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Applied Physics Reviews — 1998

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Probing ultrafast carrier and phonon dynamics in semiconductors

Andreas Othonos

J. Appl. Phys. 83, 1789 (1998); http://dx.doi.org/10.1063/1.367411 (42 pages)

Online Publication Date: 12 December 2006

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Over the past 2 decades there has been tremendous advancements in the field of ultrafast carrier dynamics in semiconductors. The driving force behind this movement other than the basic fundamental interest is the direct application of semiconductor devices and the endless need for faster response and faster processing of information. To improve and develop microelectronics devices and address these needs, there must be a basic understanding of the various dynamical processes in the semiconductors which have to be studied in detail. Therefore, the excitation of semiconductors out of their equilibrium and the subsequent relaxation processes with various rates has become a key area of semiconductor research. With the development of lasers that can generate pulses as short as a few femtoseconds the excitation and subsequent probing of semiconductors on an ultrashort timescale have become routine. Processes such as carrier momentum randomization, carrier thermalization, and energy relaxation have been studied in detail using excite-and-probe novel techniques. This article reviews the status of ultrafast carrier and phonon dynamics in semiconductors. Experimental techniques such as excite-and-probe transmission, time-resolved up-conversion luminescence, and pump-probe Raman scattering along with some of the significant experimental findings from probing semiconductors are discussed. Finally, a selfconsistent theoretical model, which correlates the carrier and phonon dynamics in germanium on an ultrashort time scale, is described in detail. ©1998 American Institute of Physics.
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01.30.Rr Surveys and tutorial papers; resource letters
72.20.Jv Charge carriers: generation, recombination, lifetime, and trapping
73.50.Gr Charge carriers: generation, recombination, lifetime, trapping, mean free paths
63.20.-e Phonons in crystal lattices
71.38.-k Polarons and electron-phonon interactions

Nitrogen in germanium

I. Chambouleyron and A. R. Zanatta

J. Appl. Phys. 84, 1 (1998); http://dx.doi.org/10.1063/1.368612 (30 pages)

Online Publication Date: 12 December 2006

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The known properties of nitrogen as an impurity in, and as an alloy element of, the germanium network are reviewed in this article. Amorphous and crystalline germanium–nitrogen alloys are interesting materials with potential applications for protective coatings and window layers for solar conversion devices. They may also act as effective diffusion masks for III-V electronic devices. The existing data are compared with similar properties of other group IV nitrides, in particular with silicon nitride. To a certain extent, the general picture mirrors the one found in Si–N systems, as expected from the similar valence structure of both elemental semiconductors. However, important differences appear in the deposition methods and alloy composition, the optical properties of as grown films, and the electrical behavior of nitrogen-doped amorphous layers. Structural studies are reviewed, including band structure calculations and the energies of nitrogen-related defects, which are compared with experimental data. Many important aspects of the electronic structure of Ge–N alloys are not yet completely understood and deserve a more careful investigation, in particular the structure of defects associated with N inclusion. The N doping of the a-Ge:H network appears to be very effective, the activation energy of the most effectively doped samples becoming around 120 meV. This is not the case with N-doped a-Si:H, the reasons for the difference remaining an open question. The lack of data on stoichiometric β-Ge3N4 prevents any reasonable assessment on the possible uses of the alloy in electronic and ceramic applications. © 1998 American Institute of Physics.
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72.80.Cw Elemental semiconductors
61.72.uf Ge and Si
01.30.Rr Surveys and tutorial papers; resource letters
81.05.Cy Elemental semiconductors
71.55.Cn Elemental semiconductors
71.23.Cq Amorphous semiconductors, metallic glasses, glasses
72.80.Ng Disordered solids
78.66.Jg Amorphous semiconductors; glasses
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Erratum: “Probing ultrafast carrier and phonon dynamics in semiconductors” [J. Appl. Phys. 83, 1789 (1998)]

