International Journal of Engineering Trends and Technology (IJETT) – Volume 8 Number 9- Feb 2014 Source Drain Engineering in FinFET – A Review I.Flavia Princess Nesamani#1, Rekha Puthenpurayil Divakaran#1,Dr.V.Lakshmi Prabha#2 ,Sujith M.B#1 #1 ECE Department, Karunya University, #2Government College of Technology, Coimbatore Abstract— Scaling poses many challenges beyond 22nm technology. In this paper, the various designs proposed by researchers about the double gate FinFET with raised source and drain have been studied. Also the significance of various parameters, different modes of operation of the FinFET, effect of fin thickness over the performance, doping level, effect of height of source and drain, advantages of using metal gate electrodes along with high-k dielectrics have been studied. Different designing techniques of double gate FinFETs and its advantages are noted so as to create a new design for better drive current and low leakage. Keywords—Source/Drain Short Channel effect engineering, SOI, I. INTRODUCTION Scaling the planar transistors to gate length below 22 nm [1] require high doping of the channel and source/drain regions to control short channel effect. As a result random dopant fluctuation [2], [3] and threshold voltage control has become a major issue. Random dopant fluctuation is seen in extremely scaled devices particularly due to the narrow device width [4]. Double gate MOSFETs has higher scalability than the single gate ones [5]. A fully depleted SOI device allows for lighter channel doping [6] or completes elimination of doping in order to obtain better threshold variability control [7]. FinFET with undoped channel [8] is a solution for the elimination of this serious concern. It is due to their extremely thin fin structure that makes them the most unique structure among the multi gate transistors. This helps to control the short channel effects and suppress the leakage current between the drain and source. It has a three dimensional structure and it operates at low voltage [9] and is less susceptible to random dopant fluctuation. ISSN: 2231-5381 Source/Drain engineering is done in order to reduce parasitic resistance. Thus the drive current will be high in source/drain engineered devices [10]. Symmetric DG-FETs [11] have both the inversion channels formed, one adjacent to the first gate and the other to the second gate. II. LITERATURE SURVEY As device is scaled down to nanometer regime, there arise many problems such as short channel effects, high leakage current, which seriously affect the device performance. A. Effect of Fin thickness and fin height on FinFET In [12], Fin thickness and fin height are the two important parameters used to control short channel effects. Thinner the fin much better is the short channel effect [13]. In thick fin device, the drain electric field lowers the barrier of channel because of reduced source/fin and drain/fin junction capacitances. Subthreshold slope also increase in thick fin device. The main reason for this is the gate loses its control over the channel. Fin-thickness plays a very important role in deciding SCEs. As the fin thickness is increased, DIBL also increases. In [27], Prathima et al. noticed that as the thickness of the fin was reduced, the off state leakage current was also found to reduce and when the fin height is increased, the drive current capability also increases. B. Metal gate electrode and work function In [13], feature such as gate-first metal gate stacks were included to control the short channel effectively. By this approach, the metal gate is formed using HfO2 gate dielectric and metal stacks. Here author mentioned about double etch method to define the gate lengths below 25 nm. In [14], Hamed Dadogur et al. mentioned about the dependency of metal work function on grain orientation. The work-function for a solid material depends on the number of metal atoms per unit area http://www.ijettjournal.org Page 472 International Journal of Engineering Trends and Technology (IJETT) – Volume 8 Number 9- Feb 2014 of the metal surface. Work function is dependent on the interaction at the metal-dielectric interface. In [28],Farkanda et al. describes if conventional poly silicon gate, is not heavily doped, then the carrier concentration vary and a built in electric field exist, thereby causing a depletion in the poly silicon/ SiO2 interface. C. Source/Drain engineering In [15], diamond shaped epi structure was proposed here to improve the parasitic resistance [16]. The main reason for this is due to the 3D structure with thin Si-body. The structure of the device has a main role to play in providing a good