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New sulfur-fullerite; its preparation, structure and spectral properties
N. Kushch, I. Majchrzak, W. Ciesielski, A. Graja, K. Woźniak, T. Krygowski
To cite this version:
N. Kushch, I. Majchrzak, W. Ciesielski, A. Graja, K. Woźniak, et al.. New sulfur-fullerite; its prepa-
ration, structure and spectral properties. Journal de Physique I, EDP Sciences, 1993, 3 (10), pp.1987-
1991. �10.1051/jp1:1993226�. �jpa-00246846�
Classification
Physics
Abstracts61.50 61.10
Short Communication
New sulfur-filllerite; its preparation, structure and spectral properties
N-D- Kushch
(~,*),
I.Majchrzak (~),
W. Ciesielski(~),
A.Graja (~),
K.Wofniak(~)
andT-M-
Krygowski (~)
(~) Institute of Molecular Physics, Polish Academy of Sciences, 60-179 Poznah, Poland
(~) Department of Chemisty, University of Warszawa, 02-093 Warszawa, Poland
(Received
8 July 1993, accepted in final form 3 August1993)
Abstract. The preparation and unit cell parameters of a novel fuflerene-containing com- pound,
(C60)6S80.C2HC13,
is described. The compound is orthorhombic with a=
10.512(6) I,
b
=
21.072(26)
I and c =38.985(50)I.
The UV-VIS-NIR-IR spectra of the compound are analysed. It is concluded that the new sulfur-fuflerite is true van der Wafls solid without stronginteractions between the constituent molecules.
1 Introduction.
Fullerenes and
especially
theirderivatives,
so-called fullerites have attracted considerable atten- tion in many scientificdisciplines. Recently,
a newfamily
of C60compounds,
which combine fullerene molecules with 58rings
and have thegeneral
formulaC2n(58)m
has beensynthe-
sized
[1-4].
Roth and Adelmann havereported
a heteromolecularcompound, CmS48,
com-prising
orderedCm
molecules andcrown-shaped
58rings
in a structure withpronounced
two-dimensional features
iii.
German [2] andindependently
Russian scientists [3] haveprepared
anew
fullerene-containing
van der Wallscompound,
C60S16 in which the C60 molecules from a three-dimensional framework with one-dimensional channelscontaining crown-shaped
58rings.
The solvent
containing compound, C60S6CS2
has been obtainedrecently
[4].C60S8CS2
hasa framework stucture with
58 rings
andCS2
dumb-bellsfilling
the channels.Unfortunately, physical properties
of whichever ones are not yet known.(*)
Permanent address: Institute of Chemical Physics, Russian Academy of Sciences, 142432Chernogolovka, Russia.
1988 JOURNAL DE PHYSIQUE I N°lo
Here,
we describe thepreparation, preliminary X-Ray
measurements and basicspectral properties
of(C60)6S80.C2HC13,
a new member of the sulfur-fullerites.2
Experimental.
C60 was
prepared
andseparated by
the usual method: an electric arc betweengraphite
elec- trodesburning
in a heliumatmosphere,
fullerene extraction with hottoluene, separation
of C60 andCm by liquid chromatography (n-hexane
+ 5~toluene)
on neutralA1203
IS,6].
New sulfur-fullerite
(C60)6S80.C2HC13
was grown from a solution of stoichiometric amounts of C60 and sulfur intrichloroethylene,
at room temperature. C60(21.6
mg, 2x10~SM)
was dis-solved under argon
atmosphere
in IS ml offreshly
distilledtrichloroethylene.
Sulfur(12.8
mg,4 x
10~~M)
dissolved in 2 mltrichloroethylene,
under argonatmosphere
was added and mix- ture was heated about 4 h. The solution was filtered and cooled downslowly
in Dewar toroom temperature. Slow
evaporation
of the solvent gaveblack, shining crystals
withtypical
dimensions up to i mm.Elemental
analysis
of the sulfur-fullerite(Found: C,
61.5;S, 37.47; H,
< 0.01 andCl,
1.03. Calculated:
C,
61.95;S,
36.51;H,
o.oi andCl, 1.52.)
suggests thecompound
formula(C60)6S80'C2HC13.
X-Ray crystallographic
measurements on thesingle crystal
wereperformed
atR-T-,
with 4-circle diffractometer KUMAusing
CUK~ radiation. Thecoumpound
isorthorhombic,
spacegroup C2 mm with a
=
10.512(6) I,
b=
21.072(26) I
and c=
38.985(50) I.
