22
Window Glass Coatings Jitka Mohelníková Abstract Thin film coatings modulate optical and thermal and other properties of window glass. Coated window glasses influence indoor climate and energy efficiency in buildings. They can be classified into groups of spectrally selective glazings, chromogenic glazed systems for switchable smart window technolo- gies and light-enhancing transparent materials. Low-emissivity glazings are typical of spectrally selective window glasses. Chromogenics have applications in light control and switching technologies that are optically, thermally, chemically or electrically activated. Transparent materials with micro-structured or holographic films and antireflective coatings serve to direct light and control light functions. An overview of several types of window glazings and coatings will be presented. 1 Introduction Energy savings and motivation toward solar energy utilization in buildings brought forth the development of advanced glazing materials [13]. These glazings with thin film coatings and selective surfaces have ability to modulate the properties of window glass. Special windows glazing influences the climate in the buildings in which they are used. This is why they have found wide applications in architecture [4, 5]. They can be used for: J. Mohelníková (&) Faculty of Civil Engineering, Brno University of Technology, Veverˇí 95, 602 00 Brno, Czech Republic e-mail: [email protected] L. Zang (ed.), Energy Efficiency and Renewable Energy Through Nanotechnology, Green Energy and Technology, DOI: 10.1007/978-0-85729-638-2_26, Ó Springer-Verlag London Limited 2011 913

[Green Energy and Technology] Energy Efficiency and Renewable Energy Through Nanotechnology || Window Glass Coatings

  • Upload
    ling

  • View
    219

  • Download
    4

Embed Size (px)

Citation preview

Window Glass Coatings

Jitka Mohelníková

Abstract Thin film coatings modulate optical and thermal and other propertiesof window glass. Coated window glasses influence indoor climate and energyefficiency in buildings. They can be classified into groups of spectrally selectiveglazings, chromogenic glazed systems for switchable smart window technolo-gies and light-enhancing transparent materials. Low-emissivity glazings aretypical of spectrally selective window glasses. Chromogenics have applicationsin light control and switching technologies that are optically, thermally,chemically or electrically activated. Transparent materials with micro-structuredor holographic films and antireflective coatings serve to direct light and controllight functions. An overview of several types of window glazings and coatingswill be presented.

1 Introduction

Energy savings and motivation toward solar energy utilization in buildings broughtforth the development of advanced glazing materials [1–3]. These glazings withthin film coatings and selective surfaces have ability to modulate the properties ofwindow glass. Special windows glazing influences the climate in the buildings inwhich they are used. This is why they have found wide applications in architecture[4, 5]. They can be used for:

J. Mohelníková (&)Faculty of Civil Engineering, Brno University of Technology,Veverí 95, 602 00 Brno, Czech Republice-mail: [email protected]

L. Zang (ed.), Energy Efficiency and Renewable Energy Through Nanotechnology,Green Energy and Technology, DOI: 10.1007/978-0-85729-638-2_26,� Springer-Verlag London Limited 2011

913

• limiting heat loses and maximizing solar gains and natural lighting in buildingsto reduce energy consumption for heating and artificial lighting,

• reducing glare and lowering the energy demands for cooling and air-conditioning,

• reducing the amount of cleaning water and solvents due to reduction in main-tenance requirements in glazed windows.

Glazings can be classified into three main groups with respect to their appli-cations in buildings [6–8]:

• spectrally selective glazings (e.g., glazings with modulated transmittance,reflectance and absorbance in the visible or infrared spectral range),

• chromogenic glazings (i.e., switchable glazings for dynamic light control),• light-enhancing glazings (e.g., light reflectors, collectors or wave-guiding trans-

parent materials, antireflective glass and glazings with self-cleaning surfaces).

2 Spectrally Selective Glazings

Spectrally selective coatings modulate the spectral properties of glass substrates.For window glazing applications they are represented mainly by thin films thatreduce absorption of infrared radiation within glass panes. They have very lowemissivity (between 0.2 and 0.05) compared to the emissivity of common windowglass 0.84 [9–11]. These thin films are called low-emissivity (low-e) coatings.The major requirements for these coatings are:

• high transmittance in visible spectral range,• high reflectance in infrared spectral region.

Low-emissivity coatings are classified into two main groups [9–15]:

• Coatings reflective in infrared spectral range (between 2 and 10 lm). This typeof low-e glazing is also called a heat mirror or a winter film. They serve toeliminate heat radiation losses of windows or collect thermal energy.

• Coatings reflective in near-infrared part of the solar radiation spectrum inspectral range between 0.78 and 2.5 lm. They are called solar controlling low-emissivity coatings or summer films. Their main application is reduction of solarthermal loads.

2.1 Low-Emissivity Glazings

Low-emissivity (low-e) glazings have special coatings deposited on their surfaces.Low-e coatings operate as transparent heat mirrors. They can be deposited as[11, 14, 15]:

914 J. Mohelníková

• doped oxides semiconductor coatings,• conducting micro-grid coatings,• multilayer thin films consisting of metal and transparent dielectric layers.

Doped oxide semiconductor coatings consist of dielectric layers with mobilecharge carriers. The coatings have high reflectance in the infrared spectral rangeand good transmittance of visible wavelengths. Materials such as SnO2:F,In2O3:Sn, SnO2:Sb, ZnO:Al or Cd2SnO4 are used for these coatings [11, 16–19].

The transparent heat mirror coatings can be also designed as micro-grid thinconducting films with small openings (around 2.5 lm). These openings transmitsolar radiation and the rest parts of the coating reflect infrared radiation. This typeof coatings has not found wide applications for window glass panes [19].

Multilayer coatings consisting of a metal film sandwiched between transparentdielectric layers are recommended for window glazings. Metals have highreflectance and low-emissivity in the infrared spectral range [20]. Figure 1 showsspectral reflectance of selected thin metal films (Aluminium-Al, Silver-Ag,Gold-Au and Copper-Cu) of equal thicknesses deposited on a glass substrate [21].The reflectance curves are compared in the visible spectral range (380–780 nm)and in the part of infrared range between 1,000 and 15,000 nm.

It is obvious that the most apt materials are silver and gold layers. The thinsilver and gold layers both have high visible transmittance and high reflectance inthe infrared spectral range. Silver is the most adept metal for low-e coatingsbecause of its high infrared reflectance and low light absorbance [21]. Aluminiumis ill suited as a glazing component due to its higher reflectance and reducedtransmittance in the visible range.

Dielectric coatings protect the thin metal layer and influence light transmittanceof the low-e coatings. Spectral transmittance of a thin metal film (M) comparedwith transmittance of the same metal film with single and double dielectric (D)layers is presented in Fig. 2 (computer simulation [22]). Dielectric layers have ananti-reflective property. The top dielectric layer on the metal film has higherinfluence on visible transmittance.

Dielectric materials with high refractive indices, such as TiO2, SnO2, SnBO2,In2O3, ZnO, ZnS, Si3N4 and Bi2O3 [23, 24], can be used in low-emissivity

Fig. 1 Spectral reflectance of silver (Ag), aluminum (Al), gold (Au) and copper (Cu) thin filmson glass, a visible spectral range 380–780 nm, b infrared spectral range 1,000–15,000 nm

Window Glass Coatings 915

coatings. Multilayer low-e coatings use combinations of dielectric materials withhigh and low refractive indices, for example, TiO2 and SiO2.