result. The source/drain is slightly extended in width than in the channel region mainly to reduce the parasitic resistance which is caused by the fin scaling. Parasitic resistance can be reduced by either using a raised S/D structure or by using self aligned silicided S/D. Side wall image transfer (SIT) technique is also mentioned in here. This technique is the best for creating the scaled fin. Here the thickness of the fin is defined by the spacer thickness. In this technique, first spacers are formed around mandrels, and after the removal of the mandrels, Si is etched using spacers which acts as a mask and finally the fins are formed. In [17], the author describes about the spike annealing. It is mentioned that spike annealing can suppress lateral diffusion in source/drain extension. In [18], Xiao Gong et al. reported about source/drain engineering technique in N-channel MOSFET featuring the in-situ doping of the source/drain with InGaAs which has very high mobility. By implanting Si in InGaAs S/D regions does not bring high doping concentration, which will lead to high S/D series resistance and better drive current performance. D. Independent gate and tied gate mode In [19], Dhruva Ghai et al. describes about tied gate mode and independent gate mode. Tied gate or Shorted gate(SG) has smallest delay, followed by Independent gate. For power consumption, Low Power(LP) mode gives the lowest power consumption, followed by IG and SG mode. In independent gate FinFET the top region of the gate is removed and both the gates are biased separately, whereas same voltage is applied to both the gates of the tied gate FinFET. In [20], Masoud Rostami et ISSN: 2231-5381 al., describes about the electrostatic force coupling both the gates together, due to this force the channel formed due to one gate is highly dependent on the other. If no voltage is applied to the back gate of an independent gate FinFET, no channel is formed near the inactive gate, but this will affect the threshold voltage of the other gate. In short if any one of the gates is disabled then the drive current of the device is reduced by half. The input capacitance of the disabled gates is half that of conventional tied gate FinFET. In [21], author mentions that tied gate has high drive current and leakage current than that of the independent gate FinFET. In independent gate, the back gate bias is to alter the threshold voltage of the front gate. In [26], author concludes that tied gate FinFET is a better option for high performance design. Symmetric and asymmetric gate work-function In [21], [22], author refers the symmetric gate work-function FinFETs as one with both the front and back gates with same work-function and if both are of different work-function, then it is called asymmetric gate work-function FinFETs. It is also suggested that it is more practical to use asymmetrical gate work-function FinFETs for ultra low leakage designs. E. Parasitic capacitance In digital application, the main aim is to have lower capacitance and high drive current. As scaling is achieved and when it reaches the nanometer regime, the gate capacitance including the intrinsic capacitance and parasitic capacitance is not reduced as the gate length is reduced and this is mainly due to the excessive parasitic capacitance. So to improve the performance of the device, parasitic capacitance reduction is important. In [23], Bhoj el al. mentioned about the parasitic capacitances in multifin multigate FET and in multigate SRAM. The fin pitch which is the distance between the centers of the two consecutive fins is varied and the parasitics were calculated for each layout. The total drain capacitance increased in bulk FETs by 11.5% when compared with SOI FETs for 22 nm node. This increase in the bulk device is mainly due to the shared drain-to-bulk capacitance. In case of total gate capacitance, there is only a slight increase from SOI to bulk. Also F. http://www.ijettjournal.org Page 473 International Journal of Engineering Trends and Technology (IJETT) – Volume 8 Number 9- Feb 2014 wordline, internal node and bitline capacitances were measured in the case of multigate SRAM. In [24], Joshi et al. presented SOI SRAMs for 3D TCAD capacitance extraction assisted with hardware data. This method consists of three segments, iterative BEOL analysis, iterative FEOL analysis and iterative yield analysis. In all these three cases, the input layouts were converted to 3D structures and then transport analysis based capacitance extraction was performed. Effect of gate oxide thickness on FinFET In [25], Yee-Chia Yeo et al. says reducing the gate oxide thickness increases the