Astron. Astrophys. 361, 795-802 (2000)
3. Glitches driven by differential rotation
Soon after the empirical discovery of glitches too large to be
accounted for by the "spheroidality" mechanism, it came to be
recognised by theorists (Anderson & Itoh 1975) that a plausible
explanation involved the superfluid property of the deeper layers of
sufficiently cool neutron stars. This property makes it possible to
conceive that an interior neutron superfluid layer with moment of
inertia, say, can rotate with an
angular velocity, say, that may
differ from the externally observable angular velocity
that characterises the part of the
star that corotates with the crust, with its own moment of inertia
![[EQUATION]](img34.gif)
In such a case it can be supposed that when an external braking
mechanism causes the corotating crust component to undergo an angular
velocity change , the angular
velocity of the independently
rotating neutron superfluid layer may in the short run be unaffected,
with negligible variation expressible by
![[EQUATION]](img36.gif)
but that, when the ensuing angular velocity difference between the
corotating crust component and the neutron superfluid layer exceeds
some critical value there will be a discontinuous adjusment whereby
this angular velocity difference is reduced by some process involving
a transfer of angular momentum between the two components. Such a
process will evidently entail a negative adjustment
of the angular velocity of the
neutron superfluid layer and an accompanying positive adjustment
of the (observable) angular velocity
of the corotating crust component, whereby the latter increases its
angular momentum by an amount that
is equal to the amount that is lost
by the neutron superfluid component, so that the total angular
momentum change during the discontinuous `glitch' process is zero,
i.e.
![[EQUATION]](img40.gif)
If this adjustment process were a hundred per cent efficient, the
net variation of the corotating
crust angular velocity would be exactly matched by the net neutron
superfluid angular velocity variation, which by (10) will be simply
given by , so that one would have
![[EQUATION]](img42.gif)
with . In practice one would
expect that there would typically be an incomplete adjustment, still
expressible by a relation of the form (12), but with an efficiency
factor having some lower value in
the range (5). By substituting (11) in (12) it can be seen that the
observable glitch magnitude will be given by
![[EQUATION]](img44.gif)
and hence, by (9), that for an efficiency factor
with any value in the range (5) the
glitch magnitude will satisfy the inequality
![[EQUATION]](img45.gif)
By comparing (14) with (7), it can be seen that, for a given
assumed value of the efficiency factor
, the differential rotation
adjustment mechanism characterised by (14) can give rise to a much
larger glitch magnitude than is
possible by the spheroidality adjusment mechanism characterised by
(7), because the factor in (14) can
be of order unity, whereas the corresponding factor in (7), namely
is very small compared to unity in
even the most rapidly rotating pulsars. Thus, unlike the spheroidality
mechanism, mechanisms involving angular momentum transfer between
differentially rotating components can plausibly be considered as
candidates for explaining the frequent large glitches observed in the
Vela pulsar.
© European Southern Observatory (ESO) 2000
Online publication: October 2, 2000
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