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    useful optical, electrical, and chemical properties such as high

    mechanical instability, and high cost. However layer-by-layer

    (LBL) self assembly method using sequential adsorptions of

    thickness of thin film can be controlled with a nanoscale [16].

    thin film comprising polyelectrolyte and TALH solution

    which is stable and double negatively charged inorganic

    precursor [21] shows high refractive index (n =1.68 1.8),e average thickness

    Thin Solid Films 499 (200refractive index [1], high relative dielectric constant [2],

    remarkable solar energy conversion [3,4], and photocatalysis

    [5]. Therefore TiO2 thin film can be a promising material for

    an optical filter [6], antireflection film [7], a self-cleaning

    coating [8], a high efficient dielectric [9], and a solar cell [10].

    TiO2 thin film has been fabricated by several methods such

    as a solgel synthesis [11], sputtering [12] and chemical vapor

    deposition (CVD) [13]. However, these processes that require

    a high temperature, a high qualitative vacuum system and

    intricate equipments have a limit of film area or thickness,

    In previous reports, TiO2 thin films composed of

    positively charged TiO2 nanoparticles [17] and oppositely

    charged polyelectrolyte [18] or consisted of polyelectrolyte

    and negatively charged titanium (IV) bis(ammonium lac-

    tato) dihydroxide (TALH) [19] have been successfully

    fabricated by a LBL self-assembly method. However the

    refractive index of the film composed of TiO2 nanoparticles

    and polyelectrolytes is significantly decreased because of

    the presence of pores and polyelectrolyte with low refractive

    index relatively [20]. On the other hand, although the TiO2applications and photocatalytic properties by decomposing methyl orange molecules gradually according to UV irradiation time. In addition, as

    the pH of TALH was decreased from pH 5.5 to 2.0, the thickness of (TiO2 /TALH)30 film was increased from ca. 85 nm to ca. 442 nm.

    D 2005 Elsevier B.V. All rights reserved.

    Keywords: Layer-by-layer self-assembly method; TiO2 thin film; Polyelectrolyte; Quartz crystal microbalance

    1. Introduction

    In the past several years, there has been increasing interest

    in the fabrication of TiO2 thin films because they present

    ionized polyelectrolytes and oppositely charged materials in

    aqueous solutions has lots of advantages such as a simple

    process, low temperature deposition, no limit of thickness and

    needless of complicated equipments [14,15]. In addition, thetemperature. Especially, by using the quartz crystal microbalance (QCM) to monitor the in-situ deposition phenomenon of TALH that is

    saturated and then separated from the film before and after the deposition of 30 s at low pH, the anatase TiO2 multilayer films fabricated with 30

    s deposition in TALH adjusted to pH 2.5 showed a higher refractive index (ca. n =1.75), a denser film growth, and a lower surface roughness

    (ca. 10.5 nm) than those of the films deposited in different conditions. This film showed a high transmittance in visible range for opticalFabrication and characterization

    layer-by-layer sel

    Jin-Ho Kim *, Shiro

    Department of Applied Physics and Physico-Informatics, Fa

    Kohoku-ku, Yakoh

    Available onli

    Abstract

    Titanium dioxide (TiO2) thin films assembled with TiO2 na

    bis(ammonium lactato) dihydroxide (TALH) were successfully f0040-6090/$ - see front matter D 2005 Elsevier B.V. All rights reserved.

    doi:10.1016/j.tsf.2005.07.001

    * Correspondi

    E-mail addresses: [email protected] (J.-H. Kim)

    [email protected] (S. Shiratori).TiO2 thin film prepared by a

    ssembly method

    ita, Seimei Shiratori

    f Science and Technology, Keio University, 3-14-1 Hiyoshi,

    223-8522, Japan

    August 2005

    ticles and oppositely charged polyelectrolytes or titanium (IV)

    ated via a layer-by-layer (LBL) self-assembly method at room

    6) 83 89

    www.elsevier.com/locate/tsfthis film has a small film growth with thng author. Fax: +81 45 566 1602.(ca.1.5 5 nm) of a bilayer [22,23]. In addition, the filmgrowth phenomenon between TALH and polyelectrolytes or

