{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:VP4ION2OEFJUOM6F2X5KT75P4Z","short_pith_number":"pith:VP4ION2O","schema_version":"1.0","canonical_sha256":"abf887374e21534733c5d5faa9ffafe64724b4803dbfbfe08e7f8352f79be152","source":{"kind":"arxiv","id":"1410.3466","version":1},"attestation_state":"computed","paper":{"title":"Nearly-linear light cones in long-range interacting quantum systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","physics.atom-ph"],"primary_cat":"quant-ph","authors_text":"Alexey V. Gorshkov, Charles W. Clark, Michael Foss-Feig, Zhe-Xuan Gong","submitted_at":"2014-10-13T20:00:00Z","abstract_excerpt":"In non-relativistic quantum theories with short-range Hamiltonians, a velocity $v$ can be chosen such that the influence of any local perturbation is approximately confined to within a distance $r$ until a time $t \\sim r/v$, thereby defining a linear light cone and giving rise to an emergent notion of locality. In systems with power-law ($1/r^{\\alpha}$) interactions, when $\\alpha$ exceeds the dimension $D$, an analogous bound confines influences to within a distance $r$ only until a time $t\\sim(\\alpha/v)\\log r$, suggesting that the velocity, as calculated from the slope of the light cone, may "},"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":"1410.3466","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2014-10-13T20:00:00Z","cross_cats_sorted":["cond-mat.quant-gas","physics.atom-ph"],"title_canon_sha256":"ce364be1d732ff1ac28ed52c5fc46bbe4edd6ab9eb0a0749f88da2faac53913d","abstract_canon_sha256":"a8a9418fc71fd545792c6b409dd364f983fac8c9ffa607dadfbdfd4a80be98ed"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:18:21.828934Z","signature_b64":"dBu81t47NEXawb8tqFGS4UTArSsXqpgiCtts7sbZ705cOF0h5aayjsAstabHoXJiYrMlwW6CxWBjhTXE95L0CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"abf887374e21534733c5d5faa9ffafe64724b4803dbfbfe08e7f8352f79be152","last_reissued_at":"2026-05-18T02:18:21.828331Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:18:21.828331Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nearly-linear light cones in long-range interacting quantum systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","physics.atom-ph"],"primary_cat":"quant-ph","authors_text":"Alexey V. Gorshkov, Charles W. Clark, Michael Foss-Feig, Zhe-Xuan Gong","submitted_at":"2014-10-13T20:00:00Z","abstract_excerpt":"In non-relativistic quantum theories with short-range Hamiltonians, a velocity $v$ can be chosen such that the influence of any local perturbation is approximately confined to within a distance $r$ until a time $t \\sim r/v$, thereby defining a linear light cone and giving rise to an emergent notion of locality. In systems with power-law ($1/r^{\\alpha}$) interactions, when $\\alpha$ exceeds the dimension $D$, an analogous bound confines influences to within a distance $r$ only until a time $t\\sim(\\alpha/v)\\log r$, suggesting that the velocity, as calculated from the slope of the light cone, may "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.3466","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1410.3466","created_at":"2026-05-18T02:18:21.828419+00:00"},{"alias_kind":"arxiv_version","alias_value":"1410.3466v1","created_at":"2026-05-18T02:18:21.828419+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.3466","created_at":"2026-05-18T02:18:21.828419+00:00"},{"alias_kind":"pith_short_12","alias_value":"VP4ION2OEFJU","created_at":"2026-05-18T12:28:54.890064+00:00"},{"alias_kind":"pith_short_16","alias_value":"VP4ION2OEFJUOM6F","created_at":"2026-05-18T12:28:54.890064+00:00"},{"alias_kind":"pith_short_8","alias_value":"VP4ION2O","created_at":"2026-05-18T12:28:54.890064+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/VP4ION2OEFJUOM6F2X5KT75P4Z","json":"https://pith.science/pith/VP4ION2OEFJUOM6F2X5KT75P4Z.json","graph_json":"https://pith.science/api/pith-number/VP4ION2OEFJUOM6F2X5KT75P4Z/graph.json","events_json":"https://pith.science/api/pith-number/VP4ION2OEFJUOM6F2X5KT75P4Z/events.json","paper":"https://pith.science/paper/VP4ION2O"},"agent_actions":{"view_html":"https://pith.science/pith/VP4ION2OEFJUOM6F2X5KT75P4Z","download_json":"https://pith.science/pith/VP4ION2OEFJUOM6F2X5KT75P4Z.json","view_paper":"https://pith.science/paper/VP4ION2O","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1410.3466&json=true","fetch_graph":"https://pith.science/api/pith-number/VP4ION2OEFJUOM6F2X5KT75P4Z/graph.json","fetch_events":"https://pith.science/api/pith-number/VP4ION2OEFJUOM6F2X5KT75P4Z/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VP4ION2OEFJUOM6F2X5KT75P4Z/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VP4ION2OEFJUOM6F2X5KT75P4Z/action/storage_attestation","attest_author":"https://pith.science/pith/VP4ION2OEFJUOM6F2X5KT75P4Z/action/author_attestation","sign_citation":"https://pith.science/pith/VP4ION2OEFJUOM6F2X5KT75P4Z/action/citation_signature","submit_replication":"https://pith.science/pith/VP4ION2OEFJUOM6F2X5KT75P4Z/action/replication_record"}},"created_at":"2026-05-18T02:18:21.828419+00:00","updated_at":"2026-05-18T02:18:21.828419+00:00"}