{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:47G3KL7U7EETJSKXLNQPY7M7DC","short_pith_number":"pith:47G3KL7U","canonical_record":{"source":{"id":"1606.05221","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-06-16T15:20:07Z","cross_cats_sorted":[],"title_canon_sha256":"6586f2b3003bcd381845d091985b211a7a3ca11d9e9bb6e4623ac39a6956886b","abstract_canon_sha256":"245d5f6d9919dfaa3c7e5800c893088e240cb77313779516e8099f14ec2fd107"},"schema_version":"1.0"},"canonical_sha256":"e7cdb52ff4f90934c9575b60fc7d9f18b123ed8994f54f07ffaf22ab2673efd2","source":{"kind":"arxiv","id":"1606.05221","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1606.05221","created_at":"2026-05-18T00:28:57Z"},{"alias_kind":"arxiv_version","alias_value":"1606.05221v2","created_at":"2026-05-18T00:28:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1606.05221","created_at":"2026-05-18T00:28:57Z"},{"alias_kind":"pith_short_12","alias_value":"47G3KL7U7EET","created_at":"2026-05-18T12:29:58Z"},{"alias_kind":"pith_short_16","alias_value":"47G3KL7U7EETJSKX","created_at":"2026-05-18T12:29:58Z"},{"alias_kind":"pith_short_8","alias_value":"47G3KL7U","created_at":"2026-05-18T12:29:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:47G3KL7U7EETJSKXLNQPY7M7DC","target":"record","payload":{"canonical_record":{"source":{"id":"1606.05221","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-06-16T15:20:07Z","cross_cats_sorted":[],"title_canon_sha256":"6586f2b3003bcd381845d091985b211a7a3ca11d9e9bb6e4623ac39a6956886b","abstract_canon_sha256":"245d5f6d9919dfaa3c7e5800c893088e240cb77313779516e8099f14ec2fd107"},"schema_version":"1.0"},"canonical_sha256":"e7cdb52ff4f90934c9575b60fc7d9f18b123ed8994f54f07ffaf22ab2673efd2","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:28:57.006818Z","signature_b64":"QWyBzi38Erai4BXXqO2CHyQ0v+Q2z29jr76J9we9p9eYlohH/TCobeTFpMjB2seUOTvZ3bpKewGK4itDKrMXDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e7cdb52ff4f90934c9575b60fc7d9f18b123ed8994f54f07ffaf22ab2673efd2","last_reissued_at":"2026-05-18T00:28:57.006451Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:28:57.006451Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1606.05221","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":"2026-05-18T00:28:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SwOYhO5CdDJ0yPJrJfJrlXCl+bYajWsQBVs5dnS+2NDeOyaSZcZXKJhjwH1rd/7cOEIoPx5g9GmUZr0uEY9wCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T13:49:04.439806Z"},"content_sha256":"d595677173bce148276b742299ed6af28905d4521f4a2680699c23c74800963b","schema_version":"1.0","event_id":"sha256:d595677173bce148276b742299ed6af28905d4521f4a2680699c23c74800963b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:47G3KL7U7EETJSKXLNQPY7M7DC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"On the Effective Field Theory of Heterotic Vacua","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Jock McOrist","submitted_at":"2016-06-16T15:20:07Z","abstract_excerpt":"The effective field theory of heterotic vacua that realise $\\mathbb{R}^{3,1}$ preserving $\\mathcal{N} =1$ supersymmetry are studied. The vacua in question admit large radius limits taking the form $\\mathbb{R}^{3,1}\\times {X}$ , with ${X}$ a smooth three-fold with vanishing first Chern class and a stable holomorphic gauge bundle $\\mathcal{E}$. In a previous paper we calculated the kinetic terms for moduli, deducing the moduli metric and Kahler potential. In this paper, we compute the remaining couplings in the effective field theory, correct to first order in alpha prime. In particular, we comp"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1606.05221","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":"2026-05-18T00:28:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"38mqGCTckPScZO1KOhq5lwYEG/+Fqes1UuRpYAz9csUJ/DZzOupsqrcXomvtVroqL4vPCDQfJfRisAoOgbCAAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T13:49:04.440530Z"},"content_sha256":"7a103f4890185fb8fba5a532893c5d0ebdd49b856aed42bea217a8e5b86b87ab","schema_version":"1.0","event_id":"sha256:7a103f4890185fb8fba5a532893c5d0ebdd49b856aed42bea217a8e5b86b87ab"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/47G3KL7U7EETJSKXLNQPY7M7DC/bundle.json","state_url":"https://pith.