• Title/Summary/Keyword: Tunnel junction

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FABRICATION OF Nb/Al SUPERCONDUCTING TUNNEL JUNCTION (Nb/Al SUPERCONDUCTING TUNNEL JUNCTION의 제작)

  • Cho, Sung-Ik;Park, Young-Sik;Park, Jang-Hyun;Lee, Yong-Ho;Lee, Sang-Kil;Kim, Sug-Whan;Han, Won-Yong
    • Journal of Astronomy and Space Sciences
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    • v.21 no.4
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    • pp.481-492
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    • 2004
  • We report the successful fabrication and I-V curve superconductivity test results of the Nb/Al-based superconducting tunnel junctions. STJs with side-lengths of 20, 40, 60 and $80{\mu}m$ were fabricated by deposition of polycrystalline Nb/Al/AlOx/Al/Nb 5-layer thin films incorporated on a 3-inch Si wafer. STJ was designed by $Tanner^{TM}$ L-Edit 8.3 program, and fabricated in SQUID fabrication facility, KRISS. S-layer STJ thin-films were fabricated using UV photolithography, DC magnetron sputtering, Reactive ion etching, and CVD(Chemical Vapor Deposition) techniques. Superconducting state test for STJ was succeeded in 4K with liquid helium cooling system. Their performance indicators such ie energy gap, normal resistance, normal resistivity, dynamic resistance, dynamic resistivity, and quality factor were measured from I-V curve. Fabricated Nb/Al STJ shows $11\%$ higher FWHM energy resolution than genuine Nb STJ.

Employing Al Etch Stop Layer for Nb-based SNS Josephson Junction Fabrication Process (Al 식각정지층을 이용한 Nb-based SNS 조셉슨 접합의 제조공정)

  • Choi, J.S.;Park, J.H.;Song, W.;Chong, Y.
    • Progress in Superconductivity
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    • v.12 no.2
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    • pp.114-117
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    • 2011
  • We report our efforts on the development of Nb-based non-hysteretic Josephson junction fabrication process for quantu device applications. By adopting and modifying the existing Nb-aluminum oxide tunnel junction process, we develop a process for non-hysteretic Josephson junction circuits using metal-silicide as metallic barrier material. We use sputter deposition of Nb and $MoSi_2$, PECVD deposition of silicon oxide as insulator material, and ICP-RIE for metal and oxide etch. The advantage of the metal-silicide barrier in the Nb junction process is that it can be etched in $SF_6$ RIE together with Nb electrode. In order to define a junction area precisely and uniformly, end-point detection for the RIE process is critical. In this paper, we employed thin Al layer for the etch stop, and optimized the etch condition. We have successfully demonstrated that the etch stop properties of the inserted Al layer give a uniform etch profile and a precise thickness control of the base electrode in Nb trilayer junctions.

Characteristic Analysis of 4-Types of Junctionless Nanowire Field-Effect Transistor (4가지 무접합 나노선 터널 트랜지스터의 기판 변화에 따른 특성 분석)

  • Oh, Jong Hyuck;Lee, Ju Chan;Yu, Yun Seop
    • Proceedings of the Korean Institute of Information and Commucation Sciences Conference
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    • 2018.10a
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    • pp.381-382
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    • 2018
  • Subthreshold swings (SSs) and on-currents of four types of junctionless nanowire tunnel field-effect transistor(JLNW-TFET) are observed. Ge-Si structure for the source-channel junction has the highest drive current among Si-Si, Si-Ge, and Ge-Ge junction, and the drive current increases up to 1000 times compared to others. Minimum SS of Si-Si junction is reduced by up to 5 times more than others.

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Comparison of Tunneling Characteristics in the MTJs of CoFeB/MgO/CoFeB with Lower and Higher Tunneling Magnetoresistance

  • Choi, G.M.;Shin, K.H.;Seo, S.A.;Lim, W.C.;Lee, T.D.
    • Journal of Magnetics
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    • v.14 no.1
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    • pp.11-14
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    • 2009
  • We investigated the I-V curves and differential tunneling conductance of two, CoFeB/MgO/CoFeB-based, magnetic tunnel junctions (MTJs): one with a low tunneling magnetoresistance (TMR; 22%) and the other with a high TMR (352%). This huge TMR difference was achieved by different MgO sputter conditions rather than by different annealing or deposition temperature. In addition to the TMR difference, the junction resistances were much higher in the low-TMR MTJ than in the high-TMR MTJ. The low-TMR MTJ showed a clear parabolic behavior in the dI/dV-V curve. This high resistance and parabolic behavior were well explained by the Simmons' simple barrier model. However, the tunneling properties of the high-TMR MTJ could not be explained by this model. The characteristic tunneling properties of the high-TMR MTJ were a relatively low junction resistance, a linear relation in the I-V curve, and conduction dips in the differential tunneling conductance. We explained these features by applying the coherent tunneling model.

MTJ based MRAM Core Cell

  • Park, Wanjun
    • Journal of Magnetics
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    • v.7 no.3
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    • pp.101-105
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    • 2002
  • MRAM (Magnetoresistive Random Access Memory) is a promising candidate for a universal memory that meets all application needs with non-volatile, fast operational speed, and low power consumption. The simplest architecture of MRAM cell is a series of MTJ (Magnetic Tunnel Junction) as a data storage part and MOS transistor as a data selection part. This paper is for testing the actual electrical parameters to adopt MRAM technology in the semiconductor based memory device. The discussed topics are an actual integration of MRAM core cell and its properties such as electrical tuning of MOS/MTJ for data sensing and control of magnetic switching for data writing. It will be also tested that limits of the MRAM technology for a high density memory.

