{"title":"早期皮层体感诱发电位的高频振荡","authors":"Isamu Ozaki , Chieko Suzuki , Yukoh Yaegashi , Masayuki Baba , Muneo Matsunaga , Isao Hashimoto","doi":"10.1016/S0168-5597(98)00032-X","DOIUrl":null,"url":null,"abstract":"<div><p><strong>Objective</strong><span>: To evaluate the characteristics of high frequency (HF) components of the early cortical somatosensory evoked potentials (SEPs).</span></p><p><strong>Methods</strong><span>: We recorded 8-channel SEPs from the frontal and left centro-parietal scalp after right median nerve stimulation with a wide band-pass (0.5–2000 Hz) and digitized at 40 kHz sampling rate in 12 healthy subjects. HF components were analyzed after digital band-pass filtering (300–1000 Hz). The power spectrum was obtained by a maximum entropy method.</span></p><p><strong>Results</strong><span>: HF oscillations<span> (maximum power at 600–800 Hz) consisting of 5 to 8 peaks were discriminated from the preceding P14 far-field in all cases and their phases were reversed between the frontal and contralateral parietal regions. In addition, in subjects with a high amplitude central P22 potential in original wide-band recordings, a single HF oscillation with a maximum at the central region was present. Furthermore, this component showed no phase reversal over the centro-parietal area.</span></span></p><p><strong>Conclusion</strong>: We therefore conclude that HF oscillations are superimposed not only on the tangential N20-P20 but on the radial P22 potential, and are generated from both tangential (area 3b) and radial (area 1) current sources.</p></div>","PeriodicalId":100401,"journal":{"name":"Electroencephalography and Clinical Neurophysiology/Evoked Potentials Section","volume":"108 6","pages":"Pages 536-542"},"PeriodicalIF":0.0000,"publicationDate":"1998-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/S0168-5597(98)00032-X","citationCount":"60","resultStr":"{\"title\":\"High frequency oscillations in early cortical somatosensory evoked potentials\",\"authors\":\"Isamu Ozaki , Chieko Suzuki , Yukoh Yaegashi , Masayuki Baba , Muneo Matsunaga , Isao Hashimoto\",\"doi\":\"10.1016/S0168-5597(98)00032-X\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p><strong>Objective</strong><span>: To evaluate the characteristics of high frequency (HF) components of the early cortical somatosensory evoked potentials (SEPs).</span></p><p><strong>Methods</strong><span>: We recorded 8-channel SEPs from the frontal and left centro-parietal scalp after right median nerve stimulation with a wide band-pass (0.5–2000 Hz) and digitized at 40 kHz sampling rate in 12 healthy subjects. HF components were analyzed after digital band-pass filtering (300–1000 Hz). The power spectrum was obtained by a maximum entropy method.</span></p><p><strong>Results</strong><span>: HF oscillations<span> (maximum power at 600–800 Hz) consisting of 5 to 8 peaks were discriminated from the preceding P14 far-field in all cases and their phases were reversed between the frontal and contralateral parietal regions. In addition, in subjects with a high amplitude central P22 potential in original wide-band recordings, a single HF oscillation with a maximum at the central region was present. Furthermore, this component showed no phase reversal over the centro-parietal area.</span></span></p><p><strong>Conclusion</strong>: We therefore conclude that HF oscillations are superimposed not only on the tangential N20-P20 but on the radial P22 potential, and are generated from both tangential (area 3b) and radial (area 1) current sources.</p></div>\",\"PeriodicalId\":100401,\"journal\":{\"name\":\"Electroencephalography and Clinical Neurophysiology/Evoked Potentials Section\",\"volume\":\"108 6\",\"pages\":\"Pages 536-542\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1998-11-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1016/S0168-5597(98)00032-X\",\"citationCount\":\"60\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Electroencephalography and Clinical Neurophysiology/Evoked Potentials Section\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S016855979800032X\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Electroencephalography and Clinical Neurophysiology/Evoked Potentials Section","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S016855979800032X","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
High frequency oscillations in early cortical somatosensory evoked potentials
Objective: To evaluate the characteristics of high frequency (HF) components of the early cortical somatosensory evoked potentials (SEPs).
Methods: We recorded 8-channel SEPs from the frontal and left centro-parietal scalp after right median nerve stimulation with a wide band-pass (0.5–2000 Hz) and digitized at 40 kHz sampling rate in 12 healthy subjects. HF components were analyzed after digital band-pass filtering (300–1000 Hz). The power spectrum was obtained by a maximum entropy method.
Results: HF oscillations (maximum power at 600–800 Hz) consisting of 5 to 8 peaks were discriminated from the preceding P14 far-field in all cases and their phases were reversed between the frontal and contralateral parietal regions. In addition, in subjects with a high amplitude central P22 potential in original wide-band recordings, a single HF oscillation with a maximum at the central region was present. Furthermore, this component showed no phase reversal over the centro-parietal area.
Conclusion: We therefore conclude that HF oscillations are superimposed not only on the tangential N20-P20 but on the radial P22 potential, and are generated from both tangential (area 3b) and radial (area 1) current sources.