science/pith/47G3KL7U7EETJSKXLNQPY7M7DC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/47G3KL7U7EETJSKXLNQPY7M7DC/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":"2026-06-07T13:49:04Z","links":{"resolver":"https://pith.science/pith/47G3KL7U7EETJSKXLNQPY7M7DC","bundle":"https://pith.science/pith/47G3KL7U7EETJSKXLNQPY7M7DC/bundle.json","state":"https://pith.science/pith/47G3KL7U7EETJSKXLNQPY7M7DC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/47G3KL7U7EETJSKXLNQPY7M7DC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:47G3KL7U7EETJSKXLNQPY7M7DC","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":"245d5f6d9919dfaa3c7e5800c893088e240cb77313779516e8099f14ec2fd107","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-06-16T15:20:07Z","title_canon_sha256":"6586f2b3003bcd381845d091985b211a7a3ca11d9e9bb6e4623ac39a6956886b"},"schema_version":"1.0","source":{"id":"1606.05221","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1606.05221","created_at":"2026-05-18T00:28:57Z"},{"alias_kind":"arxiv_version","alias_value":"1606.05221v2","created_at":"2026-05-18T00:28:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1606.05221","created_at":"2026-05-18T00:28:57Z"},{"alias_kind":"pith_short_12","alias_value":"47G3KL7U7EET","created_at":"2026-05-18T12:29:58Z"},{"alias_kind":"pith_short_16","alias_value":"47G3KL7U7EETJSKX","created_at":"2026-05-18T12:29:58Z"},{"alias_kind":"pith_short_8","alias_value":"47G3KL7U","created_at":"2026-05-18T12:29:58Z"}],"graph_snapshots":[{"event_id":"sha256:7a103f4890185fb8fba5a532893c5d0ebdd49b856aed42bea217a8e5b86b87ab","target":"graph","created_at":"2026-05-18T00:28:57Z","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 effective field theory of heterotic vacua that realise $\\mathbb{R}^{3,1}$ preserving $\\mathcal{N} =1$ supersymmetry are studied. The vacua in question admit large radius limits taking the form $\\mathbb{R}^{3,1}\\times {X}$ , with ${X}$ a smooth three-fold with vanishing first Chern class and a stable holomorphic gauge bundle $\\mathcal{E}$. In a previous paper we calculated the kinetic terms for moduli, deducing the moduli metric and Kahler potential. In this paper, we compute the remaining couplings in the effective field theory, correct to first order in alpha prime. In particular, we comp","authors_text":"Jock McOrist","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-06-16T15:20:07Z","title":"On the Effective Field Theory of Heterotic Vacua"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1606.05221","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:d595677173bce148276b742299ed6af28905d4521f4a2680699c23c74800963b","target":"record","created_at":"2026-05-18T00:28:57Z","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":"245d5f6d9919dfaa3c7e5800c893088e240cb77313779516e8099f14ec2fd107","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-06-16T15:20:07Z","title_canon_sha256":"6586f2b3003bcd381845d091985b211a7a3ca11d9e9bb6e4623ac39a6956886b"},"schema_version":"1.0","source":{"id":"1606.05221","kind":"arxiv","version":2}},"canonical_sha256":"e7cdb52ff4f90934c9575b60fc7d9f18b123ed8994f54f07ffaf22ab2673efd2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e7cdb52ff4f90934c9575b60fc7d9f18b123ed8994f54f07ffaf22ab2673efd2","first_computed_at":"2026-05-18T00:28:57.006451Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:28:57.006451Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"QWyBzi38Erai4BXXqO2CHyQ0v+Q2z29jr76J9we9p9eYlohH/TCobeTFpMjB2seUOTvZ3bpKewGK4itDKrMXDA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:28:57.006818Z","signed_message":"canonical_sha256_bytes"},"source_id":"1606.05221","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d595677173bce148276b742299ed6af28905d4521f4a2680699c23c74800963b","sha256:7a103f4890185fb8fba5a532893c5d0ebdd49b856aed42bea217a8e5b86b87ab"],"state_sha256":"0b9340d195aa9c7754ecf3b58fa4282e5aa60ecb0a2c3db0e2aad1b104f91512"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rEdVwm4QoMREmq172hfI55gnsHLR/OZGSN/zRho/IrAggri9ohL9ZLWiVVziS4A6FLPiV//p7tvVZxkTqfXTBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-07T13:49:04.444062Z","bundle_sha256":"cae2b4f3c6a5f5881aa2983c2d632f7bdb540018ff7ef278764dc0f81c2fb52e"}}