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  • The Electrochemical Society  (35)
  • 1
    Online Resource
    Online Resource
    The Electrochemical Society ; 2007
    In:  ECS Transactions Vol. 11, No. 6 ( 2007-09-28), p. 131-139
    In: ECS Transactions, The Electrochemical Society, Vol. 11, No. 6 ( 2007-09-28), p. 131-139
    Abstract: Hole resonant tunneling diodes with Si/strained Si 1-x Ge x heterostructures epitaxially grown on Si(100) were fabricated and improvement of the negative differential conductance characteristics was explored by reducing thickness of Si barriers and Si 1-x Ge x quantum well into a few nanometer order. It was clearly shown that, by reducing the Si barrier thickness down to 2 nm, high peak current density above a few kA/cm 2 can be obtained under a peak-to-valley ratio of about 2 at 11 K. From the temperature dependence of the peak and valley currents, it is suggested that local introduction of higher Ge fraction effectively suppresses increase of valley current at higher temperatures.
    Type of Medium: Online Resource
    ISSN: 1938-5862 , 1938-6737
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2007
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  • 2
    Online Resource
    Online Resource
    The Electrochemical Society ; 2014
    In:  ECS Transactions Vol. 61, No. 2 ( 2014-03-24), p. 97-104
    In: ECS Transactions, The Electrochemical Society, Vol. 61, No. 2 ( 2014-03-24), p. 97-104
    Abstract: One of the main requirements for Si-based ultrasmall device is atomic-order control of process technology. Here, we show the concept of atomically controlled processing for group IV semiconductors based on atomic-order surface reaction control in Si-based CVD epitaxial growth. On the atomic-order surface nitridation of Si 1-x Ge x by NH 3 , it is suggested that nitridation of Si atoms proceeds by transfer of N atoms from Ge atoms by heat-treatment. In the case of epitaxial Ge film, the crystallinity change is not observed by NH 3 treatment and N atoms diffuse through nm-order thick Ge layer into Si (100) substrate and form Si nitride even at 500 o C. It is also suggested that N diffusion in Ge layer is suppressed by the formation of Si nitride. These results demonstrate the capability of CVD technology for atomically controlled nitridation of Si, Si 1-x Ge x and Ge for ultralarge scale integration.
    Type of Medium: Online Resource
    ISSN: 1938-5862 , 1938-6737
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2014
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  • 3
    Online Resource
    Online Resource
    The Electrochemical Society ; 2006
    In:  ECS Transactions Vol. 3, No. 7 ( 2006-10-20), p. 1205-1210
    In: ECS Transactions, The Electrochemical Society, Vol. 3, No. 7 ( 2006-10-20), p. 1205-1210
    Abstract: Atomic order thermal nitridation of Si 1-x Ge x (100) (x=0, 0.4, 1) by NH 3 gas environment at low temperature of 400ºC has been investigated using an ultraclean low-pressure chemical vapor deposition system. After NH 3 exposure (NH 3 partial pressure of 550 Pa for 30 min), it is found that Si(100), Si 0.6 Ge 0.4 (100) and Ge(100) are nitrided in atomic-order. In the case of Ar purging at cooling period after the nitridation, N atom amounts on Si(100) and Ge(100) are 8.0x10 14 and 5.5x10 14 cm -2 , and the amount on Si 0.6 Ge 0.4 (100) is 12.5x10 14 cm -2 . In the case of H 2 purging at the cooling period, it is found that slight reduction of the N atom amount on Si(100) down to 5.6x10 14 cm -2 (70 %) is observed, although the N atom amount on Ge(100) is significantly reduced to 1.2x10 14 cm -2 (22 %).
    Type of Medium: Online Resource
    ISSN: 1938-5862 , 1938-6737
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2006
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  • 4
    Online Resource
    Online Resource
    The Electrochemical Society ; 2011
    In:  ECS Transactions Vol. 41, No. 7 ( 2011-10-04), p. 337-343
    In: ECS Transactions, The Electrochemical Society, Vol. 41, No. 7 ( 2011-10-04), p. 337-343
    Abstract: For the purpose of quantum heterointegration of group IV semiconductors, atomically controlled plasma processing by utilizing an electron-cyclotron-resonance (ECR) plasma enhanced chemical vapor deposition (CVD) at low temperature has been developed to achieve atomic-layer doping and heterostructure formation with nanometer-order thickness control as well as smooth and abrupt interfaces. In this paper, recent typical achievements in the plasma processing are reviewed: (1) By N and B atomic-layer formation and Si epitaxial growth on Si(100), heavy atomic-layer doping was demonstrated. Most of the incorporated N or B atoms can be confined in an about 2 nm-thick region. (2) highly-strained and relaxed Ge films on Si(100) with atomic-order flatness can be epitaxially grown. (3) Using a 84% relaxed Ge buffer layer formed on Si(100), formation of a highly strained Si film with nanometer-order thickness was achieved.
