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Submitted on 1 Jan 1990
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A comment upon the use of two criteria in the
identification of intrinsic esr in high Tc oxides
A. Deville, B. Gaillard
To cite this version:
2739
LE
JOURNAL DE
PHYSIQUE
Short Communication
A
comment
upon the
useof
two
criteria in the identification of
intrinsic ESR
in
high
Tc oxides
A. Deville and B.
Gaillard
Laboratoire
d’Electronique
des MilieuxCondenses(*),
Université deProvence,
CentreSaint-Jérôme,
13397 Marseille Cedex13,
France(Received
5 October1990,
accepted
9 October1990)
Résumé. 2014 Un
signal
RPE observé dans uncomposé
au bismuth a été récemment attribué à laphase
SC,
ens’appuyant
sur le fait que deux critères(valeur
etcomportement
thermique
del’intensité)
sontvérifiés. Nous attirons l’attention sur la faiblesse de cette
argumentation,
etrappelons
unexemple
canonique.
Abstract. 2014 An
ESR
signal
detected in a Bicompound
hasrecently
been attributed to the SCphase,
arguing
that two criteria(value
and thermal behaviour of theintensity)
were met. We drawattention .
to the weakness of thisargument,
recalling
a canonicalexample.
1
Phys.
France 51( 1990)
2739-2741 15 DÉCEMBRE1990,
1Classification
Physics
Abstracts 74.70 - 76.30The
magnetic
couplings
couldplay a
decisive role in the mechanism ofsuperconductivity
in thehigh
Tc
oxides[1,2].
In this context, the interest of ESR is obvious.Unfortunately,
the resonanceof the
Cu2+
ion of the SCphase
has not been detectedyet.
At the moment, theprevalent
feeling
in the
high
~’~
community
seems to be that ESR is not able tobring magnetic
informations in thesematerials,
whilepeople
using
ESR stilltry
andget
informations in severalways :
replacement
ofCu2+
by
anon-magnetic
ion,
replacement
ofY~
by
amagnetic
ion(e.g.
Gd3+ )
and,
perhaps
more
ambitious,
examination of newhigh
Tc
materials with thehope
ofdetecting
intrinsic ESR.At the recent LT19
Conference,
it was thus claimed[3]
that,
in Bi(Pb)-Sr-Ca-Cu-O,
astrong
ESRsignal
wasobserved,
and that it seemed certain that itsorigin
was notimpurities.
It wasargued
that in order not tooriginate
fromimpurities,
the ESRsignal
had to meet the twofollowing
criteria :1)
thesignal
should be related to the onset of thesuperconductivity (i.e.
disappear
belowTc),
2740
2)
the number ofspins responsible
for ESR should behigher
than10~/g.
It wasexplained
thatthese criteria were both verified in that case
(the
number ofspins
was of the order of10~°/g,
thesignal disappeared
atT~),
and concluded that thepossibility
ofimpurities
had to berejected.
Although
these criteria seem common sense, we wish to stress thatthey
represent
in factnecessary
but not sufficientconditions.
Thus,
contrary
to what seems to be oftenthought,
thedisappearance
of
theESR
signal
belowTc
just
means that themagnetic
centres(impurities
ornot)
aredistributed
in the volume of the
sample,
and that the rf fieldis
expelled
from thesample
belowTe.
In order to be moreconvincing,
webriefly
recall our results withYBa2Cu30~
single crystals
[4,5],
referring
to theoriginal
papers
for more details :- the
concentration
was 1.3 x10 20 spins/g,
- the ESR
intensity dropped abruptly
belowTc
(Fig.
1,
taken from[4,5]),
- theESR
was moreoveranisotropic.
Fig.
1. - Thermal variation of the normalized ESRintensity
I(area
under theabsorption curve)
for aYBa2Cu307
single crystal
(solid
line: Curielaw). (from
[4]
and[5]
).
In
[4]
and[5]
wegave
experimental
proofs
that thesignal
nethertheless came fromimpurities
(the
green
phase
Y2BaCu05) .
As a
conclusion,
although
the use of ESR as a tool forgetting
informationupon
themagnetic
2741
References
[1]
ANDERSON P.W.,
Science 235(1987)
1196.[2]
SIGMUNDE.,
STEVENS K. W.H., J.
Phys.
C. 20(1987)
6025.[3]
HAYASHIY.,
YOSIDAT.,
KONTANIN.,
FuKuiM.,
SAKOS.,
FUJITAT.,
SASAKURAH.,
MINAMIGAWAS.,
NAKAHIGASHI
K.,
Physica
B 165 & 166(1990)
1317,
Proceedings
of the LT19Conference,
16/22August 1990,
Brighton (G.B.).
[4]
DEVILLEA.,
GAILLARDB.,
NOELH.,
POTELM.,
GOUGEONP,
LEVET J.C.,
Physica
C 153 & 155(1988)
669,
Proceedings
of the HTM2SC Conference 28/2-4/31988, Interlaken,
Switzerland.[5]
DEVILLEA.,
GAILLARDB.,
NOELH.,
POTELM.,
GOUGEONP.,
LEVET J.C., J.
Phys.
France 50(1989)
2357.