The materials selected as layers in a low-e coating influence its visible trans-mittance. Figure 3 presents a spectral transmittance of a low-e coating with metal(M) layer and dielectric layers of materials with high (Dh) and low (Dl) refractiveindices (computer simulation [22]).

The light transmittance of the five-layer Dh/Dl/Dh/M/Dh/Dl/Dh coating is veryhigh but relatively narrow-band compared to the three-layer Dh/M/Dh coating ofthe same material composition, Fig. 3.

An optimized design of the multilayer composition of dielectric and metallayers yields visible transmittance and infrared reflectance coatings [23–26].Examples of low-e coatings include [14, 27–33]:

• a central silver layer between two dielectric layers:glass/ZnO/Ag/ZnOglass/ZnS/Ag/ZnSglass/TiO2/Ag/TiO2

glass/SnO2/Ag/SnO2

glass/Bi2O3/Ag/Bi2O3

Fig. 2 Spectraltransmittance of thin filmswith metal (M) and dielectric(D) layers deposited on glass

Fig. 3 Influence of dielectriclayers on transmittance ofa thin low-e coating (M-metallayer, Dh-dielectric layerwith high refractive index,Dl-dielectric layer withlow refractive index)

916 J. Mohelníková

• a silver layer and three dielectric layers of two different materials: glass/TiO2/Ag/TiO2/SiO2

• a copper layer between two dielectric layers: glass/SnO2/Cu/SnO2

• a titanium nitride layer between two dielectric layers: glass/TiO2/TiN/TiO2

• a zirconium nitride layer between two dielectric layers: glass/ZrO2/ZrN/ZrO2

• a gold layer between two dielectric layers: glass/In2O3/Au/In2O3.

The thin gold film is inert but metal coatings of silver or copper are notchemically stable. Their optical properties degrade by thermal oxidation andcorrosion caused mainly by atmospheric pollutants such as chlorine and sulphur[33]. The metal layer’s chemical stability and durability is increased with a pro-tective layer [34]. The metal layer is protected by a barrier layer or blocker layer[23]. A barrier layer should be deposited on one or both metal-dielectric interfaces.Materials that can be used to protect the metal layers against corrosion include Si,Ti, TiN, TiAOx, NiCr, NiCrOx, Cr, Zr, Mo, W and ZrSi [23, 35–37].

Examples of characteristic compositions of low-e window coatings with pro-tective layers:

• glazings with a single silver and a single blocker layer [35–37]:glass/SnO2/Ag/NiCrOx/SnO2 or glass/ZnO/Ag/TiAOx/SnO2, glass/SnBO2/ZnO/Ag/NiCrOx/SnBO2 or glass/TiO2/ZnO/Ag/NiCrOx/Si3N4

• glazings with a single silver and double blocker layer:glass/SnO2/TiAOx/Ag/TiAOx/SnO2 [37].

Low-e window coatings can be designed as single, double or even triple metallayer films [38, 39]. Multi-layered dielectric-metal coatings serve as the broadbandinfrared (IR) reflectors for low-emissivity glazings. It means these glazings caneliminate thermal radiation losses, provide near-IR solar control and substituteconvenient transmittance in the whole visible spectrum [40]. Compositions of suchmultifunctional coatings include:

• glass/SnO2/ZnO/Ag/NiCrOx/SnO2/Ag/NiCrOx/SnO2 [37]• glass/ZnO/Ag/Ti/ZnO/Ag/Ti/ZnO/TiO2/ZnO [40]• glass/TiOx/ZnOx/Ag/NiCrOx/TiOx/ZnOx/Ag/NiCrOx/SiNx [41, 42], the better

thermal and mechanical stability of this coating is achieved by dividing the firstlayer and middle layer of titanium oxide and also two silver layers in thefollowing way glass/TiOx/NiCrOx/TiOx/ZnOx/Ag/NiCrOx/Ag/NiCrOx/TiOx/NiCrOx/TiOx/ZnOx/Ag/NiCrOx/Ag/NiCrOx/SiNx [41, 42]

• glass/Si3N4/Ni:Cr/Ag/Ni:Cr/Si3N4/Ni:Cr/Ag/Ni:Cr/Si3N4 [43]• glass/TiOx/Si3N4/NiCr/Ag/NiCr/Si3N4/SnO2/ZnO/Ag/NiCrOx/SnO2/Si3N4 [44]

Figure 4 shows spectral transmittance of three different compositions of thelow-e coatings with single, double and triple silver layer and TiO2/SiO2 layers inthe following compositions (computer simulation [22]):

• single silver coating: glass/TiO2/Ag/TiO2

• double silver coating: glass/TiO2/Ag/TiO2/SiO2/TiO2/Ag/TiO2

• triple silver coating: glass/TiO2/Ag/TiO2/SiO2/Ag/SiO2/TiO2/Ag/TiO2

Window Glass Coatings 917

2.2 Spectrally and Angularly Selective Solar Control Glass

Solar control glazings reduce overheating and glare [45]. Glazings with spectrallyselective coatings are reflective or absorptive in the near-IR range of solar radiationspectrum. Special coatings can also influence angular selectivity of window glass.General requirements for the design of solar control reflective coatings are visibletransmittance and high near-IR reflectance. These properties are achieved by fab-ricating thin dielectric/metal/dielectric films with metal layers, such as Ag, Cu, Au,or TiN and dielectric layers of Bi2O3, In2O3, SnO2, TiO2, ZnO or ZnS [9, 14].

Solar control coatings can also consist of absorbing and reflecting materials,such as CrNx, TiNx, and FeNx, embedded in layers of a material with a highrefractive index [46]. A thin film of CuxS can be also used for solar controlpurposes [47].

The near-IR absorbing thin film and a low-e layer within one coating is anotherpossibility [48, 49]. The coating consists of SnO2 layer (deposited on the glasssubstrate) with a dopant of antimony, tungsten, vanadium, iron, chromium,molybdenum, niobium, cobalt or nickel and the low-e layer of SnO2 containing adopant of fluorine or phosphorus [48, 49].

Special near-IR absorbing glazings include a light absorptive resin laminatedbetween two glass panes [50]. The transparent acrylic resin contains copper ions,which reduce solar transmittance in the near-IR spectrum and allow for hightransmittance of visible light.

Angular selective coatings can also be designed for solar control glazings.Angle selective coatings allow for seasonal self-regulation of window glazings.They reflect part of direct solar rays affecting glass panes at high angles ofincidence, which happens in the summer, and transmit diffusive and low-angleincidence direct solar radiation characteristic of winter sunlight [51–54]. Coatingswith angularly selective oblique columnar microstructures are used for this pur-pose. These coatings are based on materials such as Al, Cr, Ta and cernet [54–57].Affected solar radiation is scattered or directly transmitted by the columnar micro-structured coating, dependent upon the angle of incidence. The scattering of directsolar radiation eliminates glare. Scattering surface patterns and thin films are

Fig. 4 Spectraltransmittance of single,double and triple silverlow-e coatings

918 J. Mohelníková

applied for special glare protection glazings [58, 59]. Such coatings reduce theneed for cooling in summer seasons.

