{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:52K5USXD2NSYHKSEFZA5LBTW7P","short_pith_number":"pith:52K5USXD","canonical_record":{"source":{"id":"2510.19275","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-10-22T06:24:57Z","cross_cats_sorted":["astro-ph.CO"],"title_canon_sha256":"11cefeb8b2334b62d918af1deb6d255a518273152e314a5062c9ec122f891e59","abstract_canon_sha256":"804682a981fa83c6d6792d6aca81e3222ebbb47c09c615bb3f9ff780802dcdf5"},"schema_version":"1.0"},"canonical_sha256":"ee95da4ae3d36583aa442e41d58676fbc93fbb1d2385171b84ba22b99eb31828","source":{"kind":"arxiv","id":"2510.19275","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2510.19275","created_at":"2026-07-14T01:19:55Z"},{"alias_kind":"arxiv_version","alias_value":"2510.19275v2","created_at":"2026-07-14T01:19:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2510.19275","created_at":"2026-07-14T01:19:55Z"},{"alias_kind":"pith_short_12","alias_value":"52K5USXD2NSY","created_at":"2026-07-14T01:19:55Z"},{"alias_kind":"pith_short_16","alias_value":"52K5USXD2NSYHKSE","created_at":"2026-07-14T01:19:55Z"},{"alias_kind":"pith_short_8","alias_value":"52K5USXD","created_at":"2026-07-14T01:19:55Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:52K5USXD2NSYHKSEFZA5LBTW7P","target":"record","payload":{"canonical_record":{"source":{"id":"2510.19275","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-10-22T06:24:57Z","cross_cats_sorted":["astro-ph.CO"],"title_canon_sha256":"11cefeb8b2334b62d918af1deb6d255a518273152e314a5062c9ec122f891e59","abstract_canon_sha256":"804682a981fa83c6d6792d6aca81e3222ebbb47c09c615bb3f9ff780802dcdf5"},"schema_version":"1.0"},"canonical_sha256":"ee95da4ae3d36583aa442e41d58676fbc93fbb1d2385171b84ba22b99eb31828","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-14T01:19:55.646690Z","signature_b64":"gwpoVkep8Y+yKzip4sNBxXBQDhxsxYhVBxgoeuhY0pc1vdbAbgzu6qzUNGzVaxSSpNEb73Blsw32EWxkD0R7DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ee95da4ae3d36583aa442e41d58676fbc93fbb1d2385171b84ba22b99eb31828","last_reissued_at":"2026-07-14T01:19:55.645766Z","signature_status":"signed_v1","first_computed_at":"2026-07-14T01:19:55.645766Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2510.19275","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":"2026-07-14T01:19:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vLzJQQORge7SwSDn5UXTamG1kP3CcOYm/PBESOfANaaQSTGpfMx58MnctmQao/EAKAAU/r4PYdUNU26DaFTICQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T16:03:48.956777Z"},"content_sha256":"347c5ff8a1c77e4fcd628da6ec3349e8be69e15d0cc456395247e029df982ef7","schema_version":"1.0","event_id":"sha256:347c5ff8a1c77e4fcd628da6ec3349e8be69e15d0cc456395247e029df982ef7"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:52K5USXD2NSYHKSEFZA5LBTW7P","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Charge distribution of the gauge-mediation type Q ball","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["astro-ph.CO"],"primary_cat":"hep-ph","authors_text":"Masahiro Kawasaki, Shinta Kasuya","submitted_at":"2025-10-22T06:24:57Z","abstract_excerpt":"We numerically study the formation of the gauge-mediation type Q balls in the logarithmic square potential on three-dimensional lattices. We obtain the broad charge distribution of the Q ball of this type for the first time, to the best of our knowledge. The charge of the Q ball at the peak of the distribution is smaller than what we estimated as the average of the largest tens of the Q balls in the logarithmic potential for the same initial amplitude of the field at the onset of its oscillation. We also discuss some impacts of the broad distribution on cosmology and astrophysics. In the B bal"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2510.19275","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2510.19275/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":"2026-07-14T01:19:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XFb720fEE0pzXy4iUPzKROanqf83ekFYVO05laIGXoHZiQy19jj+psegKblLbOLLsIwkC3ZXagDQTFFyColkAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T16:03:48.957326Z"},"content_sha256":"e4704ca47406567b9a9022f1c3975d9e2c4e8591eeaeb8e84ce0e138ab6e6611","schema_version":"1.0","event_id":"sha256:e4704ca47406567b9a9022f1c3975d9e2c4e8591eeaeb8e84ce0e138ab6e6611"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/52K5USXD2NSYHKSEFZA5LBTW7P/bundle.json","state_url":"https://pith.science/pith/52K5USXD2NSYHKSEFZA5LBTW7P/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/52K5USXD2NSYHKSEFZA5LBTW7P/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":"2026-08-04T16:03:48Z","links":{"resolver":"https://pith.science/pith/52K5USXD2NSYHKSEFZA5LBTW7P","bundle":"https://pith.science/pith/52K5USXD2NSYHKSEFZA5LBTW7P/bundle.json","state":"https://pith.science/pith/52K5USXD2NSYHKSEFZA5LBTW7P/state.json","well_known_bundle":"https://pith.science/.well-known/pith/52K5USXD2NSYHKSEFZA5LBTW7P/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:52K5USXD2NSYHKSEFZA5LBTW7P","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":"804682a981fa83c6d6792d6aca81e3222ebbb47c09c615bb3f9ff780802dcdf5","cross_cats_sorted":["astro-ph.CO"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-10-22T06:24:57Z","title_canon_sha256":"11cefeb8b2334b62d918af1deb6d255a518273152e314a5062c9ec122f891e59"},"schema_version":"1.0","source":{"id":"2510.19275","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2510.19275","created_at":"2026-07-14T01:19:55Z"},{"alias_kind":"arxiv_version","alias_value":"2510.19275v2","created_at":"2026-07-14T01:19:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2510.19275","created_at":"2026-07-14T01:19:55Z"},{"alias_kind":"pith_short_12","alias_value":"52K5USXD2NSY","created_at":"2026-07-14T01:19:55Z"},{"alias_kind":"pith_short_16","alias_value":"52K5USXD2NSYHKSE","created_at":"2026-07-14T01:19:55Z"},{"alias_kind":"pith_short_8","alias_value":"52K5USXD","created_at":"2026-07-14T01:19:55Z"}],"graph_snapshots":[{"event_id":"sha256:e4704ca47406567b9a9022f1c3975d9e2c4e8591eeaeb8e84ce0e138ab6e6611","target":"graph","created_at":"2026-07-14T01:19:55Z","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/2510.19275/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We numerically study the formation of the gauge-mediation type Q balls in the logarithmic square potential on three-dimensional lattices. We obtain the broad charge distribution of the Q ball of this type for the first time, to the best of our knowledge. The charge of the Q ball at the peak of the distribution is smaller than what we estimated as the average of the largest tens of the Q balls in the logarithmic potential for the same initial amplitude of the field at the onset of its oscillation. We also discuss some impacts of the broad distribution on cosmology and astrophysics. In the B bal","authors_text":"Masahiro Kawasaki, Shinta Kasuya","cross_cats":["astro-ph.CO"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-10-22T06:24:57Z","title":"Charge distribution of the gauge-mediation type Q ball"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2510.19275","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":"sha256:347c5ff8a1c77e4fcd628da6ec3349e8be69e15d0cc456395247e029df982ef7","target":"record","created_at":"2026-07-14T01:19:55Z","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":"804682a981fa83c6d6792d6aca81e3222ebbb47c09c615bb3f9ff780802dcdf5","cross_cats_sorted":["astro-ph.CO"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-10-22T06:24:57Z","title_canon_sha256":"11cefeb8b2334b62d918af1deb6d255a518273152e314a5062c9ec122f891e59"},"schema_version":"1.0","source":{"id":"2510.19275","kind":"arxiv","version":2}},"canonical_sha256":"ee95da4ae3d36583aa442e41d58676fbc93fbb1d2385171b84ba22b99eb31828","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ee95da4ae3d36583aa442e41d58676fbc93fbb1d2385171b84ba22b99eb31828","first_computed_at":"2026-07-14T01:19:55.645766Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-14T01:19:55.645766Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"gwpoVkep8Y+yKzip4sNBxXBQDhxsxYhVBxgoeuhY0pc1vdbAbgzu6qzUNGzVaxSSpNEb73Blsw32EWxkD0R7DQ==","signature_status":"signed_v1","signed_at":"2026-07-14T01:19:55.646690Z","signed_message":"canonical_sha256_bytes"},"source_id":"2510.19275","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:347c5ff8a1c77e4fcd628da6ec3349e8be69e15d0cc456395247e029df982ef7","sha256:e4704ca47406567b9a9022f1c3975d9e2c4e8591eeaeb8e84ce0e138ab6e6611"],"state_sha256":"8313289147a74cbdc59d5c51db7fc96fd34530e97b38a67ccfd3d4023d1aa471"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NcrnmN6uNTlBx8kMHMg2SFh5ajniScSfmHDY2eejM6dwcEYiZUZvhjLT4NdCVpXHp8DYKVmRoiEZ37hhens3Bw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-04T16:03:48.961229Z","bundle_sha256":"f5edd13c1a699a8107164aa3b65e93e3b91d5063dd9c4eed56b463571507a0da"}}