{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1994:67Z5R4ANFMVTXEAX5CLQVIJNLN","short_pith_number":"pith:67Z5R4AN","schema_version":"1.0","canonical_sha256":"f7f3d8f00d2b2b3b9017e8970aa12d5b72255422906a451bffbfe22d7ddcf102","source":{"kind":"arxiv","id":"hep-th/9410143","version":1},"attestation_state":"computed","paper":{"title":"Hamiltonian BRST Quantization of the Conformal String","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"B.Sundborg, H.Gustafsson, P.Saltsidis, R.v.Unge, U.Lindstr\\\"om","submitted_at":"1994-10-19T17:44:12Z","abstract_excerpt":"We present a new formulation of the tensionless string ($T= 0$) where the space-time conformal symmetry is manifest. Using a Hamiltonian BRST scheme we quantize this {\\em Conformal String} and find that it has critical dimension $D=2$. This is in keeping with our classical result that the model describes massless particles in this dimension. It is also consistent with our previous results which indicate that quantized conformally symmetric tensionless strings describe a topological phase away {}from $D=2$. We reach our result by demanding nilpotency of the BRST charge and consistency with the "},"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":"hep-th/9410143","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1994-10-19T17:44:12Z","cross_cats_sorted":[],"title_canon_sha256":"8a5e873b0e5465626da3667f3855787e4e21c212eb7571bdbfa8b93ab5e2e4c1","abstract_canon_sha256":"9998baa6ba42b3bc4fbafb4fe885f44a9444698f48c8e70a60cf7ba6edd3df56"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:57:52.329658Z","signature_b64":"cueeFjGgn9ZhIX4h706N12tLYdlcK9FGq8NYnj1odJkqO1x+6OJactcRpINvI94UL/ENXIfhKZrOPzqsE3mFDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f7f3d8f00d2b2b3b9017e8970aa12d5b72255422906a451bffbfe22d7ddcf102","last_reissued_at":"2026-07-04T15:57:52.329228Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:57:52.329228Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hamiltonian BRST Quantization of the Conformal String","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"B.Sundborg, H.Gustafsson, P.Saltsidis, R.v.Unge, U.Lindstr\\\"om","submitted_at":"1994-10-19T17:44:12Z","abstract_excerpt":"We present a new formulation of the tensionless string ($T= 0$) where the space-time conformal symmetry is manifest. Using a Hamiltonian BRST scheme we quantize this {\\em Conformal String} and find that it has critical dimension $D=2$. This is in keeping with our classical result that the model describes massless particles in this dimension. It is also consistent with our previous results which indicate that quantized conformally symmetric tensionless strings describe a topological phase away {}from $D=2$. We reach our result by demanding nilpotency of the BRST charge and consistency with the "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9410143","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/9410143/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"hep-th/9410143","created_at":"2026-07-04T15:57:52.329300+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9410143v1","created_at":"2026-07-04T15:57:52.329300+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9410143","created_at":"2026-07-04T15:57:52.329300+00:00"},{"alias_kind":"pith_short_12","alias_value":"67Z5R4ANFMVT","created_at":"2026-07-04T15:57:52.329300+00:00"},{"alias_kind":"pith_short_16","alias_value":"67Z5R4ANFMVTXEAX","created_at":"2026-07-04T15:57:52.329300+00:00"},{"alias_kind":"pith_short_8","alias_value":"67Z5R4AN","created_at":"2026-07-04T15:57:52.329300+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":5,"sample":[{"citing_arxiv_id":"2606.04999","citing_title":"Path integral quantization of null bosonic strings with Carroll-Weyl ghosts","ref_index":10,"is_internal_anchor":true},{"citing_arxiv_id":"2605.26185","citing_title":"Symmetries of tensionless strings","ref_index":5,"is_internal_anchor":true},{"citing_arxiv_id":"2605.25817","citing_title":"Null Strings Gauged and Reloaded, I: Null Strings Have Carroll-Weyl Gauge Symmetry","ref_index":32,"is_internal_anchor":true},{"citing_arxiv_id":"2605.26822","citing_title":"Null Strings Gauged and Reloaded, II: Consistent Classical Treatment of the Null Strings","ref_index":11,"is_internal_anchor":true},{"citing_arxiv_id":"2606.22498","citing_title":"The conformal null string in $d+2$ and $d$ dimensions","ref_index":5,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/67Z5R4ANFMVTXEAX5CLQVIJNLN","json":"https://pith.science/pith/67Z5R4ANFMVTXEAX5CLQVIJNLN.json","graph_json":"https://pith.science/api/pith-number/67Z5R4ANFMVTXEAX5CLQVIJNLN/graph.json","events_json":"https://pith.science/api/pith-number/67Z5R4ANFMVTXEAX5CLQVIJNLN/events.json","paper":"https://pith.science/paper/67Z5R4AN"},"agent_actions":{"view_html":"https://pith.science/pith/67Z5R4ANFMVTXEAX5CLQVIJNLN","download_json":"https://pith.science/pith/67Z5R4ANFMVTXEAX5CLQVIJNLN.json","view_paper":"https://pith.science/paper/67Z5R4AN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9410143&json=true","fetch_graph":"https://pith.science/api/pith-number/67Z5R4ANFMVTXEAX5CLQVIJNLN/graph.json","fetch_events":"https://pith.science/api/pith-number/67Z5R4ANFMVTXEAX5CLQVIJNLN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/67Z5R4ANFMVTXEAX5CLQVIJNLN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/67Z5R4ANFMVTXEAX5CLQVIJNLN/action/storage_attestation","attest_author":"https://pith.science/pith/67Z5R4ANFMVTXEAX5CLQVIJNLN/action/author_attestation","sign_citation":"https://pith.science/pith/67Z5R4ANFMVTXEAX5CLQVIJNLN/action/citation_signature","submit_replication":"https://pith.science/pith/67Z5R4ANFMVTXEAX5CLQVIJNLN/action/replication_record"}},"created_at":"2026-07-04T15:57:52.329300+00:00","updated_at":"2026-07-04T15:57:52.329300+00:00"}