In dispersive wave systems, when leading-order nonlinear and dispersive eff
ects, are taken into account the envelope of a small-amplitude narrow-band
wave pulse is known to satisfy the nonlinear Schrodinger (NLS) equation whi
ch, under certain conditions, admits envelope-soliton solutions. These soli
tons describe locally confined wave groups with envelopes of permanent form
and find applications in various physical contexts. Here, is addressed the
question of whether NLS envelope solitons survive when higher-order effect
s are taken into account. Based on a kinematic argument first, it is sugges
ted that oscillatory tails are inevitably emitted, and this claim is furthe
r supported by numerical computations by use of a fifth-order Korteweg-deVr
ies equation as a simple example. The radiation of tails is caused by a res
onance mechanism that lies beyond all orders of the usual multiple-scale ex
pansion leading to the NLS equation, and a procedure for calculating these
tails by use of exponential asymptotics is outlined. Despite having exponen
tially small amplitude in the asymptotic sense, the radiated tails can be s
ignificant when pulses of relatively short duration are considered.