{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:7TLME35HZBUIZJL5OHNFU5C4KJ","short_pith_number":"pith:7TLME35H","canonical_record":{"source":{"id":"1003.2462","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2010-03-12T02:03:02Z","cross_cats_sorted":["gr-qc","hep-ph","hep-th"],"title_canon_sha256":"7ef83d9ec3569f8f1f16332a66ca06698d0c4845b38c2c3af50a1807ff518745","abstract_canon_sha256":"d84d9ba7de3c962d9a3ce70854693a17062a8a849a0404427882bf9428c9567c"},"schema_version":"1.0"},"canonical_sha256":"fcd6c26fa7c8688ca57d71da5a745c5264cf69f9e607eb364d22f6530615ff18","source":{"kind":"arxiv","id":"1003.2462","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1003.2462","created_at":"2026-05-18T02:24:37Z"},{"alias_kind":"arxiv_version","alias_value":"1003.2462v1","created_at":"2026-05-18T02:24:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1003.2462","created_at":"2026-05-18T02:24:37Z"},{"alias_kind":"pith_short_12","alias_value":"7TLME35HZBUI","created_at":"2026-05-18T12:26:05Z"},{"alias_kind":"pith_short_16","alias_value":"7TLME35HZBUIZJL5","created_at":"2026-05-18T12:26:05Z"},{"alias_kind":"pith_short_8","alias_value":"7TLME35H","created_at":"2026-05-18T12:26:05Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:7TLME35HZBUIZJL5OHNFU5C4KJ","target":"record","payload":{"canonical_record":{"source":{"id":"1003.2462","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2010-03-12T02:03:02Z","cross_cats_sorted":["gr-qc","hep-ph","hep-th"],"title_canon_sha256":"7ef83d9ec3569f8f1f16332a66ca06698d0c4845b38c2c3af50a1807ff518745","abstract_canon_sha256":"d84d9ba7de3c962d9a3ce70854693a17062a8a849a0404427882bf9428c9567c"},"schema_version":"1.0"},"canonical_sha256":"fcd6c26fa7c8688ca57d71da5a745c5264cf69f9e607eb364d22f6530615ff18","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:24:37.834614Z","signature_b64":"T4PdRvwlGYWwol8n4OLZZXxwXNocy8UzgXb2ZEzUJMMF+8cIko6A0lNnzw1nuoYW+GbYQhPDGZ/UmI1B7dZFCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fcd6c26fa7c8688ca57d71da5a745c5264cf69f9e607eb364d22f6530615ff18","last_reissued_at":"2026-05-18T02:24:37.833924Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:24:37.833924Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1003.2462","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":"2026-05-18T02:24:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"y3TjWllsg4KTbgzQmspI2CLqVEwpE1w3hN8tx1abfyXuM+ugLBUSrzluF81Tk21KABvUyByt2W38MC/NcTUxAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-12T08:29:59.230207Z"},"content_sha256":"051214a29691e707ba8b5e53fcd3fac61371fce2a7477ee6395f214dbe831186","schema_version":"1.0","event_id":"sha256:051214a29691e707ba8b5e53fcd3fac61371fce2a7477ee6395f214dbe831186"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:7TLME35HZBUIZJL5OHNFU5C4KJ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Gravity Waves as a Probe of Hubble Expansion Rate During An Electroweak Scale Phase Transition","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","hep-ph","hep-th"],"primary_cat":"astro-ph.CO","authors_text":"Daniel J.H. Chung, Peng Zhou","submitted_at":"2010-03-12T02:03:02Z","abstract_excerpt":"Just as big bang nucleosynthesis allows us to probe the expansion rate when the temperature of the universe was around 1 MeV, the measurement of gravity waves from electroweak scale first order phase transitions may allow us to probe the expansion rate when the temperature of the universe was at the electroweak scale. We compute the simple transformation rule for the gravity wave spectrum under the scaling transformation of the Hubble expansion rate. We then apply this directly to the scenario of quintessence kination domination and show how gravity wave spectra would shift relative to LISA an"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1003.2462","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":"2026-05-18T02:24:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"W+7P2DUQmLQSpgoyRAP77GfEYL3LkJrcANhra7KjsjX2wgHgEVrkj3j7wsDeT/of/hQd5A6Tx9qazv+OGmgbDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-12T08:29:59.230578Z"},"content_sha256":"cbe28f448fce9ef88d2d713c2d50bb9ea39c25c3ee9ced3396bea5b6292dd09d","schema_version":"1.0","event_id":"sha256:cbe28f448fce9ef88d2d713c2d50bb9ea39c25c3ee9ced3396bea5b6292dd09d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/7TLME35HZBUIZJL5OHNFU5C4KJ/bundle.json","state_url":"https://pith.science