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Structural and optical characterization of nanostructured ZnO grown on alumina templates

Abstract

The growth of nanostructured ZnO thin films on nanoporous anodic alumina substrates (NAAF) by dc reactive magnetron sputtering using a pure Zn metal target is reported. ZnO nanostructures reproduce the pore arrays of the NAAF substrates used as templates mimicking their hexagonal long range order. Stoichiometric nanostructured ZnO samples were grown with wurtzite type structure, highly textured and oriented in the (002) direction. The study of the NAAF pore size effect in the final morphology and optical properties of the nanostructured ZnO is presented for different ZnO thicknesses. The pore size of the nanostructured ZnO films was controlled in the range of 15–65 nm by choosing appropriate NAAF and the sputtering deposition conditions. The broademission band observed in PL spectra of the samples should be associated with color centers transitions (F and H centers) appearing in the alumina templates.

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Structural and optical characterization of nanostructured ZnO grown on alumina templates

Author: Yuste, M.; Escobar-Galindo, Ramón; Martínez Sacristán, O.; Mínguez Bacho, I.; Rodríguez Sánchez, Sonia; Hernández Vélez, Manuel; Sánchez, O.
Publisher: IOP Science
Year: 2014
DOI: 10.1088/2053-1591/1/4/045028
Source: https://idus.us.es/bitstreams/d488c6ee-ff61-4080-b2c5-df6d00a65465/download
S uc u al and op ical cha ac e iza ion o
nanos uc u ed ZnO g own on alumina empla es
M Yus e
1
, R Escoba Galindo
1
, O Ma ínez Sac is án
3
, I Mínguez-Bacho
1
,
Sonia Rod iguez
2
, M He nández-Vélez
2
and O Sánchez
1,4
1
Ins i u o de Ciencia de Ma e iales de Mad id (CSIC), Spain
2
Uni e sidad Au ónoma de Mad id, Spain
3
UGdS-Op onlab G oup, Dp o. Física Ma e ia Condensada, Uni e sidad de Valladolid, Paseo
de Belén 11, 47011—Valladolid, Spain
E-mail: [email p o ec ed]
Recei ed 29 July 2014, e ised 3 Oc obe 2014
Accep ed o publica ion 24 Oc obe 2014
Published 12 No embe 2014
Ma e ials Resea ch Exp ess 1(2014) 045028
doi:10.1088/2053-1591/1/4/045028
Abs ac
The g ow h o nanos uc u ed ZnO hin films on nanopo ous anodic alumina
subs a es (NAAF) by dc eac i e magne on spu e ing using a pu e Zn me al
a ge is epo ed. ZnO nanos uc u es ep oduce he po e a ays o he NAAF
subs a es used as empla es mimicking hei hexagonal long ange o de .
S oichiome ic nanos uc u ed ZnO samples we e g own wi h wu zi e ype
s uc u e, highly ex u ed and o ien ed in he (002) di ec ion. The s udy o he
NAAF po e size e ec in he final mo phology and op ical p ope ies o he
nanos uc u ed ZnO is p esen ed o di e en ZnO hicknesses. The po e size o
he nanos uc u ed ZnO films was con olled in he ange o 15–65nm by
choosing app op ia e NAAF and he spu e ing deposi ion condi ions. The b oad
emission band obse ed in PL spec a o he samples should be associa ed wi h
colo cen e s ansi ions (F and H cen e s) appea ing in he alumina empla es.
Keywo ds: nanos uc u ed ZnO, nanopo ous anodic alumina, magne on
spu e ing
1. In oduc ion
Zinc oxide (ZnO), wi h band gap o 3.37 eV a oom empe a u e (RT) and la ge exci onic
binding ene gy, a ound 60 meV, has a ac ed inc easingly wo ldwide a en ion in he pas ew
decades due o i s unique p ope ies and a la ge numbe o po en ial applica ions such as
anspa en conduc i e con ac s [1], sola cells [2], lase diodes [3], ul a iole lase s [4], hin
4
Au ho o whom any co espondence should be add essed.