drain current. As the scaling is increased further, the use of SiO2 becomes inapplicable. The main reason for this is the increased penetration of dopants into the channel region. The main challenge to further MOSFET scaling is the increased leakage current. Scaling of gate oxide below 1.2 nm leads to increase in gate electric field. In [28], the requirement of ultra thin oxide is mentioned for scaled sub-50nm MOSFETs, thereby increasing the gate leakage current which is caused by direct tunnelling current and this increases the power consumption and hence deteriorates the device performance. [2] Leung, G., Chi On Chui, “Variability Impact of Random Dopant Fluctuation on Nanoscale Junctionless FinFETs”, IEEE Electron Device Lett,Vol.33 ,No. 6, 2012 [3] E. Baravelli, M. Jurczak, N. Speciale, K. De Meyer, A. Dixit, “Impact of LER and Random Dopant Fluctuations on FinFET Matching Performance”, IEEE Transactions on Nanotechnology, Vol.7,No.13, pp. 291-298, May 2008 [4] Meng-Hsueh Chiang , Ilan, Jeng-Nan Lin , Keunwoo Kim , Ching-Te Chuang, “Random Dopant Fluctuation in Limited-Width FinFET Technologies”, IEEE Trans. Electron Devices, Vol. 54, pp. 2055 – 2060, Aug 2007 [5] Jakub Kedzierski ,Meikei Ieong, Edward Nowak, Thomas S. Kanarsky, YingZhang, Ronnen Roy, Diane Boyd, David Fried, and H.-S.Philip Wong, “Extension and Source/Drain Design for High Performance FinFET Devices”, in IEEE Trans. On Electron Devices, Vol.50, No.4, pp. 952-958, APRIL 2003 [6] N.Kistler, J.Woo, “Symmetric CMOS in fully-depleted silicon-oninsulator using P/sup +/-polycrystalline SiGe gate electrodes”, in International Electron Devices Meeting, pp. 727 – 730, Dec 1993 [7] K.Roy, S.Mukhopadhyay, H.Mahmoodi-Meimand, “Leakage current mechanisms and leakage reduction techniques in deep-submicrometer CMOS circuits”, in Proc. of the IEEE, 2003, Vol.91, No.2, pp.305-327 [8] T. Matsukawa, S. O’uchi, K. Endo, Y. Ishikawa et al.,“Comprehensive analysis of variability sources of FinFET characteristics”, in Symposium on VLSI Technology, pp. 118-119, June 2009 [9] [Online]. https://www.synopsys.com [10] A.Dixit, A. Kottantharayil, N. Collaert et al., “Analysis of parasitic S/D resistance in multigate FET”, IEEE Transactions Electron Devices,Vol.52, No.6, June 2005 [11] Yaun Taur,“Analytic solutions of charge and capacitance in symmetric and asymmetric double-gate MOSFETs”, IEEE Transcations on Electronic Devices, Vol.48, No.12, pp. 2861-2869, Dec 2001 [12] Gaurav Saini, Ashwani K Rana ,“Physical Scaling Limits of FinFET Structure: A Simulation Study “ in International Journal of VLSI design & Communication Systems (VLSICS), Vol.2, No.1, March 2011 [13] V.Basker, T.E.Standaert, et. al,“A 0.063 µm2 FinFET SRAM cell demonstration with conventional lithography using a novel integration scheme with aggressively scaled fin and gate pitch,”in Proc. Int. Symp. VLSI Technology, 2010, pp.19–20 [14] H. Dadgour, K .Endo, V. De, and K. Banerjee, “Modeling and analysis of grain-orientation effects in emerging metal-gate devices and implications for SRAM reliability, ”in Proc. Int. Electron Devices Meeting, 2008, pp.705–708 [15] H.Kawasaki, V.S.Basker, et.al, “Challenges and solutions of FinFET integration in an SRAM cell and a logi circuit for 22 nm node and beyond,” in Proc. Int. Electron Devices Meeting ,2009,pp.1–4 [16] D Mitra and C K Maiti, “25nm Triple-Gate FinFETs with Raised Source/Drain: A 3D Simulation Study” , IETE, NateHCA-07 [17] Ching I Li, Chin Cheng Chien, et.al “Superior Spike Annealing Performance in 65nm Source/Drain Extension Engineering”in 13th IEEE International Conference on Advanced Thermal Processing of Semiconductors , Oct 2005, pp. 163 – 167 G. III. CONCLUSIONS Different FET parameters were studied and it is found in most of the literatures in scaled down technology, that metal gates are completely replacing the conventional poly silicon gates and conventional gate dielectric material i.e. SiO2 is being replaced by high–k dielectric materials. The FET parameters such as fin thickness, fin height, gate length, and gate oxide thickness all affect the performance of the device. Thinner fin is found to have better short channel control, taller fin is best when high drive current is preferred. Advantages of shorted gate were noticed and it is suited for high performance design. So by creating a design by keeping these parameters in mind would obviously bring out some better results which can further be extended to various analog and digital circuit design application. REFERENCES [1] H.Iwai, “Roadmap for 22 nm and beyond”, in Microelectronic Engineering, March 2009. 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