We present 5''-8'' resolution images of the S140 region in the HCO+ J
= 1-0 and SO J(K) = 2(2)-1(1) lines. The maps encompass the well-known
S140 dense core, bipolar outflow, and photodissociation region. Unlik
e previous aperture synthesis maps of molecular tracers in this source
, the HCO+ images, constructed from a combination of Hat Creek millime
ter-array data and NRAO 12 m telescope data, show significant structur
e in the dense gas associated with the embedded cluster. The brightest
emission in the HCO+ maps arises from the periphery of the bipolar fl
ow, suggesting the limb-brightened edges of a cavity with an apex at I
RS 1. Although HCO+ abundance variations might be expected as a result
of shock processing, comparisons with CO isotope data indicate no sig
nificant differences between the ambient material and the low-velocity
outflow (< 10 km s-1). The SO maps provide evidence for variations of
at least an order of magnitude in SO column density in the quiescent
gas on 10'' scales, with localized enhancements to the north and west
of the embedded cluster. SO emission was not detected at velocities ch
aracteristic of the outflow. No compact 89 GHz continuum emission was
detected from the IRS sources to a 3 sigma limit of 60 mJy, consistent
with previous measurements. In an appendix we discuss the effect of '
'holes'' in the (u, v) sampling on synthesis imaging extended molecula
r emission. We derive expressions to quantify the effects of holes for
Gaussian and uniform disk source distributions. We note that while sy
nthesis observations are often said to be ''sensitive'' to structures
on scales lambda/S(min), where S(min) is the length of the shortest ba
seline, the central brightness recovered from a Gaussian distribution
characterized by FWHM = lambda/S(min) is only about 3%. If the S140 HC
O+ data are typical of molecular cloud sources, then the central hole
gives rise to more significant image distortions than many scattered o
uter holes.