  • well as a gas sensor [25,26], because when material is

    deposited on the electrode of QCM, frequency is decreased

    used as a negatively charged polyelectrolyte. Titanium (IV)

    bis(ammonium lactato) dihydroxide (TALH, 50 wt.%,

    Aldrich) with double negative charges [21] was selected

    as an inorganic precursor. The molecular structure of TALH

    is shown in Fig. 1. The concentration of PPA and PDDA

    were adjusted to 0.01 M using ultra pure water (>18 MVcm) and then the pH of solutions was adjusted with NaOH

    or HCl. 0.1 wt.% of TiO2 colloidal solution was adjusted to

    H HNH3

    CH3

    CH3

    H

    H

    HH

    C

    C

    C

    CO

    OO

    OTi

    OO

    OO

    J.-H. Kim et al. / Thin Solid Films 499 (2006) 838984in proportional to the mass change by the Sauerbrey

    relation [27]:

    df f2

    NqAdm 1

    In this study, we report that TiO2 thin films assembled

    with TALH and TiO2 nanoparticles have been successfully

    fabricated with a low surface roughness, high refractive

    index, improved thickness growth and a high transmittance

    by monitoring the deposition phenomenon depended on the

    pH of solution as well as immersion time into TALH using a

    QCM. In addition, the properties of these films were

    compared with that of films comprising TiO2 nanoparticles

    and polyelectrolyte.

    2. Experimental details

    2.1. Materials

    The used starting materials were oppositely chargednanoparticles has not been sufficiently explored as functions

    of the immersion time or the pH of solution [19].

    Quartz crystal microbalance (QCM) has been used for

    the monitoring of the in-situ deposition phenomenon of

    materials on substrate in LBL assembly process [24] as

    H3N

    Fig. 1. Assumed molecular structure of the non-ionized form of TALH (the

    arrows indicated electron pairs).poly(dimethyldiammonium chloride) (PDDA, 20 wt.%,

    Aldrich) and TiO2 colloidal solution (ca. 7 nm in primary

    particle size, anatase) obtained from Ishihara Sangyo, Ltd.

    (Japan). Poly(phosphoric acid) (PPA, Wako) and poly(so-

    dium 4-styrenesulfonate) (PSS, Mw=70,000, Aldrich) were

    Fig. 2. Schematic illustration of the procedures to fabricatepH 2.5 and the pH of TALH solution was adjusted from 5.5

    to 2.0 with HNO3. Glass, Si/SiO2, and QCM (AT-cut, 10

    MHz) with a gold electrode were used as substrates.

    2.2. Preparation of thin films

    Negatively charged substrates, glass and Si/SiO2, were

    obtained by KOH (1 wt.%) treatment in ultrasonication for 5

    min and then rinsed in ultra pure water (pH 5.56.5). QCMwas also carried out KOH treatment and then the 3 bilayers

    of (PDDA/PSS) were assembled on electrode to diminish

    the surface influence of each QCM.

    Substrates and QCM were immersed into TiO2 colloidal

    solution and polyelectrolytes for 10 min and TALH solution

    for 10 s 10 min. Fig. 2 depicts the schematic illustrationof the procedures to fabricate the (TiO2/TALH) multilayer

    thin film. Rinse procedures (1 min3 times) weresubsequently carried out after immersion into solutions

    using ultra pure water. These coating procedures were

    repeated 30 times. When we deposit material B over A with

    30 times, we describe as (A/B)30.

    2.3. Characterization of multilayer thin films

    The surface microstructure and the cross-section of thin

    film deposited on glass substrate were investigated by a

    field emission scanning electron microscope (FE-SEM,

    Hitachi S-4700) and the root mean squared (RMS) surface

    roughness was measured by an atomic force microscope

    (AFM, Digital Instrument nanoscope ha) in a tapping mode.The RMS roughness was calculated according to the

    following Eq. (2):

    RMS ~ Zi Zave 2

    N

    s2

    where Zi is the height on the Z-axis of feature i, Zave is the

    average height of the entire image, and N is the number of

    points in image.the multilayer thin film consisted of (TiO2/TALH).

  • The refractive index of film assembled on Si/SiO2substrate was determined by an ellipsometry (Film Tek

    3000, Scientific Computing International) at the wavelength

    of 632 nm. The absorbance and transmittance of prepared

    TiO2 films deposited on glass were measured by a UV-vis

    spectrophotometer (UV mini-1240, Shimadzu).

    The photocatalytic properties of anatase TiO2 films to

    decompose methyl orange molecules were measured.

    Prepared thin film was put into the cell filled with methyl

    orange solution that was adjusted to ca. 0.948 absorbance at

    460 nm before UV irradiation and this cell was then exposed

    to UV light (254 nm, 22 W, SUV-16, As One) for 30 min.

