The object of this thesis is to form an understanding of the origin of the problems associated with proton-exchanged waveguides, and to investigate possible solutions. Chapter 1 gives a brief introduction to the properties of lithium niobate, and discusses the methods available for fabricating optical waveguides in the bulk material, with particular emphasis on waveguide fabrication by the proton-exchange process. Some of the devices which have been fabricated by proton-exchange are discussed. The problems associated with proton-exchanged waveguides are reviewed. Chapter 2 deals with the physical and chemical characterisation of proton-exchanged waveguides fabricated using neat benzoic acid melts. The extent of proton-exchange is determined as a function of fabrication time and temperature using optical waveguide prism-coupler measurements, infrared absorption spectroscopy, and atomic absorption spectroscopy. Chapter 3 is concerned with the problem of waveguide mode-index stability. Using a hydrogen isotopic-exchange reaction, the extent of which is obsrved via infrared absorption spectroscopy, information on the (room-temperature) mobility of protons within the guiding layer is obtained for waveguides fabricated using neat benzoic acid melts. The recently reported process of fabricating waveguides in lithium niobate by deuterium-exchange is investigated. The behaviour of proton-exchanged and deuterium-exchanged waveguides with respect to reaction with atmospheric water vapour is investigated, and the optical properties of deuterium-exchanged waveguides are studied. In Chapter 4, a study of annealed and dilute-melt proton-exchanged waveguides is presented. It is shown, using prism-coupler measurements and infrared absorption spectroscopy, that ennealed and dilute-melt waveguides can have very similar optical properties, depending on the amount of annealing and the lithium benzoate mole-fractions used. The extent of proton-exchange is determined with time (between 215oC and 235oC) for dilute-melt waveguides produced using lithium benzoate mole-fractions of up to 1.1%. Isotopic-exchange in annealed and dilute-melt waveguides is also investigated, both at room-temperature and at temperatures commonly used for annealing. A possible explanation for the poor optical properties of (neat-melt) proton-exchanged waveguides is given. Chapter 5 deals with a study of propagation losses (using the two-prism method) and the electro-optic effect in x- and z-cut proton-exchanged waveguides. Measurements of r33 (in proton-exchanged waveguides) and r22 (in titanium-indiffused waveguides) are carried out using an external interferometric method designed by the author. The results of Chapter 4 are used to establish a method by which losses below 0.5dB/cm and a substantially restored electro-optic effect can be achieved (using a combination of dilute-melt fabrication with post-exchange annealing). Prior to the waveguide measurements, the bulk electro-optic effect is investigated for congruent, incongruent, MgO-doped, and annealed (high-temperature) crystals. Finally, in Chapter 6, a summary of the thesis is presented, and suggestions for future work are given.
[1]
I. Kaminow,et al.
Metal‐diffused optical waveguides in LiNbO3
,
1974
.
[2]
H Kogelnik,et al.
Scaling rules for thin-film optical waveguides.
,
1974,
Applied optics.
[3]
R. Rue,et al.
Proton‐exchanged, lithium niobate planar‐optical waveguides: Chemical and optical properties and room‐temperature hydrogen isotopic exchange reactions
,
1987
.
[4]
T. J. Cullen,et al.
Radiation losses from single-mode optical Y junctions formed by silver-ion exchange in glass.
,
1984,
Optics letters.
[5]
E. Lippincott,et al.
One‐Dimensional Model of the Hydrogen Bond
,
1955
.
[6]
T Suhara,et al.
Proton-exchanged Fresnel lenses in Ti:LiNbO3 waveguides.
,
1986,
Applied optics.
[7]
P. Bridenbaugh,et al.
Dependence of Linear Electro‐Optic Effect and Dielectric Constant on Melt Composition in Lithium Niobate
,
1970
.
[8]
K. Yamamoto,et al.
New proton-exchange technique for LiNbO3 waveguide fabrication
,
1987
.
[9]
E. Turner,et al.
HIGH‐FREQUENCY ELECTRO‐OPTIC COEFFICIENTS OF LITHIUM NIOBATE
,
1966
.
[10]
D. Skinner,et al.
Desirability Of Electro-Optic Materials For Guided-Wave Optics
,
1987
.
[11]
Y. Okamura,et al.
Measuring mode propagation losses of integrated optical waveguides: a simple method.
,
1983,
Applied optics.
[12]
R. A. Becker,et al.
Comparison of guided‐wave interferometric modulators fabricated on LiNbO3 via Ti indiffusion and proton exchange
,
1983
.
[13]
R. Chen,et al.
Thermally annealed single-mode proton-exchanged channel-waveguide cutoff modulator.
,
1986,
Optics letters.
[14]
Shih-Kay Yao,et al.
Double ion exchanged chirp grating lens in lithium niobate waveguides
,
1983
.
[15]
A. Yariv,et al.
Guided wave optics
,
1974
.
[16]
J. Veselka,et al.
Proton exchange for high‐index waveguides in LiNbO3
,
1982
.
[17]
P. F. Heidrich,et al.
Optical waveguide refractive index profiles determined from measurement of mode indices: a simple analysis.
,
1976,
Applied optics.
[18]
K. Nassau,et al.
Ferroelectric lithium niobate. 2. Preparation of single domain crystals
,
1966
.
[19]
P. K. Tien,et al.
Theory of Prism–Film Coupler and Thin-Film Light Guides
,
1970
.
[20]
D. Skoog.
Fundamentals of analytical chemistry
,
1963
.
[21]
S. Abrahams,et al.
Defect structure dependence on composition in lithium niobate
,
1986
.
[22]
M. Werner,et al.
Electrically switched optical directional coupler: Cobra
,
1975
.
[23]
James F. Ziegler,et al.
New precision technique for measuring the concentration versus depth of hydrogen in solids
,
1976
.
[24]
W. C. Hamilton,et al.
Ferroelectric lithium tantalate—1. single crystal X-ray diffraction study at 24°C
,
1966
.
[25]
H. Levinstein,et al.
Ferroelectric lithium niobate. 5. Polycrystal X-ray diffraction study between 24° and 1200°C
,
1966
.
[26]
Ivan P. Kaminow,et al.
An introduction to electrooptic devices
,
1974
.
[27]
W. Lanford.
15N hydrogen profiling: Scientific applications
,
1978
.
[28]
E. Kaldis.
Current Topics in Materials Science
,
1980
.