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Applied Physics Reviews — 1996


Entropy generation minimization: The new thermodynamics of finite‐size devices and finite‐time processes

Adrian Bejan

J. Appl. Phys. 79, 1191 (1996); http://dx.doi.org/10.1063/1.362674 (28 pages)

Online Publication Date: 12 December 2006

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Entropy generation minimization (finite time thermodynamics, or thermodynamic optimization) is the method that combines into simple models the most basic concepts of heat transfer, fluid mechanics, and thermodynamics. These simple models are used in the optimization of real (irreversible) devices and processes, subject to finite‐size and finite‐time constraints. The review traces the development and adoption of the method in several sectors of mainstream thermal engineering and science: cryogenics, heat transfer, education, storage systems, solar power plants, nuclear and fossil power plants, and refrigerators. Emphasis is placed on the fundamental and technological importance of the optimization method and its results, the pedagogical merits of the method, and the chronological development of the field. © 1996 American Institute of Physics.
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05.70.-a Thermodynamics
07.20.Mc Cryogenics; refrigerators, low-temperature detectors, and other low-temperature equipment
44.10.+i Heat conduction

Substrate selection for high‐temperature superconducting thin films

Julia M. Phillips

J. Appl. Phys. 79, 1829 (1996); http://dx.doi.org/10.1063/1.362675 (20 pages)

Online Publication Date: 12 December 2006

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Substrate selection presents particular challenges for the production of high‐quality high‐temperature superconducting (HTS) thin films suitable for applications. Because the substrate is generally a passive component, it is often ignored and assumed to have a negligible effect on the structure residing on top of it. There is also a technological motivation to use substrates that conventional wisdom would argue are unlikely to support high‐quality HTS films. These facts have led to rediscovery of many of the fundamental issues governing the role of the substrate in determining the properties of the thin film(s) it supports. For this reason, the study of issues in substrate selection for HTS materials presents a microcosm for substrate selection more generally. We consider the major issues governing the role of the substrate in HTS thin‐film technology and discuss many of the material classes and specific materials that have been studied for their suitability as substrates for HTS films. © 1996 American Institute of Physics.
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74.78.-w Superconducting films and low-dimensional structures

Electron spectroscopic analysis of the SiO2/Si system and correlation with metal–oxide–semiconductor device characteristics

Seiichi Iwata and Akitoshi Ishizaka

J. Appl. Phys. 79, 6653 (1996); http://dx.doi.org/10.1063/1.362676 (61 pages)

Online Publication Date: 12 December 2006

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ESCA (electron spectroscopy for chemical analysis) measurement results on thin SiO2/Si samples are examined comprehensively, critically, and in detail to show that it is possible to correlate these results with MOS (metal–oxide–semiconductor) device characteristics such as flatband (threshold) voltage, oxide breakdown field, mobile‐ion density, hole and electron trap density, and hot‐carrier lifetime. Up to now, much effort has been made to detect SiOx phases at SiO2/Si interfaces since they are thought to have a significant effect on MOS device characteristics. However, correlating the SiOx phases with device characteristics is difficult and involves overcoming two problems. First, the chemical state is difficult to determine exactly due to x‐ray irradiation effects. Second, the amount of defects and impurities which influence device characteristics is usually below the ESCA detection limit (1012–1013 cm−2) in device‐quality SiO2/Si samples. Investigation of the first problem led to the conclusion that it is possible to correct for these effects from the x‐ray intensity or oxide thickness dependence of the chemical shift. However, accurate (better than ±0.2 eV) chemical state determination is not easy. It is therefore necessary to approach this detection problem from a different viewpoint. Our first attempt involves measuring the ESCA thickness, which decreases when oxide defects like unoxidized Si or uneven thickness (or pinholes) are present, resulting in breakdown field degradation. Our second attempt started while we were studying how to interpret the measured chemical shift. The photoelectron peaks of the SiO2 and the Si can be observed to shift due to small amounts of charged defects and impurities, although they cannot be detected as peaks. This method is considered to be especially useful for characterizing ultrathin (a few nm thick) SiO2/Si samples which are difficult to characterize using conventional CV (capacitance–voltage) measurements because of tunneling currents. Accordingly, we discuss the data obtained in steady‐state and transient peak position measurements of SiO2/Si samples containing 1010–1012 cm−2 of Na (sodium) ions, 1012–1013 cm−2 of hole and electron traps, and 1014–1021 cm−3 of impurities such as P (phosphorus) (in the Si). It is shown that a correlation with MOS characteristics is possible. A close scrutiny of various results concerning x‐ray irradiation time, intensity, and oxide thickness dependence of the above peak positions indicates that electric charging during ESCA measurements is correlated to the trap‐capturing process. As MOS characteristics are also related to this process, more studies in this direction are needed and will certainly yield more information on the defects influencing the MOS characteristics and the trap‐capturing mechanism. © 1996 American Institute of Physics.
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82.80.Pv Electron spectroscopy (X-ray photoelectron (XPS), Auger electron spectroscopy (AES), etc.)
79.60.Jv Interfaces; heterostructures; nanostructures
85.30.De Semiconductor-device characterization, design, and modeling