It is necessary to add that cellfilling
coefficient for(C60)6S80.C2HC13 crystal
iso.45,
I-e- somewhat smallerthan in the case of similar
crystal
structures such asCmS48 (n
"
o.52), C60(CC14)2 (n
"0.59),
C60(n-C5H12)o.88.(C7H8)o.05 (n
"0.61),
C60S16(n
"
0.62)
andC60S8.CS2 (n
"0.65).
Infrared
powder
spectra in the range of 4000-400 cm~~ were recorded in KBrpellets
with Perkin Elmer 1725 X FT IR spectrometer. UV-VIS-NIR spectra were taken in KBrpellets
andC2HC13
solution with SPECORD apparatus. ESR was measured inpolycrystal sample using SE/X
2544 X-band spectrometer madeby Radiopan.
The measurements wereperformed
at room temperature. Some IR spectra were taken after asample heating
tohigh
temperature in order toinvestigate
adecomposition
of thecomplex.
Thermal
stability
of thecrystals
was evaluatedby microscope
observation andsupplementary
verifiedby
IR spectroscopy. Themicroscope
observations have beenperformed
on a 3 mgsample
in the airatmosphere using
5K/min heating
rate in the temperature range of 300- 650 K.3.
Spectral properties.
Electronic and vibrational spectroscopy is a
powerful
method forstudying
the interactions in the solid state betweenC60,
sulfur and solvent moleculesholding
thecompound together.
Optical
spectra are sensitive indicators ofcharge
distribution among thecomplex
components.In
particular,
it ispossible
to detect acharge
transfer and a presence of C60 ions. On the otherhand,
the infrared spectroscopy should be sensitive to subtle deformations of thecomplex
components. It isimportant
for C60 derivatives because these deformations should reduce thehigh
symmetry of the fullerene. IR spectroscopy shouldgive
some information on the sulfurconfiguration
as well as on the solvent content.The VIS and NIR spectra of
(C60)6S80.C2HC13
intrichloroethylene
solution are very close to the spectra of pureC60.
We detect neither the bands characteristic forC(p
nor a shift of' '
2
~
~ l
J5
~
w o c
a ,
4
I~ b
4
~ i ,,"",,
," '~'"
i ," ',
' _,, ,
',-"
' O
30000 2sooo 20000 isooo
Frequency cm~~l
Fig. I. Electronic spectra of C60 in toluene
(a),
and(C60)6S80.C2HC13
in KBr pellet(b)
at room temperature.~
fW f
~ ,., '... .-~ -'
~ ~l
3 b
c
U
#W
fl
©O
1800 1600 1400 1200 1000 800 600 400
Frequency (crrl)
Fig. 2. Infrared absorption spectra of sulfur (a), and
(C60)6580.C2HC13
complex(b) in KBr pellet,at room temperature.
the
absorption edge.
On the contrary, the spectra recorded in KBrpellets (Fig. i)
reveal an appearance of a newabsorption
band in theregion
19000-23000 cm~~. It suggests that C60 ispartly
ionized in thecomplex
and the band centered at about 21000 cm~~ should beassigned
to a CT band. Thus it seems that the sulfur-fullerite is a very
weakly
bondedcomplex.
On the other hand the electron
spin
resonance measurementsperformed
onpolycrystalline sample
reveal a weak and narrow ESRline,
with g = 2.0016. The line withg-factor
value lower than the free electronvalue,
should beassigned
to C60 anion. A similar line was observedby Greaney
and Gorun [7] at g= 2.0002. A
large g-value depression
wasexplained by
aspin-orbit coupling.
It isinteresting
to notice that in(C60)6S80.C2HC13
the spins are localized on theC60,
contrary to the situation in the(BEDT-TTF)2C60 complex
[8] where thespins
are ratheron the
organic
cation.The infrared spectrum of
(C60 )S80.C2HC13
shown infigure
2 isessentially
asuperposition
of1990 JOURNAL DE PHYSIQUE I N°lo
Frequency (crr~)
Fig. 3. Infrared absorption spectra of C60
(a),
sulfur(b)
and (C60)6S80-C2HC13 complex(c)
in theneighborhood of two C60 bands "feeling" the complex formation.
the spectra of
C60,
sulfur andC2HC13.
The spectrum shows some smallfrequency shifts,
about 2cm~~
orless,
as isexpected
of thecomplex
with smallcharge
transfer. The IR spectrum of pure C60 consists of four narrow bands at527, 576,
i183 and 1429 cm~~. Two last bands appear in the spectrum of(C60)6S80.C2HC13
without anychanges.