Ma e ials Resea ch Exp ess 1(2014) 045028
2053-1591/14/045028+16$33.00 © 2014 IOP Publishing L d
film ansis o s [5], hin-film gas senso s [6] and op oelec onic and piezoelec ic applica ions o
su ace acous ic wa e de ices [7–9]. ZnO films g own on Si subs a es ha e been widely
epo ed, howe e , ZnO nanos uc u ed hin films show e y in e es ing addi ional p ope ies in
compa ison o con inuous hin films [10,11]. Those p ope ies a e likely o be al e ed and
con olled by he ZnO g ow h p ocesses [12] such ha many esea ch g oups ha e epo ed he
syn hesis o ZnO nanos uc u es by means o bo h bo om-up and op-down echniques, among
hem, chemical apou deposi ion (CVD) [13], molecula beam epi axy (MBE) [14],
elec ochemical deposi ion [15], e apo a ion and RF spu e ing [16].
Magne on spu e ing echniques ha e been success ully used in he deposi ion o
unc ional ma e ials such as, TiN [17] and TiO
2
[18] on nanos uc u ed empla es achie ing a
con o mal ep oduc ion o he main ea u es o he subs a e su aces. This echnique gi es
di ec ly he equi ed nanos uc u ed ma e ial wi hou addi ional ea men a e he deposi ion
p ocess. In addi ion, his echnique allows de eloping deposi ion p ocesses wi h high s abili y
and pu i y con ol o he final p oduc s. Mo eo e , he nanos uc u es a e ab ica ed using a
acuum-based echnique o e ing a highe le el o p ocess s abili y and pu i y con ol han in
he case o solu ion based me hods.
In his wo k, we epo he g ow h o nanos uc u ed ZnO hin films on nanopo ous anodic
alumina films (NAAFs) used as empla es, by dc magne on spu e ing. The su ace
mo phology and s uc u al p ope ies o he ZnO nanos uc u es we e cha ac e ized by means
o field-emission scanning elec on mic oscopy (FESEM), a omic o ce mic oscopy (AFM) and
x- ay di ac ion (XRD). The chemical composi ion was de e mined by RBS (Ru he o d
backsca e ing spec ome y). The op ical p ope ies we e de e mined by UV- isible spec o-
pho ome y and pho oluminescence (PL) measu emen s.
The use o dc magne on spu e ing echnique allows us o p oduce ma e ial deposi s wi h
g ain sizes smalle han 30–40 nm which is an ad an age wi h espec o o he physical
deposi ion echniques. In he ea ly s ages o he deposi ion, he complex s uc u es o he elie
pa e n a e pe ec ly co e ed by small pa icles o ma e ial o be deposi ed, g owing a laye o
ma e ial on ‘con o mal con ac ’wi h he pa e n whose su ace is ep oduced wi h high
e ficiency [17]. The combina ion o dc magne on spu e ing echnique and anodiza ion
echniques o p oduce ZnO nanos uc u es p o ides an economical s a egy o ob ain ZnO
nanoma e ials.
2. Expe imen al de ails
ZnO films we e g own by using a home-made high acuum dc magne on spu e ing sys em on
NAAF empla es. The spu e ing ca hode consis s o a s anda d ci cula plana magne on wi h
a high pu i y comme cial Zinc a ge (99.99%), 3-in. diame e and 0.125-in. hickness. All
expe imen s we e pe o med in oducing a mix u e o A (99.999%) and O
2
(99.992%) in he
acuum chambe a a cons an o al gas flow (A + O
2
) o 30 sccm. The chambe was pumped
ou o a base p essu e o 2 · 10
−6
mba and he wo king p essu e was app oxima ely o
3·10
−3
mba . Du ing he deposi ion p ocess he ela i e O
2
gas concen a ion in he eac i e
a mosphe e (p
O
2
) was main ained a 50%, he a ge powe a 50 W and he a ge -subs a e
dis ance a 20 cm.
