ABSTRACT
In the presence of fluctuating fields, plasma elements (particles) are subject to E × B motion. The Doppler shift of the k mode by the fluctuating velocity v ˜ E × B https://s3-euw1-ap-pe-df-pch-content-public-p.s3.eu-west-1.amazonaws.com/9780429148958/893f63fb-838b-43d9-9be3-ee81e9ce7f6a/content/eq1561.tif"/> equation (11.8), () ω E × B = v ˜ E × B ⋅ k ⊥ , https://s3-euw1-ap-pe-df-pch-content-public-p.s3.eu-west-1.amazonaws.com/9780429148958/893f63fb-838b-43d9-9be3-ee81e9ce7f6a/content/eq1562.tif"/>
