PHYSICA
Physica C 180 (1991) 3 4 - 3 7 North-Holland
SPUTTERED YBa2Cu30 z THIN FILMS ON SAPPHIRE AND SILICON S U B S T R A T E S Y T T R I A STABILIZED ZrO 2 B U F F E R LAYERS H. SCHMIDT*,
K. HRADIL*,
*Siemens AG, Corp° +Siemens AG, Corp.
G. GIERES +' W. HOSLER*,
Research Research
and Development, and Development,
USING
AND Oo EIBL*
P.O.Box 830953, 8000 M~nchen 83, FRG P00.Box 3220, 8520 Erlangen, FRG
YBazCu30 x thin films w e r e d e p o s i t e d by sputtering on (1i02) sapphire and (i00) sillcon using an i n t e r m e d i a t e buffer layer of Y - s t a b i l i z e d ZrO 2 (YSZ). On sapphire the YSZ layer and the YBa2Cu.O grew epitaxially as was c o n f i r m e d by ion channeling and RBS. The c - o r i e n t e d ~ a 2 C u 3 0 x films had a T e of up to 90 K and je was 0°51.4 * 10 ° A / c m ~ at 77 K in zero m a g n e t i c field° On silicon the YSZ and the YBa2Cu30 x layer were h i g h l y textured, but polycrystalline° These YBa2Cu30 x films had T c values of up to 79 K.
i. I N T R O D U C T I O N For the i n t e g r a t i o n
were grown at substrate temperatures in m i c r o e l e c t r o -
nics and for m i c r o w a v e
applications
ranging
from 520 °C to 780 °C. The gas
pressure
in the d e p o s i t i o n
chamber was
Y B a 2 C u 3 0 x thin films have to be deposi-
1.6 Pa w i t h the gas c o n s i s t i n g
ted on s i l i c o n and on sapphire.
argon and 10% oxygen.
epitaxial
Direct
about
growth of Y B a 2 C u 3 0 x thin temperatures
interdiffusion
at e l e v a t e d
ted. U s i n g the same d e p o s i t i o n param e t e r s YSZ films were also d e p o s i t e d
which deteriorates
superconducting
100 nm thick films were deposi-
is hindered by
films on these substrates substrate
of 90 %
During one hour
properties.
the
Therefore,
Si-substrates
on
covered by native oxide.
The Y B a 2 C u 3 0 x thin films were deposited either by p l a n a r r f - m a g n e t r o n
sput-
w h i c h acts as d i f f u s i o n b a r r i e r and al-
tering or by p l a n a r DC sputtering.
For
lows the e p i t a x i a l
the d e p o s i t i o n
an e p i t a x i a l
b u f f e r layer is required growth of Y B a 2 C u 3 0 x
films w i t h high critical ties.
current densi-
Up to n o w MgO I and SrTi032 were
found as suitable b u f f e r layers on sapphire,
whereas
Y-stabilized
(YSZ) was used s u c c e s s f u l l y con 3,4.
ZrO 2
on sili-
In this study cubic YSZ was in-
rf-magnetron
of Y B a 2 C u 3 0 x films by
sputtering
stoichiometric
a ceramic non-
target w i t h c o m p o s i t i o n
Y B a 2 C u 3 . 3 0 x was used. The Cu rich target was chosen b e c a u s e p r e v i o u s l y deposited films w e r e found slightly poorer in their copper content compared to the
s u b s t r a t e materials.
target c o m p o s i t i o n 5o The YBa2Cu30 x films were grown at a gas pressure of
2. E X P E R I M E N T A L
parts argon and one part oxygen.
vestigated
as b u f f e r layer for both
70 Pa w i t h the gas consisting
The YSZ b u f f e r
layers were d e p o s i t e d
by p l a n a r r f - m a g n e t r o n
sputtering using
a target of Y - s t a b i l i z e d sapphire
and
substrates.
ZrO 2.
(i102)
(I00) silicon were used as The YSZ films on sapphire
epitaxial perature position.
of two
film growth a substrate
For tem-
of 740°C was chosen during deThe D C - s p u t t e r e d
YBa2Cu30 x
films were d e p o s i t e d in a separate sputter chamber with a diode configura
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All rights reserved.
