{"title":"滑行纹波谱鉴别:纹波密度和滑行速度限制","authors":"A. Supin, O. Milekhina, D. Nechaev","doi":"10.1121/2.0000801","DOIUrl":null,"url":null,"abstract":"Rippled noise is a productive model of natural signals with complex spectrum patterns. It was used as a test signal to measure spectrum-pattern resolution both in normal-hearing listeners and in hearing-impaired listeners and users of cochlear implants. However, a variety of natural auditory signals feature combined spectro-temporal patterns. These signals may be modeled by rippled noise with “gliding” ripples. In the present study, ripple gliding velocity limits as a function of ripple density were measured in normal-hearing listeners. The highest gliding velocity (expressed in oct/s or ripples/s) at which the gliding ripple pattern could be distinguished from a non-rippled noise was determined. The ripple gliding velocity limit decreased from approximately 400-500 ripple/s at a ripple density of 1 ripple/oct to approximately 50 ripple/s at a ripple density of 7 ripple/oct. The data are explained by a model based on a combine action of the excitation-pattern and temporal-processing mechanisms.","PeriodicalId":20469,"journal":{"name":"Proc. Meet. Acoust.","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2018-05-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Gliding rippled spectrum discrimination: Ripple density and gliding velocity limits\",\"authors\":\"A. Supin, O. Milekhina, D. Nechaev\",\"doi\":\"10.1121/2.0000801\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Rippled noise is a productive model of natural signals with complex spectrum patterns. It was used as a test signal to measure spectrum-pattern resolution both in normal-hearing listeners and in hearing-impaired listeners and users of cochlear implants. However, a variety of natural auditory signals feature combined spectro-temporal patterns. These signals may be modeled by rippled noise with “gliding” ripples. In the present study, ripple gliding velocity limits as a function of ripple density were measured in normal-hearing listeners. The highest gliding velocity (expressed in oct/s or ripples/s) at which the gliding ripple pattern could be distinguished from a non-rippled noise was determined. The ripple gliding velocity limit decreased from approximately 400-500 ripple/s at a ripple density of 1 ripple/oct to approximately 50 ripple/s at a ripple density of 7 ripple/oct. The data are explained by a model based on a combine action of the excitation-pattern and temporal-processing mechanisms.\",\"PeriodicalId\":20469,\"journal\":{\"name\":\"Proc. Meet. Acoust.\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2018-05-29\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Proc. Meet. Acoust.\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1121/2.0000801\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proc. Meet. Acoust.","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1121/2.0000801","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Gliding rippled spectrum discrimination: Ripple density and gliding velocity limits
Rippled noise is a productive model of natural signals with complex spectrum patterns. It was used as a test signal to measure spectrum-pattern resolution both in normal-hearing listeners and in hearing-impaired listeners and users of cochlear implants. However, a variety of natural auditory signals feature combined spectro-temporal patterns. These signals may be modeled by rippled noise with “gliding” ripples. In the present study, ripple gliding velocity limits as a function of ripple density were measured in normal-hearing listeners. The highest gliding velocity (expressed in oct/s or ripples/s) at which the gliding ripple pattern could be distinguished from a non-rippled noise was determined. The ripple gliding velocity limit decreased from approximately 400-500 ripple/s at a ripple density of 1 ripple/oct to approximately 50 ripple/s at a ripple density of 7 ripple/oct. The data are explained by a model based on a combine action of the excitation-pattern and temporal-processing mechanisms.