(i) The systematic downward propagation of geopotential height and zonal wind anomalies in the extratropics;
(Kodera and Kuroda 1990; Baldwin and Dunkerton 1999; Baldwin and Dunkerton 2001; Cai and Ren 2007; Ren and Cai 2007)
(ii) The delayed feedbacks of the stratosphere to the upward propagation of tropospheric Rossby waves;
(Hartley et al. 1998; Limpavusan and Hartmann 2000; Ambaum and Hoskins 2002; Polvani and Waugh 2004; Kuroda 2008)
(iii) The downward control principle and with transient eddy feedbacks;
(Haynes et al. 1991; Song and Robinson 2004)
(iv) The reflection of planetary waves;
(Perlwitz and Harnik 2003)
(v) The invertibility principle of potential vorticity.
(Hartley et al. 1998)
![](/var/ezwebin_site/storage/images/media/images/all-common-shared-graphics/underlying-science4/2144116-1-eng-US/underlying-science_large.jpg)
Figure 1. Atmospheric meridional mass circulation in isentropic levels. The mass circulation quantifies the net transport of air mass of different entropy in a given latitude band. Solid contours and numbers indicate the winter DJF mean mass transport (units: 109 kg s-1) in each branch of the mass circulation and dashed contours indicate the isentropic levels (units: K) in pressure coordinate. By definition, mass transport along isentropic level is purely due to adiabatic processes, and mass transport across isentropic levels is due to diabatic heating/cooling. (Johnson 1989; Cai and Shin 2014)