• Title/Summary/Keyword: Local doping

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3D TCAD Analysis of Hot-Carrier Degradation Mechanisms in 10 nm Node Input/Output Bulk FinFETs

  • Son, Dokyun;Jeon, Sangbin;Kang, Myounggon;Shin, Hyungcheol
    • JSTS:Journal of Semiconductor Technology and Science
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    • v.16 no.2
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    • pp.191-197
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    • 2016
  • In this paper, we investigated the hotcarrier injection (HCI) mechanism, one of the most important reliability issues, in 10 nm node Input/Output (I/O) bulk FinFET. The FinFET has much intensive HCI damage in Fin-bottom region, while the HCI damage for planar device has relatively uniform behavior. The local damage behavior in the FinFET is due to the geometrical characteristics. Also, the HCI is significantly affected by doping profile, which could change the worst HCI bias condition. This work suggested comprehensive understanding of HCI mechanisms and the guideline of doping profile in 10 nm node I/O bulk FinFET.

A New Trench Termination for Power Semiconductor Devices (전력소자를 위한 새로운 홈구조 터미네이션)

  • Min, W.G.;Park, N.C.
    • Proceedings of the KIEE Conference
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    • 1998.07d
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    • pp.1337-1339
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    • 1998
  • The trench termination scheme is introduced for high voltage devices. The curvature of the depletion region at field limiting ring is critical factor to determine the breakdown voltage. The smooth curvature of the depletion junction alleviate the electric field crowding effect around this region. In the trench field limiting ring, the radius of the depletion region is smaller than conventional field limiting ring, but the distance between every trench is spaced small enough to punchthrough before initiation of local breakdown. The trench field limiting ring on silicon can ne formed by RIE followed by oxidation on side wall surface of the trench, and polysilicon filling. The combined termination of this trench floating field ring and field plate have been designed and analyzed. The breakdown simulation by 2-dimensional TCAD shows that the cylindrical junction breakdown voltage for substrate doping might be 99 percent of the ideal breakdwon voltage for substrate doping concentration of $3\times10^{14}cm^{-3}$ with about $100{\mu}m$ of lateral termination width.

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EFFECTS OF Co-DOPING LEVEL ON THE MICROSTRUCTURAL AND FERROMAGNETIC PROPERTIES OF LIQUID-DELIVERY METALORGANIC-CHEMICAL-VAPOR-DEPOSITED $Ti_{1-x}Co_xO_2$ THIN FILMS

  • Seong, N.J.;Seong, S.G.
    • Proceedings of the Korean Magnestics Society Conference
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    • 2002.12a
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    • pp.42-43
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    • 2002
  • Spintronics is a rapidly expanding research area because of recent developments in the physics of spin-dependent phenomena. For use as spintronic materials, dilute magnetic semiconductors (DMS) are of considerable interest as spin injectors for spintronic devices.$^{[1]}$ Many researchers have studied DMS, in which transition metal atoms are introduced into the lattice, thus inserting local magnetic moments into the lattice. (omitted)

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RADIAL UNIFORMITY OF NEUTRON IRRADIATION IN SILICON INGOTS FOR NEUTRON TRANSMUTATION DOPING AT HANARO

  • KIM MYONG-SEOP;LEE CHOONG-SUNG;OH SOO-YOUL;HWANG SUNG-YUL;JUN BYUNG-JIN
    • Nuclear Engineering and Technology
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    • v.38 no.1
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    • pp.93-98
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    • 2006
  • The radial uniformity of neutron irradiation in silicon ingots for neutron transmutation doping (NTD) at HANARO is examined by both calculations and measurements. HANARO has two NTD holes named NTD1 and NTD2. We have been using the NTD2 hole for 5 in. NTD commercial service, and we intend to use two holes for 6 in. NTD. The objective of this study is to predict the radial uniformity of 6 in. NTD at the two holes. The radial neutron flux distributions inside single crystal and noncrystal silicon loaded at the NTD2 hole are calculated by the VENTURE code. For NTD1, the radial distributions of the reaction rate for a 6 in. NTD with a neutron screen are calculated by MCNP, and measured by gold wire activation. The results of the measurements are compared with those of the calculations. From the VENTURE calculation, it is confirmed that the neutron flux distribution in the single crystal silicon is much flatter than that in the non-crystal silicon. The non-uniformities of the measurements for radial neutron irradiation are slightly larger than those of the calculations. However, excluding local dips in the measurements, the overall trends of the distributions are similar. The radial resistivity gradient (RRG) for a 5 in. silicon ingot is estimated to be about $1.5\%$. For a 6 in. ingot, the RRG of a silicon ingot irradiated at HANARO is predicted to be about $2.1\%$. Also, from the experimental results, we expect that the RRG would not be larger than $4.4\%$.

Fluorine and Heavy Metal Oxide Effects on Spectral Properties of Tm3+ in Silicate Glasses

  • Cho, Doo-Hee;Seo, Hong-Seok;Park, Bong-Je;Park, Yong-Gyu
    • Journal of the Korean Ceramic Society
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    • v.40 no.8
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    • pp.725-729
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    • 2003
  • The fluorine doping along with heavy metal oxides remarkably raised the $^3$H$_4$ lifetime and the quantum efficiency in Tm$^{3+}$-doped silicate glasses. 29 mol% of fluorine substitution for oxygen in 70SiO$_2$-15Pbo-12ZnO-3KO$_{1}$2/ glass raised $^3$H$_4$ lifetime to 193 $mutextrm{s}$. Refractive indices were raised by heavy metal oxide substitution, but hardly changed by fluorine substitution. The fluorine doping changed the local structure around Tm$^{3+}$ions, then low energy vibrations related to fluorine are considered to largely reduce the multi-phonon relaxation rates in the oxyfluoride silicate glasses. The $^3$H$_4$ lifetimes and absorption and emission spectra of Tm$^{3+}$doped silicate and oxyfluoride silicate glasses are reported, and Judd-Ofelt calculation results are discussed in this paper.

