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1.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 04 | Apr 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 2588 Simulation of High k dielectric MOS with Hfo2 as a gate dielectric Kajal Yadav1, Shivani Saxena2 1Student of M .Tech (VLSI Design), Department of Electronics, Banasthali Vidyapith, Rajasthan, India 2Assistant Professor, Department of Electronics, Banasthali Vidyapith, Rajasthan, India ---------------------------------------------------------------------***------------------------------------------------------------------- Abstract- Conventional MOS over 40years has been fabricated using Silicon substrate with polysilicon in gate material. As scaling of SiO2 increases, a seriousissue interms of tunneling current and oxide breakdown raises. To overcome of these problems, silicon based MOS with High-k dielectric material in gate is becoming a strong alternative for replacing the conventional SiO2 dielectrics gates MOSFETs. High-k oxides provide a solution to leakage problems and improve performance such types of MOS can be used in both application of high performance and low power consumption. In this paper, HFO2 based high k dielectric gate is used for the formation of device because HFO2 is having high dielectric constant value and improves the performance of the device. On the basisofsomeelectrical parameters, a comparative study in between conventional MOS and High k dielectric MOS is also presented. Keywords: High k material, Hfo2, Leakage current, power consumption, output resistance, gate oxide. 1. Introduction: The National Technology Roadmap of semiconductor (NTRS) and ITRS having scaling predication from 100 components per IC in 1965 to 15 billion in the current state. There are less gain in device performance i.e. power Consumption, short channel effects and parasitic capacitance as scaling goes further below sub-100 nm. In 2007, the use of high-k dielectrics [6] is first time introduced, to show gate leakage issues. High K dielectric devices have applications in low power dissipation, low leakage current and high performance over conventional MOS. Basic difference in structure of conventional MOS over high k dielectric device is gate material. The materials used for the conventional MOS is SiO2 but in high K dielectric based device gate material can be HFO2, Al2O3, Y2O3, La2O3, Sc2O3 [7]. For further downward scaling, dielectric having a higher dielectric constant will be the solution for achieving the same transistor performancewhilemaintaininga relativelythick physical thickness [6]. Table: 1 Electrical properties of high k material [5-6]. As from above table, it can be seen that HFO2 is having higher dielectric constant value and it is widely used material for the simulation of MOS device. In the below figure the schematic of high k dielectric based gate oxideis shown. Gate dielectric Material Dielectric constant (k) Energy band gap Eg (eV) Applications SiO2 3.9 9 Passivation Al2O3 8 8.8 High channel mobility TiO2 80 3.5 Low leakage current up to 1 nA/ cm2 ZrO2 25 5.8 high- permittivity HfO2 35 5.7 Higher Breakdown voltage Ta2O5 25 6 high durability and stability to heat Y2O3 13 6 effective mobility
2.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 04 | Apr 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 2589 Fig.1 Schematic of high K dielectric based MOS [5]. Table: 2 Comparison of High K dielectric MOS with Conventional MOS [8]. Parameters Conventional MOS High k dielectric material Leakage current As the thickness decreases below 2 nm, leakage current increase drastically and leading to high power consumption problem and reduces device reliability. Increased gate capacitance and reduced leakage effects. Gate resistance It is having higher gate resistance. Metal gate has much lower gate resistance and desirable work function. Mobility Mobility of silicon based MOS was less which increases leakage current. Effective mobility increased and leakage current decreased in the case of HfO2. As from above table 2, it is shown thatconventional MOSFET have higher leakage current, offer high value of gate resistance and having less speed. The used of high k-dielectric based material providing improvement in the performance of the device. Among the three main terminals of the MOS transistor – gate stack (Scaling of the gate stack is a key to enhancing the performance of complementary metal-oxide-semiconductor (CMOS), field-effect transistors (FETs) of past technology generations).Source/drain, and channel length; gatestack is most sophisticated and sensitive part for performance,yield and reliability [1]. Many alternate of high-k gate dielectrics have been studied to replace SiO2.Among them, Hf-based oxides has been recently highlighted as the most suitable dielectric materials because of its comprehensive performance. 2. Evolution & Device Development: 1. The industry has employed oxy-nitride gate dielectrics since the 1990s, but in conventional siliconoxidedielectricis infused with the help of small amount of nitrogen. [2]. 2. In early 2007, Intel has announced the deployment of hafnium-based high-k dielectrics with a metallic gate for components worked one the technology of 45 nanometer and has been used it in the 2007 processor series.[5] 3. In 2007, IBM also announced the transition to high-k materials, also hafnium-based, for some products in 2008. 4. NEC Electronics has also announced the use of an HfSiON dielectric in their 55 nm. 5. The 2006 ITRS roadmap predicted that the implementation of high-k materials to be commonplace in the industry by 2010[6]. 3. Modeling and Simulation of HfO2 based MOSFET: Fabrication process flow is: 1. Define silicon substrate. 2. Deposition of high k dielectric HFO2 in gate. 3. Partially etch out the high k material (HFO2). 4. Formation of drain and source using ion implantation having phosphorous impurity. 5. Deposition of electrodes using aluminum material. 6. Deposition of tungsten material on HFO2 layer for the formation of gate. 7. Deposition of low resistance material (aluminum) on the tungsten layer. Step: 1 For <100> boron is used to doped silicon wafer, choose ADD region from Region menu and from right side window click on silicon material and select set base impurity.