NAAF empla es we e p epa ed by ollowing he wo-s ep anodiza ion p ocess desc ibed
elsewhe e [19]. Sul u ic and oxalic acid solu ions we e used as elec oly es in he anodiza ion
2
Ma e . Res. Exp ess 1(2014) 045028 M Yus e e al
p ocesses. Table 1summa izes he po e sizes, Φ, and in e -po e dis ances, D
in
. o he NAAF
used as subs a es. In o de o pe o m he op ical cha ac e iza ion o he samples (in
ansmi ance mode) he aluminum back subs a es we e emo ed by an e ching p ocess using
an acid solu ion (CuCl
2
/HCl). These s uc u es exhibi high op ical anspa ency in he UV-
isible anges and high chemical and he mal s abili y which makes hem e y sui able o use
as subs a es-pa e ns, as will be shown la e .
RBS expe imen s we e ca ied ou o elucida e he chemical composi ion o he deposi ed
ZnO films. RBS we e pe o med using he 5MeV HVEE Tande on accele a o loca ed a he
‘Cen o de Mic o-Análisis de Ma e iales o Uni e sidad Au ónoma de Mad id’. The samples
we e i adia ed wi h 3.035 MeV He
+
ions o make use o he c oss sec ion esonance
16
O(α,α)
a ha pa icula ene gy and, he e o e, o imp o e he sensi i i y o oxygen nucleus. The
chemical composi ion o he ZnO films has been ex ac ed using he RBX so wa e [20].
C ys alline s uc u e o he films was de e mined by XRD using a Cu anode (Cu
K
α
= 1.54 Å) egis e ed unde g azing incidence condi ions wi h an incidence angle o 0.7° a
oom empe a u e. The XRD measu emen s we e pe o med on a Siemens D-5000
di ac ome e . The su ace and ac u e c oss-sec ion mo phologies o he hin films we e
examined by a No a NanoSEM 230 FEG scanning elec on mic oscope (HRSEM). An AFM
sys em om Nano ec Elec ónica S. L. wo king in non-con ac mode a ambien condi ions was
also used o cha ac e ize he su ace mo phology o he samples.
Op ical cha ac e iza ion o NAAFs is no abundan in he cu en li e a u e and hei
influence on he op ical p ope ies o unc ional hin films deposi ed on hem has been sca cely
epo ed. Ce ainly i is no an easy ask. The e o e, as a fi s app oach, we made a s udy o he
op ical beha iou o he NAAF empla es used in his wo k o comple eness a e he op ical
cha ac e iza ion o he ZnO/NAAF samples. T ansmi ance measu emen s we e acqui ed in a
SolidSpec-3700 nea UV- isible and nea in a ed ange (190–1500 nm) spec opho ome e . PL
spec a we e ca ied ou by means o a LabRAM sys em om Ho iba Jobin-Y on, model
HR800 UV, wi h an He–Cd lase (325 nm) as he exci a ion ligh sou ce.
3. Resul s and discussion
3.1. ZnO nanos uc u es
P io o he g ow h o ZnO on NAAF empla es we pe o med a s udy o op imize he
expe imen al condi ions o g owing his compound o ming well defined nanos uc u es on he
selec ed empla es displayed in able 1.
Table 1. Po e size and in e -po e dis ance o he NAAF subs a es.
NAAF Φ(nm) D
in
(nm)
M0 15 44
M1 15.5 45
M2 18 51
M3 21.5 57
M4 25 65
M5 35 105
M6 50 105
3
Ma e . Res. Exp ess 1(2014) 045028 M Yus e e al
In ag eemen wi h ou esul s p e iously epo ed [21], he expe imen al spu e ing
condi ions chosen in his wo k led o he g ow h o nea ly s oichiome ic ZnO films a a low
deposi ion a e (8 nm min
−1
) which enhanced he con o mal cha ac e o he spu e ing
echnique. Hence, unde hese condi ions, 150 nm o ZnO we e g own on M4 and M5 samples
wi h o de pa ame e s alues (Φand D
in
) in he in e media e ange o he p e iously ab ica ed
NAAFs (see able 1).
