{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1995:5R5UILIK3RYBH54H5Y6XHGF2DU","short_pith_number":"pith:5R5UILIK","canonical_record":{"source":{"id":"hep-ph/9511376","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1995-11-20T23:02:17Z","cross_cats_sorted":[],"title_canon_sha256":"f15741a6af26389364bc37652ad9e34dc0e70f511317c12ea2889ec8d22b72dc","abstract_canon_sha256":"60d48bd11b4edb1dac842050704e3ad5a1dd1905b542609ad3458b3b4fecc73a"},"schema_version":"1.0"},"canonical_sha256":"ec7b442d0adc7013f787ee3d7398ba1d278364be82ec892e5ee9465cc0424a63","source":{"kind":"arxiv","id":"hep-ph/9511376","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9511376","created_at":"2026-07-04T15:59:16Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9511376v2","created_at":"2026-07-04T15:59:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9511376","created_at":"2026-07-04T15:59:16Z"},{"alias_kind":"pith_short_12","alias_value":"5R5UILIK3RYB","created_at":"2026-07-04T15:59:16Z"},{"alias_kind":"pith_short_16","alias_value":"5R5UILIK3RYBH54H","created_at":"2026-07-04T15:59:16Z"},{"alias_kind":"pith_short_8","alias_value":"5R5UILIK","created_at":"2026-07-04T15:59:16Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1995:5R5UILIK3RYBH54H5Y6XHGF2DU","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/9511376","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1995-11-20T23:02:17Z","cross_cats_sorted":[],"title_canon_sha256":"f15741a6af26389364bc37652ad9e34dc0e70f511317c12ea2889ec8d22b72dc","abstract_canon_sha256":"60d48bd11b4edb1dac842050704e3ad5a1dd1905b542609ad3458b3b4fecc73a"},"schema_version":"1.0"},"canonical_sha256":"ec7b442d0adc7013f787ee3d7398ba1d278364be82ec892e5ee9465cc0424a63","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:59:16.870738Z","signature_b64":"yJCDmy17omOd5E8HQo7UPJlDZMYps8ZP57BCSneaYRPUr/eBgc+KwE4UcuhkijoysGaMqHSH1V2vIEiizAxFDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ec7b442d0adc7013f787ee3d7398ba1d278364be82ec892e5ee9465cc0424a63","last_reissued_at":"2026-07-04T15:59:16.870388Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:59:16.870388Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/9511376","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":"2026-07-04T15:59:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"q+xS9HrBVGVoDC15Z/p8JUwwrQvD6x+xypcYDm317cYC2ELeyEXPb9qwgw0vQ5+yo0Sb7mF4rNm7bX6tUu+fDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T01:06:58.700068Z"},"content_sha256":"5fd02a1c7977dfd8ca3394dcf6739bd2c0758a4175f50ed22c45eb9787dcb36f","schema_version":"1.0","event_id":"sha256:5fd02a1c7977dfd8ca3394dcf6739bd2c0758a4175f50ed22c45eb9787dcb36f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1995:5R5UILIK3RYBH54H5Y6XHGF2DU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Solution to the Strong CP Problem: Supersymmetry with Parity","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ravi Kuchimanchi","submitted_at":"1995-11-20T23:02:17Z","abstract_excerpt":"There is a natural solution to the strong CP problem in the Minimal Supersymmetric Standard Model if it arises from a parity symmetric theory which is spontaneously broken to MSSM at Planck, GUT or intermediate scales. The strong CP phase is zero at the tree level and is not induced to two loops. The SUSY phase problems are also solved. The universal soft SUSY breaking parameters A, B, \\mu, m_{1/2} are all automatically real and the only additional CP violation effects of the low-energy MSSM are characterized by a Hermitian squark mass matrix whose phases depend on the CKM phase. Cases with no"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9511376","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/hep-ph/9511376/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":"2026-07-04T15:59:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8/UK9+GD0QDNQ+WXyvXQCEHFBucMJAE8UPROnZFhRY+/rIy9QrJb3qd0mrIZxmdnpwU12oci0EorQ307CGdTCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T01:06:58.700567Z"},"content_sha256":"6a4671e9da444ff93ecdbdb09b4a7689db0f224b25dbba57aefa24c103ba8360","schema_version":"1.0","event_id":"sha256:6a4671e9da444ff93ecdbdb09b4a7689db0f224b25dbba57aefa24c103ba8360"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5R5UILIK3RYBH54H5Y6XHGF2DU/bundle.json","state_url":"https://pith.science/pith