H. Schmidt et al. / Sputtered YBa2Cu30x thin films on sapphire and silicon substrates
35
tion 6. For the deposition on YSZ/
600 °C and 720 °C were only weakly
sapphire the DC glow discharge ran in
textured,
pure oxygen at a pressure of 200 Pa
780 °C were single-crystalline.
yielding a deposition rate of 2nm/min.
crystal quality of the YSZ films was
whereas
films deposited at The
The distance between the target and the
also studied by ion channeling combined
substrate was 30 mm. In this case the
with Rutherford Backscattering Spectro-
substrate temperature was 720 °C. After
metry
deposition the YBa2Cu30 x films were
energy the minimum backscatter yield
cooled to room temperature in pure oxy-
(chimin)
(RBS). Using He ions of 2 MeV from the YSZ films was 0.06 to
gen at atmospheric pressure in about 30
0.09 of the yield for non-aligned
minutes.
orientation.
These values are compar-
able to values measured on single-crystals of reasonable perfection and con-
3. RESULTS AND DISCUSSION 3.1 YBa2Cu30 x ON YSZ/AI203 X-ray diffraction proved that all YSZ films were single phase and (h00)-ori-
firm the epitaxial growth of the YSZlayer on (li02)-sapphire.
The increase
of the backscatter yield at the inter-
ented except the YSZ film grown at
face between sapphire and YSZ is caused
520 °C. This film showed
by defects originating from the mis-
(hhh) reflec-
tions in addition to the (h00) reflec-
match between the (ii02) plane of hexa-
tions. YSZ films deposited between
gonal sapphire and the (001) plane of
FIGURE 1 High resolution TEM image of the YBa2Cu3-YSZ interface showing an intermediate BaZr03 layer
/ Sputtered
H. Schmidt et aL
36
cubic YSZ. At this interface mechanical
YBa2Cu30 . thin films on sapphire and silicon substrates
stoichiometry.
local
strain fields were also ob-
served by t r a n s m i s s i o n
electron micro-
scopy 7 .
Y B a 2 C u 3 0 x films were also deposited by DC-sputtering
on sapphire with YSZ buf-
fer layers 8. X - r a y d i f f r a c t i o n
The i n t e r f a c e Y B a 2 C u 3 O x / Y S Z
was studied
on a Y B a 2 C u 3 0 x film w h i c h was d e p o s i t e d by r f - m a g n e t r o n deposition
sputtering.
During the
of the Y B a 2 C u 3 0 x film at a
temperature
of 740 °C a 3-5 nm thick
intermediate
BaZrO 3 layer was formed
proved
that these films were h i g h l y c-textured.
Ion c h a n n e l i n g
on these films
showed a chimi n of 0.16
(Figure2) which
confirmed
growth of the
the epitaxial
Y B a 2 C u 3 0 x layer.
The 350 nm thick films
b e t w e e n the YSZ and the Y B a 2 C u 3 0 x (Fi-
had a T c of 90 K and Jc values of 1.21.4,106 A / c m 2 at 77 K in zero magnetic
gure i). The s t r a i g h t n e s s
field.
Y B a 2 C u 3 0 x lattice planes exhibits
of the in Figure 1
the good c r y s t a l l i n e
of the s u p e r c o n d u c t i n g the i n t e r m e d i a t e
quality
layer although
BaZrO 3 layer consists
3.2 Y B a 2 C u 3 0 x on Si/YSZ YSZ films d e p o s i t e d on Si(100) strates highly line.
of small regions with slight spread
sub-
covered by native oxide were (100)-textured,
but p o l y c r y s t a l -
The r f - s p u t t e r e d
Y B a 2 C u 3 0 x films
(max. 5 ° tilt)
in their orientation.
on these b u f f e r layers were c-oriented
Ion-channeling
on this c-oriented
and also p o l y c r y s t a l l i n e 9 . Deposited at
Y B a 2 C u 3 0 x film r e s u l t e d in a chimi n of 0.19 and the c o m p o s i t i o n was d e t e r m i n e d
800 °C these films had a T c of only
by RBS as Y0.gBa2.1CU3Ox.
