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Submitted on 1 Jan 1978

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MAGNETIC SUSCEPTIBILITY AS A PROBE OF

OXYGEN SYSTEMS OF RESTRICTED GEOMETRY

S. Gregory

To cite this version:

(2)

JOURNAL DE PHYSIQUE

Colloque C6, supplkment

au no

8, Tome 39, aolit 1978, page C6-334

MAGNETIC S U S C E P T I B I L I T Y AS A PROBE OF OXYGEN SYSTEMS OF R E S T R I C T E D GEOMETRY

S. Gregory

Laboratory o f Atomic and S o l i d S t a t e Physics Come22 U n i v e r s i t y Ithaca, New York 14853 U.S.A.

RiSsum6.- Nous discutons les r6sultats obtenus sur la susceptibilitd magngtique des phases dloxygSne adsorb6 sur deux substrats. Nous observons que la gdomstrie particulisre aux films d'oxygsne et que les propri6tgs microscopiques des substrats influencent le comportement de cette susceptibilit6. Abstract.- Experiments are discussed in which the magnetic susceptibility of adsorbed phases of oxygen has been studied. The observed behavior is seen to be influenced both by the restricted geometry of the oxygen films and by microscopic properties of the substrates.

Recent papers /1,2/ have reported some measu- Susceptibility data for submonolayer coverages

rements of the magnetic susceptibility of oxygen of oxygen on Grafoil and Vycor are shown in the

physisorbed on two substrates, Vycor and Grafoil. In figure.

many investigations, the substrate serves primarily to define a restrected geometry. However, the subs-

trate cannot usually be considered as a smoothplane

=

(*iiquid'manolayers)

which presents a single Van der Waals potential to

0.22

an adsorbent. In general, the substrate potential

+

0.41

0.69

Grafoil does not appear to register anyphase of adsorbed oxygen /3/ and might therefore provide a relatively straightforward enforcer of two-dimen- sional geometry for this system. (The interaction between the axis of the molecule and the spin is

weak. Therefore, one might expect the effective spin T(K)

-

and microscopic geometry will play an evident role

-

0

in the physics of adsorbed systems. I shall briefly

examine adsorbed oxygen experiments for indications

3

of how one might select substrates to create some

y

2.0-

interesting physical conditions.

2

2

dimensionality to be 3 for temperatures greater than those of liquid helium even if the molecules are oriented perpendicular to the substrate either by the substrate-molecule interaction or by the requirements of packing in the various surface

phases. ) I A 0 :

-

Grafoil 't X 0.70

:

v 080 o A \\ I Precision of Grafoil p i n t s ' +

...\

a '\ + 0 A* \.

The substrate Vycor provides a very interes- ting contrast to Grafoil. Whereas both substrates

have large (%

lo3

K) binding energies for typical

adsorbents, the (periodic) variation across the

graphite surface is % 10 K. Vycor, on the otherhand

presents a distribution of binding energies with

%

lo2

-

l o 3 K and it is supposed that the existence

of his wide distribution enforces a random locali- zation of molecules on the substrate surface.

Fig. : Magnetic susceptibility of sub-monolayer

oxygen adsorbed on Vycor and Grafoil substrates. Coverages are expressed as a fraction of a "liquid"

monolayer

-

a monolayer of molecules packed with

mean area of crcupation 12.9

d2

per molecule. (The

precision of the Vycor data is not indicated as it is about an order of magnitude better than that of the Grafoil data.) The dashed line indicates the Curie behavior appropriate to oxygen spins.

The Grafoil data indicate a transition in the

region 25

-

30 K for both averages. Although enough

coverages have not yet been studied, it is antici- pated that a fairly constant and large value of pa- ramagnetic Curie temperature will characterize all bet the smallest sub-monolayers. This is because,on Grafoil, oxygen molecules adsorbed at several tens of degrees absolute should form "islands" in which

Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphyscol:19786148

(3)

the local environment of a molecule is fairly un- changing. Thus, the effective coverage is constant

-

only the total amount of oxygen adsorbed varies.

In the case of oxygen on Vycor, at low coverages the data tend toward Curie-like behavior appro- priate to a system of non-interacting spins. With increasing coverage they become more characteristic of an amorphous antiferromagnetic system, with in- creasingly negative paramagnetic Curie temperatures and excess low-temperature susceptibility.

It appears that the first monolayer on

Vycor is constrained to be .amorphous by the subs-

trate forces. Interesting hysteresis effects in the susceptibility dependence on temperature are observed with coverages greater than one monolayer /I/ which might be explicable in terms of competi- tion between ordering tendencies in upper layers and the requirements of the interface with the dis- ordered first layer. The absence of these particu- lar effects in the oxygen-Grafoil system is, there- fore, not unexpected. Further experiments are planned to investigate the development of the hys- teretic behavior at higher coverages using porous glass with larger pore sizes.

This work is supported by the Department of Energy through Contract No. EY-76-S-02-3151, Technical Report No. COO-3151-82.

References

/ I / Gregory, S. Phys. Rev. Lett.

2

(1977) 1035.

/2/ Gregory, S. Phys. Rev. Lett.

40

(1978) 723.

/3/ Mctague, J.P. and Nielsen, M. Phys. Rev. Lett.

37 (1976) 596.

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