    Type of Medium: Online Resource
    ISSN: 1938-5862 , 1938-6737
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2011
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  • 5
    Online Resource
    Online Resource
    The Electrochemical Society ; 2010
    In:  ECS Transactions Vol. 33, No. 6 ( 2010-10-01), p. 379-387
    In: ECS Transactions, The Electrochemical Society, Vol. 33, No. 6 ( 2010-10-01), p. 379-387
    Abstract: For the purpose of heterointegration of Si-based group IV semiconductor quantum effect devices into Si large-scale integrated circuit, formation of atomically flat heterointerfaces in quantum heterostructure by lowering Si barrier growth temperature was investigated in order to improve negative differential conductance (NDC) characteristics of high-Ge-fraction strained Si 1-x Ge x /Si hole resonant tunneling diode. It was found that roughness generation at heterointerfaces is drastically suppressed by utilizing, Si barriers with nanometer order thickness deposited using Si 2 H 6 reaction at a lower temperature of 400 o C instead of SiH 4 reaction at 500 o C after the Si 0.42 Ge 0.58 growth. NDC characteristics show that difference between peak and valley currents is effectively enhanced at 11-295K by using Si 2 H 6 at 400 o C, compared with that using SiH 4 at 500 o C. Thermionic-emission dominant characteristics at higher temperatures above 100 K indicates a possibility that introduction of larger barrier height (i.e., larger band discontinuity) enhances the NDC at room temperature by suppression of thermionic-emission current.
    Type of Medium: Online Resource
    ISSN: 1938-5862 , 1938-6737
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2010
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  • 6
    Online Resource
    Online Resource
    The Electrochemical Society ; 1998
    In:  Journal of The Electrochemical Society Vol. 145, No. 12 ( 1998-12-01), p. 4252-4256
    In: Journal of The Electrochemical Society, The Electrochemical Society, Vol. 145, No. 12 ( 1998-12-01), p. 4252-4256
    Type of Medium: Online Resource
    ISSN: 0013-4651 , 1945-7111
    RVK:
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 1998
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  • 7
    Online Resource
    Online Resource
    The Electrochemical Society ; 2013
    In:  ECS Meeting Abstracts Vol. MA2013-02, No. 33 ( 2013-10-27), p. 2230-2230
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2013-02, No. 33 ( 2013-10-27), p. 2230-2230
    Abstract: Abstract not Available.
    Type of Medium: Online Resource
    ISSN: 2151-2043
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2013
    detail.hit.zdb_id: 2438749-6
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  • 8
    Online Resource
    Online Resource
    The Electrochemical Society ; 2010
    In:  ECS Meeting Abstracts Vol. MA2010-02, No. 30 ( 2010-07-08), p. 1895-1895
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2010-02, No. 30 ( 2010-07-08), p. 1895-1895
    Abstract: Abstract not Available.
    Type of Medium: Online Resource
    ISSN: 2151-2043
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2010
    detail.hit.zdb_id: 2438749-6
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  • 9
    Online Resource
    Online Resource
    The Electrochemical Society ; 2013
    In:  ECS Meeting Abstracts Vol. MA2013-02, No. 33 ( 2013-10-27), p. 2228-2228
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2013-02, No. 33 ( 2013-10-27), p. 2228-2228
    Abstract: Abstract not Available.
