Non volatile molecular memory in silicon IC application

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Non volatile molecular memory in silicon IC application

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NON-VOLATILE MOLECULAR MEMORY IN SILICON IC APPLICATION TAN YOKE PING NATIONAL UNIVERSITY OF SINGAPORE 2007 Spine NON-VOLATILE MOLECULAR MEMORY IN SILICON IC APPLICATION TAN YOKE PING 2007 NON-VOLATILE MOLECULAR MEMORY IN SILICON IC APPLICATION TAN YOKE PING ( B.Eng (Hons.), NUS ) A THESIS SUBMITTED FOR THE DEGREE OF MASTER OF ENGINEERING DEPARTMENT OF ELECTRICAL AND COMPUTER ENGINEERING NATIONAL UNIVERSITY OF SINGAPORE ACKNOWLEDGMENTS I would like to take this opportunity to acknowledge the direct or indirect help of many people to complete my Master of Engineering degree in NUS and the thesis Firstly, I wish to express appreciation and gratitude to my project supervisor, Assoc Professor Zhu Chun Xiang, for his consistent guidance and encouragement I am also grateful for his patience and understanding, for giving the opportunity to learn and contribute my part to the project More importantly, he showed concern to the future plans and explain the possible scenarios on my field of research Deep felt appreciation to the following people who have rendered their help generously during the project 1) Postgraduates, Song Yan and Teo Yeow Hwee Eric, who have given me valuable advice and render their expertise to him systematically 2) Lastly, I will like to thank the staff and students of the Chemical and Biomolecular Engineering for their resources and technical support TAN YOKE PING AUGUST 2007 i TABLE OF CONTENTS ACKNOWLEDGMENTS I TABLE OF CONTENTS II SUMMARY…… IV LIST OF FIGURES V LIST OF SYMBOLS & ABBREVIATIONS XI CHAPTER INTRODUCTION .1 1.1 PROJECT BACKGROUND .1 1.2 MOORE’S LAW IN MOSFET TECHNOLOGY 1.3 CONVENTIONAL FLOATING GATE MEMORY 1.4 EMERGING TECHNOLOGIES FOR MEMORY DEVICES 1.5 MOTIVATION OF THE PROJECT .9 1.6 THESIS OUTLINE 10 CHAPTER RESEARCH ON POLYMER MEMORY .12 2.1 BY TUNNELING MECHANISM: 12 2.2 BY CHARGE TRANSFER MECHANISM .15 2.3 BY CONFORMATIONAL CHANGE MECHANISM 20 2.4 POLYMER MEMORY WORK ON SILICON SUBSTRATE .27 2.5 SUMMARY… .30 CHAPTER EXPERIMENTAL SETUP FOR SILICON-BASED POLYMER MEMORY BASED ON PF6EU .33 3.1 PURPOSE OF RECTIFYING PERFORMANCE 33 3.2 EXPERIMENTAL WORK .35 3.2.1 OHMIC CONTACT 35 ii 3.2.2 SYNTHESIS OF POLYMER SOLUTION .38 3.2.3 FABRICATION OF DEVICE: AL/PF6EU (DBM)/N-TYPE SILICON SUBSTRATE .42 3.2.4 TEST SETUP FOR MEMORY PERFORMANCE 44 CHAPTER ELECTRICAL PERFORMANCE FOR SILICON-BASED POLYMER MEMORY BASED ON PF6EU 45 4.1 MEMORY DEVICE BASED ON N-TYPE SILICON SUBSTRATES 45 4.1.1 MEMORY PERFORMANCE CHARACTERISTICS (N-TYPE SILICON SUBSTRATE) 45 4.1.2 CONDUCTION MECHANISMS ON N-TYPE SILICON SUBSTRATES .51 4.1.3 COMPARISON STUDY ON DIFFERENT TOP ELECTRODES 54 4.2 MEMORY DEVICE BASED ON P-TYPE SILICON SUBSTRATES 55 4.2.1 MEMORY PERFORMANCE CHARACTERISTICS (P-TYPE SILICON SUBSTRATE) 55 4.2.2 CONDUCTION MECHANISMS ON P-TYPE SILICON SUBSTRATES .58 4.3 MECHANISM FOR CONDUCTANCE CHANGE .62 4.3.1 CHARGE POLARONS .62 4.3.2 ELECTRO-CHEMICAL CHARACTERIZATION OF POLYMER FILM 63 4.3.3 SIMULATION RESULTS ON POLYMER FILM 67 CHAPTER CONCLUSION AND RECOMMENDATION .70 5.1 ACCOMPLISHMENT OF THE PROJECT 70 5.2 IMPLICATIONS OF SILICON-BASED POLYMER MEMORY DEVICES .71 5.3 SUGGESTION FOR FUTURE WORKS .71 REFERENCES… 74 APPENDIX…… .77 iii SUMMARY The thesis focuses on a novel memory device structure incorporating polymer film as the switching medium in memory devices, contrary to the conventional floating gate memory In my work, an attempt was made to fabricate memory devices on silicon substrates using polymer film as the switching element Electrical tests are performed on the devices to access their switching performances and retention stability, which include: voltage sweep test, constant voltage stress test and read pulse cycles test Chemical tests such as ultraviolet