{"doi":"10.1121/1.413040","title":"Conversion of an <i>SH</i> wave into a Stoneley wave under weak distortion of the elastic isotropic space material of a crystal lattice","abstract":"<jats:p>The problem of the conversion of a volume SH wave propagating in an isotropic elastic space into a Stoneley wave as a consequence of the conversion of this space into a three-layered medium by small variations in material elastic moduli in a portion of the space is considered. Three-layered medium of two types have been investigated: A weakly anisotropic layer of cubic symmetry between two isotropic half-spaces and an isotropic layer between two slightly anisotropic half-spaces of cubic symmetry. The elastic moduli of the isotropic material and the isotropic parts of the moduli of the weakly anisotropic material are the same. Small anisotropic values added to the isotropic elastic moduli are introduced by various means, in such a manner that velocities of the SH waves in the slightly anisotropic materials with cubic symmetry may be smaller, bigger, or equal to the velocity of the SH wave in the corresponding isotropic material. It is shown that in cases when the Stoneley wave exists it refers to a weakly inhomogeneous quasitransverse wave of SH type, because among three displacement components weakly decaying with depth, the transverse one parallel to the interface of three mediums predominates.</jats:p>","journal":"The Journal of the Acoustical Society of America","year":1995,"id":642963,"datarank":0.0,"base_score":0.0,"endowment":0.0,"self_citation_contribution":0.0,"citation_network_contribution":0.0,"self_endowment_contribution":0.0,"citer_contribution":0.0,"corpus_percentile":null,"corpus_rank":null,"citation_count":0,"citer_count":0,"citers_with_citation_signal":0,"citers_with_endowment":0,"datacite_reuse_total":0,"is_dataset":false,"is_dataset_confidence":null,"is_data_producer":false,"deposit_databanks":null,"is_oa":false,"file_count":0,"downloads":0,"has_version_chain":false,"published_date":null,"fair_score":null,"fair_percentile":null,"algorithm_id":"datarank_citation_only_1hop_v6","ranking_scope":"data_only","authors":[{"id":1672697,"name":"Marina V. Shitikova","orcid":null,"position":1,"is_corresponding":false},{"id":1672696,"name":"Yuriy A. Rossikhin","orcid":null,"position":0,"is_corresponding":false}],"reference_count":0,"raw_metadata":{"has_enrichment":true,"resolved":true,"title":"Conversion of an <i>SH</i> wave into a Stoneley wave under weak distortion of the elastic isotropic space material of a crystal lattice","abstract":"<jats:p>The problem of the conversion of a volume SH wave propagating in an isotropic elastic space into a Stoneley wave as a consequence of the conversion of this space into a three-layered medium by small variations in material elastic moduli in a portion of the space is considered. Three-layered medium of two types have been investigated: A weakly anisotropic layer of cubic symmetry between two isotropic half-spaces and an isotropic layer between two slightly anisotropic half-spaces of cubic symmetry. The elastic moduli of the isotropic material and the isotropic parts of the moduli of the weakly anisotropic material are the same. Small anisotropic values added to the isotropic elastic moduli are introduced by various means, in such a manner that velocities of the SH waves in the slightly anisotropic materials with cubic symmetry may be smaller, bigger, or equal to the velocity of the SH wave in the corresponding isotropic material. It is shown that in cases when the Stoneley wave exists it refers to a weakly inhomogeneous quasitransverse wave of SH type, because among three displacement components weakly decaying with depth, the transverse one parallel to the interface of three mediums predominates.</jats:p>","is_dataset_classified":null,"base_score":0.0,"endowment":0.0,"datacite_reuse_total":0,"file_count":0,"downloads":0,"views":0,"has_version_chain":false,"is_dataset":false,"is_oa":false,"pmid":"19910364","pmcid":null,"openalex_id":"https://openalex.org/W2054246028","authors":[],"funders":[],"total_grants":0,"fwci":0.0,"citation_percentile":0.15906476,"influential_citations":0,"citation_trend":[],"oa_status":"closed","license":null,"oa_locations":[{"url":"https://pubs.aip.org/asa/jasa/article-pdf/97/5/2826/11818785/2826_1_online.pdf","host_type":"publisher"},{"url":"https://doi.org/10.1121/1.413040","host_type":"journal"}],"fields_of_study":["Electromagnetic Effects on Materials","Geophysics and Sensor Technology","Material Properties and Failure Mechanisms"],"mesh_terms":[],"keywords":["Isotropy","Anisotropy","Transverse isotropy","Isotropic solid","Elastic modulus","Condensed matter physics","Lattice (music)","Symmetry (geometry)","Physics","Materials science","Geometry","Optics","Composite material","Mathematics","Acoustics"],"sdg_mappings":[{"sdg_number":0,"sdg_label":"Sustainable cities and communities"}],"linked_datasets":[],"clinical_trials":[],"software_tools":[],"database_accessions":[],"source":"live","citation_network_status":"fetched"},"created_at":"2026-08-08T11:12:55.053782Z","pmid":null,"pmcid":null,"fwci":null,"citation_percentile":null,"influential_citations":0,"oa_status":null,"license":null,"views":0,"total_file_size_bytes":0,"version_count":0,"fair_f":null,"fair_a":null,"fair_i":null,"fair_r":null,"fair_zscore":null,"fair_rationale":null,"fair_model":null,"fair_agent_version":null,"fair_fulltext_source":null,"fair_has_llm":null,"fair_computed_at":null,"clinical_trials":[],"software_tools":[],"db_accessions":[],"linked_datasets":[],"topics":[]}