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  1. No Access

    Chapter

    Material Technology for Vortex Electronics

    High-T_c superconductor (HTSC) thin films are typically grown by mean of pulsed laser deposition (PLD), metalorganic chemical vapor deposition (MOCVD), sputtering or molecular beam epitaxy (MBE). This cha...

    T. Kobayashi, S. Oda, O. Michikami, T. Terashima in Vortex Electronis and SQUIDs (2003)

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    Chapter

    Vortices in High-T_c

    In this chapter we describe the behavior of vortices in high-T_c superconductors. Because of two-dimensional-like and spatially anisotropic electronic structures, the vortices in these materials exhibit chara...

    S. Kuriki, S. Hirano, A. Maeda, T. Kiss in Vortex Electronis and SQUIDs (2003)

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    Chapter

    New Aspect of Vortex in HTSC

    Some topics related to a new aspect of the vortices observed in high-T_c superconductors (HTSCs) are reviewed in this chapter. One of the most important physical properties of vortices created in type-II supe...

    M. Tonouchi, G. Oya, Y. Matsuda, K. Kumagai in Vortex Electronis and SQUIDs (2003)

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    Chapter

    Applications of HTSC SQUIDs

    Recently a high temperature superconductor (HTSC)-SQUID has been made with high magnetic field resolution and its application is expected to be practical for many fields. The HTSC-SQUID can work using...

    H. Itozaki, K. Sakuta, T. Kobayashi, K. Enpuku, N. Kasai in Vortex Electronis and SQUIDs (2003)

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    Chapter

    Introduction

    In the history of modern physics and engineering, the electron quantum mechanical effect and its utilization in electronics have attracted much attention. With increase in demand for ultrahigh sensiti...

    T. Kobayashi in Vortex Electronis and SQUIDs (2003)

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    Chapter

    Observation of Vortices

    Various kinds of special techniques have been developed to visualize quantized magnetic flux in superconductors, i.e. vortex. This chapter reviews the experimental techniques and discusses the vortex distribu...

    S. Ohshima, K. Tanabe, T. Morishita, M. Tonouchi in Vortex Electronis and SQUIDs (2003)

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    Chapter

    High-T_c SQUIDs

    This chapter reviews the development of magnetometers based on high-T_c superconducting quantum interference devices (HTSC-SQUID) operated in liquid nitrogen. A HTSC-SQUID is usually made of a grain-boundary J...

    K. Enpuku, S. Kuriki, S. Tanaka in Vortex Electronis and SQUIDs (2003)

  8. No Access

    Chapter

    Introduction

    In this chapter we will outline the theory of semiconductor laser devices, and summarize the associated fabrication technology and their importance in opto-electronics. A brief history of semiconductor lasers ...

    Professor Dr. Kenichi Iga in Process Technology for Semiconductor Lasers (1996)

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    Chapter

    Basic Design of Semiconductor Lasers

    A double heterostructure is a very basic, necessary design for semiconductor lasers capable of confining both electronic carriers and lightwaves in its cavity. The introduction of double heterostructures into ...

    Professor Dr. Kenichi Iga in Process Technology for Semiconductor Lasers (1996)

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    Chapter

    Liquid Phase Epitaxy and Growth Technology

    Liquid-Phase Epitaxy (LPE) has many advantages and is capable of producing reliable semiconductor devices. This chapter provides a detailed description of the equipment necessary for LPE and the epitaxial tech...

    Professor Dr. Kenichi Iga in Process Technology for Semiconductor Lasers (1996)

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    Chapter

    Characterization of Laser Materials

    The preceeding chapters have described crystal growth for semiconductor lasers, with an emphasis on liquid-phase epitaxial growth techniques. Now we turn our attention to the evaluation of grown wafers and dev...

    Professor Dr. Kenichi Iga in Process Technology for Semiconductor Lasers (1996)

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    Chapter

    Mode-Control Techniques in Semiconductor Lasers

    It is very important for semiconductor lasers to have stable transverse and longitudinal modes in order to obtain reliable performance. This is achieved by using an index waveguide structure. One of the most c...

    Professor Dr. Kenichi Iga in Process Technology for Semiconductor Lasers (1996)

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    Chapter

    Materials for Semiconductor Lasers

    Compound semiconductors, especially III-V compound semiconductors, are well suited for semiconductor lasers. The most basic, necessary condition required of laser materials is, of course, that the input energy...

    Professor Dr. Kenichi Iga in Process Technology for Semiconductor Lasers (1996)

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    Chapter

    Epitaxy of III–V Compound Semiconductors

    This chapter summarizes the fundamental concepts of the epitaxial growth of III–V compound semiconductors. The relevant crystal-growth technologies encompass two categories: bulk crystal preparation for a subs...

    Professor Dr. Kenichi Iga in Process Technology for Semiconductor Lasers (1996)

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    Chapter

    Vapor Phase and Beam Epitaxies

    The Liquid-Phase Epitaxy (LPE) growth technique is based on simple principles and resrs upon simple apparatuses. It is described in Chap. 5. Recently, superlattice devices composed of finer heterostructures ha...

    Professor Dr. Kenichi Iga in Process Technology for Semiconductor Lasers (1996)

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    Chapter

    Semiconductor-Laser Devices — Fabrication and Characteristics

    In this chapter, we examine the fabrication of actual laser devices and the relevant characterization techniques. The design criteria stated in Chap. 3 should be checked as the first step of device evaluation....

    Professor Dr. Kenichi Iga in Process Technology for Semiconductor Lasers (1996)

  17. No Access

    Chapter

    Surface-Emitting Lasers

    The surface-emitting laser began to be considered one of the crucial devices for the next generation of optoelectronics when advantage was taken of its high degree of parallelism. In this chapter, we review th...

    Professor Dr. Kenichi Iga in Process Technology for Semiconductor Lasers (1996)

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    Chapter and Conference Paper

    Is the 13C Nuclear Spin-Lattice Relaxation in A3C60 (A = Rb, K) Unconventional?

    I want to point out that the simple Korringa relation does not hold for A3C60 ,i.e. density of states information cannot be obtained from T 1 data. A modified Korringa relation must be applied ins...

    M. Mehring in Electronic Properties of Fullerenes (1993)

  19. No Access

    Chapter and Conference Paper

    NMR Studies of Fullerene C60-Based Compounds

    We present NMR studies performed on AnC60 compounds, where A can be K, Rb, I2, O2 and n can be 1, 2, 3 and 6 depending on the system. Using high resolution NMR we have obtained information on the molecular dynami...

    P. Bernier, F. Rachdi, M. Ribet, J. Reichenbach in Electronic Properties of Fullerenes (1993)

  20. No Access

    Chapter and Conference Paper

    Anharmonic Effects in the Apex O Phonon in Relation to the Background Continuum in High-Tc Cuprates

    The observed temperature dependence of the apex O phonon self-energy has been found to be described well by a static aharmonicity in the apex O vibrational potential in YBa2Cu3O6.9, TIBa2CaCu2O7 and T12Ba2CaCu2O8

    D. Mihailovic in Electronic Properties of High-Tc Superconductors (1993)

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