absorption spectrum and cyclic voltammetry tests are also conducted to access the redox potential and energy levels of the polymer They mainly serve to provide a better understanding of material properties In addition, a simulation based on density-functional theory is conducted and the result is used to account for the conductivity changes Lastly, various metals with different workfunctions are used as the top electrodes to provide a better understanding of the switching behavior Curve fitting models are also plotted to obtain an agreement about the conduction mechanisms with the electrical testing data The feasibility of integration of polymer film on silicon substrates is also discussed Lastly, suggestion for future work is given Keywords: heterojunction, polymer, rectifying iv LIST OF FIGURES FIGURE 1.1: CLASSIFICATION OF MEMORY TYPES FIGURE 1.2: ENERGY BAND DIAGRAM OF THE FLOATING GATE STRUCTURE FIGURE 1.3: EMERGING TECHNOLOGY FOR MEMORY DEVICES FIGURE 2.1: STRUCTURE OF SANDWICHED MEMORY DEVICE [5] 13 FIGURE 2.2: ENERGY DIAGRAM FOR OPERATING MECHANISM OF MEMORY DEVICE [5] 14 FIGURE 2.3: COMPARISON OF I-V CURVES OF FRESH OBD (FILLED DIAMOND) AND PRE BIASED (OPEN CIRCLES) OBD [5] 15 FIGURE 2.4: MOLECULAR STRUCTURE OF PF8EU [8] 16 FIGURE 2.5: DEVICE STRUCTURE OF FABRICATED MEMORY DEVICE [8] 17 FIGURE 2.6: J-V PERFORMANCE OF MEMORY DEVICE WITH THE ON/OFF CURRENT RATIO [8] 18 FIGURE 2.7: READ PULSE CYCLE OF AL/PF8EU/ITO DEVICE IN THE OFF AND ON STATES [8] 18 FIGURE 2.8: CONSTANT STRESS OF AL/PF8EU/ITO DEVICE IN THE OFF AND ON STATES [8] 19 FIGURE 2.9: CHARGE TRANSFER MECHANISMS BY I-V CURVE FITTING [8] 20 FIGURE 2.10: MOLECULAR STRUCTURE OF A) (I) PCZ AND (II) PVK B) DEVICE STRUCTURE [11] 21 FIGURE 2.11: SWITCHING PERFORMANCE OF AL/PCZ/ITO DEVICE [11] 22 v FIGURE 2.12: J-V CHARACTERISTICS USING PVK AS ACTIVE LAYER [11] 23 FIGURE 2.13: TIME DEPENDENT STRESS TEST IN THE ON AND OFF STATES AT -1V [11] 24 FIGURE 2.14: CURVE FITTING OF DEVICE IN A) OFF AND B) ON STATES [11] 24 FIGURE 2.15: ENERGY BAND DIAGRAM OF THE MEMORY DEVICE[11] 26 FIGURE 2.16: X-RAY DIFFRACTION PATTERNS OF PVK AND PCZ AT GROUND STATE [11] 26 FIGURE 2.17: QUASISTATIC SWITCHING OF DEVICES BASED ON SILICON SUBSTRATES [12] 28 FIGURE 2.18: J-V CHARACTERISTICS OF AU/PEDOT: PSS/N-SI [12] 28 FIGURE 2.19: TRANSIENT CURRENT RESPONSE FOR A AU/PEDOT: PSS/N-SI DEVICE[12]29 FIGURE 2.20: ENERGY BAND DIAGRAM OF THE DEVICES BASED ON N AND P SILICON SUBSTRATES [12] 30 FIGURE 3.1: PASSIVE MATRIX CIRCUITS WITH DIODE-LIKE CELL 34 FIGURE 3.2: I-V CHARACTERISTICS ON BARE SILICON WAFERS 36 FIGURE 3.3 (A): I-V CHARACTERISTICS OF AL/N-SI/AL STRUCTURE 37 FIGURE 3.3 (B): I-V CHARACTERISTICS OF AU/P-SI/AU STRUCTURE 38 FIGURE 3.4(A): SYNTHESIS OF EUROPIUM TRIISOPROPOXIDE FROM ANHYDROUS EUROPIUM CHLORIDE [14] 39 FIGURE 3.4(B): SYNTHESIS OF COPOLYMERS WITH ACTIVE CARBOXYLIC LIGANDS VIA SUZUKI REACTION AND SUBSEQUENT HYDROLYSIS PROCESS [14] 40 vi FIGURE 3.4(C): FORMATION OF COPLYMERS WITH EUROPIUM COMPLEXES VIA CHELATION [14] 41 FIGURE 3.5:FULL CHEMICAL STRUCTURE OF 9, 9-DIHEXYFLUORENE AND EUCOMPLEXED PF6EU (DBM), 10MG/ML, X: Y = 11 : 42 FIGURE 3.6(A): DEVICE STRUCTURE 43 FIGURE 3.6(B): VACUUM EVAPORATOR 43 FIGURE 4.1: I-V CHARACTERISTICS OF SILICON BASED MEMORY DEVICE WITHOUT BACK METALLIC CONTACT 46 FIGURE 4.2: READ PULSE CYCLES TEST OF THE DEVICE 47 FIGURE 4.3: I-V CHARACTERISTICS OF SILICON BASED MEMORY DEVICE WITHOUT BACK METALLIC CONTACT 47 FIGURE 4.4: FULL I-V CHARACTERISTICS OF THE DEVICE (INSET SHOWS THE CURRENT DEPENDENCE ON THE CONTACT AREA) 48 FIGURE 4.5: READ PULSE TEST AT OFF AND ON STATES 50 FIGURE 4.4: READ CYCLES PULSE TEST 50 FIGURE 4.6: TIME DEPENDENT STRESS TEST 50 FIGURE 4.7(A): CURRENT-VOLTAGE CURVE SHOWING THERMIONIC EMISSION FOR ASFABRICATED AT FORWARD BIAS (OFF STATE) 52 FIGURE 4.7(B): CURRENT-VOLTAGE CURVE OF THE TURNED-ON DEVICE SHOWING DIODE CHARACTERISTICS AT LOW FORWARD BIAS 52 vii Chapter Electrical performance for silicon-based