{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:7B6ZMPTSMUNIGQZRMT4PM6KMET","short_pith_number":"pith:7B6ZMPTS","canonical_record":{"source":{"id":"1702.07840","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-02-25T06:59:02Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"f77e169b223f3c30b2fb2dda1e1c5214720a376126283e497876ce59c7620f6a","abstract_canon_sha256":"c26043c129ea22c14a4522d3a664c8fef5edc2c64800c708d90633eb80235510"},"schema_version":"1.0"},"canonical_sha256":"f87d963e72651a83433164f8f6794c24fa637564f3c4bbdb14f7878331e6c62e","source":{"kind":"arxiv","id":"1702.07840","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1702.07840","created_at":"2026-05-18T00:49:56Z"},{"alias_kind":"arxiv_version","alias_value":"1702.07840v1","created_at":"2026-05-18T00:49:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.07840","created_at":"2026-05-18T00:49:56Z"},{"alias_kind":"pith_short_12","alias_value":"7B6ZMPTSMUNI","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_16","alias_value":"7B6ZMPTSMUNIGQZR","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_8","alias_value":"7B6ZMPTS","created_at":"2026-05-18T12:31:03Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:7B6ZMPTSMUNIGQZRMT4PM6KMET","target":"record","payload":{"canonical_record":{"source":{"id":"1702.07840","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-02-25T06:59:02Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"f77e169b223f3c30b2fb2dda1e1c5214720a376126283e497876ce59c7620f6a","abstract_canon_sha256":"c26043c129ea22c14a4522d3a664c8fef5edc2c64800c708d90633eb80235510"},"schema_version":"1.0"},"canonical_sha256":"f87d963e72651a83433164f8f6794c24fa637564f3c4bbdb14f7878331e6c62e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:49:56.885000Z","signature_b64":"ikssSF6X4Y6Xu5JF7/Pl+c+SLKrOOOUDpYQ9NzCXJ44mBRqrjVxMZOkAHpFKoJlOeBfaEtsSwLfmyKCQirF9Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f87d963e72651a83433164f8f6794c24fa637564f3c4bbdb14f7878331e6c62e","last_reissued_at":"2026-05-18T00:49:56.884390Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:49:56.884390Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1702.07840","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":"2026-05-18T00:49:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OkKBONnTxzunqPqMr2tDZ2q99MsYCJRiRYiH9NJj5HWkTTLpHOYD5I8YBID8dSRCuR61Nq9v5KZG0rEhc9QPDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T10:53:52.944907Z"},"content_sha256":"175d00a14478ad7a3fcbc1e9110798048a87dc51a0b38b8eb396a67a22058d39","schema_version":"1.0","event_id":"sha256:175d00a14478ad7a3fcbc1e9110798048a87dc51a0b38b8eb396a67a22058d39"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:7B6ZMPTSMUNIGQZRMT4PM6KMET","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Fluctuations In The Inhomogeneous Chiral Transition","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"R. Yoshiike, T.-G. Lee, T. Tatsumi","submitted_at":"2017-02-25T06:59:02Z","abstract_excerpt":"Chiral pair fluctuation are considered near the phase boundary of the inhomogeneous chiral phase (iCP). The fluctuations are then bosonized and an effective action for the chiral pair fluctuation is basically constructed by considering the ring diagram of the polarization function. We can evaluate the self-energy and effective four point interaction among fluctuations in a consistent way. The peculiar dispersion of the fluctuation, reflecting the spatially inhomogeneous transition, gives rise to interesting and qualitative results. Thermal fluctuations prohibit the second-order transition, whi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.07840","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":"2026-05-18T00:49:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VkVqUojIKzgGO+zlsHowPu+jjf8jjOHRMuCFmKvvHy2htguiIjAYlPgc4PYj6eC8ioLdj+ZNLRhuAwJ92pjYBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T10:53:52.945544Z"},"content_sha256":"2d0dd51550c3797c2727407d0f18cbda1cca5e8a287a4774ffe73bd5f7821135","schema_version":"1.0","event_id":"sha256:2d0dd51550c3797c2727407d0f18cbda1cca5e8a287a4774ffe73bd5f7821135"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/7B6ZMPTSMUNIGQZRMT4PM6KMET/bundle.json","state_url":"https://pith.science/pith/7B6ZMPTSMUNIGQZRMT4PM6KMET/