LiNbO3: AN EFFICIENT PHASE MATCHABLE NONLINEAR OPTICAL MATERIAL

Boyd, G. D.; Miller, Robert C.; Nassau, K.; Bond, W. L.; Savage, A.

doi:10.1063/1.1723604

Cited by 512 publications

(197 citation statements)

References 18 publications

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“…(1) which for a scattering angle B = 90° takes the following form: [7]. Table I lists the experimentally determined phonon velocities and comparison is made to those measured in ultrasonics [8].…”

Section: Discussion and Resultsmentioning

confidence: 99%

Brillouin Scattering in Lithium Niobate

O’Brien

Rosasco

Weber

1969

Light Scattering Spectra of Solids

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Section: Discussion and Resultsmentioning

confidence: 99%

Brillouin Scattering in Lithium Niobate

O’Brien

Rosasco

Weber

1969

Light Scattering Spectra of Solids

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“…The crystal laser operating on neodymium-activated calcium tungstate (CaWO 4 : Nd a+) emits light of wavelength 1.0582/~m, which is well adapted to the observation of the second harmonic, which has a wavelength of 529.1 nm lying in a region where the human eye is highly sensitive. Miller [48] applied a laser of this kind for SHG in quartz, ferroelectric crystalline BaTiO3, KDP, ADP, CdS [49] and strongly nonlinear LiNbO3 and LiTaOa crystals [50]. Geusic et al [51] observed SHG at 532nm in Ba2NaNbO15 and KrLi4NbO3 using a lightly focused, continuously pumped, repetitively Q-switched Nd : YAG laser emitting light of wavelength 1.064/zm.…”

Section: Shg In Transmitted Lightmentioning

confidence: 99%

Optical harmonic generation and laser light frequency mixing processes in nonlinear media

Kielich

1970

Opto-electronics

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The essential results achieved during the ten years since the coming of lasers, in the fields of second, third and higher harmonic generation in reflected and transmitted, continuous and pulsed laser light, frequency mixing processes in various materials, and nonlinear optical properties of liquids, gases, crystals and other materials are reported concisely from the available literature. Stress is laid on the newer and more stimulating experimental results, and on their relation with other nonlinear phenomena.

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“…The poling direction of each crystal was determined by measuring the sign of the pyroelectric voltage that developed across the sample upon heating. 21,22 Following the convention used in previous studies, the positive ͑c + ͒ face corresponds to one that had a negative pyroelectric voltage, and the negative ͑c − ͒ face to the one that had a positive voltage. 9,21 Experiments were performed using an ultrahigh vacuum chamber ͑base pressure, 2 ϫ 10 −10 torr͒ equipped with a mass spectrometer ͑UTI 100C͒, which was used for TPD experiments, and a cylindrical electron energy analyzer ͑Omicron͒ and an electron gun, which were used to collect AES data.…”

Section: Methodsmentioning

confidence: 99%

Ferroelectric polarization dependent interactions at Pd–LiNbO3(0001) interfaces

Zhao

Bonnell

Vohs

2009

Journal of Vacuum Science &Amp; Technology A: Vacuum, Surfaces, and Films

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A combination of Auger electron spectroscopy and temperature-programed desorption was used to characterize the growth and interaction of Pd films with positively and negatively terminated ferroelectric LiNbO 3 (0001) surfaces. The growth mode of vapor-deposited Pd layers at 300 K was found to be dependent on the direction of the ferroelectric polarization with layer-by-layer growth occurring on the negative (c−) surface and particle formation occurring on the positive (c+) surface. The Pd metal layers were also found to be more thermally stable on the c− surface relative to the c+ surface. These results provide another example of how the polarization orientation in ferroelectric materials affects adsorption and reaction on their exposed surfaces. A combination of Auger electron spectroscopy and temperature-programed desorption was used to characterize the growth and interaction of Pd films with positively and negatively terminated ferroelectric LiNbO 3 ͑0001͒ surfaces. The growth mode of vapor-deposited Pd layers at 300 K was found to be dependent on the direction of the ferroelectric polarization with layer-by-layer growth occurring on the negative ͑c − ͒ surface and particle formation occurring on the positive ͑c + ͒ surface. The Pd metal layers were also found to be more thermally stable on the c− surface relative to the c+ surface. These results provide another example of how the polarization orientation in ferroelectric materials affects adsorption and reaction on their exposed surfaces. Disciplines Engineering | Materials Science and Engineering Comments

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LiNbO3: AN EFFICIENT PHASE MATCHABLE NONLINEAR OPTICAL MATERIAL

Cited by 512 publications

References 18 publications

Brillouin Scattering in Lithium Niobate

Brillouin Scattering in Lithium Niobate

Optical harmonic generation and laser light frequency mixing processes in nonlinear media

Ferroelectric polarization dependent interactions at Pd–LiNbO3(0001) interfaces

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