sputtering
The m e a s u r e d
60 K, whereas pressure
films d e p o s i t e d by DC-
in pure oxygen with a gas
of 350 Pa at a lower substrate
T c of only 84 K and the reduced Jc of 5"105 A / c m 2 at 77K are a t t r i b u t e d to
temperature
the d e v i a t i o n
For an e p i t a x i a l
from the exact cation
of 685 °C had a T c of 79 K. growth of YSZ and
Y B a 2 C u 3 0 x the amorphous Energy 1.0 T
o.5 [
60
ved b y HF e t c h i n g or by e v a p o r a t i n g
(MeV) 1.5 I
2.O F
SiO 2 above now,
IC u i Ii [I i ;
E o = 2.0 MeV ~Z
i
r~l
non-epitaxial
i00
whereas e--beam
e v a p o r a t i o n 4,10 and laser ablation 3 are
I I
0
of
film growth could not be
(see alsol0),
known to result in epitaxial
,'i'f,I ,,/
the r e o x i d a t i o n
I, iB a
i
J
for
the silicon surface and c o n s e q u e n t l y a
L/ r a n d o m
\ :~
the
But up to
a p p l y i n g the sputter process
avoided
I oI
1100 °C in vacuum.
the YSZ d e p o s i t i o n y
':I
SiO 2 was remo-
/'< '
200
i \~L
YSZ films
on silicon. channeled
L
300
400
Channel
4. C O N C L U S I O N S Using Y - s t a b i l i z e d
ZrO 2 as buffer
layer Y B a 2 C u 3 0 x films with high critiFIGURE
2
RBS s p e c t r u m of the e p i t a x i a l YBa-Cu30 • Z X f~im on Y S Z / s a p p h i r e for r a n d o m orientation and for c h a n n e l i n g in <001>
cal current densities ter-deposited w h i c h makes
have been sput-
epitaxially
it a p r o m i s i n g
on sapphire, substrate
14. Schmidt et aL / Sputtered YBaFu30x thin films on sapphire and silicon substrates for superconducting
passive microwave
devices. Up to now the in-situ reoxidation the pre-cleaned
of epitaxial
YSZ
films on silicon.
The authors
thank B. Jobst for X-ray
diffraction
analyses,
technical
4. H. Myoren, Y. Nishiyama, N.Miyamoto, Y. Kai, Y. Yamanaka, Y. Osaka, and F. Nishiyama, Jap. J. Appl. Phys. 29 (1990) 955 5. H. Schmidt, R. Bruchhaus, O. Eibl, W. H6sler, L. Hofmann, W. Holubarsch, and G. Zorn, J. Less-CommonMet., 151 (1989) 411
ACKNOWLEDGEMENTS
patterning
3. D.K. Fork, A. Barrera, T.H. Geballe, A.M. Viano, and D.B. Fenner, Appl. Phys. Lett. 57 (1990) 2504
of
silicon has prevented
the sputter-deposition
G. Daalmans
for
the films and B. Sipos for assistance
concerning
6. H. Behner, G. Gieres, and B. Sipos, Proceed. ICMC'90, Topical Conf. High Temperature Superconductors, May 1990, Garmisch-Partenkirchen
the
sputter deposition of YBa2Cu30 x films. This work was supported by the BMFT,
7. O. Eibl, K. Hradil, in print
Federal Ministry
8. H. Schmidt, K. Hradil, W. Wersing, G. Gieres, Seeb6ck, in print
logy
37
of Science and Techno-
(13N5812).
REFERENCES i. A.B. Beresin, C.W. Yuan, and A.L. de Lozanne, Appl. Phys. Lett. 57 (1990) 90 2. K. Char, N. Mewman, S.M. Garrison, R.W. Barton, R.C. Taber, S.S. Laderman, and R.D. Jacowitz, AppI. Phys. Lett. 57 (1990) 409
and H. Schmidt, W. H6sler, and R.J.
9. H. Schmidt, O. Eibl, and B. Jobst, Proceed. ICMC'90, Topical Conf. High Temperature Superconductors, May 1990, Garmisch-Partenkirchen 10.H. Fukomoto, M. Yamamoto, and Y. Osaka, Proceedings Electrochemical Society 90-7 (1990) 239