    Type of Medium: Online Resource
    ISSN: 2151-2043
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2013
    detail.hit.zdb_id: 2438749-6
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  • 10
    Online Resource
    Online Resource
    The Electrochemical Society ; 2014
    In:  ECS Meeting Abstracts Vol. MA2014-01, No. 36 ( 2014-04-01), p. 1359-1359
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2014-01, No. 36 ( 2014-04-01), p. 1359-1359
    Abstract: Atomically controlled processing has become indis-pensable for the fabrication of Si-based ultrasmall devices and heterodevices for ultralarge scale integration. Our concept of atomically controlled processing is based on atomic-order surface reaction control [1-3]. The final goal is the generalization of atomic-order surface reaction processes and the creation of new properties in Si-based ultimate small structures which will lead to nanometer scale Si devices as well as Si-based quantum devices. Introduction of N atomic layer at the interface between the high-k dielectric and the channel has been employed to suppress the interface trap formation [4] . Additionally, the insertion of N atomic layer within the channel may be beneficial for high mobility channel formation [5,3]. In this work, we describe atomic-order thermal nitridation of Si 1-x Ge x (100) (x=0 - 1) Si(100) in an NH 3 environment in a low temperature range of 300-650°C using an ultraclean low-pressure CVD system and furthermore the thermal stability of nitride surface are discussed. It has been found that silicon nitride films are formed even at 300-650°C on Si(100) [6]. At 500°C or higher, N initially increases and tends to saturate to a certain value (N atomic amount (n N ) of about 2.7 x 10 15 cm -2 ; 4 atomic layers). At 400°C or lower, on the H-terminated Si surface after wet cleaning, the n N increases and the Si-hydride coverage decreases with increasing NH 3 exposure time. The Si-hydride becomes hardly observable when n N reaches the surface Si atomic amount (6.8 x 10 14 cm -2 ). On the H-free Si surface after preheating in Ar at 650°C, n N increases up to 2 x 10 14 cm -2 ( Fig.1 ) with the appearance of the Si-hydride instantly after NH 3 exposure at 300 and 400°C, indicating that NH 3 molecules dissociatively are adsorbed on the Si dangling bonds. Further ultrathin nitridation is accompanied by a decrease of the Si-hydride coverage. It is found that n N is well described by Langmuir-type physical adsorption and reaction of NH 3 on the Si surface [3] based on a fitting assuming that the NH 3 adsorption equilibrium constant with flash heating is the same as that without flash heating [7] ( Fig.2 ). For 30 min exposure of NH 3 at partial pressure of 550 Pa and 400°C, Si 1-x Ge x (100) and Ge (100) are also nitrided at atomic level [8-9]. After Ar or H 2 heat treatment at 400-700 °C under 60 Pa, N atomic amount on the atomic-order nitrided Si (100) and Si 0.6 Ge 0.4 (100) is scarcely changed. On the atomic-order nitrided Ge (100), N atomic amount tends to decrease with increasing the heat-treatment temperature and even by H 2 purging at the cooling period after the nitridation. On the nitrided Si 0.5 Ge 0.5 (100), amount of the nitrided Si atoms increases for the higher heat-treatment temperature, although the amount of the nitrided Ge atoms decreases ( Fig.3 ). It is suggested that N atoms bound to Ge atoms tend to be transferred to Si atoms at temperatures above 400 °C. It is confirmed by angle-resolved XPS that preferential nitridation of Si atoms at surface over Ge atoms induces Ge segregation beneath the surface nitrided layer. Additionally, N atoms for the nitrided Si 0.3 Ge 0.7 (100) dominantly form a Si 3 N 4 structure which stably remains even during heat treatment in H 2 at 400 °C [10]. References [1] J. Murota et al., Jpn. J. Appl. Phys. , 33 , 2290 (1994). [2] B. Tillack et al., Thin Solid Films , 369 ,.189 (2000). [3] J. Murota et al, Jpn. J. Appl. Phys. , 45 , 6767 (2006). [4] J. Huang et al., Appl. Phys. Lett., 88 , 143506 (2006). [5] Y. Jeong et al., Mat. Sci. Semicond. Process., 8 , 121 (2005). [6] T. Watanabe et al., J. Electrochem. Soc. , 145 , 4252 (1998). [7] T. Watanabe et al., Jpn. J. Appl. Phys. , 38 , 515(1999). [8] N. Akiyama et al., Appl. Surf. Sci., 254 , 6021 (2008). [9] N. Akiyama et al., Thin Solid Films 517 , 219 (2008). [10] T. Kawashima et al. Thin Solid Films 520 , 3392 (2012).
    Type of Medium: Online Resource
    ISSN: 2151-2043
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2014
    detail.hit.zdb_id: 2438749-6
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