International Journal of Emerging Technology and Advanced Engineering Website: www.ijetae.com (ISSN 2250-2459, ISO 9001:2008 Certified Journal, Volume 3, Issue 2, February 2013) An Improved Device Consideration for Ultra-Low Power Applications in Junction Field Effect Transistor Mayank Kumar1, Mukesh Kumar2, Anil Kumar3, Ashish Das4, A.K.Jaiswal5, Gaurav Nigam6, Kamal Prakash Pandey7 1 Student,2,3,4Assistant Professor,5Professor,6Student Dept .of Electronics & Comm. Engineering SHIATS Allahabad, Uttar Pradesh State, India 7 Assistant Professor, Dept .of Electronics & Comm. Engineering SIET Allahabad, Uttar Pradesh State, India JFET a unipolar-transistor, which acts as a voltage controlled current device and is a device in which current at two electrodes is controlled by the action of an electric field at a p-n junction. The JFET consists semiconductor material (usually Si) which constitutes a channel for the majority carrier flow and gates. In a conducting semiconductor there are two ohmic contacts between channels i.e. source and drain. The figure II shows the device of JFET. The major disadvantage of JFETs are large input capacitance and gate leakage [1] [7]. To overcome these disadvantages we have used Silicon–on-Insulator (SOI) and thus improve the better performance of JFETs. Silicon-on-insulator (SOI) technology has long been used in many special applications, such as radiationhardened or high-voltage integrated circuits. It is only in recent years that SOI has emerged as a serious contender for low-power high-performance applications. The figure I shows the device symbol of SOI. Abstract -- This paper presents an improved device consideration for low power applications in junction field effect transistor. The need for low power applications and scaling of JFET is beyond 30nm. The enhancement mode dual gate n- channel JFET devices offer a grid potential for low power applications. In the designing of low power circuits, there are several limitations in case of C-MOS and MOSFET devices. Here the Junction field effect transistor (JFET) device which is easily designed and offers great applications. Over conventional JFET architecture and performance of 45nm silicon on insulator (SOI) and a N-channel JFET [8]. The simulation results shown the enhancement mode n channel JFET offer low threshold voltage 0.23V at a power supply voltage of 0.5V i.e. very good for low voltage integrated circuits. Keywords - Junction field effect transistor (JEFT), nchannel JEFTs, Silicon on -insulator JFETs. I. INTRODUCTION In today’s driven world, numbers of integrated circuits (ICs) are increases every year. The increasing chip capacity or the density along with the field communications we need the ultra low power analog integrated circuits(IC’s) due to this used C-MOS and MOSFET. In the field (mobile) communication increases the components which increase the power dissipation and it has limited the maximum supply voltage in complementary MOSFET (CMOS) ICs [1-3]. In the case of analog integrated circuits the CMOS ICs at ultra low voltage which down to 0.5V [4-5] . Thus there are a several limitations in scaled CMOS for ultra low voltage applications and in the designing. To improve this limitations study the silicon-on-insulator (SOI) and the enhancement N-channel Junction Field Effect Transistor for designing the ultra-low voltage analog integrated circuits. The enhancement JFET is reducing the voltage supply limitation for ultra-low voltage. Figure I SOI device symbol Objective of this paper is to analyze the potential performance of characteristics to designed N-channel junction field effect transistors (JFETs) by using of simulation tools. 292 International Journal of Emerging Technology and Advanced Engineering Website: www.ijetae.com (ISSN 2250-2459, ISO 9001:2008 Certified Journal, Volume 3, Issue 2, February 2013) JFET CharacteristicsCut-off regionWhen Vgs<Vp and drain current goes to zero (Id=0). Triode regionWhen Vp<Vgs<0 and Vds<Vgs-Vp thus Id=Idss[2(1-Vgs/Vp)(Vds/-Vp)-(Vds/-Vp)2] (I) Saturation RegionWhen Vp<Vgs<0 and Vds>Vgs-Vp. In the simulation process we analyze this in N type JFETs i.e. Ids=(q*µ*Nd*w*t)(Vds-2/3))(Vds+Vbi-Vg)3/2-((VbiVg)3/2/Vp1/2) (II) Using this equation we simulate the device characteristics for the N-JFET devices study in this paper. The Pinch Off voltage is occur when the gate to source voltage is made more negative (-Vgs).Vp=q*Nd*A2/(2*Ɛ) (III) Built in voltage Vbi=Vt-Vp (IV) II. T HEORY AND METHDOLOGY The Junction field effect transistor in N channel (nJFET) the cross-sectional diagram is shown in figure II which generates its structures and its characteristics i.e.(Ids Vs Vgs & Ids Vs Vds) and characterize their performance at ultra low voltage i.e. Vdd = 0.5V. The structures simulation was generated by some parameters in the using of simulation tools. In the N-JFET structures shown in figure II as N type channel are heavily doped. N-type semiconductor channel with a P-type region called the Gate diffused into the Ntype channel forming a reverse biased PN-junction and it is this junction which forms the depletion region around the gate area when no external voltages are applied. JFETs are therefore known as depletion mode devices. With no external Gate voltage (VG = 0), and a small voltage (VDS) applied between the Drain and the Source, maximum saturation current (IDSS) will flow through the channel from the Drain to the Source restricted only by the small depletion region around the junctions. If a small negative voltage (-VGS) is now applied to the gate the size of the depletion region begins to increase reducing the overall effective area of the channel and thus reducing the current flowing through. So by applying