3.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 04 | Apr 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 2590 Fig.1 Deposition of silicon substrate. Step: 2 HFO2is thermally grown from the region menu, then from the Right window select materialHFO2. Fig.2 Deposition of high k-dielectric layer (HFO2). Step: 3 HFO2 is etched out first and etching of silicon substrate, for this chooses the region which will etchoutand click on apply button. Fig.3 Etch out the extra material. Step: 4 Drain and source is created using phosphorus impurity. Fig.4 Drain and source is doped. Step: 5 Aluminum materials are used for the formation of electrodes. Fig.5 Electrodes are deposited Step: 6 Gate is placed on the high k material using tungsten material. Fig 6.Making of gate
4.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 04 | Apr 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 2591 Step: 7 High k devices are ready by applying the low resistance metal layer on the gate. Fig.7 High k-dielectric based device. IV. Software details: Dr. Ivan Pasic founded Silvaco in 1984. Silvaco is an interactive tool. It has different parts such as Deck build, Tony plot, Maskview. Silvaco is used to provide analog semiconductor process, device and design automation solutions in CMOS. Among these interactive tools, Devedit is a tool of silvaco which is used for simulation of device, it will be used to either create a device by remesh or edit an existing device. It helps to create standard silvaco structure which can be easily integrated into 2D or 3D simulators of silvaco tool. V. Conclusion: When decreasing size of MOS technology it required the replacement of the SiO2 with gate dielectrics material that have a high dielectric constant value (high-k). When the thickness of SiO2 is decreased below 1.4 nm then electron tunneling effects and high leakage currents will occur which causes a serious obstacles for device reliability. Therefore, MOSFET structure with high k dielectric is useful toimprove electrical performance of the design. VI. References: [1]George James T, Saji Joseph and Vincent Mathew, “Effect of counter-doping thickness on Double-Gate MOSFET characteristics”, Journal of Semiconductor Technology and Sciences, Vol.10, No. 2, pp. 130,132, June 2010. [2] M. H. Chowdhury, M. A. Mannan and S. A. Mahmood, “High-k Dielectrics for Submicron MOSFET”, IJETSE International Journal of Emerging Technologies in Sciences and Engineering, vol. 2, no. 2, pp. 8-10, July 2010. [3] MaizanMuhammad, SunailyLokman, HaninHussin, “optimization in fabricating 90nm NMOS transistors using silvaco”, IEEE student conference on research and development. pp. 2, 2009. [4] L. Manchanda etal.,“High K Gate DielectricsfortheSilicon Industry,” Ext. Abst.IWGI, pp.56-60, 2001. [5] A. P. Huang1, Z. C. Yang and Paul K. Chu, “Hafnium-based High-k Gate Dielectrics”, Advances in Solid State Circuits Technologies, Book edited by: Paul K. Chu, ISBN 978-953-307-086-5, pp. 446, April 2010. [6] Prerna “Review Literature for Mosfet DevicesUsingHigh K”, international journal for research in applied science, Vol.1IssueIV, November 2013. [7] Saied Mohsenifar*, M. H. Shahrokhabadi,“Gate Stack High-κ Materials for Si-Based MOSFETs Past, Present, and Futures”, Microelectronics and Solid State Electronics 2015, 4(1): 12-24. [8] A thesis on “Preparation and Characterization of High-k Aluminum Oxide Thin Films by Atomic Layer Deposition for Gate Dielectric Applications”, by Anu Philips, Chapter 1, 2010.
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