Figu e 1shows ypical sec ional HRSEM images o M4 (a) and M5 (b) NAAFs a e
spu e ing o ZnO films. The g ow h o nanos uc u ed ZnO films is clea ly shown ep oducing
he po e a angemen o NAAFs pe pendicula ly o he Al subs a es. The x- ay di ac og ams
co esponding o M4 and M5 samples coa ed wi h ZnO a e displayed in figu e 2. In bo h
spec a, signals o cubic aluminum phase [22] (JCPDS ca d No. 40–787) coming om he
aluminum disk used o g ow he NAAF empla es a e p esen . Fo compa a i e pu poses
figu e 2also shows he spec um o a ZnO film 150nm hick g own in he same condi ions on
Silicon 〈100〉. Acco ding o ou p e ious esul s [21], ZnO film on silicon p esen s wu zi e
ype s uc u e, highly ex u ed and o ien ed in he 〈002〉di ec ion. The mean c ys al size alue
in ha p e e ed di ec ion was es ima ed in 22 ± 5 nm by using Sche e ’s o mula [23]. When
ZnO is deposi ed on he NAAF empla es, he 〈002〉p e e ed o ien a ion emains o bo h
coa ings bu wi h a g ea e FWHM han hose exhibi ed by he hin film on silicon. This ac
esul s in lowe c ys al sizes achie ing alues o 16 ± 5 nm in bo h samples. O he di ac ion
peaks co esponding o ZnO hexagonal c ys alline s uc u e could also be ound in hese
Figu e 1. Sec ional iew o samples M4 (a) and M5 (b) (25 and 35 nm po e size,
espec i ely), a e deposi ing ZnO on i s su ace.
4
Ma e . Res. Exp ess 1(2014) 045028 M Yus e e al
di ac og ams. The dispe sion in he p e e ed o ien a ions is a ibu ed o he su ace
oughness o he g own ZnO nanos uc u es mimicking he su ace ea u es o he NAAF
empla es. I is known ha subs a es wi h small oughness p omo e be e c ys alline quali y o
ZnO films [24].
Figu e 3(a) shows he expe imen al and simula ed RBS spec a o he NAAFs M4 (a) and
M5 (b) be o e and a e being coa ed wi h ZnO. F om RBS fi ings we de i ed Zn/O a ios o
49/51 and 48/52 o he films deposi ed on M4 and M5, espec i ely i.e. a ZnO compound
almos s oichiome ic). In he case o M4 a signal has been de ec ed loca ed a 1850 keV,
co esponding o he sul u con amina ion coming om he sul u ic acid used in he NAAF
g ow h. Elemen al concen a ions ob ained om he NAAF fi s we e Al/O/S = 38/59/3 o M4
and Al/O = 39/61 o M5, hese alues being e y close o he s oichiome ic composi ion o
alumina (Al
2
O
3
). In he case o M4 empla e, a signal a 1850 keV has been de ec ed,
co esponding o he sul u con amina ion coming om he sul u ic acid used in he NAAF
g ow h. The main di e ences be ween bo h RBS analyses a ise when s udying he ZnO/NAAF
in e ace (see do ed lines in figu e 3(a)). Fo he case o he ZnO film deposi ed on M4, he
ZnO/NAAF in e ace is ab up and he ise o he aluminum signal was ound o esemble he
one o he uncoa ed M4 subs a e. By con as , o he sample deposi ed on M5 he e a e
e idences o di usion o he ZnO in o he subs a e. In o de ob ain a mo e accu a e
de e mina ion o he ZnO/NAAF in e ace we ha e calcula ed he in-dep h concen a ion
p ofiles. Figu e 3(b) shows he p ofiles o samples M4 (a) and M5 (b) a e he deposi ion o