    After taking the film out of the solution, the absorbance of

    methyl orange solution was measured by UV-vis spectro-

    photometer. These procedures were repeated until the total

    irradiation time became 5.5 h.

    resulted in the separation from TiO2 nanoparticles deposited

    during previous procedure. We assume that this phenom-

    larger clusters than that of Fig. 5 (ac). On the other hand,

    the film fabricated using TALH adjusted to pH 5.5 showed

    the formation of pores on film however the presence of pores

    was remarkably decreased in TALH solution adjusted to pH

    2.5 or 2.0 and these films contain ca. 70 100 nm clustersformed from the agglomeration of nanoparticles and TALH.

    Fig. 5 (b) film showed a flat and dense surface morphology.

    Fig. 6 shows the surface morphologies and cross-

    sectional images of [(TiO2/TALH)(pH 2.5)]30 multilayers

    as a function of immersion time into TALH. The prepared

    thin films with 10 or 30 s immersion time present a dense

    surface, however when the immersion time is increased to

    10 min, the amount of pores is also increased on the film.

    We consider that this result is caused by the separation of

    TiO2 from film after 30 s from the film as shown in Fig. 3

    (a). Fig. 6 (d) shows the cross-sectional image of Fig. 6 (b).

    The thickness was ca. 275 nm, which was in good

    accordance with an ellipsometry measurement.

    J.-H. Kim et al. / Thin Solid F3. Results and discussion

    3.1. Frequency shift of QCM

    Fig. 3 shows the frequency shift of QCM deposited TiO2nanoparticles (pH 2.5) or PDDA (pH 2.5) in TALH solution

    adjusted to pH 2.5 for 10 min. In this figure, the frequency

    shift of QCM coated with PDDA that has a remarkably

    larger charge density [28] than that of colloidal particles was

    saturated in short time and then there is no large change of

    frequency shift, however the frequency shift of QCM

    deposited TiO2 nanoparticles was saturated after about 30

    s and then decreased significantly. This decrease of

    frequency shift after 30 s in TALH may be derived from

    the separation of precipitated TiO2 on QCM because at low

    pH, the destabilization of chelate results in TiO2 precipitate

    or films and the TiO2 precipitates formed from titanium

    lactate solution are charged positively [19], which hasFig. 3. Frequency shift of a QCM in TALH (pH 2.5) solution after the

    deposition of TiO2 or PDDA: (a) TiO2 (pH 2.5) and (b) PDDA (pH 2.5).enon is gradually carried out after deposition for 30 s with

    TiO2 nanoparticles. Therefore the deposition for 30 s in

    TALH will be suitable for obtaining the reasonable TiO2thin film with high thickness growth.

    The frequency shift for 30 s as a function of the pH of

    TALH are given in Fig. 4. The frequency shift in TALH

    adjusted to pH 5.5, 2.5, and 2.0 were 50, 145, and 210 Hz,

    respectively. Hence, the thickest film can be assembled in

    the pH 2.0 of TALH.

    3.2. Surface morphology and thickness of films

    Fig. 5 (a c) present the surface morphologies ofprepared (TiO2/TALH)30 multilayers thin films as a function

    of the pH of TALH. Substrates were immersed into TALH

    for 30 s. Fig. 5 (d) is the surface image of [(PDDA/

    TALH)(pH 2.5)]30 thin film assembled using solutions

    adjusted to pH 2.5. In this figure, the film was consisted of

    Fig. 4. Frequency shifts of QCM in TALH solution as a function of the pH

    of TALH after immersion into TiO2: (a) pH 5.5, (b) pH 2.5, and (c) pH 2.0.

    ilms 499 (2006) 8389 85The RMS values of [(TiO2/TALH)(pH 2.5)]30 and

    [(TiO2/PPA)(pH 2.5)]30 are shown in Fig. 7. In order to

  • Fig. 5. FE-SEM images of (TiO2/TALH)30 thin films as a function of the pH of TALH solution and (PDDA/TALH)30 film: (a) pH 5.5, (b) pH 2.5, (c) pH 2.0

    pH 2

    J.-H. Kim et al. / Thin Solid Films 499 (2006) 838986prepare films, glass substrates were immersed into TiO2colloidal and PPA solution for 10 min and TALH for 30 s.

    The RMS of [(TiO2/TALH)(pH 2.5)]30 film as shown in Fig.

