To fully exploit the capability of vertical head sensors, it is necessary t
o increase the gap immediately after the front contact region located at th
e air bearing surface. Because of fringing of the flux as it leaves the sen
sor and passes to the shields, the effective gap is less than the physical
gap. An analysis has been performed using an electrical, SPICE, analog mode
l for the field equations to determine the relationship between the change
in the physical gap and the effective gap in terms of the signal decay alon
g the sensor [A. V. Pohm, R. S. Beech, J. M. Anderson, and W. C. Black, IEE
E Trans. Magn. 33, 2392 (1997)]. Three enlarged half gaps were considered:
one with an abrupt increase, one with a slope of two, and one with a slope
of one. The analysis considered mostly back gaps which were ten times large
r than the front gaps, going from 0.1 to 1.0 mu m, for example. The results
show an abrupt step yields an effective slope of 0.9 and a physical step w
ith a slope of 1 yields an effective slope of 0.75. The effective slopes ar
e being used to more accurately model the decay of signal flux along vertic
al head sensors. (C) 1999 American Institute of Physics. [S0021-8979(99)311
08-7].