{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:XWCKSZQGULO4BMMZCFEB3JNZCM","short_pith_number":"pith:XWCKSZQG","canonical_record":{"source":{"id":"1411.1859","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-11-07T09:07:11Z","cross_cats_sorted":[],"title_canon_sha256":"e44506975bbd633d99ea2147b96a7403d364374ef05cfb0c7aa8eb9d08b3a172","abstract_canon_sha256":"0530671a760f065b5a759d3151f337741144112040181d0d36725a1f9a3d5bd9"},"schema_version":"1.0"},"canonical_sha256":"bd84a96606a2ddc0b19911481da5b9131ebc6936c501420651c1474c7c943d10","source":{"kind":"arxiv","id":"1411.1859","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1411.1859","created_at":"2026-05-18T01:41:34Z"},{"alias_kind":"arxiv_version","alias_value":"1411.1859v1","created_at":"2026-05-18T01:41:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.1859","created_at":"2026-05-18T01:41:34Z"},{"alias_kind":"pith_short_12","alias_value":"XWCKSZQGULO4","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_16","alias_value":"XWCKSZQGULO4BMMZ","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_8","alias_value":"XWCKSZQG","created_at":"2026-05-18T12:28:57Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:XWCKSZQGULO4BMMZCFEB3JNZCM","target":"record","payload":{"canonical_record":{"source":{"id":"1411.1859","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-11-07T09:07:11Z","cross_cats_sorted":[],"title_canon_sha256":"e44506975bbd633d99ea2147b96a7403d364374ef05cfb0c7aa8eb9d08b3a172","abstract_canon_sha256":"0530671a760f065b5a759d3151f337741144112040181d0d36725a1f9a3d5bd9"},"schema_version":"1.0"},"canonical_sha256":"bd84a96606a2ddc0b19911481da5b9131ebc6936c501420651c1474c7c943d10","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:41:34.116886Z","signature_b64":"WOPqvs0bYYs4MMusd12Tmxq0MJRs8vSrOnzDO0bmY6rWMXYVYAUcg8lFePZUOa2Zfik4ze4EjRJF9QAmulMeDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bd84a96606a2ddc0b19911481da5b9131ebc6936c501420651c1474c7c943d10","last_reissued_at":"2026-05-18T01:41:34.116261Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:41:34.116261Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1411.1859","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":"2026-05-18T01:41:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1NuLpiaMEVcQuodmXnWW2n3kzfmfALeTe/vWsoZHhENTnYB/0UDm/n2pWSZj7azwm4Dnxdk0/dYCXH7qPdKcBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T21:47:36.646308Z"},"content_sha256":"3ea609ff78544586de5fda1bd2cfb3933a488348831afe078e9507888801379d","schema_version":"1.0","event_id":"sha256:3ea609ff78544586de5fda1bd2cfb3933a488348831afe078e9507888801379d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:XWCKSZQGULO4BMMZCFEB3JNZCM","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Bound states on the lattice with partially twisted boundary conditions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A. Rusetsky, D. Agadjanov, F.-K. Guo, G. R\\'ios","submitted_at":"2014-11-07T09:07:11Z","abstract_excerpt":"We propose a method to study the nature of exotic hadrons by determining the wave function renormalization constant $Z$ from lattice simulations. It is shown that, instead of studying the volume-dependence of the spectrum, one may investigate the dependence of the spectrum on the twisting angle, imposing twisted boundary conditions on the fermion fields on the lattice. In certain cases, e.g., the case of the $DK$ bound state which is addressed in detail, it is demonstrated that the partial twisting is equivalent to the full twisting up to exponentially small corrections."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.1859","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":"2026-05-18T01:41:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FRugAanSwMf0kSKdcfjC1UlbWaS5ntIEYY5/nQdT0myCRueoUNIJWWpGNjiU+wwitKHFCikd3y4QmbF3CwtDCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T21:47:36.647030Z"},"content_sha256":"69375a53b8e20f72b92c6a61e7fd3462015ef3744231f9dd7f97a8a099cc0504","schema_version":"1.0","event_id":"sha256:69375a53b8e20f72b92c6a61e7fd3462015ef3744231f9dd7f97a8a099cc0504"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/XWCKSZQGULO4BMMZCFEB3JNZCM/bundle.json","state_url":"https://pith.science/pith/XWCKSZQGULO4BMMZCFEB3JNZCM/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/XWCKSZQGULO4BMMZCFEB3JNZCM/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":"2026-05-28T21:47:36Z","links":{"resolver":"https://pith.science/pith/XWCKSZQGULO4BMMZCFEB3JNZCM","bundle":"https://pith.science/pith/XWCKSZQGULO4BMMZCFEB3JNZCM/bundle.json","state":"https://pith.science/pith/XWCKSZQGULO4BMMZCFEB3JNZCM/state.json","well_known_bundle":"https://pith.science/.well-known/pith/XWCKSZQGULO4BMMZCFEB3JNZCM/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:XWCKSZQGULO4BMMZCFEB3JNZCM","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":"0530671a760f065b5a759d3151f337741144112040181d0d36725a1f9a3d5bd9","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-11-07T09:07:11Z","title_canon_sha256":"e44506975bbd633d99ea2147b96a7403d364374ef05cfb0c7aa8eb9d08b3a172"},"schema_version":"1.0","source":{"id":"1411.1859","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1411.1859","created_at":"2026-05-18T01:41:34Z"},{"alias_kind":"arxiv_version","alias_value":"1411.1859v1","created_at":"2026-05-18T01:41:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.1859","created_at":"2026-05-18T01:41:34Z"},{"alias_kind":"pith_short_12","alias_value":"XWCKSZQGULO4","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_16","alias_value":"XWCKSZQGULO4BMMZ","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_8","alias_value":"XWCKSZQG","created_at":"2026-05-18T12:28:57Z"}],"graph_snapshots":[{"event_id":"sha256:69375a53b8e20f72b92c6a61e7fd3462015ef3744231f9dd7f97a8a099cc0504","target":"graph","created_at":"2026-05-18T01:41:34Z","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 propose a method to study the nature of exotic hadrons by determining the wave function renormalization constant $Z$ from lattice simulations. It is shown that, instead of studying the volume-dependence of the spectrum, one may investigate the dependence of the spectrum on the twisting angle, imposing twisted boundary conditions on the fermion fields on the lattice. In certain cases, e.g., the case of the $DK$ bound state which is addressed in detail, it is demonstrated that the partial twisting is equivalent to the full twisting up to exponentially small corrections.","authors_text":"A. Rusetsky, D. Agadjanov, F.-K. Guo, G. R\\'ios","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-11-07T09:07:11Z","title":"Bound states on the lattice with partially twisted boundary conditions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.1859","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":"sha256:3ea609ff78544586de5fda1bd2cfb3933a488348831afe078e9507888801379d","target":"record","created_at":"2026-05-18T01:41:34Z","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":"0530671a760f065b5a759d3151f337741144112040181d0d36725a1f9a3d5bd9","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-11-07T09:07:11Z","title_canon_sha256":"e44506975bbd633d99ea2147b96a7403d364374ef05cfb0c7aa8eb9d08b3a172"},"schema_version":"1.0","source":{"id":"1411.1859","kind":"arxiv","version":1}},"canonical_sha256":"bd84a96606a2ddc0b19911481da5b9131ebc6936c501420651c1474c7c943d10","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"bd84a96606a2ddc0b19911481da5b9131ebc6936c501420651c1474c7c943d10","first_computed_at":"2026-05-18T01:41:34.116261Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:41:34.116261Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"WOPqvs0bYYs4MMusd12Tmxq0MJRs8vSrOnzDO0bmY6rWMXYVYAUcg8lFePZUOa2Zfik4ze4EjRJF9QAmulMeDA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:41:34.116886Z","signed_message":"canonical_sha256_bytes"},"source_id":"1411.1859","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3ea609ff78544586de5fda1bd2cfb3933a488348831afe078e9507888801379d","sha256:69375a53b8e20f72b92c6a61e7fd3462015ef3744231f9dd7f97a8a099cc0504"],"state_sha256":"54a0a61b8d523f4839b3b79720c6d102cb46375d6cef89a0cd03c4c9efb14816"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xU+L7x7qN1NQbKyV3J/tlP6tG0MXO393Vif5WOt/HkWCZ5mjyp/lVtBxnvrn89nOX5GIknTr/CeFV/dEyIBABA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T21:47:36.650933Z","bundle_sha256":"7c26dd26da37e74fe1bff9ac03b948284407d11fc1d749b50a9dda14ef826ff6"}}