/5R5UILIK3RYBH54H5Y6XHGF2DU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5R5UILIK3RYBH54H5Y6XHGF2DU/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":"2026-08-04T01:06:58Z","links":{"resolver":"https://pith.science/pith/5R5UILIK3RYBH54H5Y6XHGF2DU","bundle":"https://pith.science/pith/5R5UILIK3RYBH54H5Y6XHGF2DU/bundle.json","state":"https://pith.science/pith/5R5UILIK3RYBH54H5Y6XHGF2DU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5R5UILIK3RYBH54H5Y6XHGF2DU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1995:5R5UILIK3RYBH54H5Y6XHGF2DU","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":"60d48bd11b4edb1dac842050704e3ad5a1dd1905b542609ad3458b3b4fecc73a","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1995-11-20T23:02:17Z","title_canon_sha256":"f15741a6af26389364bc37652ad9e34dc0e70f511317c12ea2889ec8d22b72dc"},"schema_version":"1.0","source":{"id":"hep-ph/9511376","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9511376","created_at":"2026-07-04T15:59:16Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9511376v2","created_at":"2026-07-04T15:59:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9511376","created_at":"2026-07-04T15:59:16Z"},{"alias_kind":"pith_short_12","alias_value":"5R5UILIK3RYB","created_at":"2026-07-04T15:59:16Z"},{"alias_kind":"pith_short_16","alias_value":"5R5UILIK3RYBH54H","created_at":"2026-07-04T15:59:16Z"},{"alias_kind":"pith_short_8","alias_value":"5R5UILIK","created_at":"2026-07-04T15:59:16Z"}],"graph_snapshots":[{"event_id":"sha256:6a4671e9da444ff93ecdbdb09b4a7689db0f224b25dbba57aefa24c103ba8360","target":"graph","created_at":"2026-07-04T15:59:16Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/hep-ph/9511376/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"There is a natural solution to the strong CP problem in the Minimal Supersymmetric Standard Model if it arises from a parity symmetric theory which is spontaneously broken to MSSM at Planck, GUT or intermediate scales. The strong CP phase is zero at the tree level and is not induced to two loops. The SUSY phase problems are also solved. The universal soft SUSY breaking parameters A, B, \\mu, m_{1/2} are all automatically real and the only additional CP violation effects of the low-energy MSSM are characterized by a Hermitian squark mass matrix whose phases depend on the CKM phase. Cases with no","authors_text":"Ravi Kuchimanchi","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"1995-11-20T23:02:17Z","title":"Solution to the Strong CP Problem: Supersymmetry with Parity"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9511376","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":"sha256:5fd02a1c7977dfd8ca3394dcf6739bd2c0758a4175f50ed22c45eb9787dcb36f","target":"record","created_at":"2026-07-04T15:59:16Z","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":"60d48bd11b4edb1dac842050704e3ad5a1dd1905b542609ad3458b3b4fecc73a","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1995-11-20T23:02:17Z","title_canon_sha256":"f15741a6af26389364bc37652ad9e34dc0e70f511317c12ea2889ec8d22b72dc"},"schema_version":"1.0","source":{"id":"hep-ph/9511376","kind":"arxiv","version":2}},"canonical_sha256":"ec7b442d0adc7013f787ee3d7398ba1d278364be82ec892e5ee9465cc0424a63","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ec7b442d0adc7013f787ee3d7398ba1d278364be82ec892e5ee9465cc0424a63","first_computed_at":"2026-07-04T15:59:16.870388Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:59:16.870388Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"yJCDmy17omOd5E8HQo7UPJlDZMYps8ZP57BCSneaYRPUr/eBgc+KwE4UcuhkijoysGaMqHSH1V2vIEiizAxFDQ==","signature_status":"signed_v1","signed_at":"2026-07-04T15:59:16.870738Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/9511376","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5fd02a1c7977dfd8ca3394dcf6739bd2c0758a4175f50ed22c45eb9787dcb36f","sha256:6a4671e9da444ff93ecdbdb09b4a7689db0f224b25dbba57aefa24c103ba8360"],"state_sha256":"1cbbbcbb5645e7d1321c93e6ff3b72a958c9a15ed7f4d80ce7a679980fcbe645"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wmktM2/WPDLglzysc0wbv2iDazpwxDHlOhVzys7X1wFaKjrHotg50ox9/4dxD2FFUhCYwpaZNG3OAJsyWtJqDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-04T01:06:58.705331Z","bundle_sha256":"da633a0cec5be6f1d76549be766cfdec9af7fa382f44e5fe95d9d642caa67f01"}}