu5Bg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T13:29:18.257439Z"},"content_sha256":"2ac518fcd38e6a6f3ba11527ebffbb9004da5409f306e732e7a36d3dfbedadf8","schema_version":"1.0","event_id":"sha256:2ac518fcd38e6a6f3ba11527ebffbb9004da5409f306e732e7a36d3dfbedadf8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2022:P3JTP5M5GQNI3YVM7WOUQVQFVI","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The Boring Monopole","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Michael Nee, Prateek Agrawal","submitted_at":"2022-02-22T19:00:00Z","abstract_excerpt":"We study false vacuum decays catalysed by magnetic monopoles which act as tunnelling sites with exponentially enhanced decay rates. The field profiles describing the decay do not have the typically assumed $O(3)/O(4)$ symmetry, thus requiring an extension of the usual decay rate calculation. To numerically determine the saddle point solutions which describe the tunnelling process we use a new algorithm based on the mountain pass theorem. This method can be applied more widely to phase transitions with reduced symmetry, such as decays away from the zero and infinite temperature limits. Our resu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2202.11102","kind":"arxiv","version":3},"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/2202.11102/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":"2026-07-05T04:54:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"l+wzSenJn4EDIp/M71xLuz75ZDTdHCaxNnyAz7LmELRst21O0mn5xZXWlTfX1sw3KaxVBq/WziIfxxT2IemeBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T13:29:18.258003Z"},"content_sha256":"d2331706e098eccf9fc441a988ac25d032c77bbf26c60078ac5bf7455b60adbc","schema_version":"1.0","event_id":"sha256:d2331706e098eccf9fc441a988ac25d032c77bbf26c60078ac5bf7455b60adbc"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/P3JTP5M5GQNI3YVM7WOUQVQFVI/bundle.json","state_url":"https://pith.science/pith/P3JTP5M5GQNI3YVM7WOUQVQFVI/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/P3JTP5M5GQNI3YVM7WOUQVQFVI/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":"2026-08-12T13:29:18Z","links":{"resolver":"https://pith.science/pith/P3JTP5M5GQNI3YVM7WOUQVQFVI","bundle":"https://pith.science/pith/P3JTP5M5GQNI3YVM7WOUQVQFVI/bundle.json","state":"https://pith.science/pith/P3JTP5M5GQNI3YVM7WOUQVQFVI/state.json","well_known_bundle":"https://pith.science/.well-known/pith/P3JTP5M5GQNI3YVM7WOUQVQFVI/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:P3JTP5M5GQNI3YVM7WOUQVQFVI","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":"cd29294af84c4b963abb4d65b9a5538f38453c665b316b8ddd6811181580c3dd","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-02-22T19:00:00Z","title_canon_sha256":"94f3fa722980db2a42b1ffdc844bf8e96fe1b9dee589c1dbeb822c93909894ba"},"schema_version":"1.0","source":{"id":"2202.11102","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2202.11102","created_at":"2026-07-05T04:54:52Z"},{"alias_kind":"arxiv_version","alias_value":"2202.11102v3","created_at":"2026-07-05T04:54:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2202.11102","created_at":"2026-07-05T04:54:52Z"},{"alias_kind":"pith_short_12","alias_value":"P3JTP5M5GQNI","created_at":"2026-07-05T04:54:52Z"},{"alias_kind":"pith_short_16","alias_value":"P3JTP5M5GQNI3YVM","created_at":"2026-07-05T04:54:52Z"},{"alias_kind":"pith_short_8","alias_value":"P3JTP5M5","created_at":"2026-07-05T04:54:52Z"}],"graph_snapshots":[{"event_id":"sha256:d2331706e098eccf9fc441a988ac25d032c77bbf26c60078ac5bf7455b60adbc","target":"graph","created_at":"2026-07-05T04:54:52Z","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/2202.11102/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We study false vacuum decays catalysed by magnetic monopoles which act as tunnelling sites with exponentially enhanced decay rates. The field profiles describing the decay do not have the typically assumed $O(3)/O(4)$ symmetry, thus requiring an extension of the usual decay rate calculation. To numerically determine the saddle point solutions which describe the tunnelling process we use a new algorithm based on the mountain pass theorem. This method can be applied more widely to phase transitions with reduced symmetry, such as decays away from the zero and infinite temperature limits. Our resu","authors_text":"Michael Nee, Prateek Agrawal","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-02-22T19:00:00Z","title":"The Boring Monopole"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2202.11102","kind":"arxiv","version":3},"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":"sha256:2ac518fcd38e6a6f3ba11527ebffbb9004da5409f306e732e7a36d3dfbedadf8","target":"record","created_at":"2026-07-05T04:54:52Z","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":"cd29294af84c4b963abb4d65b9a5538f38453c665b316b8ddd6811181580c3dd","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-02-22T19:00:00Z","title_canon_sha256":"94f3fa722980db2a42b1ffdc844bf8e96fe1b9dee589c1dbeb822c93909894ba"},"schema_version":"1.0","source":{"id":"2202.11102","kind":"arxiv","version":3}},"canonical_sha256":"7ed337f59d341a8de2acfd9d485605aa13a3e69599fa08e3536133a67230afe1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7ed337f59d341a8de2acfd9d485605aa13a3e69599fa08e3536133a67230afe1","first_computed_at":"2026-07-05T04:54:52.925461Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:54:52.925461Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"h32i5b8xl3H2cSUY06MHui71iKPr7Uo0h8kci3heHQ+hJGDPR5QlF/J9CCy/cHBj1gePwtI11+uMFxR2M2V/AQ==","signature_status":"signed_v1","signed_at":"2026-07-05T04:54:52.925882Z","signed_message":"canonical_sha256_bytes"},"source_id":"2202.11102","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2ac518fcd38e6a6f3ba11527ebffbb9004da5409f306e732e7a36d3dfbedadf8","sha256:d2331706e098eccf9fc441a988ac25d032c77bbf26c60078ac5bf7455b60adbc"],"state_sha256":"f6d7607287d7a860b4028f1c867ee34bdc8b4386f03752755cff95bbee64a4b7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jglp3J8qCDgPpAd8Pw602KHB7umbFrGCUpPz2v4YBWpxvLxKSShGzQWcGpq4dBj5WhYh+DxOHE4bBT+OWxbqCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-12T13:29:18.263746Z","bundle_sha256":"29f91c815253a0bf40ad3d8e6eedccb565483c2dc87f99fff33209ec1672d69d"}}