3 Chromogenic Glazings

Chromogenic glazing materials offer solar control switching activated optically,thermally, chemically or electrically [7, 60, 61]. Switchable glazings have manyapplications including architectural glazed roofs and façades, automotivewindscreens and sunroofs or aircraft windows and displays [61].

Window chromogenic glazings allow dynamic changes in solar transmittancedependent upon external conditions, such as solar radiation intensity or tempera-ture variations. Chromogenic glazings fall into two categories:

• non-electrically activated devices: photochromic (optical activation), thermo-chromic and thermotropic (thermal activation) and gasochromic glazings(chemical activation). Some of the glazings can also be connected to an externalswitch, allowing for user-defined operation with electronic control.

• electrically activated devices, such as electrochromic, electrochromic-photo-voltaic glazings, photoelectrochromic glazings (they can also be applied in anelectrically non-activated variation) and glazing devices with liquid crystals orsuspended particles.

3.1 Photochromic Glazings

The photochromic phenomenon is a reversible change between two energy statesof a material due to light absorption [62]. Photochromism has been known since1880s [62–64]. Photochromic glass color centers are activated under radiationexposure, causing glass coloration (darkening). The destruction of the color cen-ters of the photochromic glass occurs in the state without radiation present, whenthe glass is in the initial transparent state. Color centers are activated in response toexposure to ultraviolet and short-wave visible radiation. The destruction of colorcenters is influenced by long-wave visible and short-wave infrared radiation.

Photochromic materials are metal halides, such as silver, copper halides, cad-mium halides, europium or cerium. Chromium, molybdenum or tungsten and themineral hackmanit can be also used [62–65]. Investigations in the kinetics ofphotochemical reactions of photochromic glasses confirm desirability of silverhalides [64, 65] as AgCl or AgBr. Another group of photochromics is organicmaterials. Examples include certain dyes, stereoisomers and polynuclear aromatichydrocarbons [66, 67].

The best-known variation is ophthalmic photochromic glass. Photochromicglasses have few applications for large-area glazings in buildings [62–68].A glazed photochromic element with special thin film based on magnesium–nickel

Window Glass Coatings 919

alloy has been developed [68] and is expected to be implementable as a windowcoating [69]. The diffuse-reflection type of photochromic thin film (e.g. SnO2)forms pyramidal crystal grain projections. This irregular surface is coated withMg6Ni layer. In a double glass unit configuration, the photochromic film faces aninternal cavity. The cavity is filled with diluted hydrogen which influencesreflective and transparent state variations of the unit.

The aforementioned photochromic material, SnO2, implemented in the follow-ing device, glass/SnO2:F/electrolyte/Pd/Mg6Ni/irregularly-shaped SnO2:F/glass,can be activated electrically when connected to an appropriate controller [69].

Another special photochromic device features user-controllable light trans-mittance. This device bleaches at the user’s discretion [70]. Such a device iscomprised of a radiation sensitive electrode/interconnecting medium/ion interca-lative layer, embedded between two panes of glass with deposited transparentconductive oxide (TCO) layers. An electrical connection exists between the twoTCO electrodes. Radiation sensitive electrode materials include zinc–cadmiumsulfide and titanium oxide with dopants Ta, Nb, Sb, V and Ru [70].

3.2 Thermochromic and Thermotropic Glazings

Thermochromic glass alters its optical properties with response to temperaturechanges [71–73]. Thermochromic materials’ colors are modified by a thermallyinduced chemical reaction or by a phase transformation. The phase transformationfrom semiconductor state (high visible transmittance) to metallic state (highinfrared reflectance) occurs in transition metal oxides. Thermochromic coatings inthe metallic state have similar properties as low-emissivity coatings.

Organic and inorganic compounds are known for their thermochromic prop-erties [72, 73]. Such organic compounds are anil, spiropyrans, polyvinyl acetalresins and hydroxide groups. Examples of inorganic thermochromic compoundsinclude AgI, Ag2HgI4, Cd3P3Cl, HgI, HgI2 and SrTiO3. Vanadium dioxide VO2

has been used for thermochromic window applications [7, 74–78]. Reversiblemetal-to-semiconductor phase transformation can be achieved by doping VO2.Tungsten is a frequently used dopant [76, 77]. Thin films VO2:Mg [78] andmultilayer coatings TiO2/VO2/TiO2/VO2/TiO2 [7] have also been investigated forwindow coating applications.

Thermotropic glazings change their translucence with temperature changesfrom clear states to light-scattering, non-transparent states. Thermotropic devicescontain special gels embedded between two glass panes. The gels influence theradiation and conductive heat transfer through the glazing. They consist of ther-motropic materials of two components with different refractive indices [79–83].These components are homogenous for low temperatures (transparent state).If temperature rises above the limit value (between 20 and 50�C) the componentsare phase-separate, forming very small nanoparticles. The separation causesscattering of solar radiation, leaving a non-transparent, white-colored glazing [83].

920 J. Mohelníková

3.3 Gasochromic Glazings

Dynamic transmittance changes of gasochromic glazings are caused by chemicalreactions of hydrogen with wolfram oxide [83–88]. Gasochromic devices consistof a double-glazed unit with connections to a gas supply unit and an electroniccontrol unit. An example of a gasochromic double-glazed unit compositionis: glass/WO3/Pt/cavity filled with gas (e.g. H2, O2)/glass [86, 87]. The opticallyactive component of the gasochromic glazing is a thin porous WO3 film. The Ptlayer serves as a catalyst. The glazed unit changes color when the gasochromicfilm is exposed to a low concentration of H2. The bleaching process that producesa transparent state occurs with exposure of diluted O2. The following chemicalreaction WO3 (colorless) ? xH2(Cat) ? 2xH+ ? WO3 ? H2xWO3 (blue) causesblue coloration of the gasochromic glazing [88]. Color intensity depends on theWO3 film thickness and hydrogen concentration. The effect of the gasochromiccoloration is also used in the aforementioned photochromic reflective light controlelement [69].

A switchable gasochromic mirror device based on Pd/Ni-WO3 anodic doublelayer coating deposited on the glass has been developed [89]. The hydrogen gasdissociates from the Pd catalyst into H atoms, which diffuse into the Ni-WO3 film,causing coloration.

3.4 Electrochromic Glazings

The electrochromic phenomenon has been the subject of many scientific researchprograms and investigations [90–110]. Electrochromic (EC) smart window glaz-ings are just one possible application of this phenomenon.

EC glazings reversibly change their optical properties under an applied voltage.The presence of electric current causes variation of the material’s chemicalcomposition and its optical properties. EC glazings require only a small voltage(between 1 and 5 V) for switching. They are transparent when no voltage isapplied. A typical composition of EC glass is the following [93–95]: glass/trans-parent electrode (TCO)/EC layer/central electrolyte-ion conductor/ion-storagelayer/transparent electrode (TCO)/glass.

The switchable process of glazing coloration and bleaching is caused by ionmigration between the EC and ion-storage layer. Ions of the EC layer move towardthe ion-storage layer through the central electrolyte when voltage is appliedbetween two transparent electrodes. The ions transport to the ion-storage layercauses EC glazing coloration. A change in electric polarity causes ion flow in theopposite direction, causing bleaching of the EC device.

