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Induced fit growth of Ga-based semiconductor thin films for brain-inspired electronics and optoelectronics. [PDF]
Sa Z +16 more
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High-fidelity chip delayering using green (515 nm) femtosecond lasers. [PDF]
Anaei MTM +13 more
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Strategies for Photoelectrochemical Splitting of Water. [PDF]
Ortiz BA +3 more
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Bidirectional Semiconductor Laser
Science, 1999A semiconductor laser capable of operating under both positive and negative bias voltage is reported. Its active region behaves functionally as two different laser materials, emitting different wavelengths, depending on the design, when biased with opposite polarities. This concept was used for the generation of two wavelengths (6.3 and 6.5 micrometers)
Gmachl C +5 more
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Chemical Reviews, 2007
AbstractChemInform is a weekly Abstracting Service, delivering concise information at a glance that was extracted from about 200 leading journals. To access a ChemInform Abstract, please click on HTML or PDF.
I D W, Samuel, G A, Turnbull
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AbstractChemInform is a weekly Abstracting Service, delivering concise information at a glance that was extracted from about 200 leading journals. To access a ChemInform Abstract, please click on HTML or PDF.
I D W, Samuel, G A, Turnbull
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Semiconductor Interferometric Laser
Topical Meeting on Integrated and Guided-Wave Optics, 1982Wavelength control of semiconductor lasers is important in optical communication, where mode stability, tunability, and FM modulation are vital to high quality transmission. Numerous work had been done in optimizing stripe geometry lasers to achieve mode stability.
Ismail H. A. Fattah, Shyh Wang
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Journal of Applied Physics, 1980
The semiconductor Raman laser has been realized by using a GaP crystal. Pumping is made by a Q-switched YAG laser operating at 1.064 μm. The round-trip loss in the Fabry-Perot resonator is 2% or less. The Raman scattering from LO phonons stimulates in the 〈100〉 direction, while the forward and backward Raman scattering from TO phonons stimulate in the 〈
K. Suto, J. Nishizawa
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The semiconductor Raman laser has been realized by using a GaP crystal. Pumping is made by a Q-switched YAG laser operating at 1.064 μm. The round-trip loss in the Fabry-Perot resonator is 2% or less. The Raman scattering from LO phonons stimulates in the 〈100〉 direction, while the forward and backward Raman scattering from TO phonons stimulate in the 〈
K. Suto, J. Nishizawa
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CLEO/Europe - EQEC 2009 - European Conference on Lasers and Electro-Optics and the European Quantum Electronics Conference, 2009
A key advantage that semiconductor ring lasers have over Fabry-Perot (FP) devices for relatively high power applications, is that they do not suffer from Catastrophic Optical Damage (COD) to the cleaved facets of the device bar[1]. However, the directional coupler (DC) section in the ring geometry, equivalent to the facet conditions in a FP laser ...
Strain, M.J. +7 more
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A key advantage that semiconductor ring lasers have over Fabry-Perot (FP) devices for relatively high power applications, is that they do not suffer from Catastrophic Optical Damage (COD) to the cleaved facets of the device bar[1]. However, the directional coupler (DC) section in the ring geometry, equivalent to the facet conditions in a FP laser ...
Strain, M.J. +7 more
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Terahertz semiconductor-heterostructure lasers
Summaries of Papers Presented at the Lasers and Electro-Optics. CLEO '02. Technical Diges, 2002Semiconductor devices have become indispensable for generating electromagnetic radiation in everyday applications. Visible and infrared diode lasers are at the core of information technology, and at the other end of the spectrum, microwave and radio-frequency emitters enable wireless communications. But the terahertz region (1-10 THz; 1 THz = 10(12) Hz)
KOEHLER R. +8 more
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