{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:SC3M4VCF7KLMKGG36GIRNF37WF","short_pith_number":"pith:SC3M4VCF","schema_version":"1.0","canonical_sha256":"90b6ce5445fa96c518dbf19116977fb14d935aad85c3d594da07a15dd9aed28a","source":{"kind":"arxiv","id":"1703.09158","version":1},"attestation_state":"computed","paper":{"title":"Compared study of Shannon, Tsallis and Gaussian entropy of bound magnetopolaron in nanostructures","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.mes-hall","authors_text":"A. J. Fotue, H. B. Fotsin, L. C. Fai, M. Tiotsop","submitted_at":"2017-03-27T16:00:37Z","abstract_excerpt":"Many methods have been experimented to study decoherence in nanostructures. Tsallis, Shannon and Gaussian entropy have been used to study decoherence separately; in this paper, we compared the results of the sus-mentioned entropies in nanostructures. The linear combination operator and the unitary transformation was used to derive the magnetopolaron spectrum that strongly interact with the LO phonons in the presence of electric field in the pseudo harmonic and delta quantum dot. Numerical results revealed for the quantum pseudo dot that: (i) The amplitude of Gauss entropy is greater than the a"},"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":"1703.09158","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-03-27T16:00:37Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"7345764f6f7edc3b7e29c84f642fa720c5f1934cb42c7f205399998acd6e72ef","abstract_canon_sha256":"a324aabde734e933fdceb49a217e4ad50af845645ffed0ef1068295b20b58231"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:47:54.114987Z","signature_b64":"VmtPIgQA/Lm5fN/EtBy2tUb6Gk/3Ic0nuJI5RaH1MyZwKewRM6PW10dD8NGvdypp75lhVnNDEM7ylIxQ2xDFBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"90b6ce5445fa96c518dbf19116977fb14d935aad85c3d594da07a15dd9aed28a","last_reissued_at":"2026-05-18T00:47:54.114420Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:47:54.114420Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Compared study of Shannon, Tsallis and Gaussian entropy of bound magnetopolaron in nanostructures","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.mes-hall","authors_text":"A. J. Fotue, H. B. Fotsin, L. C. Fai, M. Tiotsop","submitted_at":"2017-03-27T16:00:37Z","abstract_excerpt":"Many methods have been experimented to study decoherence in nanostructures. Tsallis, Shannon and Gaussian entropy have been used to study decoherence separately; in this paper, we compared the results of the sus-mentioned entropies in nanostructures. The linear combination operator and the unitary transformation was used to derive the magnetopolaron spectrum that strongly interact with the LO phonons in the presence of electric field in the pseudo harmonic and delta quantum dot. Numerical results revealed for the quantum pseudo dot that: (i) The amplitude of Gauss entropy is greater than the a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.09158","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":"1703.09158","created_at":"2026-05-18T00:47:54.114504+00:00"},{"alias_kind":"arxiv_version","alias_value":"1703.09158v1","created_at":"2026-05-18T00:47:54.114504+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.09158","created_at":"2026-05-18T00:47:54.114504+00:00"},{"alias_kind":"pith_short_12","alias_value":"SC3M4VCF7KLM","created_at":"2026-05-18T12:31:43.269735+00:00"},{"alias_kind":"pith_short_16","alias_value":"SC3M4VCF7KLMKGG3","created_at":"2026-05-18T12:31:43.269735+00:00"},{"alias_kind":"pith_short_8","alias_value":"SC3M4VCF","created_at":"2026-05-18T12:31:43.269735+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/SC3M4VCF7KLMKGG36GIRNF37WF","json":"https://pith.science/pith/SC3M4VCF7KLMKGG36GIRNF37WF.json","graph_json":"https://pith.science/api/pith-number/SC3M4VCF7KLMKGG36GIRNF37WF/graph.json","events_json":"https://pith.science/api/pith-number/SC3M4VCF7KLMKGG36GIRNF37WF/events.json","paper":"https://pith.science/paper/SC3M4VCF"},"agent_actions":{"view_html":"https://pith.science/pith/SC3M4VCF7KLMKGG36GIRNF37WF","download_json":"https://pith.science/pith/SC3M4VCF7KLMKGG36GIRNF37WF.json","view_paper":"https://pith.science/paper/SC3M4VCF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1703.09158&json=true","fetch_graph":"https://pith.science/api/pith-number/SC3M4VCF7KLMKGG36GIRNF37WF/graph.json","fetch_events":"https://pith.science/api/pith-number/SC3M4VCF7KLMKGG36GIRNF37WF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SC3M4VCF7KLMKGG36GIRNF37WF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SC3M4VCF7KLMKGG36GIRNF37WF/action/storage_attestation","attest_author":"https://pith.science/pith/SC3M4VCF7KLMKGG36GIRNF37WF/action/author_attestation","sign_citation":"https://pith.science/pith/SC3M4VCF7KLMKGG36GIRNF37WF/action/citation_signature","submit_replication":"https://pith.science/pith/SC3M4VCF7KLMKGG36GIRNF37WF/action/replication_record"}},"created_at":"2026-05-18T00:47:54.114504+00:00","updated_at":"2026-05-18T00:47:54.114504+00:00"}