{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:RHH6WWFFZBTC55DHHXRWEJKO6U","short_pith_number":"pith:RHH6WWFF","canonical_record":{"source":{"id":"1409.6508","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-09-23T12:28:16Z","cross_cats_sorted":[],"title_canon_sha256":"4dcc77c7d7c58326799771681c864c5853070aaf4047e3311f8b54b500f60746","abstract_canon_sha256":"d2dcf157b5dc3be4629fd7fe740dcb5f6468f780da579735f31abf3eeb458d12"},"schema_version":"1.0"},"canonical_sha256":"89cfeb58a5c8662ef4673de362254ef5367b02245198284ec492492688711716","source":{"kind":"arxiv","id":"1409.6508","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1409.6508","created_at":"2026-05-18T02:20:10Z"},{"alias_kind":"arxiv_version","alias_value":"1409.6508v2","created_at":"2026-05-18T02:20:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.6508","created_at":"2026-05-18T02:20:10Z"},{"alias_kind":"pith_short_12","alias_value":"RHH6WWFFZBTC","created_at":"2026-05-18T12:28:46Z"},{"alias_kind":"pith_short_16","alias_value":"RHH6WWFFZBTC55DH","created_at":"2026-05-18T12:28:46Z"},{"alias_kind":"pith_short_8","alias_value":"RHH6WWFF","created_at":"2026-05-18T12:28:46Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:RHH6WWFFZBTC55DHHXRWEJKO6U","target":"record","payload":{"canonical_record":{"source":{"id":"1409.6508","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-09-23T12:28:16Z","cross_cats_sorted":[],"title_canon_sha256":"4dcc77c7d7c58326799771681c864c5853070aaf4047e3311f8b54b500f60746","abstract_canon_sha256":"d2dcf157b5dc3be4629fd7fe740dcb5f6468f780da579735f31abf3eeb458d12"},"schema_version":"1.0"},"canonical_sha256":"89cfeb58a5c8662ef4673de362254ef5367b02245198284ec492492688711716","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:20:10.091391Z","signature_b64":"PwIVu8ykV+FU11exfKkOJYo+Xxb2JWSyMsal6xnlbO5bN7i2OUVgktZWdfsNr9JeWH6xGKAZVsGeLNZ70nxKAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"89cfeb58a5c8662ef4673de362254ef5367b02245198284ec492492688711716","last_reissued_at":"2026-05-18T02:20:10.090740Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:20:10.090740Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1409.6508","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":"2026-05-18T02:20:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"o1OwOqjC6xXGwzc2cfWMBbydZ4m36JASYoMs5GNFE0n1rBme4yWLi2QuXDYc+VZULWJw1RzOajZZgXYvAJ8/AA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T20:46:57.478047Z"},"content_sha256":"71470ca6c820fed7b5d8cddd93a477a62b8c383c81b7c3834fbba2e695da5667","schema_version":"1.0","event_id":"sha256:71470ca6c820fed7b5d8cddd93a477a62b8c383c81b7c3834fbba2e695da5667"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:RHH6WWFFZBTC55DHHXRWEJKO6U","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Weak Scale From the Maximum Entropy Principle","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Hikaru Kawai, Kiyoharu Kawana, Yuta Hamada","submitted_at":"2014-09-23T12:28:16Z","abstract_excerpt":"The theory of multiverse and wormholes suggests that the parameters of the Standard Model are fixed in such a way that the radiation of the $S^{3}$ universe at the final stage $S_{rad}$ becomes maximum, which we call the maximum entropy principle. Although it is difficult to confirm this principle generally, for a few parameters of the Standard Model, we can check whether $S_{rad}$ actually becomes maximum at the observed values. In this paper, we regard $S_{rad}$ at the final stage as a function of the weak scale ( the Higgs expectation value ) $v_{h}$, and show that it becomes maximum around"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.6508","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":"2026-05-18T02:20:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"D53wJCCuaapgO4i4fxnWBPdRyt35xgh01j6Q/R50RJvlljZZKinX+Fd68OJnKgVdDEimUMfvT5KLIIJrNJ+vCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T20:46:57.478753Z"},"content_sha256":"a81f84c89936450e747670312bf906007d23c1fa6c341b02b01a6ae03ca346a8","schema_version":"1.0","event_id":"sha256:a81f84c89936450e747670312bf906007d23c1fa6c341b02b01a6ae03ca346a8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RHH6WWFFZBTC55DHHXRWEJKO6U/bundle.json","state_url":"https://pith.science