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A comment upon the use of two criteria in the identification of intrinsic esr in high Tc oxides

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HAL Id: jpa-00212567

https://hal.archives-ouvertes.fr/jpa-00212567

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:

(2)

2739

LE

JOURNAL DE

PHYSIQUE

Short Communication

A

comment

upon the

use

of

two

criteria in the identification of

intrinsic ESR

in

high

Tc oxides

A. Deville and B.

Gaillard

Laboratoire

d’Electronique

des Milieux

Condenses(*),

Université de

Provence,

Centre

Saint-Jérôme,

13397 Marseille Cedex

13,

France

(Received

5 October

1990,

accepted

9 October

1990)

Résumé. 2014 Un

signal

RPE observé dans un

composé

au bismuth a été récemment attribué à la

phase

SC,

en

s’appuyant

sur le fait que deux critères

(valeur

et

comportement

thermique

de

l’intensité)

sont

vérifiés. Nous attirons l’attention sur la faiblesse de cette

argumentation,

et

rappelons

un

exemple

canonique.

Abstract. 2014 An

ESR

signal

detected in a Bi

compound

has

recently

been attributed to the SC

phase,

arguing

that two criteria

(value

and thermal behaviour of the

intensity)

were met. We draw

attention .

to the weakness of this

argument,

recalling

a canonical

example.

1

Phys.

France 51

( 1990)

2739-2741 15 DÉCEMBRE

1990,

1

Classification

Physics

Abstracts 74.70 - 76.30

The

magnetic

couplings

could

play a

decisive role in the mechanism of

superconductivity

in the

high

Tc

oxides

[1,2].

In this context, the interest of ESR is obvious.

Unfortunately,

the resonance

of the

Cu2+

ion of the SC

phase

has not been detected

yet.

At the moment, the

prevalent

feeling

in the

high

~’~

community

seems to be that ESR is not able to

bring magnetic

informations in these

materials,

while

people

using

ESR still

try

and

get

informations in several

ways :

replacement

of

Cu2+

by

a

non-magnetic

ion,

replacement

of

Y~

by

a

magnetic

ion

(e.g.

Gd3+ )

and,

perhaps

more

ambitious,

examination of new

high

Tc

materials with the

hope

of

detecting

intrinsic ESR.

At the recent LT19

Conference,

it was thus claimed

[3]

that,

in Bi

(Pb)-Sr-Ca-Cu-O,

a

strong

ESR

signal

was

observed,

and that it seemed certain that its

origin

was not

impurities.

It was

argued

that in order not to

originate

from

impurities,

the ESR

signal

had to meet the two

following

criteria :

1)

the

signal

should be related to the onset of the

superconductivity (i.e.

disappear

below

Tc),

(3)

2740

2)

the number of

spins responsible

for ESR should be

higher

than

10~/g.

It was

explained

that

these criteria were both verified in that case

(the

number of

spins

was of the order of

10~°/g,

the

signal disappeared

at

T~),

and concluded that the

possibility

of

impurities

had to be

rejected.

Although

these criteria seem common sense, we wish to stress that

they

represent

in fact

necessary

but not sufficient

conditions.

Thus,

contrary

to what seems to be often

thought,

the

disappearance

of

the

ESR

signal

below

Tc

just

means that the

magnetic

centres

(impurities

or

not)

are

distributed

in the volume of the

sample,

and that the rf field

is

expelled

from the

sample

below

Te.

In order to be more

convincing,

we

briefly

recall our results with

YBa2Cu30~

single crystals

[4,5],

referring

to the

original

papers

for more details :

- the

concentration

was 1.3 x

10 20 spins/g,

- the ESR

intensity dropped abruptly

below

Tc

(Fig.

1,

taken from

[4,5]),

- the

ESR

was moreover

anisotropic.

Fig.

1. - Thermal variation of the normalized ESR

intensity

I

(area

under the

absorption curve)

for a

YBa2Cu307

single crystal

(solid

line: Curie

law). (from

[4]

and

[5]

).

In

[4]

and

[5]

we

gave

experimental

proofs

that the

signal

nethertheless came from

impurities

(the

green

phase

Y2BaCu05) .

As a

conclusion,

although

the use of ESR as a tool for

getting

information

upon

the

magnetic

(4)

2741

References

[1]

ANDERSON P.

W.,

Science 235

(1987)

1196.

[2]

SIGMUND

E.,

STEVENS K. W.

H., J.

Phys.

C. 20

(1987)

6025.

[3]

HAYASHI

Y.,

YOSIDA

T.,

KONTANI

N.,

FuKui

M.,

SAKO

S.,

FUJITA

T.,

SASAKURA

H.,

MINAMIGAWA

S.,

NAKAHIGASHI

K.,

Physica

B 165 & 166

(1990)

1317,

Proceedings

of the LT19

Conference,

16/22

August 1990,

Brighton (G.B.).

[4]

DEVILLE

A.,

GAILLARD

B.,

NOEL

H.,

POTEL

M.,

GOUGEON

P,

LEVET J.

C.,

Physica

C 153 & 155

(1988)

669,

Proceedings

of the HTM2SC Conference 28/2-4/3

1988, Interlaken,

Switzerland.

[5]

DEVILLE

A.,

GAILLARD

B.,

NOEL

H.,

POTEL

M.,

GOUGEON

P.,

LEVET J.

C., J.

Phys.

France 50

(1989)

2357.

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