Physica C 196 (1992) 17-26
North-Holland
PHYSICA
Bean-Livingston surface barrier and magnetic properties of granular
superconductors
K.I. Kugel and A.L. Rakhmanov
Institute for High Temperatures, 127412 Moscow,Russia
Received 3 January 1992
The magnetic flux penetration into a granular superconductor is studied, accounting for the Bean-Livingston surface barrier
(BLSB). It is shown that the magnetic flux distribution is strongly affected by the BLSB in the case of large, closely packed
granules. In particular, the intergranular magneticfield Ho appears to be much higher than the external field Hwhen H<Hs=2H_,2/
lg (where l s is the characteristic granular size and 2 is the London penetration depth ). The effects related to the difference between
H and Ho are discussed in the framework of a simplified model of a granular superconductor. The magnetic flux distribution is
studied in the regular system of isotropic and anisotropic granules. The form of the Ho(H) curve is calculated for both increasing
and decreasing field H. It is shown that the existence of the BLSBresults in the strong hysteresis of the Ho(H) curve. The relation
between these effects and the form of the magnetic field dependence of critical current in ceramic superconductors is discussed.
I. Introduction
In high-Tc superconducting ceramics the magnetic
field Ito in intergranular regions may appreciably
differ from the external field H owing to magnetic
flux expulsion from superconducting granules. This
effect results in peculiarities of the field dependences
of critical current j~(H), I-V characteristic, mag-
netic susceptibility and some other properties of
granular superconductors. Such phenomena are ev-
idently of importance in weak fields H<H~, where
Hc~ is the lower critical field for the granules. How-
ever, there are two effects which lead to the broad-
ening of the field range where the above-mentioned
peculiarities may be appreciable. The first one is in-
tragranular pinning. The influence of pinning on the
magnetic flux distribution and on critical current j~
versus H curves in granular superconductors was
considered, for example, in ref. [ 1 ]. The second ef-
fect is the Bean-Livingston surface barrier (BLSB)
[ 2 ] which impedes the penetration of flux lines into
a superconductor owing to repulsive interaction be-
tween the surface and an entering vortex. It was
shown [3 ] that the existence of the BLSB leads to
the sufficient difference between Ho and H in the
granular system in the external field range extending
up to several Hc, where Hc is the thermodynamic
critical field for the granule. In the present paper the
effect of the BLSB on flux penetration and on the
jc(H) dependence for the granular system is
discussed.
The superconducting ceramics may be presented
schematically as a system of granules with average
size Is separated by narrow normal layers with char-
acteristic thickness li. Usually, it is supposed that the
normal layers are weak links. The magnetic flux pen-
etrates the sample at H> hcl, where hot is the lower
critical field of the intergranular weak links network.
The local magnetic induction B may be defined as
the value of magnetic flux intensity averaged over a
sufficiently large volume. The local value of the in-
tergranular field Ho may be much higher than B ow-
ing to the flux expulsion from the granules. At H>> hcl
the simple estimates give for the ratio Ho/B in a vol-
ume element AV:Ho/B~ AV/AVef, where AVef is the
part of A Vincluding the volume of the normal layers
A Vi and the effective volume of the granules occu-
pied by the magnetic flux. Obviously, the ratio Ho/
B has the highest value for the system of sufficiently
large closely packed granules
li <<2 <<l s , ( 1 )
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