Optimization of antireflection coating for VO2-based energy efficient window

Abstract Vanadium dioxide (VO 2 ) films have been proposed as energy efficient window coatings for their thermochromism, with which the solar energy transmission in the IR region may be controlled passively. These coatings suffer from low visible (or luminous) transmission (380–760 nm in wavelength), which hinders their practical uses. We here consider an antireflection (AR) coating for the VO 2 -based window. Optical calculation was first performed upon a basic structure for thermochromic window composed of a VO 2 layer on glass with an AR layer of refractive index n and thickness d . Optimization was carried out on n and d for a maximum integrated luminous transmittance ( T lum ). The calculation demonstrates that the optimal n value changes with thickness of VO 2 , and at n ≈2.2 it gives the highest T lum enhancement from 32% (without AR coating) to 55% for 50-nm VO 2 . Experiment was done on a structure of 50-nm VO 2 on quartz glass using ZrO 2 , of which n ≈2.2 matching the best n value, as AR coating. Formation of an optimized structure, ZrO 2 (56 nm)/VO 2 (50 nm)/quartz, was done by sputtering, and its optical properties were characterized with spectrophotometry. An improvement of T lum from 32.3% to 50.5% was confirmed for the semiconductor phase with similarity also for the metallic one. The IR switching properties were not much deteriorated.

[1]  A. Scharmann,et al.  W- and F-doped VO2 films studied by photoelectron spectrometry , 1999 .

[2]  M. Nygren,et al.  A D.T.A. study of the semiconductor-metallic transition temperature in V1−xWxO2, 0 ≤ x ≤ 0.067 , 1969 .

[3]  Claes-Goeran Granqvist,et al.  Window coatings for the future , 1990 .

[4]  F. Case,et al.  Modifications in the phase transition properties of predeposited VO2 films , 1984 .

[5]  E. Palik Handbook of Optical Constants of Solids , 1997 .

[6]  C. Granqvist,et al.  Materials science for solar energy conversion systems , 1991 .

[7]  F. J. Morin,et al.  Oxides Which Show a Metal-to-Insulator Transition at the Neel Temperature , 1959 .

[8]  C. N. Berglund,et al.  Optical Properties of V O 2 between 0.25 and 5 eV , 1968 .

[9]  Mats Nygren,et al.  Electrical and magnetic properties of V1−xWxO2, 0 ≤ x ≤ 0.060 , 1972 .

[10]  O. S. Heavens,et al.  Optical Properties of Thin Solid Films , 2011 .

[11]  Charles B. Greenberg,et al.  Undoped and doped VO2 films grown from VO(OC3H7)3 , 1983 .

[12]  Moon-Hee Lee,et al.  Better thermochromic glazing of windows with anti-reflection coating , 2000 .

[13]  John B. Goodenough,et al.  The two components of the crystallographic transition in VO2 , 1971 .

[14]  R. Smoluchowski,et al.  Elements of X‐Ray Diffraction , 1957 .

[15]  Claes-Goeran Granqvist,et al.  Thermochromic sputter‐deposited vanadium oxyfluoride coatings with low luminous absorptance , 1989 .

[16]  B. Harbecke,et al.  Coherent and incoherent reflection and transmission of multilayer structures , 1986 .

[17]  C. H. Griffiths,et al.  Influence of stoichiometry on the metal‐semiconductor transition in vanadium dioxide , 1974 .

[18]  S. Tanemura,et al.  Optical constants of V(1-x)W(x)O(2) Films. , 1998, Applied optics.

[19]  Gunnar A. Niklasson,et al.  Thermochromic VO2 Films for Energy-Efficient Windows , 1987, Optics & Photonics.