At shorter lead times (24-96 h), the predictability horizon was also limited by uncertainty associated with the establishment of an arctic air mass over the Northeast U.S. and the potential for upper-level trough phasing in split flow east of the Rockies. Cumulative trough passages in the northern part of this split flow introduced a low-level arctic air mass into the Northeast U.S. as a polar anticyclone spread eastward across southern central and eastern Canada. A strong lower tropospheric baroclinic zone along the southern boundary of this arctic air mass anchored strong lower tropospheric warm-air advection ahead of mobile upper-level disturbances in the aforementioned split flow. These disturbances phased near the Atlantic coast, resulting in a stronger and more northwestward-displaced surface cyclone for which the predictability horizon was only 48–72 h.
Mesoscale snowbands embedded within the larger-scale cyclone further limited the predictability horizon to < 12 h. Observations from the New York State Mesonet, and radar and satellite loops revealed that two mesoscale snowbands accounted for the heaviest snowfalls. One snowband formed in central Pennsylvania after 0600 UTC 14 March, pivoted cyclonically, and became quasi-stationary from northeastern Pennsylvania to the southwestern Adirondacks. A second snowband formed across Delmarva, eastern Pennsylvania and central New Jersey after 1200 UTC 14 March and moved northward while rotating cyclonically about a pivot point ~75–100 km west of Albany, NY. Snowfall rates of 12.5–15.0 cm per hour occurred during the passage of this second snowband. Areas impacted by both snowbands received storm-total snowfall accumulations near 1 m with a maximum of ~1.2 m reported in the vicinity of Cooperstown, NY.