Lhermitte R M, Atlas D. Precipitation motion by pulse Doppler. Preprints Ninth Weather Radar Conference. Amer. Meteor. Soc., 1961: 218~223.
[9]
Armijo L. A theory for the determination of wind and precipitation velocities with Doppler radar. J. Atmos. Sci., 1969, 26 (3): 570~573.
[10]
Kropfli R A, Miller L J. Kinematic structure and flux quantities in a convective storm from dual-Doppler radar observation. J. Atmos. Sci., 1976, 33 (3): 520~529.
[11]
Browning K A, Foote G B. Airflow and hail growth in supercell storms and some implications for hail suppression. Quart. J. Roy. Meteor. Soc. , 1976, 102 (433): 499~533.
[12]
Houze R A, Rutledge S A, Biggerstaff M I, et al. Interpretation of Doppler weather radar display of midlatitude mesoscale convective system. Bull. Amer. Meteor. Soc., 1989, 70 (3): 608~619.
[13]
Dowell D C, Bluestein H B. The arcadia Oklahoma storm of 17 May 1981:analysis of a super-cell during tornadogensis. Mon. Wea. Rev., 1997, 125 (12): 2562~2582.
[14]
Lin Y J, Pasken R W, Chang H W. The structure of a prefrontal convective rain-band. Part I: Mesoscale kinematic structure determined from dual-Doppler measurements. Mon. Wea. Rev., 1992, 120 (9): 1816~1836.
Bousquet O, Chong M. A multiple-Doppler synthesis and continuity adjustment technique (MUSCAT) to recover wind components from Doppler radar measurement. J. Atmos. Oceanic Technol., 1998, 13 (2): 343~359.