{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:V2CWKTLSULNP4AWSXDSPCPZGD7","short_pith_number":"pith:V2CWKTLS","schema_version":"1.0","canonical_sha256":"ae85654d72a2dafe02d2b8e4f13f261fdb4556891c09be12e48054853f57a051","source":{"kind":"arxiv","id":"1308.2217","version":3},"attestation_state":"computed","paper":{"title":"Exact results for boundaries and domain walls in 2d supersymmetric theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Daigo Honda, Takuya Okuda","submitted_at":"2013-08-09T19:47:56Z","abstract_excerpt":"We apply supersymmetric localization to N=(2,2) gauged linear sigma models on a hemisphere, with boundary conditions, i.e., D-branes, preserving B-type supersymmetries. We explain how to compute the hemisphere partition function for each object in the derived category of equivariant coherent sheaves, and argue that it depends only on its K theory class. The hemisphere partition function computes exactly the central charge of the D-brane, completing the well-known formula obtained by an anomaly inflow argument. We also formulate supersymmetric domain walls as D-branes in the product of two theo"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1308.2217","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-08-09T19:47:56Z","cross_cats_sorted":[],"title_canon_sha256":"e9cde40ef20676a8177d7a30c079316cf7c2592b5703fc0ec0aef9b17cc33119","abstract_canon_sha256":"7448e5926ce8ffd6a1f5e0a3e50b960dc18af6e6f83aca31c17ccf98e7a5db06"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:34:51.261268Z","signature_b64":"ao+V5CnA4ymCmhav/YvgZA7IrzUOXei402e6CpGbiydDGG2yjAsLtkW2W9WSNFfe0JfKwUFteKZGFSsE/vpbCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ae85654d72a2dafe02d2b8e4f13f261fdb4556891c09be12e48054853f57a051","last_reissued_at":"2026-05-18T01:34:51.260863Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:34:51.260863Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Exact results for boundaries and domain walls in 2d supersymmetric theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Daigo Honda, Takuya Okuda","submitted_at":"2013-08-09T19:47:56Z","abstract_excerpt":"We apply supersymmetric localization to N=(2,2) gauged linear sigma models on a hemisphere, with boundary conditions, i.e., D-branes, preserving B-type supersymmetries. We explain how to compute the hemisphere partition function for each object in the derived category of equivariant coherent sheaves, and argue that it depends only on its K theory class. The hemisphere partition function computes exactly the central charge of the D-brane, completing the well-known formula obtained by an anomaly inflow argument. We also formulate supersymmetric domain walls as D-branes in the product of two theo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1308.2217","kind":"arxiv","version":3},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1308.2217","created_at":"2026-05-18T01:34:51.260926+00:00"},{"alias_kind":"arxiv_version","alias_value":"1308.2217v3","created_at":"2026-05-18T01:34:51.260926+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1308.2217","created_at":"2026-05-18T01:34:51.260926+00:00"},{"alias_kind":"pith_short_12","alias_value":"V2CWKTLSULNP","created_at":"2026-05-18T12:28:02.375192+00:00"},{"alias_kind":"pith_short_16","alias_value":"V2CWKTLSULNP4AWS","created_at":"2026-05-18T12:28:02.375192+00:00"},{"alias_kind":"pith_short_8","alias_value":"V2CWKTLS","created_at":"2026-05-18T12:28:02.375192+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2605.18514","citing_title":"Monodromy of Calabi-Yau threefold flops via grade restriction rule and their quantum Kahler moduli","ref_index":32,"is_internal_anchor":true},{"citing_arxiv_id":"2509.25976","citing_title":"Hyperfunctions in $A$-model Localization","ref_index":21,"is_internal_anchor":true},{"citing_arxiv_id":"2604.17975","citing_title":"Localisation of $\\mathcal{N} = (2,2)$ theories on spindles of both twists","ref_index":11,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/V2CWKTLSULNP4AWSXDSPCPZGD7","json":"https://pith.science/pith/V2CWKTLSULNP4AWSXDSPCPZGD7.json","graph_json":"https://pith.science/api/pith-number/V2CWKTLSULNP4AWSXDSPCPZGD7/graph.json","events_json":"https://pith.science/api/pith-number/V2CWKTLSULNP4AWSXDSPCPZGD7/events.json","paper":"https://pith.science/paper/V2CWKTLS"},"agent_actions":{"view_html":"https://pith.science/pith/V2CWKTLSULNP4AWSXDSPCPZGD7","download_json":"https://pith.science/pith/V2CWKTLSULNP4AWSXDSPCPZGD7.json","view_paper":"https://pith.science/paper/V2CWKTLS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1308.2217&json=true","fetch_graph":"https://pith.science/api/pith-number/V2CWKTLSULNP4AWSXDSPCPZGD7/graph.json","fetch_events":"https://pith.science/api/pith-number/V2CWKTLSULNP4AWSXDSPCPZGD7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/V2CWKTLSULNP4AWSXDSPCPZGD7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/V2CWKTLSULNP4AWSXDSPCPZGD7/action/storage_attestation","attest_author":"https://pith.science/pith/V2CWKTLSULNP4AWSXDSPCPZGD7/action/author_attestation","sign_citation":"https://pith.science/pith/V2CWKTLSULNP4AWSXDSPCPZGD7/action/citation_signature","submit_replication":"https://pith.science/pith/V2CWKTLSULNP4AWSXDSPCPZGD7/action/replication_record"}},"created_at":"2026-05-18T01:34:51.260926+00:00","updated_at":"2026-05-18T01:34:51.260926+00:00"}