{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:KC3ENBI3X4AM2HDEBTP7YYOGAU","short_pith_number":"pith:KC3ENBI3","canonical_record":{"source":{"id":"1702.06289","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-02-21T08:01:46Z","cross_cats_sorted":[],"title_canon_sha256":"b5aef107502b39a9a7a981969c8822a30638f1c2a79b7c8b432f95a03fbecd03","abstract_canon_sha256":"8151b2cf4ca54ae6018f01150d659bfad0fb095eff100ccde243dfc3d14e8979"},"schema_version":"1.0"},"canonical_sha256":"50b646851bbf00cd1c640cdffc61c60502966d6aa09f82dff26851fe77381b9e","source":{"kind":"arxiv","id":"1702.06289","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1702.06289","created_at":"2026-05-18T00:26:01Z"},{"alias_kind":"arxiv_version","alias_value":"1702.06289v1","created_at":"2026-05-18T00:26:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.06289","created_at":"2026-05-18T00:26:01Z"},{"alias_kind":"pith_short_12","alias_value":"KC3ENBI3X4AM","created_at":"2026-05-18T12:31:24Z"},{"alias_kind":"pith_short_16","alias_value":"KC3ENBI3X4AM2HDE","created_at":"2026-05-18T12:31:24Z"},{"alias_kind":"pith_short_8","alias_value":"KC3ENBI3","created_at":"2026-05-18T12:31:24Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:KC3ENBI3X4AM2HDEBTP7YYOGAU","target":"record","payload":{"canonical_record":{"source":{"id":"1702.06289","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-02-21T08:01:46Z","cross_cats_sorted":[],"title_canon_sha256":"b5aef107502b39a9a7a981969c8822a30638f1c2a79b7c8b432f95a03fbecd03","abstract_canon_sha256":"8151b2cf4ca54ae6018f01150d659bfad0fb095eff100ccde243dfc3d14e8979"},"schema_version":"1.0"},"canonical_sha256":"50b646851bbf00cd1c640cdffc61c60502966d6aa09f82dff26851fe77381b9e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:26:01.124478Z","signature_b64":"HW5cm40hyotBHtObPnTEEh05v39LuwZBvFOuEMP2x8I0MdNpJRbq1jAnG42VGebmlnejOo+US7zunqbrhpJ9BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"50b646851bbf00cd1c640cdffc61c60502966d6aa09f82dff26851fe77381b9e","last_reissued_at":"2026-05-18T00:26:01.123787Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:26:01.123787Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1702.06289","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":"2026-05-18T00:26:01Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GpuOUmjXhrlgwe8Q+PeaNq9O9yk8q1Rq9jLnPVq76UH9Cgc52PLe2o06I1cW11Z8Cp8A9zfCgjTrG8hHRan7Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T15:00:46.488788Z"},"content_sha256":"da5d053aa615bff51cd5a7074776ff5436ae6844a8958f2bd1acce1603b48d19","schema_version":"1.0","event_id":"sha256:da5d053aa615bff51cd5a7074776ff5436ae6844a8958f2bd1acce1603b48d19"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:KC3ENBI3X4AM2HDEBTP7YYOGAU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Non-perturbative determination of the $\\Lambda$-parameter in the pure SU(3) gauge theory from the twisted gradient flow coupling","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Ayaka Nakamura, Issaku Kanamori, Ken-Ichi Ishikawa, Masanori Okawa, Ryoichiro Ueno, Yuko Murakami","submitted_at":"2017-02-21T08:01:46Z","abstract_excerpt":"We evaluate the $\\Lambda$-parameter in the $\\overline{\\mathrm{MS}}$ scheme for the pure SU(3) gauge theory with the twisted gradient flow (TGF) method. A running coupling constant $g_{\\mathrm{TGF}}^2(1/L)$ is defined in a finite volume box with size of $L^4$ with the twisted boundary condition. This defines the TGF scheme. Using the step scaling method for the TGF coupling with lattice simulations, we can evaluate the $\\Lambda$-parameter non-perturbatively in the TGF scheme. In this paper we determine the dimensionless ratios, $\\Lambda_{\\mathrm{TGF}}/\\sqrt{\\sigma}$ and $r_{0}\\Lambda_{\\mathrm{T"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.06289","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":"2026-05-18T00:26:01Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PsKJv4JGvbWxzgSSUN9KKMypKh2xGxDtHN+CT9TIxWtddO6YqEU5xsfed13UT1W5RfmWWKFbdEYUnW0EM3Z1CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T15:00:46.489344Z"},"content_sha256":"e5c01ef7685d80f953830aebbd6e073c7385a0fcc07535ac018ad1d10c0223c1","schema_version":"1.0","event_id":"sha256:e5c01ef7685d80f953830aebbd6e073c7385a0fcc07535ac018ad1d10c0223c1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KC3ENBI3X4AM2HDEBTP7YYOGAU/bundle.json","state_url":"https://pith.science