    7 (a and b) was ca. 10.5 nm and the RMS of [(TiO2/

    PPA)(pH 2.5)]30 as shown in Fig. 7 (c and d) was ca. 22.4

    nm. From this result, it was turned out that the thin film

    consisted of TiO2 nanoparticles and TALH has a lower RMS

    value and the denser surface of TiO2 than that of the film

    fabricated with nanoparticles and PPA. The refractive

    and (d) [(PDDA/TALH)(pH 2.5)]30. TiO2 colloidal solution was adjusted toindices of thin films consisted of (TiO2/TALH) and (TiO2/

    Fig. 6. Surface morphologies of [(TiO2/TALH)(pH 2.5)]30 thin films as a function o

    (d) cross-sectional image of (b). Immersion time into TiO2 solution is 10 min.PPA) were ca. 1.70 1.75 and ca. 1.45 1.50 at 632 nm,respectively. These results will be important information for

    optical applications.

    Table 1 summarizes the properties of prepared (TiO2/

    TALH)30 films as functions of the pH value and the

    immersion time of TALH solution as well as a rinse process

    after TALH assemble. As the immersion was increased from

    10 to 30 s, the thickness of films was also increased from ca.

    162 nm to ca. 275 nm in the pH 2.5 of TiO2 colloidal and

    .5.TALH solutions and was then gradually decreased to ca. 50

    f the immersion time into TALH solution: (a) 10 s, (b) 30 s, (c) 10 min, and

  • ng mo

    10 A.

    J.-H. Kim et al. / Thin Solid Fnm as the deposition was increased from 30 s to 10 min.

    From this data, we suppose that at low pH, the negative

    charge density of film formed from titanium lactate was

    gradually increased until 30 s, which became the driving

    force to deposit lots of positively charged TiO2 nano-

    particles during next deposition. However, as the deposition

    time in TALH was increased from 30 s to 10 min, the

    formation of cationic TiO2 from TALH was gradually

    carried out on the surface of film, which decreased the

    negative charge of surface and then, the cationic TiO2complexes were finally separated from film deposited with

    cationic TiO2 nanoparticles. This thickness decrease of film

    Fig. 7. AFM images of (TiO2/TALH)30 and (TiO2/PPA)30 thin films in tappi

    view, and (d) section analysis of (TiO2/PPA)30. Scan size and height is 10solution and 30 s into TALH solution. All solutions are adjusted to pH 2.5with the deposition over 30 s is consistent with the

    frequency shift of QCM as shown in Fig. 3 (a).

    The RMS values of films assembled with an immersion

    for 20 or 30 s in TALH were lower than that of other films.

    As the immersion time was increased from 30 s, the RMS

    values were also gradually increased. In addition, as the pH

    value of TALH was decreased from pH 5.5 to pH 2.0, the

    Table 1

    Properties of prepared (TiO2/TALH)30 thin films as functions of the pH and

    immersion time of TALH solution as well as rinse process after TALH

    deposition

    Sample pH of

    (TiO2/TALH)

    Immersion

    time into

    TAHL

    Rinse process

    after TALH

    deposition

    Thickness

    (nm)

    Surface

    roughness

    (nm)

    T1 (2.5/2.5) 10 s 1 min1 162 14.2T2 (2.5/2.5) 20 s 1 min1 170 10.2T3 (2.5/2.5) 30 s 1 min1 275 10.5T4 (2.5/2.5) 1 min 1 min1 155 12.7T5 (2.5/2.5) 5 min 1 min1 105 13.2T6 (2.5/2.5) 10 min 1 min1 50 16.2T7 (2.5/2.5) 30 s 1 min1 442 27.5T8 (2.5/2.5) 30 s 1 min1 85 17.5T9 (2.5/2.5) 1 min 1 min3 62 20.6film thickness was increased. Especially, the thin film

    deposited in TALH adjusted to pH 2.0 was showed a high

    thickness growth with ca. 442 nm. However the RMS value

    was also largest than that of thin film fabricated in TALH

    adjusted to pH 5.5 or 2.5.

    Rinse process after TALH deposition also influenced the

    thickness of films. Comparing the T4 and T9, the thickness

    of film was decreased by the addition of rinse steps and the

    RMS roughness was also increased because the cationic

    TiO2 complexes were formed and separated from film

    during rinse procedure.

    de: (a) surface view, and (b) section analysis of (TiO2/TALH)30, (c) surface

    m and 200 nm, respectively. Immersion time is 10 min into TiO2 and PPA

    ilms 499 (2006) 8389 873.3. Absorbance, transmittance, and refractive index of

    films

    Fig. 8 shows the absorbance of prepared thin films as

    functions of the pH of TALH and immersion time into

    TALH solution. As shown in Fig. 8 (a), as the pH of

    TALH was decreased from pH 5.5 to 2.0, the maximum

    absorbance of TiO2 multilayer thin films was increased.