ZnO. The RBX fi made in figu e 2(a) was ob ained assuming a single ZnO laye on Al
2
O
3
subs a e. This p ofile p esen ed an ab up in e ace down o he esolu ion limi o RBS
(app oxima ely 1 nm [25]) wi h he composi ion o bo h Al
2
O
3
and ZnO, being homogeneous
h oughou he en i e hickness. On he o he hand, o M5 sample, in o de o ob aining a good
RBX fi o he spec um (figu e 2(b)) i was necessa y o conside he p esence o in e media e
laye s wi h a a iable composi ion Zn
x
Al
y
O
z
(x+y+z= 1) be ween he ZnO and he NAAF
subs a e. The e o e, in his sample he in- dep h concen a ion p ofile e eals ha he ZnO/
NAAF in e ace is no comple ely ab up ha ing app oxima ely 50 nm in hickness. These
esul s sugges ha he e is some g ow h o ZnO in o he alumina bu only in he NAAFs wi h
Figu e 2. XRD pa e ns o samples M4 and M5 coa ed wi h ZnO.
5
Ma e . Res. Exp ess 1(2014) 045028 M Yus e e al

highe po e size, i.e. M5 empla e. This di usi e e ec in he g ow h o unc ional ma e ials on
NAAFs has been epo ed elsewhe e [18].
On he o he hand, one o he c ucial pa ame e s o ob ain well defined nanos uc u es on
po ous su aces is he hickness o he unc ional ma e ial o be spu e ed on hem, in o de o
a oid he comple ed co e age o he po ous in he NAAF empla e. In o de o s udy he
co e age o he NAAF su aces, MO empla es (wi h he smalles po e size i.e. 15 nm) we e
coa ed wi h h ee di e en ZnO hicknesses: 29, 43 and 108 nm. HRSEM images o hese
samples (no shown) e ealed ha only o he hinnes coa ing (29 nm) was a po ous ZnO
su ace de eloped. Fo a ZnO hickness a ound 40nm he po e su ace s uc u e collapse and
only a small pe cen age (∼20%) o po es could be dis inguished. Besides, mos obse ed
po ous su aces lose he long ange o de wi h hexagonal symme y and he ypical g ain
g ow h o ZnO hin films on fla subs a es [21] was obse ed. Finally, in he case o coa ings
hicke han 108 nm, no e idence o po e g ow h was de ec ed. Taking in o accoun hese
esul s, ZnO films wi h cons an hickness o 30 nm we e g own on a NAAF se ies (samples
Figu e 3. (a) RBS spec a (expe imen al and simula ed) o samples M4 and M5 be o e
and a e he deposi ion o ZnO, (b) concen a ion dep h p ofiles ex ac ed om RBS
measu emen s o M4 (a) and M5 (b) a e he deposi ion o ZnO.
6
Ma e . Res. Exp ess 1(2014) 045028 M Yus e e al
Figu e 4. SEM images o NAAF su aces be o e and a e deposi ing 30 nm o ZnO.
7
Ma e . Res. Exp ess 1(2014) 045028 M Yus e e al
M1–M6) wi h inc easing po e diame e sizes, om 15 o 50 nm, o s udy he po e diame e
e ec s in he mo phology and op ical p ope ies o nanos uc u ed ZnO films.
Figu e 4shows HRSEM images o he s a ing NAAF and a e he deposi ion o 30nm o
ZnO on hem. The e is a change in he con as o he HRSEM images a e he ZnO deposi ion.
This e ec is ela ed o he pa ial educ ion o po e diame e s being mo e p onounced o
samples wi h smalle po e diame e sizes, i.e., samples M1 and M2. In o de o ob ain a
quan i a i e analysis o he po e diame e educ ion a e 30nm o ZnO deposi ion he HRSEM
images we e p ocessed by using he Image J p og am [26].