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/7B6ZMPTSMUNIGQZRMT4PM6KMET/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":"2026-05-31T10:53:52Z","links":{"resolver":"https://pith.science/pith/7B6ZMPTSMUNIGQZRMT4PM6KMET","bundle":"https://pith.science/pith/7B6ZMPTSMUNIGQZRMT4PM6KMET/bundle.json","state":"https://pith.science/pith/7B6ZMPTSMUNIGQZRMT4PM6KMET/state.json","well_known_bundle":"https://pith.science/.well-known/pith/7B6ZMPTSMUNIGQZRMT4PM6KMET/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:7B6ZMPTSMUNIGQZRMT4PM6KMET","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":"c26043c129ea22c14a4522d3a664c8fef5edc2c64800c708d90633eb80235510","cross_cats_sorted":["nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-02-25T06:59:02Z","title_canon_sha256":"f77e169b223f3c30b2fb2dda1e1c5214720a376126283e497876ce59c7620f6a"},"schema_version":"1.0","source":{"id":"1702.07840","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1702.07840","created_at":"2026-05-18T00:49:56Z"},{"alias_kind":"arxiv_version","alias_value":"1702.07840v1","created_at":"2026-05-18T00:49:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.07840","created_at":"2026-05-18T00:49:56Z"},{"alias_kind":"pith_short_12","alias_value":"7B6ZMPTSMUNI","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_16","alias_value":"7B6ZMPTSMUNIGQZR","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_8","alias_value":"7B6ZMPTS","created_at":"2026-05-18T12:31:03Z"}],"graph_snapshots":[{"event_id":"sha256:2d0dd51550c3797c2727407d0f18cbda1cca5e8a287a4774ffe73bd5f7821135","target":"graph","created_at":"2026-05-18T00:49:56Z","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":"Chiral pair fluctuation are considered near the phase boundary of the inhomogeneous chiral phase (iCP). The fluctuations are then bosonized and an effective action for the chiral pair fluctuation is basically constructed by considering the ring diagram of the polarization function. We can evaluate the self-energy and effective four point interaction among fluctuations in a consistent way. The peculiar dispersion of the fluctuation, reflecting the spatially inhomogeneous transition, gives rise to interesting and qualitative results. Thermal fluctuations prohibit the second-order transition, whi","authors_text":"R. Yoshiike, T.-G. Lee, T. Tatsumi","cross_cats":["nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-02-25T06:59:02Z","title":"Fluctuations In The Inhomogeneous Chiral Transition"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.07840","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":"sha256:175d00a14478ad7a3fcbc1e9110798048a87dc51a0b38b8eb396a67a22058d39","target":"record","created_at":"2026-05-18T00:49:56Z","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":"c26043c129ea22c14a4522d3a664c8fef5edc2c64800c708d90633eb80235510","cross_cats_sorted":["nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-02-25T06:59:02Z","title_canon_sha256":"f77e169b223f3c30b2fb2dda1e1c5214720a376126283e497876ce59c7620f6a"},"schema_version":"1.0","source":{"id":"1702.07840","kind":"arxiv","version":1}},"canonical_sha256":"f87d963e72651a83433164f8f6794c24fa637564f3c4bbdb14f7878331e6c62e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f87d963e72651a83433164f8f6794c24fa637564f3c4bbdb14f7878331e6c62e","first_computed_at":"2026-05-18T00:49:56.884390Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:49:56.884390Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ikssSF6X4Y6Xu5JF7/Pl+c+SLKrOOOUDpYQ9NzCXJ44mBRqrjVxMZOkAHpFKoJlOeBfaEtsSwLfmyKCQirF9Ag==","signature_status":"signed_v1","signed_at":"2026-05-18T00:49:56.885000Z","signed_message":"canonical_sha256_bytes"},"source_id":"1702.07840","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:175d00a14478ad7a3fcbc1e9110798048a87dc51a0b38b8eb396a67a22058d39","sha256:2d0dd51550c3797c2727407d0f18cbda1cca5e8a287a4774ffe73bd5f7821135"],"state_sha256":"0b9e3436fd70ef603f8c8dd8a9e141edc456bee2be6ea87ebe999d92741f0251"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KeZSZGzYS0Y26n83qzWRbx0glvytf0T3J1mhH043OsA+BCQmtHN8FWLo+YVLRyFQG51HWwvF+ImVzLvGg/B/Cw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T10:53:52.949086Z","bundle_sha256":"b1e1af276c6bbfad88ce8d49e35ad13c12d1f9713558a48f93592d17b862cf48"}}