/pith/7TLME35HZBUIZJL5OHNFU5C4KJ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/7TLME35HZBUIZJL5OHNFU5C4KJ/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":"2026-06-12T08:29:59Z","links":{"resolver":"https://pith.science/pith/7TLME35HZBUIZJL5OHNFU5C4KJ","bundle":"https://pith.science/pith/7TLME35HZBUIZJL5OHNFU5C4KJ/bundle.json","state":"https://pith.science/pith/7TLME35HZBUIZJL5OHNFU5C4KJ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/7TLME35HZBUIZJL5OHNFU5C4KJ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:7TLME35HZBUIZJL5OHNFU5C4KJ","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":"d84d9ba7de3c962d9a3ce70854693a17062a8a849a0404427882bf9428c9567c","cross_cats_sorted":["gr-qc","hep-ph","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2010-03-12T02:03:02Z","title_canon_sha256":"7ef83d9ec3569f8f1f16332a66ca06698d0c4845b38c2c3af50a1807ff518745"},"schema_version":"1.0","source":{"id":"1003.2462","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1003.2462","created_at":"2026-05-18T02:24:37Z"},{"alias_kind":"arxiv_version","alias_value":"1003.2462v1","created_at":"2026-05-18T02:24:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1003.2462","created_at":"2026-05-18T02:24:37Z"},{"alias_kind":"pith_short_12","alias_value":"7TLME35HZBUI","created_at":"2026-05-18T12:26:05Z"},{"alias_kind":"pith_short_16","alias_value":"7TLME35HZBUIZJL5","created_at":"2026-05-18T12:26:05Z"},{"alias_kind":"pith_short_8","alias_value":"7TLME35H","created_at":"2026-05-18T12:26:05Z"}],"graph_snapshots":[{"event_id":"sha256:cbe28f448fce9ef88d2d713c2d50bb9ea39c25c3ee9ced3396bea5b6292dd09d","target":"graph","created_at":"2026-05-18T02:24:37Z","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":"Just as big bang nucleosynthesis allows us to probe the expansion rate when the temperature of the universe was around 1 MeV, the measurement of gravity waves from electroweak scale first order phase transitions may allow us to probe the expansion rate when the temperature of the universe was at the electroweak scale. We compute the simple transformation rule for the gravity wave spectrum under the scaling transformation of the Hubble expansion rate. We then apply this directly to the scenario of quintessence kination domination and show how gravity wave spectra would shift relative to LISA an","authors_text":"Daniel J.H. Chung, Peng Zhou","cross_cats":["gr-qc","hep-ph","hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2010-03-12T02:03:02Z","title":"Gravity Waves as a Probe of Hubble Expansion Rate During An Electroweak Scale Phase Transition"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1003.2462","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":"sha256:051214a29691e707ba8b5e53fcd3fac61371fce2a7477ee6395f214dbe831186","target":"record","created_at":"2026-05-18T02:24:37Z","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":"d84d9ba7de3c962d9a3ce70854693a17062a8a849a0404427882bf9428c9567c","cross_cats_sorted":["gr-qc","hep-ph","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2010-03-12T02:03:02Z","title_canon_sha256":"7ef83d9ec3569f8f1f16332a66ca06698d0c4845b38c2c3af50a1807ff518745"},"schema_version":"1.0","source":{"id":"1003.2462","kind":"arxiv","version":1}},"canonical_sha256":"fcd6c26fa7c8688ca57d71da5a745c5264cf69f9e607eb364d22f6530615ff18","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"fcd6c26fa7c8688ca57d71da5a745c5264cf69f9e607eb364d22f6530615ff18","first_computed_at":"2026-05-18T02:24:37.833924Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:24:37.833924Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"T4PdRvwlGYWwol8n4OLZZXxwXNocy8UzgXb2ZEzUJMMF+8cIko6A0lNnzw1nuoYW+GbYQhPDGZ/UmI1B7dZFCw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:24:37.834614Z","signed_message":"canonical_sha256_bytes"},"source_id":"1003.2462","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:051214a29691e707ba8b5e53fcd3fac61371fce2a7477ee6395f214dbe831186","sha256:cbe28f448fce9ef88d2d713c2d50bb9ea39c25c3ee9ced3396bea5b6292dd09d"],"state_sha256":"78fb4431ac450f892772a1cfda499238f4f383ffa1348859c41318ffb2727990"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"EmDEySf5FgFoVKMiTO1XgO29e9coq3iTrNwOtM/jLz+MDqQw0yTDFj07s9bQxYVonQBqAfsTSooHfsZZuviJCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-12T08:29:59.232674Z","bundle_sha256":"bc7bf8d4dc394a0a1f3f7b09385a5f7aa651492f7b85b24039fd9c96f0c7a050"}}