Many materials have been tested for EC applications. Typical materials whichare used for EC devices are [90–105], for example:

Window Glass Coatings 921

• EC layer: inorganic materials, such as WO3, LixWO3, HxWO3, NiO or organicmaterials, such as viologen,

• ion conduction layer: LiClO4 ? PC, Ta2O5, PMMA ? organic,• ion-storage layer: WO3, WO3:MO, Nb2O5, NiO, Prussian Blue, LiyV2O5,• transparent electrode: In2O3:Sn or SnO2:F.

The coloration process is achieved by the oxidation–reduction reaction inorganic EC materials [103]. The EC effect occurs in inorganic metal oxides due tothe dual injection (cathodic) or ejection (anodic) of ions and electrons (e-).A typical reaction for the cathodic coloring material is:

WO3 (transparent) ? yH+ ? ye- $ HyWO3 (blue) [103, 104]Ions such as Li+, Na+ and Ag+ can also cause EC coloration.A typical coloring anodic reaction is, for example:

LiyV2O5 light yellowð Þ� yLiþ � ye� $ V2O5 blueð Þ [103]

or Ir OHð Þx transparentð Þ $ IrOx blackð Þ + XHþ + xe� [104]

Possibilities of enhancing an EC glazing visible transmittance in its transparentstate can be achieved through adding Al or Mg to the Ni oxide [106] or antire-flective layers [107]. EC safety glass laminated with ion-conducting PVB (Poly-vinyl butyral) sheets [108] and flexible polyester-based foils with EC coatings[109] have also been developed.

3.5 Photoelectrochromic Glazings

Photoelectrochromic glazings combine electrochromic and photochromic princi-ples [110–114]. Such glazing units consist of an electrochromic material (WO3,IrOx, V2O5 or NiO) and a semiconductor film (TiO2, CdS, ZnS, ZnO or WO)[110]. The composition of the photoelectrochromic glazing can be [111, 112]:glass/transparent electrode/WO3 layer/nanoporous TiO2 layer/dye monolayer/electrolyte LiI/Pt layer/transparent electrode/glass.

The thin film of TiO2 is porous and covered with a dye monolayer. The dye isexcited under illumination and donates electrons to the TiO2, which conduct themto the WO3 layer. This reduces the tungsten and changes its color from transparentto blue. The Pt thin film catalyzes the reverse reaction. The process takes placeunder illumination. This means that the whole system operates as a passivephotochromic element. The device can also have transparent electrodes connectedto an external switch. Electrons from the WO3 layer can flow to the counter-electrode in case of the closed external switch (darkening state). The device istransparent in the electrically non-activated state.

922 J. Mohelníková

3.6 Electrochromic and PV Glazing

Photovoltaics can be used as power sources for switchable glazings, creating acomplete smart window system [115]. Another interesting application of photo-voltaic (PV) technology for windows is the integration of PV thin films of specialcolors into the glazings [116]. An electrochromic (EC) device powered by anintegrated amorphous silicon carbide (a-SiC:H) PV film is an example of aphotovoltaic/electrochromic (PV/EC) glazing [117–119]. The PV part serves as asemitransparent power supply and the EC thin film serves as a modulator oftransmittance. These two parts of the PV/EC coating consists of:

• PV part: TCO/a-SiC:H-n/a-SiC:H-i/a-SiC:H-p• EC part: TCO/V2O5 (ion-storage layer)/LiAlF4 (ion conductor layer)/Liy-

WO3(EC layer)/TCO

The whole composition of a PV/EC glazing can be as follows: glass/TCO/a-SiC:H-n/a-SiC:H-i/a-SiC:H-p/TCO/V2O5/LiAlF4/LiyWO3/TCO. The device isdarkened when the top and bottom TCO layers are electrically connected viaexternal switch. The middle TCO layer is used for battery charging and usercontrol [119].

3.7 Liquid Crystal and Suspended Particle Glazings

Liquid crystals (LC) are materials comprised of thin, needle-shaped organicmolecules that are randomly distributed and flow like liquids. Under certainconditions they could be aligned and ordered. They exist in several liquid crys-talline phases, such as [120]:

• nemanic phase (LC orientation order but no position order),• cholesteric phase (LC local orientation in a helical or spiral configuration),• smetic phase (LC orientation and position order).

LC orientation alters with electric field. Orientation influences the light trans-mittance of the LC glazing. There are several types of LC used in switchabledevices. Polymer dispersed liquid crystals (PDLC) and nemanic curvilinearaligned phase of encapsulated liquid crystals (NCAP) are used in large-areaglazing applications [63, 120, 121]. Guest-host LC represents another possibilityfor windows [63]. PDLC have wide applications for architectural and automotiveglazings [122].

These window glazings have LC within an index matched polymer matrixbetween two transparent conductive oxides TCO electrodes. The composition ofthe LC glazing can be: glass/TCO/dielectric layer/PDLC layer/dielectric layer/TCO/glass [14, 124]. LC molecules are dispersed between two conductive elec-trodes. Activation of the electric field causes alignment of the LC. This allows forenhanced light transmittance. The device appears translucent and white in the

Window Glass Coatings 923

off-state. LC glazings require electrical activation to be in the transparent state[14, 121–126].

A new LC glazing technology which does not require constant power has beendeveloped. A reverse mode of PDLC glazing is achieved by doping with photo-conductive molecules in the polymer LC matrix [127, 128, 129].

Suspended particle glazings also require electrical activation to reach trans-parency. They are not transparent in the non-activated state [130–136]. A sus-pended particle (SP) switchable device consists of glass/TCO/dielectric layer/SPlayer/dielectric layer/TCO/glass [130, 131]. Polyester sheets can be also usedinstead of the glass panes.

The active SP layer has needle-shaped dipole particles (less l lm long). Theyare suspended randomly in an organic fluid or gel in the electrically non-activatedstate, causing absorption and scattering of incident light. The suspended particlesalign if an electric field is applied, causing bleaching of the device.

SP glazing with modified particles could provide darkening in several colors.SP glazings with encapsulated particles in polymers and laminated the compositebetween polyester sheets show promise for large glazed areas applications [136].

4 Light Enhancing and Controlling Glazings

Modern solar technologies offer light enhancement and control systems. Thesesystems serve to transport and redirect light into the interiors of buildings toimprove indoor visual comfort. Optical fibers, transparent materials with micro-structured surfaces or holographic films, fluorescent concentrators and mirrors canguide, redirect and concentrate light [137–140].

These materials integrated into façades and glazed roofs can eliminate glare andoverheating problems in building interiors. They can also be used for solar con-version systems [140, 141]. Combinations of prismatic materials and switchabletechnology provide smart solar control transparent devices [116, 142–149].

Enhancement of light and solar transmittance in window glass can be achievedthrough antireflective coatings [150–158]. Special self-cleaning functional coat-ings also positively influence light transmittance of windows [159–169].