polymer memory based on PF6Eu The conduction is poor, under the first positive sweep, as current is dependent on the injected carriers which is able to surmount the large barriers at the contacts with an external bias However, since Fluorene moiety and Europium-complexes are electron donors and acceptors respectively, they become charged when subjected to sufficient electric field and radical ion pairs of charged PF6+ (cations) and Eu-complex (anions) are formed Effectively, an electron from the fluorene moiety is donated to the Eucomplex to string a doped (positively charged) conjugated backbone state The charged defects that could be formed when polymers are ionized by an electron acceptor are termed radical cations21 It is reported that organic molecules tend to adopt equilibrium geometry of the ionized state This causes a distortion which will lead to an upward shift in HOMO level and downward shift in LUMO level, as illustrated by the dotted lines shifts in Figure 4.16 Report of PEDOT polymer after doped (charged) has seen similar trends.12 As such, once PF6 is doped positively, its HOMO and LUMO levels will shift towards midgap, leading to a decrease in barrier height at both contacts Hence, when a positive voltage is applied between the electrode and n-type silicon, the device will be forward biased, and the majority carriers (electrons) of the substrate will dominate the conduction path As a result, an exponentially increase in current with voltage is obtained At higher positive voltages, the forward current will be larger so that the current will be limited by SCLC If the forward current is high enough, the substrate resistance of Si substrate will limit the current and becomes more ohmic in nature 66 Chapter Electrical performance for silicon-based polymer memory based on PF6Eu Figure 4.16: HOMO and LUMO energy level for fluorene moiety of PF6Eu along with work function of top aluminum electrode and silicon substrate 4.3.3 Simulation results on polymer film In order to access the trend of HOMO and LUMO energy levels of the charged polymer film, a simulation study based on the density functional theory was conducted to obtain the energy levels as an indirect means to assess the HOMO and LUMO energy levels of the fluorene moiety in its charged states The HOMO and LUMO levels of the uncharged states of the fluorene moiety were also simulated for comparison Throughout the simulation, the energy levels of the respective HOMO and LUMO are evaluated each time as the number of fluorene moiety is increased from unity From Figure 4.17, it can be seen that the bandgap of the fluorene moiety 67 Chapter Electrical performance for silicon-based polymer memory based on PF6Eu is significantly reduced after it is charged Such phenomenon is observed for all simulated units of fluorene moiety (comparing charged and uncharged states) As the number of fluorene moiety increases, the simulated results also show that the shift in the HOMO and LUMO levels are towards the midgap Stimulation code can be referred in the Appendix provided The transition of the device from OFF state to ON state is permanent With respect to radical-ion compounds, in electrochemical terms, the interconversions of the system of neutral molecule and charged states are characterized by redox potentials The stability constant (K) of the radical anions can be estimated from the onset potentials of the first and second reduction peaks in the Cyclic Voltammetry curve: lg K = E red − E red = 13.6 ,22 indicating that the radical anions are stable The high 0.059 stability of the radical anion will help to preserve the doped state of the backbone to maintain the overall charge neutrality of the polymer film Besides, stable cations can be formed in oligofluorene structures and oxidation is found not reversible at increasing electrode potentials.23 Coupled with sufficient delocalization of the charge24 in fluorene moiety, more stringent