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21.
A. Dinger R. Ell A. Reznitsky A. Klochikhin C. Klingshirn 《physica status solidi b》2000,221(1):485-490
The exciton dephasing at low temperature in CdS1—xSex is investigated in the composition range from x = 0.07 to 0.8. Trends of fast and slowly decaying components in four wave mixing are revealed depending on the composition x. A plane‐parallel platelet, which exhibits strong Fabry‐Perot modes, shows a periodic, photon energy dependent modulation of the four wave mixing signal as a function of the delay between the incident pulses, which can be attributed to propagation effects of polariton wave packets or to beating between adjacent Fabry‐Perot modes. Another sample shows quantum beats with unusual properties, the origin of which will be discussed. 相似文献
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C. Klingshirn 《physica status solidi b》2007,244(9):3019-3019
The cover picture of the current issue depicts a selection of luminescence colours of zinc oxide and relates to the Review Article by Claus Klingshirn (University of Karlsruhe) [1]. Zinc oxide is a wide band gap semiconductor which shows intrinsic luminescence in the blue and near‐UV spectral range as well as extrinsic emission from the blue to the infrared. The author discusses in detail why ZnO is a promising material for optoelectronics, in particular for the blue and ultraviolet region of the spectrum. His fields of research include the (non)linear, temporally or spatially resolved spectroscopy of semiconductors and their growth by molecular beam epitaxy. (© 2007 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
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C. Klingshirn 《physica status solidi b》2007,244(9):3027-3073
Several hundred thousands of tons of ZnO are used by per year, e.g. as an additive to concrete or to rubber. In the field of optoelectronics, ZnO holds promises as a material for a blue/UV optoelectronics, alternatively to GaN, as a cheap, transparent, conducting oxide, as a material for electronic circuits, which are transparent in the visible or for semiconductor spintronics. The main problem is presently, however, a high, reproducible and stable p‐doping. We review in this contribution partly critically the material growth, fundamental properties of ZnO and of ZnO‐based nanostructures, doping as well as present and future applications, with emphasis on the electronic and optical properties including stimulated emission. (© 2007 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
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C. Weber U. Becker R. Renner C. Klingshirn 《Applied physics. B, Lasers and optics》1988,45(3):113-120
There are a great variety of optical nonlinearities that can lead to the phenomenon of laser-induced gratings (LIG) in semiconductors. In the present contribution the dynamic behaviour of an induced absorber with intrinsic bistability is investigated under excitation in a LIG self-diffraction arrangement. Using CdS as a model substance, the comparison of our theoretical model with our experimental findings gives an insight into the nonlinear dynamics of the degenerate carrier system and also an estimation of the transport properties of the electron-hole plasma. 相似文献
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ZnO: material, physics and applications. 总被引:1,自引:0,他引:1
C Klingshirn 《Chemphyschem》2007,8(6):782-803
ZnO is presently experiencing a research boom with more than 2000 ZnO-related publications in 2005. This phenomenon is triggered, for example, by hope to use ZnO as a material for blue/UV optoelectronics as an alternative to GaN, as a cheap, transparent, conducting oxide, as a material for electronic circuits that are transparent in the visible or for semiconductor spintronics. Currently, however, the main problem is to achieve high, reproducible and stable p-doping. Herein, we critically review aspects of the material growth, fundamental properties of ZnO and ZnO-based nanostructures and doping as well as present and future applications with emphasis on the electronic and optical properties including stimulated emission. 相似文献
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Collisional deactivation of the first excited electronic 1Δg(υ = 0) state of O2 involves intersystem crossing to higher vibrational levels (υ < 5) of the electronic ground state 3Σ?g. It is followed by rapid vibrational-vibrational energy exchange which populates the first excited 3Σ?g(υ = 1) vibrational level. The suggested relaxation mechanism is supported by experimental results on the time dependence of the populations of the 1Δg(υ = 0) and 3Σ?g(υ = 1) states in liquid natural O2 and 18O2. 相似文献