The band at 576 cm~~ is shifted to 578 cm~~ and broadened from 4 to 6 cm~~(Fig. 3). Insignificant broadening
andshifting
is also observed for 527cm~~
band. It is characteristic that no new modes emerge,arguing
that C60 symmetry is retained. These results show that the nature of ourcomplex
iscompletely
different from that of the A6C60compounds (A
= K,
Rb).
Fu et al. [9] observed thatabsorption
intensities, band positions overall and some modes(e.g.
1429cm~~)
inparticular,
are
strongly changed
inA6C60 crystals.
The bands of the enhanced modes aresignificantly
broadened. These results
suggested
that the vibronicdynamics
in A6C60 arestrongly
modifiedin contrast to our observation for
(C60)6S80.C2HC13.
A characteristic
absorption
band ofcrown-shaped
58rings
at 468 cm~~ in the pure sulfur is somewhat shifted(up
to 470cm~~)
and broadened. Other bands of58 (e.g.
667cm~~) keep
their
frequency
and form.The IR spectrum of the
complex
includes also very weak bandscorresponding
to the strongestabsorption
bands of the solvent.C2HC13
strongest bands at 927, 844 and 788 have their counterparts at927,
839 and 774 cm~~. These resultstestify
the solvent inclusion within thecrystal
andspecific
interactions between the chlorine atoms of thetrichloroethylene
and(C60)6S80
franiework.All these observations suggest that
(C60)S80.C2HC13 complex
ismostly molecular, perhaps
those of
C(p,
where « 1. C60 is very little modified in thecomplex
and testifies that thecharge
transfer is small. Conclusions drawn from thespectral investigation
of(C60
)6S80.C2HC13
are close to that for other C60
compounds [8-1ii. Decomposition
of thecompound
occurs in the range of about 380-490 K. An intensive liberation of the sulfurbegins
at about 460 Kresulting
in about 25 To mass loss. It means that after thermaltreating
the solvent androughly
about 65 To of the sulfur is lost. Infrared spectrum of a heatedsample (Fig. 4)
shows that except sulfur and solvent losses new components appear. It suggests that sulfur reacts with an oxygen and a carbon. The main new bands observed in the heated anddecomposed complex
are:iogg
cm~~
(UC=S,),
io32 cm~~iv S=O)
and 712 cm~~iv C-S).
3~ b
<
~
g +
W
E
Iw
©
a
l100 1000 900 800 700
Frequency (crrl )
Fig. 4. Infrared spectra of freshly prepared
(C60)6S80.C2HC13 complex(a)
and afterheating (b).
4. Conclusion.
A new
complex
ofC60 withsulfur, containing
the solventmolecules,
has beensynthesized.
From thespectral
observation we think that thecrystals
of the newsulfur-fullerite,
as fullereneitself,
are true van der Waals solid without
strong
interaction between the constituent molecules. AnX-Ray crystallographic analysis
and studies ofphysical properties
of(C60)6S80 .C2HC13 complex
are now in progress.
Acknowledgements.
We thank Dr. R.
§wietlik
for discussions.References
ii]
Roth G. and Adelmann P., J. Phys. I Hance 2(1992)
1541.[2] Roth G. and Adelmann P., App. Phys. A56
(1993)169.
[3] Buravov L-I-, Oyachenko O-A-, Konovalikhin S-V-, Kushch N-D-, Lavrentiev I-P-, Spitsyna N.G., Shilov G-V- and Yagubskii E.B., Mendeleev Commun.
(in press).
[4] Roth G., Adelmann P. and Knitter R., Mater. Lett.,
(in
press).[5] Kritschmer W., Lamb L-D-, Festiropolous K. and Huflmann D-R-, Nature 347
(1990)
354.[6] Ciesielski W. and Majchrzak I., Wiadomold Chemiczne
(in preparation).
[7] Greaney M.A. and Gorun S.M., J. Pl~ys. Cl~em. 95
(1991)
7142.[8] Laukhina E.E., Majchrzak I., Ciesielski W. and Graja A., J. Chem. Soc., Chem. Commun.
(subnfitted).
[9] Fu K.-J., Karney W.L., Chapman O.L., Huang S.-M., Kaner R-B-, Diederich F., Holczer K. and Wl~etten RI., Phys. Rev. 846
(1992)1937.
[10] Pradeep T., Singh K.K., Sinha A.P.B. and Morris D-E-, J. Cl~em. Sac., Cl~em. Commun.
(1992)
1747.
Ii
II Kamar£s K., Breitscl~werdt A., Pekker S., Fader-Csorba K., Faigel G. and Tegze M., Appl. Pl~ys.A56