/pith/RHH6WWFFZBTC55DHHXRWEJKO6U/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RHH6WWFFZBTC55DHHXRWEJKO6U/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":"2026-05-28T20:46:57Z","links":{"resolver":"https://pith.science/pith/RHH6WWFFZBTC55DHHXRWEJKO6U","bundle":"https://pith.science/pith/RHH6WWFFZBTC55DHHXRWEJKO6U/bundle.json","state":"https://pith.science/pith/RHH6WWFFZBTC55DHHXRWEJKO6U/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RHH6WWFFZBTC55DHHXRWEJKO6U/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:RHH6WWFFZBTC55DHHXRWEJKO6U","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":"d2dcf157b5dc3be4629fd7fe740dcb5f6468f780da579735f31abf3eeb458d12","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-09-23T12:28:16Z","title_canon_sha256":"4dcc77c7d7c58326799771681c864c5853070aaf4047e3311f8b54b500f60746"},"schema_version":"1.0","source":{"id":"1409.6508","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1409.6508","created_at":"2026-05-18T02:20:10Z"},{"alias_kind":"arxiv_version","alias_value":"1409.6508v2","created_at":"2026-05-18T02:20:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.6508","created_at":"2026-05-18T02:20:10Z"},{"alias_kind":"pith_short_12","alias_value":"RHH6WWFFZBTC","created_at":"2026-05-18T12:28:46Z"},{"alias_kind":"pith_short_16","alias_value":"RHH6WWFFZBTC55DH","created_at":"2026-05-18T12:28:46Z"},{"alias_kind":"pith_short_8","alias_value":"RHH6WWFF","created_at":"2026-05-18T12:28:46Z"}],"graph_snapshots":[{"event_id":"sha256:a81f84c89936450e747670312bf906007d23c1fa6c341b02b01a6ae03ca346a8","target":"graph","created_at":"2026-05-18T02:20:10Z","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":"The theory of multiverse and wormholes suggests that the parameters of the Standard Model are fixed in such a way that the radiation of the $S^{3}$ universe at the final stage $S_{rad}$ becomes maximum, which we call the maximum entropy principle. Although it is difficult to confirm this principle generally, for a few parameters of the Standard Model, we can check whether $S_{rad}$ actually becomes maximum at the observed values. In this paper, we regard $S_{rad}$ at the final stage as a function of the weak scale ( the Higgs expectation value ) $v_{h}$, and show that it becomes maximum around","authors_text":"Hikaru Kawai, Kiyoharu Kawana, Yuta Hamada","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-09-23T12:28:16Z","title":"Weak Scale From the Maximum Entropy Principle"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.6508","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":"sha256:71470ca6c820fed7b5d8cddd93a477a62b8c383c81b7c3834fbba2e695da5667","target":"record","created_at":"2026-05-18T02:20:10Z","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":"d2dcf157b5dc3be4629fd7fe740dcb5f6468f780da579735f31abf3eeb458d12","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-09-23T12:28:16Z","title_canon_sha256":"4dcc77c7d7c58326799771681c864c5853070aaf4047e3311f8b54b500f60746"},"schema_version":"1.0","source":{"id":"1409.6508","kind":"arxiv","version":2}},"canonical_sha256":"89cfeb58a5c8662ef4673de362254ef5367b02245198284ec492492688711716","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"89cfeb58a5c8662ef4673de362254ef5367b02245198284ec492492688711716","first_computed_at":"2026-05-18T02:20:10.090740Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:20:10.090740Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"PwIVu8ykV+FU11exfKkOJYo+Xxb2JWSyMsal6xnlbO5bN7i2OUVgktZWdfsNr9JeWH6xGKAZVsGeLNZ70nxKAA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:20:10.091391Z","signed_message":"canonical_sha256_bytes"},"source_id":"1409.6508","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:71470ca6c820fed7b5d8cddd93a477a62b8c383c81b7c3834fbba2e695da5667","sha256:a81f84c89936450e747670312bf906007d23c1fa6c341b02b01a6ae03ca346a8"],"state_sha256":"ffad08fde0403939af24c01d3bb304a4bbe091723d1d26a809f72d741595d343"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"k4keM2yop8x3WQl9wJKdreBa7i+ZEohzarVJme1pjfhUZpa5jrGL8691GLc20v84kpkp+pXLakHb77E1+q4IBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T20:46:57.482777Z","bundle_sha256":"f559edb55b076af2ea65457778c827aabd8cbe0044c826232c2a6a733e4d82ec"}}