a reverse bias voltage increases the width of the depletion region which in turn reduces the conduction of the channel. The Gate voltage is made more negative and the width of the channel decreases until no more current flows between the Drain and the Source and the FET is said to be "pinched-off". The voltage at which the channel closes is called the "pinch-off voltage" (VP ). III. RESULTS AND D ISCUSSIONS Characterize the N channel JFETs device and the analytical study which the device was performed to generate the Ids vs Vds characteristics when Vgs is constant for some values and the next characteristics between Ids Vs Vgs characteristics when Vds is constant for some values and form the simulation data from the equation (II) and the values are extracted. VDS Source Electron drift velocity V=µ*f (V) Ids vs Vds Characteristics n-JFETs figure III shows Ids Vs Vds. Characteristics of n-channel JFET at various gate to source voltage values and the threshold voltages Vth=0.23v.The devices simulation results shows that NJFETs devices offers low threshold voltages as compared to MOSFETS. Drain P-type VGS N-type Channel P-type Gate Depletion Layer Figure.II N channel JFET structure 293 International Journal of Emerging Technology and Advanced Engineering Website: www.ijetae.com (ISSN 2250-2459, ISO 9001:2008 Certified Journal, Volume 3, Issue 2, February 2013) Figure.III shows the values at constants values of Vgs=0.1,0.2,0.3,0.4V Figure.IV shows the values at constants values of Vds=0.2,0.3,0.4,0.5V It observed from figure IV that V gs increases at Vth=0.23V, increasing the cross-section of the channel and as a result Ids increases with increases in V gs≥Vth. Ids vs Vgs Characteristics n-JFETs- Figure.IV shows Ids vs Vgs Characteristics of n-channel JFET at various drain to source voltage values and the threshold voltages Vth=0.23V. The devices simulation results shows that NJFETs devices offers low threshold voltages as compared to MOSFETS. Table I Major Parameters are used in DG-JFETs 294 DEVICE PARAMETERS UNITS VALUES Threshold Voltages V 0.23 CHANNEL LENGTH Nm 16 CHANNEL WIDTH Nm 45 International Journal of Emerging Technology and Advanced Engineering Website: www.ijetae.com (ISSN 2250-2459, ISO 9001:2008 Certified Journal, Volume 3, Issue 2, February 2013) Mayank Kumar obtained B.Tech. in ECE and presently pursuing M.Tech. (Communication System engg.) from SHIATS-Allahabad. He guided various projects at engineering level. His area of interest includes communication systems and solid state electronics. IV. CONCLUSION In this paper, some important parameters are defined i.e. threshold voltage, length, width and charge. Simulation based study on the device architecture and performance of enhancement type JFETs. The device simulation shows better results in V-I characteristics at 0.5V. The graph obtained between the gate to source voltage (Vgs) and drain to source current (Ids) and the another graph shows between the drain to source voltage (Vds) and drain to source current (Ids) and a slight linear graph found. We have seen the advantage of CMOS and MOSFET technology over enhancement JFETs. Thus, the nJFETs, presented in this paper are highly valuable device for the ultra low-voltage analog application. Mukesh Kumar is Asst. Prof. at SHIATSAllahabad. He obtained B.Tech. in ECE & M.Tech. in Advanced Communication System Engineering. He guided various projects at engineering level. His area of interest includes Signal processing & communication system Anil Kumar is Asst. Prof. at SHIATSAllahabad. He obtained B.E (MMMEC, Gorkhpur) in ECE & M.Tech. (IIT B.H.U Formerely IT B.H.U.) in Microwave Commun--ication Engg. and presently pursuing Ph.D (Elect.). He guided various projects & research He guided various projects & research at undergraduate & years postgraduate level. He has more than 10 teaching experience and actively involved in research and publications. His area of interest includes Antenna, microwave, artificial neural network and VLSI. REFERENCES [1 ] P.E. Allen, B.J. Blalock, and G.A. Rincon "Low voltage analog circuits using standard CMOS technology," Proc. Int. Symp. LowPower Electron. & Design, pp. 209-214, 1995. [2 ] S.Saha, “Design considerations for 25 nm MOSFET devices,”SolidSt Electron., vol. 45, no.10, pp. 1851-1857, Oct. 2001. [3 ] S. Saha, “Scaling considerations for high performance 25 nm metaloxide-semiconductor field effect transistors”, J. Vac. Sci.Technol. B,vol. 19, no. 6, pp. 2240-2246, Nov. 2001. [4 ] S. Chatterjee, Y. Tsividis, and P. Kinget, “Ultra-low voltage analog integrated circuits,” IEICE Trans. Electron, vol. E89-C,no. 6, pp.673-680, Jun. 2006. [5 ] S. Chatterjee, Y. Tsividis, and P. Kinget, "0.5-V analog circuit techniques and their application in OTA and filter design," IEEE J.Solid-State Circuits, vol. 40, no. 12, pp. 2373–2387, Dec. 2005. [6 ] C. Hu, “Future CMOS scaling and reliability”, Proc. of the IEEE,vol. 81, No. 5, pp. 682-652, May 1993. [7 ] S.K. Saha, “Source-drain engineering for sub-90 nm junctionfieldeffect transistors,” IEDST 2009, pp. 1-6. [8 ] N.M.Biju and R.Komaragiri“Dual Gate enhancement-mode JFET (DG-JFET)for ultra low power applicationss,” IEEE 2012, pp. 1-4. Ashish Xavier Das is Asst. Prof. at SHIATSAllahabad. He obtained B.Tech. in ECE & M.Tech. in Advanced Communication System Engineering. He guided various projects at engineering level. His area of interest includes Signal processing and communication system. A.K. Jaiswal is Prof. and Head of ECE-Dept at SHIATS-Allahabad. He Obtained M.Sc. in Tech. Electronic & Radio Engg. from Allhabad University in1967. He guided various projects & research at undergraduate & postgraduate level. He has more than 40 years Industrial, 295