Andreas Othonos

J. Appl. Phys. 84, 1708 (1998); http://dx.doi.org/10.1063/1.368243 (1 page)

Online Publication Date: 12 December 2006

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Abstract Unavailable
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01.30.Rr Surveys and tutorial papers; resource letters
72.20.Jv Charge carriers: generation, recombination, lifetime, and trapping
73.50.Gr Charge carriers: generation, recombination, lifetime, trapping, mean free paths
63.20.-e Phonons in crystal lattices
71.38.-k Polarons and electron-phonon interactions
99.10.Cd Errata
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Local probe techniques for luminescence studies of low-dimensional semiconductor structures

Anders Gustafsson, Mats-Erik Pistol, Lars Montelius, and Lars Samuelson

J. Appl. Phys. 84, 1715 (1998); http://dx.doi.org/10.1063/1.368613 (61 pages)

Online Publication Date: 12 December 2006

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With the rapid development of technologies for the fabrication of, as well as applications of low-dimensional structures, the demands on characterization techniques increase. Spatial resolution is especially crucial, where techniques for probing the properties of very small volumes, in the extreme case quantum structures, are essential. In this article we review the state-of-the-art in local probe techniques for studying the properties of nanostructures, concentrating on methods involving monitoring the properties related to photon emission. These techniques are sensitive enough to reveal the electronic structure of low-dimensional semiconductor structures and are, therefore, able to give detailed information about the geometrical structure, including fabrication-related inhomogeneities within an ensemble of structures. The local luminescence probe techniques discussed in this review article can be divided into four categories according to the excitation source: (i) spatially localized microphotoluminescence spectroscopy using either strong focusing or masking; (ii) near-field optical microscopy to reach below the diffraction limitation of far-field optics, by either exciting, detecting, or both exciting and detecting in the near field; (iii) cathodoluminescence using focused energetic electrons in an electron microscope; and (iv) scanning tunneling luminescence, using low-energy electrons injected or extracted from the tip of a scanning tunneling microscope. © 1998 American Institute of Physics.
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73.40.Kp III-V semiconductor-to-semiconductor contacts, p-n junctions, and heterojunctions
73.40.Lq Other semiconductor-to-semiconductor contacts, p-n junctions, and heterojunctions
78.60.Hk Cathodoluminescence, ionoluminescence
01.30.Rr Surveys and tutorial papers; resource letters
78.55.-m Photoluminescence, properties and materials

Crystal grain nucleation in amorphous silicon

Corrado Spinella, Salvatore Lombardo, and Francesco Priolo

J. Appl. Phys. 84, 5383 (1998); http://dx.doi.org/10.1063/1.368873 (32 pages)

Online Publication Date: 12 December 2006

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The solid phase crystallization of chemical vapor deposited amorphous silicon films onto oxidized silicon wafers, induced either by thermal annealing or by ion beam irradiation at high substrate temperatures, has been extensively developed and it is reviewed here. We report and discuss a large variety of processing conditions. The structural and thermodynamical properties of the starting phase are emphasized. The morphological evolution of the amorphous towards the polycrystalline phase is investigated by transmission electron microscopy and it is interpreted in terms of a physical model containing few free parameters related to the thermodynamical properties of amorphous silicon and to the kinetical mechanisms of crystal grain growth. A direct extension of this model explains also the data concerning the ion-assisted crystal grain nucleation. © 1998 American Institute of Physics.
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68.55.-a Thin film structure and morphology
81.05.Cy Elemental semiconductors
81.05.Gc Amorphous semiconductors
61.43.Dq Amorphous semiconductors, metals, and alloys
61.80.Jh Ion radiation effects
65.20.-w Thermal properties of liquids
65.40.gd Entropy
81.15.Gh Chemical vapor deposition (including plasma-enhanced CVD, MOCVD, ALD, etc.)
01.30.Rr Surveys and tutorial papers; resource letters
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