Electrical Characteristics of 500V LIGBT for Intelligent Power ICs (인텔리전트 파워 IC용 500V급 LIGBT의 전기적 특성에 관한 연구)

  • Kang, Ey-Goo;Sul, Won-Ji;Seo, Hyun-Ju;Kim, Hyun-Mi;Sung, Man-Young
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2005.07a
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    • pp.183-184
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    • 2005
  • In this paper. a new small size Lateral Trench Electrode Power IGBT is proposed. The entire electrode of proposed LIGBT is placed in trench oxide. The forward blocking voltage of the proposed LIGBT is improved by 1.6 times with that of the conventional LIGBT. The forward blocking voltage of proposed LIGBT is 500V. At the same size. a increase of the forward blocking voltage of about 1.6 times relative to the conventional LIGBT is observed by using TMA-MEDICI which is used for analyzing device characteristics. Because the electrodes of the proposed device are formed in trench oxide. the electric field in the device are crowded to trench oxide. We observed that the characteristics of i the proposed device was improved by using TMA-MEDICI and that the fabrication of the proposed device is possible by using TMA-TSUPREM4.

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Local Oxidation of 4H-SiC using an Atomic Force Microscopy (원자현미경을 이용한 탄화규소 (SiC)의 국소산화)

  • Jo, Yeong-Deuk;Bahng, Wook;Kim, Sang-Cheol;Kim, Nam-Kyun;Koo, Sang-Mo
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.22 no.8
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    • pp.632-636
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    • 2009
  • The local oxidation using an atomic force microscopy (AFM) is useful for Si-based fabrication of nanoscale structures and devices. SiC is a wide band-gap material that has advantages such as high-power, high-temperature and high-frequency in applications, and among several SiC polytypes, 4H-SiC is the most attractive polytype due to the high electron mobility. However, the AFM local oxidation of 4H-SiC for fabrication is still difficult, mainly due to the physical hardness and chemical inactivity of SiC. In this paper, we investigated the local oxidation of 4H-SiC surface using an AFM. We fabricated oxide patterns using a contact mode AFM with a Pt/Ir-coated Si tip (N-type, 0.01-0.025 ${\Omega}cm$) at room temperature, and the relative humidity ranged from 40 to 50 %. The height of the fabricated oxide pattern (1-3 nm) on SiC is similar to that of typically obtained on Si ($10^{15}^{\sim}10^{17}$ $cm^{-3}$). We perform the 2-D simulation to further analyze the electric field between the tip and the surface. We demonstrated that a specific electric field (4 ${\times}$ $10^7\;V/m$) and a doping concentration ($^{\sim}10^{17}$ $cm^{-3}$) is sufficient to switch on/off the growth of the local oxide on SiC.

Fabrication and Electrical Properties of Local Damascene FinFET Cell Array in Sub-60nm Feature Sized DRAM

  • Kim, Yong-Sung;Shin, Soo-Ho;Han, Sung-Hee;Yang, Seung-Chul;Sung, Joon-Ho;Lee, Dong-Jun;Lee, Jin-Woo;Chung, Tae-Young
    • JSTS:Journal of Semiconductor Technology and Science
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    • v.6 no.2
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    • pp.61-67
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    • 2006
  • We fabricate local damascene FinFET cell array in sub-60nm feature sized DRAM. The local damascene structure can remove passing-gate-effects in FinFET cell array. p+ boron in-situ doped polysilicon is chosen for the gate material, and we obtain a uniform distribution of threshold voltages at around 0.7V. Sub-threshold swing of 75mV/d and extrapolated off-state leakage current of 0.03fA are obtained, which are much suppressed values against those of recessed channel array transistors. We also obtain a few times higher on-state current. Based on the improved on- and off-state current characteristics, we expect that the FinFET cell array could be a new mainstream structure in sub-60nm DRAM devices, satisfying high density, low power, and high-speed device requirements.

Determination of Memory Trap Distribution in Charge Trap Type SONOSFET NVSM Cells Using Single Junction Charge Pumping Method (Single Junction Charge Pumping 방법을 이용한 전하 트랩 형 SONOSFET NVSM 셀의 기억 트랩 분포 결정)

  • 양전우;흥순혁;박희정;김선주;서광열
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 1999.11a
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    • pp.453-456
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    • 1999
  • The Si-SiO$_2$interface trap and nitride bulk trap distribution of SONOSFET(polysilicon-oxide-nitride-oxide-semiconductor)NVSM(nonvolatile semiconductor memory) cell were investigated by single charge pumping method. The used device was fabricated by 0.35 7m standard logic fabrication including the ONO cell process. This ONO dielectric thickness is tunnel oxide 24 $\AA$, nitride 74 $\AA$, blocking oxide 25 $\AA$, respectively. Keeping the pulse base level in accumulation and pulsing the surface into inversion with increasing amplitudes, the charge pumping current flow from the single junction. Using the obtained I$_{cp}$-V$_{h}$ curve, the local V$_{t}$ distribution, doping concentration, lateral interface trap distribution and lateral memory trap distribution were extracted. The maximum N$_{it}$($\chi$) of 1.62$\times$10$^{19}$ /cm$^2$were determined.mined.d.

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