/pith/KC3ENBI3X4AM2HDEBTP7YYOGAU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KC3ENBI3X4AM2HDEBTP7YYOGAU/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":"2026-05-26T15:00:46Z","links":{"resolver":"https://pith.science/pith/KC3ENBI3X4AM2HDEBTP7YYOGAU","bundle":"https://pith.science/pith/KC3ENBI3X4AM2HDEBTP7YYOGAU/bundle.json","state":"https://pith.science/pith/KC3ENBI3X4AM2HDEBTP7YYOGAU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KC3ENBI3X4AM2HDEBTP7YYOGAU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:KC3ENBI3X4AM2HDEBTP7YYOGAU","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":"8151b2cf4ca54ae6018f01150d659bfad0fb095eff100ccde243dfc3d14e8979","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-02-21T08:01:46Z","title_canon_sha256":"b5aef107502b39a9a7a981969c8822a30638f1c2a79b7c8b432f95a03fbecd03"},"schema_version":"1.0","source":{"id":"1702.06289","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1702.06289","created_at":"2026-05-18T00:26:01Z"},{"alias_kind":"arxiv_version","alias_value":"1702.06289v1","created_at":"2026-05-18T00:26:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.06289","created_at":"2026-05-18T00:26:01Z"},{"alias_kind":"pith_short_12","alias_value":"KC3ENBI3X4AM","created_at":"2026-05-18T12:31:24Z"},{"alias_kind":"pith_short_16","alias_value":"KC3ENBI3X4AM2HDE","created_at":"2026-05-18T12:31:24Z"},{"alias_kind":"pith_short_8","alias_value":"KC3ENBI3","created_at":"2026-05-18T12:31:24Z"}],"graph_snapshots":[{"event_id":"sha256:e5c01ef7685d80f953830aebbd6e073c7385a0fcc07535ac018ad1d10c0223c1","target":"graph","created_at":"2026-05-18T00:26:01Z","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":"We evaluate the $\\Lambda$-parameter in the $\\overline{\\mathrm{MS}}$ scheme for the pure SU(3) gauge theory with the twisted gradient flow (TGF) method. A running coupling constant $g_{\\mathrm{TGF}}^2(1/L)$ is defined in a finite volume box with size of $L^4$ with the twisted boundary condition. This defines the TGF scheme. Using the step scaling method for the TGF coupling with lattice simulations, we can evaluate the $\\Lambda$-parameter non-perturbatively in the TGF scheme. In this paper we determine the dimensionless ratios, $\\Lambda_{\\mathrm{TGF}}/\\sqrt{\\sigma}$ and $r_{0}\\Lambda_{\\mathrm{T","authors_text":"Ayaka Nakamura, Issaku Kanamori, Ken-Ichi Ishikawa, Masanori Okawa, Ryoichiro Ueno, Yuko Murakami","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-02-21T08:01:46Z","title":"Non-perturbative determination of the $\\Lambda$-parameter in the pure SU(3) gauge theory from the twisted gradient flow coupling"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.06289","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:da5d053aa615bff51cd5a7074776ff5436ae6844a8958f2bd1acce1603b48d19","target":"record","created_at":"2026-05-18T00:26:01Z","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":"8151b2cf4ca54ae6018f01150d659bfad0fb095eff100ccde243dfc3d14e8979","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-02-21T08:01:46Z","title_canon_sha256":"b5aef107502b39a9a7a981969c8822a30638f1c2a79b7c8b432f95a03fbecd03"},"schema_version":"1.0","source":{"id":"1702.06289","kind":"arxiv","version":1}},"canonical_sha256":"50b646851bbf00cd1c640cdffc61c60502966d6aa09f82dff26851fe77381b9e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"50b646851bbf00cd1c640cdffc61c60502966d6aa09f82dff26851fe77381b9e","first_computed_at":"2026-05-18T00:26:01.123787Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:26:01.123787Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"HW5cm40hyotBHtObPnTEEh05v39LuwZBvFOuEMP2x8I0MdNpJRbq1jAnG42VGebmlnejOo+US7zunqbrhpJ9BA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:26:01.124478Z","signed_message":"canonical_sha256_bytes"},"source_id":"1702.06289","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:da5d053aa615bff51cd5a7074776ff5436ae6844a8958f2bd1acce1603b48d19","sha256:e5c01ef7685d80f953830aebbd6e073c7385a0fcc07535ac018ad1d10c0223c1"],"state_sha256":"ce3217ad5684430594c53a3e9e6cd67b426b5e522079616bed999491889f85e0"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dGvIAVjonIKh5cf0tQZZ24wHfWgEuqYGW3jfrS5tr54qLJJZvVEvMTMV/Gz3C+h79P7oaKZFGArzq//BDVQzDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T15:00:46.491932Z","bundle_sha256":"845f7f74f8d39180c52147d64585d10bb301c65e4497082c30117e49ce22e7bd"}}