{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:WLSWKCFWUZPBENUS2NDGCFBXIE","short_pith_number":"pith:WLSWKCFW","schema_version":"1.0","canonical_sha256":"b2e56508b6a65e123692d34661143741290f01503aec170c6269dd98211288d8","source":{"kind":"arxiv","id":"2010.07942","version":2},"attestation_state":"computed","paper":{"title":"Near-Schr\\\"odinger dynamics at large charge","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Domenico Orlando, Susanne Reffert, Vito Pellizzani","submitted_at":"2020-10-15T18:00:01Z","abstract_excerpt":"In this note we discuss a non-relativistic system at large charge in a regime where Schr\\\"odinger symmetry is slightly broken by an explicit mass term for the dilaton field which non-linearly realizes non-relativistic scale invariance. To get there, we first develop the large-charge formalism from the linear sigma model perspective, including the harmonic trapping potential necessary for the non-relativistic state-operator correspondence. As a signature of the explicit breaking, we identify a $\\sqrt{Q}\\log{Q}$ term, which depending on the space dimension is either of the same order as the effe"},"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":"2010.07942","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2020-10-15T18:00:01Z","cross_cats_sorted":[],"title_canon_sha256":"9168c05ccd35786ea6d8cb4b233fd08bfbc5e9ebd954700e71f931b8697ed90c","abstract_canon_sha256":"4f3d8def31cb6439b7519cccf1fabf6cfd002ac3203701522f04b693b784c090"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:43:10.012197Z","signature_b64":"hkRdOJhcEC/7yPGg8UXG/irX9l8gDRbPZuGMf1YEMiAqdvGe10mWVpHeKywH5iT9sqKGR4KAsFV8XgbWbp+XAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b2e56508b6a65e123692d34661143741290f01503aec170c6269dd98211288d8","last_reissued_at":"2026-07-05T02:43:10.011810Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:43:10.011810Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Near-Schr\\\"odinger dynamics at large charge","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Domenico Orlando, Susanne Reffert, Vito Pellizzani","submitted_at":"2020-10-15T18:00:01Z","abstract_excerpt":"In this note we discuss a non-relativistic system at large charge in a regime where Schr\\\"odinger symmetry is slightly broken by an explicit mass term for the dilaton field which non-linearly realizes non-relativistic scale invariance. To get there, we first develop the large-charge formalism from the linear sigma model perspective, including the harmonic trapping potential necessary for the non-relativistic state-operator correspondence. As a signature of the explicit breaking, we identify a $\\sqrt{Q}\\log{Q}$ term, which depending on the space dimension is either of the same order as the effe"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2010.07942","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2010.07942/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":"2010.07942","created_at":"2026-07-05T02:43:10.011862+00:00"},{"alias_kind":"arxiv_version","alias_value":"2010.07942v2","created_at":"2026-07-05T02:43:10.011862+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2010.07942","created_at":"2026-07-05T02:43:10.011862+00:00"},{"alias_kind":"pith_short_12","alias_value":"WLSWKCFWUZPB","created_at":"2026-07-05T02:43:10.011862+00:00"},{"alias_kind":"pith_short_16","alias_value":"WLSWKCFWUZPBENUS","created_at":"2026-07-05T02:43:10.011862+00:00"},{"alias_kind":"pith_short_8","alias_value":"WLSWKCFW","created_at":"2026-07-05T02:43:10.011862+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.10505","citing_title":"Unnuclear matter at large-charge","ref_index":16,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WLSWKCFWUZPBENUS2NDGCFBXIE","json":"https://pith.science/pith/WLSWKCFWUZPBENUS2NDGCFBXIE.json","graph_json":"https://pith.science/api/pith-number/WLSWKCFWUZPBENUS2NDGCFBXIE/graph.json","events_json":"https://pith.science/api/pith-number/WLSWKCFWUZPBENUS2NDGCFBXIE/events.json","paper":"https://pith.science/paper/WLSWKCFW"},"agent_actions":{"view_html":"https://pith.science/pith/WLSWKCFWUZPBENUS2NDGCFBXIE","download_json":"https://pith.science/pith/WLSWKCFWUZPBENUS2NDGCFBXIE.json","view_paper":"https://pith.science/paper/WLSWKCFW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2010.07942&json=true","fetch_graph":"https://pith.science/api/pith-number/WLSWKCFWUZPBENUS2NDGCFBXIE/graph.json","fetch_events":"https://pith.science/api/pith-number/WLSWKCFWUZPBENUS2NDGCFBXIE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WLSWKCFWUZPBENUS2NDGCFBXIE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WLSWKCFWUZPBENUS2NDGCFBXIE/action/storage_attestation","attest_author":"https://pith.science/pith/WLSWKCFWUZPBENUS2NDGCFBXIE/action/author_attestation","sign_citation":"https://pith.science/pith/WLSWKCFWUZPBENUS2NDGCFBXIE/action/citation_signature","submit_replication":"https://pith.science/pith/WLSWKCFWUZPBENUS2NDGCFBXIE/action/replication_record"}},"created_at":"2026-07-05T02:43:10.011862+00:00","updated_at":"2026-07-05T02:43:10.011862+00:00"}