{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:6QTZCGUAYNWLMYGDA2OPXAVPTG","short_pith_number":"pith:6QTZCGUA","schema_version":"1.0","canonical_sha256":"f427911a80c36cb660c3069cfb82af99abb581353363105d14097bcb4eb0571a","source":{"kind":"arxiv","id":"1710.10960","version":2},"attestation_state":"computed","paper":{"title":"Tuning linear response dynamics near the Dirac points in the bosonic Mott insulator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"A. S. Sajna","submitted_at":"2017-10-30T14:15:42Z","abstract_excerpt":"Optical lattice systems offer the possibility of creating and tuning Dirac points which are present in the tight-binding lattice dispersions. For example, such a behavior can be achieved in the staggered flux lattice or honeycomb type of lattices. Here we focus on the strongly correlated bosonic dynamics in the vicinity of Dirac points. In particular, we investigate bosonic Mott insulator phase in which quasiparticle excitations have a simple particle-hole interpretation. We show that linear response dynamics around Dirac points, can be significantly engineered at least in two ways: by the typ"},"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":"1710.10960","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2017-10-30T14:15:42Z","cross_cats_sorted":[],"title_canon_sha256":"2b7c57c15e0774d2584f791923756a586c5046a675aa57213b92477f393d2048","abstract_canon_sha256":"9aa73cb4e64d4957f06ca5f18b7d9d42ffb990dd7822365c481a64f8df388e33"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:15:05.272444Z","signature_b64":"/X+6dqHUOs38I5YRdW1Cf+2NmeMLMfS12y3ckuI7Y/Sk3JSc3QO3+kDTwSbNQ/eTbVauzTo+EfmpkZTd8yM+CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f427911a80c36cb660c3069cfb82af99abb581353363105d14097bcb4eb0571a","last_reissued_at":"2026-05-18T00:15:05.271926Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:15:05.271926Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Tuning linear response dynamics near the Dirac points in the bosonic Mott insulator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"A. S. Sajna","submitted_at":"2017-10-30T14:15:42Z","abstract_excerpt":"Optical lattice systems offer the possibility of creating and tuning Dirac points which are present in the tight-binding lattice dispersions. For example, such a behavior can be achieved in the staggered flux lattice or honeycomb type of lattices. Here we focus on the strongly correlated bosonic dynamics in the vicinity of Dirac points. In particular, we investigate bosonic Mott insulator phase in which quasiparticle excitations have a simple particle-hole interpretation. We show that linear response dynamics around Dirac points, can be significantly engineered at least in two ways: by the typ"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.10960","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1710.10960","created_at":"2026-05-18T00:15:05.272010+00:00"},{"alias_kind":"arxiv_version","alias_value":"1710.10960v2","created_at":"2026-05-18T00:15:05.272010+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.10960","created_at":"2026-05-18T00:15:05.272010+00:00"},{"alias_kind":"pith_short_12","alias_value":"6QTZCGUAYNWL","created_at":"2026-05-18T12:31:03.183658+00:00"},{"alias_kind":"pith_short_16","alias_value":"6QTZCGUAYNWLMYGD","created_at":"2026-05-18T12:31:03.183658+00:00"},{"alias_kind":"pith_short_8","alias_value":"6QTZCGUA","created_at":"2026-05-18T12:31:03.183658+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6QTZCGUAYNWLMYGDA2OPXAVPTG","json":"https://pith.science/pith/6QTZCGUAYNWLMYGDA2OPXAVPTG.json","graph_json":"https://pith.science/api/pith-number/6QTZCGUAYNWLMYGDA2OPXAVPTG/graph.json","events_json":"https://pith.science/api/pith-number/6QTZCGUAYNWLMYGDA2OPXAVPTG/events.json","paper":"https://pith.science/paper/6QTZCGUA"},"agent_actions":{"view_html":"https://pith.science/pith/6QTZCGUAYNWLMYGDA2OPXAVPTG","download_json":"https://pith.science/pith/6QTZCGUAYNWLMYGDA2OPXAVPTG.json","view_paper":"https://pith.science/paper/6QTZCGUA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1710.10960&json=true","fetch_graph":"https://pith.science/api/pith-number/6QTZCGUAYNWLMYGDA2OPXAVPTG/graph.json","fetch_events":"https://pith.science/api/pith-number/6QTZCGUAYNWLMYGDA2OPXAVPTG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6QTZCGUAYNWLMYGDA2OPXAVPTG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6QTZCGUAYNWLMYGDA2OPXAVPTG/action/storage_attestation","attest_author":"https://pith.science/pith/6QTZCGUAYNWLMYGDA2OPXAVPTG/action/author_attestation","sign_citation":"https://pith.science/pith/6QTZCGUAYNWLMYGDA2OPXAVPTG/action/citation_signature","submit_replication":"https://pith.science/pith/6QTZCGUAYNWLMYGDA2OPXAVPTG/action/replication_record"}},"created_at":"2026-05-18T00:15:05.272010+00:00","updated_at":"2026-05-18T00:15:05.272010+00:00"}