4.1 Switchable Devices and Prismatic Surfaces

Microprismatic glass coatings and retro-reflecting prisms serve for angle selectivesolar control. They allow variation of transmittance dependent upon the angle ofsolar radiation incidence [138–140]. High-angle incident light is retro-reflected butlow-angle incident and diffuse light is transmitted.

The microprismatic surface patterns are produced by the interference holog-raphy or micro-machining technology. The microstructure can be periodic

924 J. Mohelníková

(triangular, sinusoidal and parabolic) or random (periods between 0.2 and 50 lm)[140, 141]. The surface is laminated on the inner surfaces of double-glazed units inbuilding applications.

Transparent materials with micro and/or macro-structured surfaces can becombined with switchable devices to achieve a user-controlled system, Fig. 5c[116, 142–144]. This combination provides dynamic regulation of solar trans-mittance. Parts of the prismatic surfaces exposed to high solar incidence have thinchromogenic coatings. These coatings reduce transmittance due to a switchablecoloration process. Glare protection is achieved through prismatic surface retro-reflecting and light-scattering effects.

Another possible application of switchable glazing technology is the combi-nation of laminated glass with light emitting diodes (LEDs), with a liquid crystalinterlayer embedded between two glass panes with transparent conductive oxidelayers [145–147].

A switchable glazing system with surface micro-blinds has been developed, asshown in Fig. 6. The device controls light transmittance in response to appliedvoltage. Thin metal micro-blinds are deposited on a glass substrate with a trans-parent conductive oxide layer and an insulator layer. The micro-blinds are rolled inthe transparent electrically non-activated state. When electric field is activated apotential difference between the thin rolled metal and transparent conductive layercauses the micro-blinds to stretch and limit light transmittance (shading effect)[148, 149].

4.2 Antireflective Glazings

Special low-iron glasses and glazings with antireflective coatings can be used toimprove visible and solar transmittance.

Generally an antireflective (AR) coating consists of alternating dielectric layersof materials with high (as ZrO2, Ta2O5 or TiO2) and low (as MgF2, SiO2 and

Fig. 5 Prismatic transparentmaterials, a transmission oflow-angle incident solar rays,b retro-reflection of high-angle incident solar rays,c retro-reflection andabsorption of solar radiationon switchable coatings(deposited on the obliqueparts of the prisms)[116, 142–144]

Window Glass Coatings 925

Al2O3) refractive indices [150, 151]. Devices comprised of TiO2 and SiO2 layersare commonly used [152]. Multilayer dielectric AR coatings can enhance thetransmittance of visible light. A single AR layer with low refractive index and highporosity is recommended for solar energy applications. A third type of the ARcoating can improve both visible and solar near-IR transmittance [152].Non-porous materials can also achieve the AR effect through surface etching,nano-patterns or gratings [152–155].

An example of a practical application of AR coatings for windows is theenhancement of the visible transmittance of low-e glazings. An AR coating ofporous SiO2 can be deposited on both sides of a glazing with a pyrolytic low-etin-oxide coating [156]. Antireflective coatings are also useful in switchableglazing technologies, such as electrochromic glazings [157, 158].

4.3 Self-Cleaning Glazings and Coatings

Special coatings can create self-cleaning or easy-to-clean surfaces [159–161].These coatings can provide:

• photocatalytic function (decomposition of organic materials on the glasssurface),

• hydrophilic function (strongly wettable surface which allows water sheeting,which cleans the surface),

• hydrophobic function (weakly wettable surface).

A porous TiO2 thin film coating can exhibit both the photocatalytic andhydrophilic effects [159–161]. Incident solar radiation (UV part) generates thecatalytic activity within the TiO2 surface coating. The excited titanium transfers itsenergy to the oxygen molecules, which loses an electron. Electrons migrate to the

Fig. 6 Function of micro-blinds, a in the electricallynon-activated state(transparent), b in theelectrically activated state(shading), 1-glass substrate,2-adhesion layer andtransparent conductive layer,3-insulator, 4-reflectiveresilient metal micro-blind(4a-rolled blind, 4-stretchedblind) [148, 149]

926 J. Mohelníková

organic material on the glass surface and decompose it. This process also changesthe glass surface to hydrophilic by creating oxygen vacancies, which react withwater. Due to this activity water droplets wet the surface. The water washes awaythe decomposed organic materials. The thin TiO2 photo-catalytically activecoating should be covered by a special corrosion protective coating [162, 163] forlarge façade or roof glazing applications.

Another self-cleaning system is a hydrophobic surface coating. It consists of awater polymer matrix which creates a surface with nanoscale pores. The self-cleaning effect is achieved due to water surface tension. Water drops form almostspherical droplets on the hydrophobic surface. They fall off the surface due togravity and roll dust and small dirt with them. Water drops are removed beforethey can evaporate on the surface [164], as shown in Fig. 7.

Special smart switchable coatings provide protective, hydrophobic or hydro-philic and other properties. Such smart coatings can also reversibly alter thewetting properties of surfaces [165–169] in response to external stimuli.

5 Conclusion

An overview of several types of window glazings and coatings has been presented.Implementations of thin film coatings for multifunctional glazed window unitsprovide integrated systems with spectrally selective glazings of high visibletransmittance and low-emissivity, which can be completed with solar control andswitchable glazings with light retro-reflecting and guiding units.

The development of glazing systems continues to interest researchers. There isa trend toward applications of chromogenic glazings for large glazed areas ofbuilding envelopes. Improvements in durability, maintenance-free service andlow-cost production will be the focal points of future work.

Photovoltaics offer self-powered glazed devices. Systems based on nanotechnol-ogy and advanced materials provide new types of self-activated switchable coatingsfor multifunctional smart glazing devices with reversibly modified properties.

Fig. 7 Self-cleaningsurfaces, a water drop rolledon the hydrophobic surface,b water drop spread on thehydrophilic surface [164]

Window Glass Coatings 927

Integrated multi-function glazings are representatives of systems that are ableto dynamically modulate their properties in the response to external climaticconditions. Such changes can increase energy efficiency, and indoor visual andthermal comfort in buildings.

Acknowledgments The window glazings and coatings overview was elaborated within theframe of research projects MŠMT MEB 080804 and GACR 101/09/H050. The authoracknowledges Dr. Pavel Pokorny, ISI AS CR, Brno for consultations on the thin film design andcomputer simulations.

References

1. IEA SH&C: Task 10 solar materials, Task 18 advanced glazing materials, Task 27 energyperformance of switchable glazing. http://www.iea-shc.org

2. Hutchins MG (1998) Advanced glazing materials. Sol Energy 62:145–1473. Lampert CM (1992) Advanced glazing technology. Fenestration 2000, phase III-glazing

materials. LBL-31616, Berkeley4. Robinson PD, Hutchins MG (1994) Advanced glazing technology for the low energy

buildings in the UK. Renew Energy 5:298–3095. Bauchot M (2001) Energy, environmental and economic benefits from advanced double

glazing in EU dwellings. Glass performance days, Tampere 20016. O’Shaughnessy D (2009) TH18-global megatrends and next-generation architectural glass.

