{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:3FAIIYNL3WLCEXYVZN7TSCZGWX","short_pith_number":"pith:3FAIIYNL","schema_version":"1.0","canonical_sha256":"d9408461abdd96225f15cb7f390b26b5fd1253bcd12c13c52f2f3a9138d54c51","source":{"kind":"arxiv","id":"1310.1433","version":1},"attestation_state":"computed","paper":{"title":"The nematic phase in stripe forming systems within the self consistent screening approximation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Alejandro Mendoza-Coto, Daniel A. Stariolo, Daniel G. Barci","submitted_at":"2013-10-05T02:42:52Z","abstract_excerpt":"We show that in order to describe the isotropic-nematic transition in stripe forming systems with isotropic competing interactions of the Brazovskii class it is necessary to consider the next to leading order in a 1/N approximation for the effective Hamiltonian. This can be conveniently accomplished within the self-consistent screening approximation. We solve the relevant equations and show that the self-energy in this approximation is able to generate the essential wave vector dependence to account for the anisotropic character of two-point correlation function characteristic of a nematic pha"},"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":"1310.1433","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2013-10-05T02:42:52Z","cross_cats_sorted":[],"title_canon_sha256":"f09fb08d71d7d6ebb725262affd3cab2b744fb5938ebf3bfeb614fea4e62561c","abstract_canon_sha256":"6763f64c8410244bfd29f4e678fc6b66691d5de003d1091b606d8cd0698b0deb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:50:42.837574Z","signature_b64":"ZTEbtfpUe5fEnyz46DFVR4Qm+e6bAmIHwLozuUZZIG5lHVl50mOmJRM9r8oYZrLGUzRLXr7gdHUJ05DRwL2rBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d9408461abdd96225f15cb7f390b26b5fd1253bcd12c13c52f2f3a9138d54c51","last_reissued_at":"2026-05-18T02:50:42.836821Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:50:42.836821Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The nematic phase in stripe forming systems within the self consistent screening approximation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Alejandro Mendoza-Coto, Daniel A. Stariolo, Daniel G. Barci","submitted_at":"2013-10-05T02:42:52Z","abstract_excerpt":"We show that in order to describe the isotropic-nematic transition in stripe forming systems with isotropic competing interactions of the Brazovskii class it is necessary to consider the next to leading order in a 1/N approximation for the effective Hamiltonian. This can be conveniently accomplished within the self-consistent screening approximation. We solve the relevant equations and show that the self-energy in this approximation is able to generate the essential wave vector dependence to account for the anisotropic character of two-point correlation function characteristic of a nematic pha"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.1433","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":"1310.1433","created_at":"2026-05-18T02:50:42.836962+00:00"},{"alias_kind":"arxiv_version","alias_value":"1310.1433v1","created_at":"2026-05-18T02:50:42.836962+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.1433","created_at":"2026-05-18T02:50:42.836962+00:00"},{"alias_kind":"pith_short_12","alias_value":"3FAIIYNL3WLC","created_at":"2026-05-18T12:27:32.513160+00:00"},{"alias_kind":"pith_short_16","alias_value":"3FAIIYNL3WLCEXYV","created_at":"2026-05-18T12:27:32.513160+00:00"},{"alias_kind":"pith_short_8","alias_value":"3FAIIYNL","created_at":"2026-05-18T12:27:32.513160+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/3FAIIYNL3WLCEXYVZN7TSCZGWX","json":"https://pith.science/pith/3FAIIYNL3WLCEXYVZN7TSCZGWX.json","graph_json":"https://pith.science/api/pith-number/3FAIIYNL3WLCEXYVZN7TSCZGWX/graph.json","events_json":"https://pith.science/api/pith-number/3FAIIYNL3WLCEXYVZN7TSCZGWX/events.json","paper":"https://pith.science/paper/3FAIIYNL"},"agent_actions":{"view_html":"https://pith.science/pith/3FAIIYNL3WLCEXYVZN7TSCZGWX","download_json":"https://pith.science/pith/3FAIIYNL3WLCEXYVZN7TSCZGWX.json","view_paper":"https://pith.science/paper/3FAIIYNL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1310.1433&json=true","fetch_graph":"https://pith.science/api/pith-number/3FAIIYNL3WLCEXYVZN7TSCZGWX/graph.json","fetch_events":"https://pith.science/api/pith-number/3FAIIYNL3WLCEXYVZN7TSCZGWX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3FAIIYNL3WLCEXYVZN7TSCZGWX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3FAIIYNL3WLCEXYVZN7TSCZGWX/action/storage_attestation","attest_author":"https://pith.science/pith/3FAIIYNL3WLCEXYVZN7TSCZGWX/action/author_attestation","sign_citation":"https://pith.science/pith/3FAIIYNL3WLCEXYVZN7TSCZGWX/action/citation_signature","submit_replication":"https://pith.science/pith/3FAIIYNL3WLCEXYVZN7TSCZGWX/action/replication_record"}},"created_at":"2026-05-18T02:50:42.836962+00:00","updated_at":"2026-05-18T02:50:42.836962+00:00"}