Semiconductor ultraviolet detectors

M. Razeghi and A. Rogalski

J. Appl. Phys. 79, 7433 (1996); http://dx.doi.org/10.1063/1.362677 (41 pages)

Online Publication Date: 12 December 2006

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In this review article a comprehensive analysis of the developments in ultraviolet (UV) detector technology is described. At the beginning, the classification of UV detectors and general requirements imposed on these detectors are presented. Further considerations are restricted to modern semiconductor UV detectors, so the basic theory of photoconductive and photovoltaic detectors is presented in a uniform way convenient for various detector materials. Next, the current state of the art of different types of semiconductor UV detectors is presented. Hitherto, the semiconductor UV detectors have been mainly fabricated using Si. Industries such as the aerospace, automotive, petroleum, and others have continuously provided the impetus pushing the development of fringe technologies which are tolerant of increasingly high temperatures and hostile environments. As a result, the main efforts are currently directed to a new generation of UV detectors fabricated from wide band‐gap semiconductors the most promising of which are diamond and AlGaN. The latest progress in development of AlGaN UV detectors is finally described in detail. © 1996 American Institute of Physics.
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85.60.Gz Photodetectors (including infrared and CCD detectors)
72.40.+w Photoconduction and photovoltaic effects

Stresses and strains in lattice‐mismatched stripes, quantum wires, quantum dots, and substrates in Si technology

S. C. Jain, H. E. Maes, K. Pinardi, and I. De Wolf

J. Appl. Phys. 79, 8145 (1996); http://dx.doi.org/10.1063/1.362678 (21 pages)

Online Publication Date: 12 December 2006

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We discuss recent advances made in the theory and measurements of stresses and strains in Si‐based heterostructures containing submicron‐ and micron‐size features. Several reports on theoretical as well as experimental studies of stresses in the substrates with local oxidation of silicon structures on the surface have been published recently. With the advent of GeXSi1−X strained layers and stripes extensive studies of both the stripe and the substrate stresses have also been made. Unlike the previous calculations and analytical models, recent finite element (FE) calculations take into account the coupling between the film–substrate stresses without making the approximation that the interface is rigid or that there is no variation of stresses in the stripes in a direction perpendicular to the interface. The results of these calculations have been compared with the analytical models and limitations of the analytical models have been pointed out. Micro‐Raman measurements of the stresses in the stripes, quantum wires, quantum dots, and substrates have been made. The measured values of stresses in GeSi stripes and quantum structures agree well with the calculated values by the FE method. The micro‐Raman measurements showed that as the ratio R=2l/h (2l is the width and h is the thickness of the stripe) decreases, the shape of the measured normal stresses in the substrate under the stripe (plotted in a direction parallel to the interface) changes dramatically, from concave upward to convex upward. Generation of dislocations in laterally small layers is also discussed briefly. FE calculations of trench‐induced stresses which include the effect of the anisotropy of Si have also been made recently. In these calculations realistic experimental conditions were simulated to determine the oxide shape, oxide–interface stresses, and intrinsic and thermal stresses of the polysilicon fill. These values were then used as inputs for the FE calculations. Calculations of stresses induced by oxide‐filled trenches were also made assuming that Si is isotropic and that the oxide fill has the same elastic constants as Si. These calculations and results of an earlier analytical model implemented under the same assumptions gave identical results; however, the calculated stress values were in error of 20%–30%. The maximum resolved shear stress for the 60° dislocation induced by a trench is 30% more if it is aligned in 〈110〉 direction rather than in the 〈100〉 direction. This explains the common observation that the 〈100〉‐oriented trenches cause fewer dislocations than the 〈110〉 trenches. The characteristics of trench isolated as well as junction isolated bipolar transistors have been studied. The trench isolated transistors had 20% higher gain; however, the collector–base capacitance was higher by up to 50% in the trenched transistors. The increase in capacitance was caused by the anomalous diffusion of the antimony dopant from the buried collector layer induced by the stress field of the trenches. The effect could be eliminated by increasing the depth of the trench. The trenched devices also had higher emitter–collector leakage current caused by the dislocations generated by the trench induced stress field. © 1996 American Institute of Physics.
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68.65.-k Low-dimensional, mesoscopic, nanoscale and other related systems: structure and nonelectronic properties
68.60.Bs Mechanical and acoustical properties

Poled polymers for sensors and photonic applications

Siegfried Bauer

J. Appl. Phys. 80, 5531 (1996); http://dx.doi.org/10.1063/1.363604 (28 pages)

Online Publication Date: 12 December 2006

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A brief survey of the electrical and optical properties of poled polymer electrets for sensors and photonic applications is given. Semicrystalline ferroelectric polymers are highly suitable for piezo‐ and pyroelectric applications, while amorphous polymers containing molecular dipoles with acceptor and donor groups linked by delocalized π electrons (A‐π‐D) are interesting for photonic applications. The large variety of poling techniques, such as electrode, corona, electron‐beam, and photothermal poling, is discussed in detail together with specifically developed poling techniques for ferroelectric or amorphous polymers. Methods for the experimental investigation of the polar order are based on the piezo‐, and pyroelectric effect, birefringence, the electro‐optical effect and second‐harmonic generation. Newly developed thermal analysis techniques and dipole relaxation spectroscopies complement traditional techniques, such as thermally stimulated depolarization and broadband linear and nonlinear dielectric relaxation spectroscopy. The compatibility of polymers with semiconductor technology is illustrated with selected applications in hybrid integrated thermal and acoustical imaging devices, electro‐optical modulators and second‐harmonic generators. © 1996 American Institute of Physics.
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77.84.Jd Polymers; organic compounds
77.22.Ej Polarization and depolarization
77.65.-j Piezoelectricity and electromechanical effects
77.70.+a Pyroelectric and electrocaloric effects
77.22.Gm Dielectric loss and relaxation
77.22.Jp Dielectric breakdown and space-charge effects
42.65.Ky Frequency conversion; harmonic generation, including higher-order harmonic generation
78.20.Fm Birefringence
78.20.Jq Electro-optical effects
42.79.Hp Optical processors, correlators, and modulators
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