Proc Construct 2009, Indianopolis7. Granqvist CG et al (2010) Advances in chromogenic materials and devices. Thin Solid

Films 518:3046–30538. Lee ES, Selkowitz SE et al (2006) Active load management with advanced window wall

systems: research and industry perspectives. Final project report CEC-500-2006-052-AT1.LBNL, California

9. Johnson ET (1991) Low-e glazing design guide. Butterworth Architecture, Boston10. Pulker HK (1998) Coatings on glass. Elsevier, Amsterdam11. Lampert CM (1981) Heat mirror coatings for energy conserving windows. Sol Energy

Mater 6:1–4112. Fan JC (1981) Sputtered films for wavelength-selective applications. Thin Solid Films

80:125–13613. Berning PH (1983) Principles of design of architectural coatings. Appl Opt 22:4127–414114. Terry Hollands KG et al (2001) Glazings and coatings. In: Gordon J (ed) Solar energy: the

state of the art, ISES position papers. James & James, London15. Karlsson B (1981) Materials for solar transmitting heat reflecting coatings. Thin Solid Films

86:91–9816. Stjerna B et al (1994) Optical and electrical properties of radio frequency sputtered tin oxide

films doped with oxygen vacancies, F, Sb, or Mo. J Appl Phys 76:3797–381717. Hamberg I, Granqvist CG (1986) Evaporated Sn-doped In2O3 film: basic optical properties

and applications to energy efficient windows. J Appl Phys 60:R123–R16018. Jin ZC et al (1988) Optical properties of sputter-deposited ZnO:Al film. J Appl Phys

64:5117–513119. Terry Hollands KG et al (2001) Glazings and coatings. High transmittance in the visible

region and reflectance in the IR. In: Gordon J (ed) Solar energy: the state of the art, ISESposition papers. James & James, London, pp 56–70

20. Valkonen E et al (1984) Solar optical properties of thin films of Cu, Ag, Au. Sol Energy32:211

928 J. Mohelníková

21. Palik (ed) (1991) Handbook of optical constants of solids. Academic Press, New York22. Computer program FILM*CALC 3.03—advanced optical thin film technology, FTG

software associates, Princeton23. Bräuer G (1999) Large area glass coating. Surf Coat Technol 112:358–36524. Schaefer C et al (1997) Low emissivity coatings on architectural glass. Surf Coat Technik

93:37–4525. Smith GB et al (2004) Energy-efficient coatings in nanohouseTM initiative. Curr Appl Phys

4:381–38426. Granqvist CG (1990) Window coatings for the future. Thin Solid Films 193:730–74127. Gläser HJ The European history of coatings on architectural glazing. http://www.

glassfiles.com28. Fan et al (1985) Transparent heat-mirror. US Patent 455627729. Kim D (2010) Low temperature deposition of transparent conducting ITO/Au/ITO films by

reactive magnetron sputtering. Appl Surf Sci 256:1774–177730. Martin-Palma RJ et al (1998) Silver-based low-emissivity coatings for architectural

windows: optical and structural properties. Sol Energy Mater Sol Cells 53:55–6631. Miyazaki M, Ando E (1994) Durability improvement of Ag-based low-emissivity coatings.

J Non-Cryst Solids 178:245–24932. Andersson KE et al (1994) Zirconium nitride based transparent heat mirror coatings

preparation and characterisation. Sol Energy Mater Sol Cells 32:199–21233. Kusano E et al (1986) Thermal stability of heat-reflective films consisting of oxide-

Ag-oxide deposited by dc magnetron sputtering. J Vac Sci Technik A: Vacuum, Surfaces,and Films 4:2907–2910

34. Lampert CM (1981) Heat Mirror Coatings for Energy Conserving Windows. Solar EnergyMater 6:1–41

35. Szczyrbowski J et al (1999) New low emissivity coating based on TwinMag� sputteredTiO2 and Si3N4 layers. Thin Solid Films 351:254–259

36. Beister G et al (1995) Progress in large-area glass coatings by high-rate sputtering. SurfCoat Technol 76–77:776–785

37. Schaefer C et al (1997) Low emissivity coatings on architectural glass. Surf Coat Technik9:37–45

38. Lu Y et al (2009) Method of making low-e coating using ceramic zinc inclusive target andtarget used in same. USPTO Patent Application 20090205956

39. Boor WP (2008) Studying low-e glass performance. Constr Specif, http://www.ppg.com/corporate/ideascapes/SiteCollectionDocuments/274404_final.pdf

40. Steven J et al (2007) Durable low-e coated glass for use in warm temperate climates. Glassperformance days 2007, Tampere

41. Glenn D et al (2009) Double silver low emissivity and solar control coating. US Patent7632572 B2

42. Glenn D et al (2003) Double silver low emissivity and solar control coating. US PatentApplication Publication 2003/0049464 A1

43. Hartig KW et al (1996) Dual silver low-e glass coating system and insulating glass madethereform. US Patent 5557462

44. Neuman G et al (2008) Coated article with low-e coating including IR reflecting layer(s)and corresponding method. US Patent 7419725

45. Manfrè G (2005) The need of innovation for solar control technologies, Glass performancedays 2005, Tamper

46. Ochs D et al (2007) Progressive power supplies for architectural glass coating. Glassperformance days 2007, Tampere

47. Nair PK et al (1991) Optimisation of chemically deposited CuxS solar control coatings.J Appl Phys 24:441–449

48. Russo D et al (2003) Solar control coated glass. US Patent 659639849. McKown C et al (2001) Solar control coated glass. US Patent 6218018

Window Glass Coatings 929

50. Ujiie T, Katono H (2005) High performance solar control material. Glass performance days2005, Tampere

51. Smith GB (1990) Theory of angular selective transmittance in oblique columnar thin filmscontaining metal and voids. Appl Opt 29:3685–3693

52. Elkadi H (2006) Cultures of glass architecture. Ashgate, Hampshire53. Reppel J, Edmonds IR (1998) Angle-selective glazing for radiant heat control in buildings:

Theory. Sol Energy 62:245–25354. Smith GB et al (1998) Thin film angular selective glazing. Sol Energy 62:229–24455. Dligatch S (1998) An analysis of Ag/Al2O3 angular selective films by X-ray reflectivity.

Thin Solid Films 312:4–656. Smith GB et al (1998) Angular selective thin film glazing. Renew Energy 15:183–18857. Bellac DL et al (1995) Angular selective optical transmittance through Cr-based films made

by oblique angle sputtering experiment and theory. J Phys D Appl Phys 28:60058. Ishizuka S (1992) Optical properties of angle dependent light control film. Proc SPIE

1727:24159. Gombert A (2006) Optically functional surfaces for solar applications. ISES, Eurosun 2006,

Glasgow60. Lampert CM (2004) Chromogenic smart materials. Mater Today 7:28–3561. Lampert CM (1995) Chromogenic switchable glazing: towards the development of the

smart window. In: Proceedings of window innovations ’95, Toronto62. Hoffmann HJ (1990) Photochromic glass. In: Lampert CM, Granqvist CG (eds) Large-area

chromogenics: materials and devices for transmittance control, vol IS4. SPIE, Bellingham,pp 86–101

63. Wiggington M (1996) Glass in architecture. Phaidon Press, London64. Fanderlík I (1996) Vlastnosti skel. Informatorium, Prague65. Araujo RJ (1980) Photochromism in glasses containing silver halides. Contemp Phys 21:7766. Chu N (1990) Photochromic plastics. In: Lampert CM, Granqvist CG (eds) Large-area

chromogenics: materials and devices for transmittance control, vol IS4. SPIE Bellingham,pp 102–121