conditions may be required to uncharge the doped conjugated backbone back to its intrinsic state 68 Chapter Electrical performance for silicon-based polymer memory based on PF6Eu -1 -2 Energy (eV) charged (calculated) charged (calculated) -3 uncharged (calculated) uncharged (calculated) -4 -5 -6 -7 No of F moiety Figure 4.17: Simulation of fluorene moiety in its charged and uncharged states based on density functional theory 69 Chapter Conclusion and recommendation CHAPTER CONCLUSION AND RECOMMENDATION In this chapter, a summary of the simulation is given, followed by the implications, advantages and disadvantages of polymer memory compared to its conventional silicon counterparts (floating gate memory) Finally, suggestions for future improvement will be included 5.1 Accomplishment of the project The objective of the project is to examine the possibility of fabricating polymer memory devices based on silicon substrate and access its performance As far as possible, the fabrication steps are made to be simpler and less time consuming as compared to the process steps of making a floating gate memory Ultimately, based on this research work conducted, it remains promising that silicon substrate is a feasible candidate as a substrate in polymer memory devices The experimental results have shown that rectifying performance can be achieved in organic-inorganic heteorojunction devices on both N- and P-type silicon substrates However, due to its complexity, the fabrication of passive matrix array will require much more stringent process steps in order to fully demonstrate the capability of rectifying effects in matrix cells 70 Chapter Conclusion and recommendation 5.2 Implications of silicon-based polymer memory devices Based on my account, the process steps of fabricating polymer memory device are definitely simpler and less costly As mentioned in chapter 2, since most of the polymer devices reported are mainly two-terminal devices, it will have a much simpler integration scheme, flexibility, better scalability, with low cost potential which will lead to a higher device density Normally, low cost substrates, such as glass, plastics or metal foils are used for its fabrication The main challenge is to enhance the quality of the polymer film However, when dealing with polymer memory devices, the yield of functional devices often falls short of expectations Normally, for each batch of devices, the highest yield obtained is less than 50% Also, the quality of the polymer film after each process step may drop due to contamination since particles may seep into polymer film during the spin coating process As such, it will be a huge challenge to obtain a thorough understanding of the integrated device and improve the yield of each fabrication step to promote it to commercial line eventually 5.3 Suggestion for future works Currently, flash-type memory device based on silicon substrate has yet to be reported Thus, it remains promising and provides great research value to fabricate a memory device which is able to show dual states (reversible) and rectified I-V property 71 Chapter Conclusion and recommendation A self-proposed model, based purely on the theoretical aspects of the device structure and polymer electrical performance is as such: Assuming the polymer film is able to transit from a low/high state to a high/low state under a certain voltage direction sweep and is also able recover its initial state under voltage sweep of opposite polarity across metal electrodes Al (1) Polyme r Nickel/Copper (2) N-Si Al (3) Figure 5.1 Proposed 3-terminal device structure The proposed scheme is requires a diode-like structure based on metal-Si junction (Figure 5.1) As such, the polymer in its high conductance state can be treated as a low-value resistor while the polymer in its low conductance state can be treated as an insulator Since it is ideal to confine electric field between metal electrodes across the polymer film, a