Voltage Fluctuation of a Nb/Al-Al$O_{x}$/Nb Tunnel Junction Observed at the Gap Voltage (갭전압에서 나타난 Nb/Al-Al$O_{x}$/Nb 터널 접합의 전압 요동 현상)

  • 홍현권;김규태;박세일;김구현;남두우
    • Proceedings of the Korea Institute of Applied Superconductivity and Cryogenics Conference
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    • 2002.02a
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    • pp.123-126
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    • 2002
  • Samples of Nb/Al-Al$O_{x}$/Nb tunnel junction with the size of 50$\mu$m $\times$ 50$\mu$m were fabricated by employing self-aligning and reactive ion etching technique. In the samples with high-quality, $V_{m}$ value (the product of the critical current and subgap resistance measured at 2 mV) was 34 mV at the critical current density $J_{c}$ = 500 A/$cm^{2}$ and $V_{g}$ value (the gap voltage) was 2.8 mV. In the higher $J_{c}$, voltage fluctuation in the current rising at the gap voltage was observed. The $V_{m}$ and $J_{c}$ value were 8 mV and 900 A/$cm^{2}$, respectively.

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A Study of Memory Device based on Tunneling Mechanism (터널링 메커니즘을 이용한 메모리 소자 연구)

  • Lee Jun-Ha
    • Journal of the Semiconductor & Display Technology
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    • v.5 no.1 s.14
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    • pp.17-20
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    • 2006
  • This paper presents of a new type of memory cell that could potentially replace both DRAM and flash memory. The proposed device cell operates by sensing the state of about 1,000 electrons trapped between unique insulating barriers in the channel region of the upper transistor. These electrons are controlled by a side gate on the transistor, and their state in turn controls the gate of the larger transistor, providing signal gain within the memory cell. It becomes faster and more reliable memory with lower operation voltage. Moreover, the use of a multiple tunnel junction (MTJ) fur the vertical transistor can significantly improve the data retention and operation speed.

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Investigation of Junction-less Tunneling Field Effect Transistor (JL-TFET) with Floating Gate

  • Ali, Asif;Seo, Dongsun;Cho, Il Hwan
    • JSTS:Journal of Semiconductor Technology and Science
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    • v.17 no.1
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    • pp.156-161
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    • 2017
  • This work presents a novel structure for junction-less tunneling field effect transistor (JL-TFET) with a floating gate over the source region. Introduction of floating gate instead of fixed metal gate removes the limitation of fabrication process suitability. The proposed device is based on a heavily n-type-doped Si-channel junction-less field effect transistor (JLFET). A floating gate over source region and a control-gate with optimized metal work-function over channel region is used to make device work like a tunnel field effect transistor (TFET). The proposed device has exhibited excellent ID-VGS characteristics, ION/IOFF ratio, a point subthreshold slope (SS), and average SS for optimized device parameters. Electron charge stored in floating gate, isolation oxide layer and body doping concentration are optimized. The proposed JL-TFET can be a promising candidate for switching performances.

Characterization of $Nb/Al-Al_2O_3/Nb$ Josephson junction arrays fabricated With and Without cooling substrate (기판 냉각과 비냉각으로 제작된 $Nb/Al-Al_2O_3/Nb$ 조셉슨 접합 어레이의 특성)

  • Hong, Hyun-Kwon;Kim, Kyu-Tae;Park, Se-Il;Lee, Kie-Young
    • Proceedings of the KIEE Conference
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    • 2001.07c
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    • pp.1402-1404
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    • 2001
  • Josephson junction arrays of the type $Nb/Al-Al_2O_3/Nb$ were prepared by DC magnetron sputtering. The tunnel barrier was formed by in-situ thermal oxidation. Individual junctions were defined using selective niobium etching process(SNEP). The characteristic curves of Josephson junction arrays fabricated with and without cooling the substrate were represented. The junctions deposited without cooling showed poor characteristics(high leakage current, low gap voltage), and a high quality Josephson junction array of 2,000 junctions with high hysteresis was obtained with cooling and when operated at 74.6 GHz, it generated stable quantized voltage steps up to 2.2 V.

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PRESENT AND FUTURE OF SUPER HIGH-EFFICIENCY TANDEM SOLAR CELLS

  • Yamaguchi, Masafumi
    • Electrical & Electronic Materials
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    • v.11 no.11
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    • pp.37-45
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    • 1998
  • In this paper, present status of super high-efficiency tandem solar cells has been reviewed and key issues for realizing super high-efficiency have also been discussed. In addition, the terretrial R&D activities of tandem cells, in the New Sunshine Program of MITI(Ministry of International Trade and Industry) and NEDO(New Energy and Industrial Technology Development Organization) in Japan are reviewed briefly. The mechanical stacked 3-junction cells of monolithically grown InGaP/GaAs 2-junction cells and InGaAs cells have reached the highest efficiency achieved in Japan of 33.3% at 1-sun AM1.5. This paper also reports high-efficiency InGaP/GaAs 2-junction solar cells with a world-record efficiency of 26.9% at AM0, 28$^{\circ}C$ and radiation damage recovery phenomena of the tandem cell performance due to minority-carrier injection under light illumination or forward bias, which causes defect annealing in InGaP top cells. Future prospects for realizing super-high efficiency and low-cost tandem solar cells are also described.

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