67. Chu N (1986) Photochromic performance of spiroindolinonaphthoxazines in plastics. SolEnergy Mater 14:215

68. Richardson TJ et al (2001) Switchable mirrors based on nickel–magnesium films. Appl PhysLett 78:3047

69. Yoshimura K, Okada M (2007) Reflective light control element with diffusible reflectingsurface. US Patent 7259902

70. Teowee G et al (2001) Photochromic devices. US Patent 624650571. Day J, Willet R (1990) Science and technology of thermochromic materials. In: Lampert

CM, Granqvist CG (eds) Large-area chromogenics: materials and devices for transmittancecontrol, vol IS4. SPIE, Bellingham, pp 122–147

72. Jorgenson GV, Lee JC (1990) Thermochromic materials and devices: inorganic systems.In: Lampert CM, Granqvist CG (ed) Large-area chromogenics: materials and devices fortransmittance control, vol IS4. SPIE, Bellingham, pp 142–159

73. Sone K, Fukuda Y (1987) Inorganic thermochromism. Springer, Berlin74. Babulanam SM et al (1987) Thermochromic VO2 films for energy efficient windows.

Sol Energy Mat 16:34775. Jorgenson GV, Lee JC (1986) Doped vanadium oxide for optical switching films.

Sol Energy Mat 14:20576. Parkin I, Manning T (2007) Thermochromic coatings. US Patent 004843877. Blackman Ch et al (2009) Atmospheric pressure chemical vapour deposition of

thermochromic tungsten doped vanadium dioxide thin films for use. Thin Solid Films517:4565–4570

78. Mlyuka NR et al (2009) Mg doping of thermochromic VO2 films enhances the opticaltransmittance and decreases the metal-insulator transition temperature. Appl Phys Lett95:171909

930 J. Mohelníková

79. Haldimann M et al (2008) Structural use of glass. International Association for Bridge andStructural Engineering, Zürich

80. Wilson HR (1994) Optical properties of thermotropic layers. Proc SPIE 2255:47381. Seeboth A et al (2004) Chromogenic polymer gels for reversible transparency and color

control. In: Samson A et al (ed) Chromogenic phenomena in polymers, vol 888, chapter 80.ACS Symposium Series, Washington DC, pp 110–121

82. Nitz P, Hartwig H (2005) Solar control with thermotropic layers. Sol Energy 79:573–58283. Georg A et al (1998) Switchable glazing with a large dynamic range in total solar energy

transmittance (TSET). Sol Energy 62:215–22884. Wilson HR et al (2002) The optical properties of gasochromic glazing. In: Proceedings of

the 4th international conference on coating on glass, Braunschweig85. Schwarz M (2008) Smart materials. CRC Press, Taylor & Francis, Boca Raton86. Wittwer V et al (2004) Gasochromic windows. Sol Energy Mater Sol Cells 84:305–31487. Wittwer V, Graf W (2001) Gaschromic glazings with a large dynamic range in total solar

energy transmittance. Glass performance days 2001, Tampere88. Lampert CM (2002) Electrochromics-history, technology, and the future, 6.1 gas-chromics.

In: Chowdari B et al (ed) Solid state ionics: trends in the new millenium. Proceedings of the8th Asian conference on world scientific, London

89. Se-hee L et al (2004) Pd/Ni-WO3 anodic double layer gasochromic device. US Patent6723566

90. Lampert CM, Granqvist CG (1990) Large-area chromogenics: materials and devices fortransmittance control, vol IS 4. SPIE Institutes for Advanced Optical technologies,Bellingham

91. Granqvist CG (1995) Handbook of inorganic electrochromic materials. Elsevier,Amsterdam

92. Monk P et al (2007) Electrochromism and electrochromic devices. Cambridge UniversityPress, London

93. Deb SK et al (1978) Electrochromic cell with protective overcoat layer. US Patent 412056894. Granqvist CG (2005) Electrochromic device. J Eur Ceram Soc 25:2907–291295. Granqvist CG (1992) Electrochromism and smart window design. Solid State Ionics

53–56:479–48996. Granqvist CG (2008) Oxide electrochromics: why, how, and whither. Sol Energy Mater Sol

Cells 92:203–20897. Granqvist CG et al (2007) Nanomaterials for benign indoor environments: electrochromics

for ‘‘smart windows’’, sensors for air quality, and photo-catalysts for air cleaning. SolEnergy Mater Sol Cells 91:355–365

98. Granqvist CG et al (2003) Electrochromic coating devices: survey of some recent advances.Thin Solid Films 442:201–211

99. Granqvist CG (2000) Electrochromic tungsten oxide films: review of progress 1993–1998.Sol Energy Mater Sol Cells 60:201–262

100. Granqvist CG et al (1997) Towards the smart window: progress in electrochromics.J Non-Cryst Solids 218:273–279

101. Granqvist CG (1990) Window coatings for the future. Thin Solid Films 193–194:730–741102. Lampert CM (2002) Electrochromism-history, technology and the future. In: Chowdari, B

et al (ed) Solid state ionics: trends in the new millenium. Proceedings of the 8th Asianconference on world scientific, London

103. Lampert CM (1998) Smart switchable glazing for solar energy and daylight control. SolEnergy Mater Sol Cells 52:207–221

104. Lampert CM (1993) Optical switching technology for glazing. Thin Solid Films 236:6–13105. Lampert CM (1984) Electrochromic materials and devices for energy efficient windows. Sol

Energy Mat 11:1–27106. Avendaño E et al (2004) Electrochromism in nickel oxide films containing Mg, Al, Si, V,

Zr, Nb, Ag, or Ta. Sol Energy Mater Sol Cells 84:337–350

Window Glass Coatings 931

107. Jonson A, Roos A (2006) Influence of the performance of antireflective coatings inelectrochromic windows. In: Proceedings of ISES EuroSun 2006, Glasgow

108. Rottmann M et al (2005) Large area electrochromic safety glass; switching behaviour andtransmission control of solar radiation. Glass performance days 2005, Tampere

109. Granqvist CG (2006) Solar energy materials of the future: electrochromic foils for energyefficiency and indoor comfort. In: Proceedings of ISES EuroSun 2006, Glasgow

110. Bechinger CS et al (2002) Self bleaching photoelectrochemical-electrochromic device. USPatent 6369934

111. Pichot F et al (1999) Flexible solid-state photoelectrochromic windows. J Electrochem Soc146:4324–4326

112. Georg A, Opara Krašovec U (2006) Photoelectrochromic window with Pt catalyst. ThinSolid Films 502:246–251

113. Hauch A et al (2001) New photoelectrochromic device. Electrochim Acta 46:2131–2136114. Gombert A (2007) New development in glazing for a better use of solar energy in buildings.

Glass performance days 2007, Tampere115. Lampert CM (2003) Large-area smart glass and integrated photovoltaics. Sol Energy Mater

Sol Cells 76:489–499116. Gombert A (2007) New developments in glazing for better use of solar energy in buildings.