    This result is in accordance with the thickness increase of

    film as shown in Table 1. However, the absorbance of

    films was not increased in proportional to the thickness of

    film. Although the T7 film was fabricated with ca. 442 nm

    in thickness, the absorbance was not remarkably higher

    than that of T3 film. This means that the T7 film has a

    high thickness growth with high RMS roughness during

    deposition. Therefore some pores may be formed inside of

    film.

    Fig 8 (b) shows that the absorbance of films prepared

    with deposition time from 10 to 30 s was gradually

    increased and was then decreased from 30 s to 10 min at

    285 nm. These data are in good accordance with the

    thickness of films prepared in different conditions as shown

    in Table 1.

  • Fig. 9. Transmittance of prepared (TiO2/TALH)30 thin films as a function of

    the pH value of TALH with TiO2 solution adjusted to pH 2.5: (a) pH 2.5

    and (b) pH 2.0. Immersion time is 10 min into TiO2 and 30 s into TALH,

    respectively.

    Fig. 8. UV-vis spectra of (TiO2/TALH)30 thin films prepared as functions as

    (a) the pH of TALH solution with 30 s immersion time and (b) the

    immersion time into TALH solution adjusted to pH 2.5. The pH and

    immersion time of TiO2 solution are pH 2.5 and 10 min.

    J.-H. Kim et al. / Thin Solid F88Fig. 9 presents the transmittances of sample T3 and T7

    multilayers thin films. Sample T3 film showed a high

    transmittance in a visible range, therefore this film may be

    suitable for an optical application as a high refractive layer

    because the refractive index of thin film was ca. 1.70 1.75at 632 nm. On the other hand, the transmittance of sample

    T7 film was decreased in visible range. Even if it is clearly

    difficult to identify the volume of pores and the roughness in

    Fig. 5 (c) compared with Fig. 5 (b). When we compare the

    thickness and absorbance of films, T7 film has a lower

    density of TiO2 than that of T3 film by the formation of

    pores, high roughness and thick film thickness. In fact, a

    few cracks were shown on film. Therefore we think that the

    T7 film may show a higher light reflectance in visible range

    than that of T3 film.

    3.4. Photocatalysis of film

    Fig. 10. Absorbance at 460 nm in UV-vis spectra of aqueous methyl orange

    solution decomposited by the (TiO2/TALH)30 thin film as a function of UV

    irradiation time.ilms 499 (2006) 8389The absorbance changes of methyl orange solution by the

    anatase TiO2 thin film (T3) were measured. The absorbance

    of methyl orange solution at 460 nm as a function of UV

    irradiation time was shown in Fig. 10. The absorbance of

    methyl orange in UV-vis spectra was gradually decreased

    from ca. 0.948 according to the increase of irradiation time

    because methyl orange molecules were decomposed by

    anatase TiO2 with UV irradiation. After 3 h, the decom-

    position rate of methyl orange was slightly decreased since

    the concentration of methyl orange remained was gradually

    decreased. The film irradiated for 5.5 h still showed the

    reproducible photocatalytic performance in new methyl

    orange solution.

    4. Conclusions

    (TiO2/TALH)30 multilayer thin films consisted of TiO2nanoparticles and TALH were successfully fabricated via

    LBL-SA method with an advanced growth in thickness ( ca.

  • 275 nm) by adjusting the pH and the immersion time of

    TALH solution. The in situ assembly of TALH that shows

    the phenomenon to be saturated and separated before and

    after 30 s was clearly monitored by a QCM. As the pH of

    TALH was decreased, the thickness of films was increased.

    Finally, by using TiO2 colloidal solution and TALH adjusted

    to pH 2.5 with the immersion of 30 s into TALH, we

    fabricated an anatase TiO2 thin film that has a lower RMS

    roughness (ca. 10.5 nm), a higher refractive index (ca. 1.75)

    than that of the film composed of TiO2 nanoparticles and

    PPA. In addition, this film showed a high transmittance in

    visible range for optical applications as well as good

    photocatalytic performances to decompose the methyl

    orange molecules with UV light irradiation.

    Acknowledgements

    This work was partially supported by Grant-in-Aid for

    the 21st Century COE program KEIO Life Conjugate

    Chemistry from the Ministry of Education, Culture, Sports,

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    Fabrication and characterization of TiO2 thin film prepared by a layer-by-layer self-assembly methodIntroductionExperimental detailsMaterialsPreparation of thin filmsCharacterization of multilayer thin films

    Results and discussionFrequency shift of QCMSurface morphology and thickness of filmsAbsorbance, transmittance, and refractive index of filmsPhotocatalysis of film

    ConclusionsAcknowledgementsReferences