In able 2, he nominal and final po e diame e s, as well as he es ima ed po e diame e
educ ion a e shown. In his way i was possible o modula e he po e diame e size and also
hei la ice pa ame e o he nanos uc u ed ZnO films by choosing he app op ia e NAAF
empla e o ailo ing o he s no epo ed in his wo k.
Figu e 5(a) shows a ypical AFM image o he su ace o he deposi ed samples along wi h
i s Fou ie as ans o m (FFT) pa e n acqui ed om image p ocessing so wa e [27]. The FFT
image p o ides he high hexagonal o de ing deg ee o nanos uc u ed ZnO laye , e ealing he
exis ence o a sel -o de ed po es s uc u e (up o 3 d neighbou s) in a single domain. This ac
allows us o confi m he guided g ow h o ZnO nanos uc u e on he NAAF empla e su aces.
In figu e 5(b) he su ace p ofile along he pa h eflec s an accu a e measu emen o he po e size
and in e po e dis ance a e he ZnO deposi ion. The wid h and heigh o he peaks in he
su ace p ofile ga e place o an a e age po e diame e (Φ) and in e po e dis ance (D
in
) alues o
45 ± 4 nm and 112 ± 5 nm, espec i ely acco ding o he expec ed da a indica ed in able 1.
3.2. Op ical cha ac e iza ion o ZnO/NAAF nanos uc u es
The cha ac e iza ion o samples o med o mo e han one phase is no an easy ask. In ou case
we ha e ab ica ed nanos uc u es compound by wo di e en solid phases, i.e., on one side he
nanopo ous anodic alumina wi h insula o p ope ies and on he o he hand, zinc oxide, which is
a well-known II–VI semiconduc o . The e o e, we ha e s udied he op ical p ope ies o hese
nanos uc u es in wo s eps, fi s ly hose o he NAAF and la e on he join e ec on such
p ope ies o he nanos uc u ed ZnO/NAAF.
Table 2. Po e diame e s ob ained p ocessing HRSEM images o samples wi h and
wi hou ZnO deposi .
Sample heo e ical Φ(nm) calcula ed Φ(nm) % Reduc ion
M1 15.5 15 31
M1+ZnO —10.5 —
M2 18 19 16
M2+ZnO —16 —
M3 21.5 21 11
M3+ZnO —19 —
M4 25 27 8
M4+ZnO —25 —
M5 35 39 2.5
M5+ZnO —38 —
M6 50 57 7
M6+ZnO —53 —
8
Ma e . Res. Exp ess 1(2014) 045028 M Yus e e al
Figu es 6and 7show he ansmi ance spec a o he uncoa ed NAAF subs a es, samples
M1–M6, and he ones co esponding o 30nm o ZnO spu e ed on hose NAAFs, espec i ely.
Figu e 7has shi ed e ically o clea pu poses. Bo h spec a g oups e eal he high
anspa ency (>80%) o all samples in he UV-Visible ange. The obse ed Fab i–Pe o
in e e ence inges o he longes wa eleng hs a e associa ed wi h in e e ences among
mul iple eflec ions coming om he ai –film in e aces, and also p obably om in e nal
in e aces exis ing in he bulk NAAFs due o hei complex composi ional s uc u e, as RBS
esul s sugges .
3.2.1. NAAF abso p ion coe icien s and band gaps. In his wo k, he abso p ion coe ficien s
o he all samples we e de i ed om he ansmi ance spec a and by using he Bee –Lambe
Law [28] gi en by:
Figu e 5. (a) AFM image o sample M6 co e ed wi h 30 nm o ZnO wi h he
co esponding FFT, (b) opog aphic su ace p ofile along he line shown in (a).
9
Ma e . Res. Exp ess 1(2014) 045028 M Yus e e al
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