Glass performance days 2007, Tampere117. Benson DK, Branz HM (1995) Design goals and challenges for a photovoltaic-powered

electrochromic window covering. Sol Energy Mater Sol Cells 39:204–211118. Gao W et al (2000) Approaches for large-area a-SiC:H photovoltaic-powered

electrochromic window coatings. J Non-Cryst Solids 266–269:1140–1144119. Gao W et al (1999) First a-SiC:H photovoltaic-powered monolithic tandem electrochromic

smart window device. Sol Energy Sol Cells 59:243–254120. Lampert CM (1990) Introduction to liquid crystals. Large-area chromogenics: materials and

devices for transmittance control, vol IS 4. SPIE, Bellingham121. Amstock JS (1997) Liquid crystals and suspended-particle device. Handbook of glass in

construction. McGraw-Hill, New York122. Sucheol P, Hong JW (2009) Polymer dispersed liquid crystal film for variable-transparency

glazing. Thin Solid Films 517:3183–3186123. Lampert CM (1999) Advances in materials and technology for switchable glazing. Glass

performance days 1999124. Lampert CM (1994) Glazing materials for solar and architectural applications, IEA SH&C

Task 10 C, LBL-34436125. Sixou P et al (2001) Switchable liquid-crystal/polymer micro-composite glazings. Glass

processing days 2001126. Baughmann et al (1990) Dual-pane thermal window with liquid crystal shade. US Patent

4964251127. Garnier DJ et al (2009) High-efficiency multistable switchable glazing using smetic A liquid

crystals. Sol Energy Mater Sol Cells 93:301–306128. Cupelli D et al (2009) Self-adjusting smart windows based on polymer-dispersed liquid

crystals. Sol Energy Mater Sol Cells 93:2008–2012129. Cupelli D et al (2004) Fine adjustment of conductivity in polymer-dispersed liquid crystals.

Appl Phys Lett 85:3292–3294130. Lampert CM (1995) Chromogenic switchable glazing: towards the development of the

smart window. In: Conference proceedings of window innovations ‘95, Toronto131. Amstock JS (1997) Liquid crystals and suspended-particle device. Handbook of glass in

construction, McGraw-Hill, New York132. Vergaz R et al (2008) Modelling and electro-optical testing of suspended particle device.

Sol Energy Mater Sol Cells 92:1483–1487133. Check JA (1995) Light modulating film of improved clarity for a light valve. US Patent

5463492

932 J. Mohelníková

134. Saxe RL (1981) Light valve containing improved light valve suspension. US Patent4247175

135. Thompson et al (1978) Light valve. US Patent 4078856136. Lampert CM (1999) Advances in materials and technology for switchable glazing. Glass

processing days 1999, Tampere137. Riccobono J, Ludman J (2002) Solar holography. In: Luxman J et al (eds) Holography for

the new millenium. Springer, New York138. Hans DT et al (1993) Design optimization and manufacturing of holographic windows for

daylighting applications in buildings. In: Lampert CM (ed) Optical materials technology forenergy efficiency and solar energy conversion XII. SPIE, Bellingham 2017, pp 35–45

139. Stojanoff CG (2006) Engineering applications of HOEs manufactured with enhancedperformance DCG films. In: Bjelkhagen HI, Lessard RA (eds) Practical holography XX:materials and applications. SPIE Proceedings 6136 613601

140. Hoßfeld W et al (2003) Application of microstructured surfaces in architectural glazings.In: Proceedings of ISES solar world congress 2003, Göteborg

141. Gunther W et al (2005) Combination of microstructures and optically functional coatingsfor solar control glazing. Sol Energy Mater Sol Cells 89:233–248

142. Wilson V et al (2002) The optical properties of gasochromic glazings. In: Proceedings of4th international conference coating on glass, Braunschweig

143. Gombert A (2006) Optically functional surfaces for solar applications. In: Proceedings ofISES EuroSun 2006, Glasgow

144. Graf et al (2003) Device for guiding light. WO Patent WO/2003/071079145. Shavit D (2007) LED-and SMD-polyester film embedded in glass: history, current and

future developments. Glass performance days 2007, Tampere146. Lefèvre H (2009) Laminated glass with embedded LEDs: the use of specific power supplies

able to provide continuous high voltage allows new lighting applications and colour changesin decorative applications. Glass performance days 2009, Tampere

147. http://www.glassonweb.com148. Lamontagne B et al (2006) Microblinds and methods of fabrication thereof. US Patent

0196613149. Lamontagne B et al (2009) The next generation of switchable glass: the micro-blinds. Glass

performance days 2009, Tampere150. Ochs D, Rettich T (2007) Progressive power supplies for architectural glass coating. Glass

performance days 2007, Tampere151. Boire P et al (2000) Glazing pane having an anti-reflection Coating. US Patent 6086914152. Gombert A et al (1998) Glazing with very high solar transmittance. Sol Energy 62:177–178153. Hofmann T, Kursawe M (2003) Antireflective coating on glass for solar applications glass.

Glass performance days 2003, Tampere154. Olsson G (2003) Low cost industrial manufacturing of a thin single layer antireflective

surface on sheet glass. Glass performance days 2003, Tampere155. Southwell WH (1991) Pyramid-array surface relief structures producing anti-reflection

index matching on optical surfaces. J Opt Soc Am A 8:549–553156. Hammarberg E, Roos A (2003) Antireflection treatment of low-emitting glazings for energy

efficient windows with high visible transmittance. Thin Solid Films 442:222–226157. Jonsson A, Roos A (2006) Antireflective coatings on different window surfaces. In:

Proceedings of the 6th international conference on coatings on glass and plastics, Dresden158. Roos A et al (2009) Applications of coated glass in high performance energy efficient

windows. Glass performance days 2009, Tampere159. Armand P (2003) Self-cleaning coatings for architectural application. Glass performance

days 2003, Tampere160. Hüber M (2003) TiO2-coatings from inorganic soles: a new approach to hydrophilic and

photocatalytically active glasses. Glass performance days 2003, Tampere161. Gläser HJ The effects of weather onto glazing and their influence, Part II. http://www.

glassfiles.com

Window Glass Coatings 933

162. Hohenstein H (2003) Coatings with nano-particles for windows and façades. Glassperformance days 2003, Tampere

163. Nakamura M et al (2004) Hydrophilic property of SiO2/TiO2 double layer films. In: Plütz Jet al (ed) Proceedings of ICCG5, 2004, Saarbrücken

164. Overs M (2005) Coatings for decorative glass surfaces based on chemical nanotechnology.Glass performance days 2005, Tampere

165. Lahann J et al (2006) Switchable surfaces. US Patent 7020355166. Shen L et al (2009) Mechanism of sliding friction on a film-terminated fibrillar interface.

Langmuir 25:2772–2780167. Autumn K et al (2000) Adhesive force of a single gecko foot-hair. Nature 405:681–685168. Provder T, Baghdachi J (2007) Smart Coatings. ACS Symposium Series 957, American

Chemical Society, Oxford University Press, Washington169. Provder T, Baghdachi J (2009) Smart Coatings II. ACS Symposium Series 1002, American

Chemical Society, Oxford University Press, Washington

934 J. Mohelníková