flash type memory with rectified property can be achieved Probing and 3: To assess the diode-like property of the structure (rectified property can be observed-main function) Probing 1and 2: To confine the electric field efficiently within the polymer film (switch it back to its initial state- main function) 72 Chapter Conclusion and recommendation However, a well and stable polymer film needs to be developed and the fabrication steps needs to be optimized 73 References REFERENCES Chenming Hu, “SOI and Device Scaling”, Proceedings 1998 IEEE International SOI Conference, (1998) International Roadmap Committee, “International Technology Roadmap for Semiconductors Update 2006”, European Semiconductor Industry Association Q.D Ling, Y Song, S J Ding, C Zhu, D.S.H Chan, D.L Kwong, E.T Kang, and K.G Neoh, “A Non-volatile Polymer Memory Device Based on a Novel Copolymer of N-Vinylcarbazole and Eu-complexed Vinylbenzoate” Adv Mater., 17, 455 (2005) J.H.A Smits, S.C.J Meskers, R.A.J Janssen, A.W Marsman and D.M de Leeuw, “Electrically rewritable memory cells from poly(3-hexylthiophene) schottky diodes” Adv Mater., 17, 1169 (2005) L.P Ma, S Pyo, J Ouyang, Q Xu and Y Yang, “Nonvolatile electrical bistability of organic/metal-nanocluster/organic system” Appl Phys Lett., 82, 1419 (2003) J Ouyang, C.W Chu, 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Zhu, “Non-volatile WORM memory device based on an acrylate polymer with electron donating carbazole pendant groups” Organics Electronics, 7, 173 (2006) 12 S Smith and S.R Forrest, “A Low switching volatge organic-on-inorganicheterojunction memory element utilizing a conductive polymer fuse on a doped silicon substrate” Appl Phys Lett., 84, 5019 (2004) 13 D.K Schroder, Semiconductor material and device characterization, p 128129, IEEE press 14 Q.D Ling, E.T Kang, K.G Neoh and Wei Huang, “Synthesis and Nearly Monochromatic Photoluminescence Properties of Conjugated Copolymers Containing Fluorene and Rare Earth Complexes” Macromolecules, 36, 6995 (2003) 15 P.W May, M.-T Kuo and M.N.R Ashfold, “Field emission conduction mechanisms in chemical-vapour-deposited diamond and diamond-like carbon films” Diamond and Related Materials”, 8, 1490 (1999) 16 S Moller, C Perlov, W Jackson, C Taussig and S.R Forrest, ”A polymer/semiconductor write-once-read-many-times memory” Nature, 426, 166 (2003) 17 D Tondelier, K Lmimouni, D Vuillaume, C Fery and G Haas, ”Metal/organic/metal bistable memory devices” Appl Phys Lett., 85, 5763 (2004) 18 M Lauters, B McCarthy, D Sarid and G E Jabbour, “Multilevel conductance switching in polymer films” Appl Phys Lett., 89, 013507 (2006) 19 J L Bredas and G B Street, “Polarons, Bipolarons, and Solitons in Conducting Polymers” Acc Chem Res., 18, 309 (1985) 20 G H Gelinck, Excitons and Polarons in Luminescent Conjugated Polymers, 75 References p 6, Delft University Press, Delft _1998 21 C.K Chen and L Raimonds, Electrical properties of polymer: chemical principles, p 268, Hanser Publishers (1987) 22 V Khodorkovsky and J Y Becker, Organic Conductors: Fundamentals and Applications, p 79, Marcel Dekker, Inc., New York (1994) 23 C.Y Chi and G Wegner, “Chain-Length Dependence of the Electrochemical Properties of Conjugated Oligofluorenes” Macromol Rapid Commun., 26, 1532 (2005) 24 Y H Yan, Z An, and C Q Wu, “Dynamics of polaron in a polymer chain with impurities” Eur Phys J B, 42, 157 (2004) 25 Q.D Ling, Y Song, S.L Lim, Eric Y.H Teo, Y.P Tan, C.X Zhu, E.T Kang and K.G Neoh, “A Dynamic Random Access Memory Based on a Conjugated Copolymer Containing Electron-Donor and –Acceptor Moieties”, Angew Chem Int Ed., 45, 2947 (2006) 76 Appendix APPENDIX Input file for gauss view simulation (1 unit of fluorene moiety) %chk=1F+.chk %mem=256Mb %nproc=3 #p rob3lyp/6-31g(d) opt freq geom=connectivity test Charged Fluorene1 12 C C C C C C H H H H C C C C C C C H H H H C H H H C H H H B1 11 12 13 14 15 16 13 14 15 16 11 22 22 22 11 26 26 26 B1 B2 B3 B4 B5 B6 B7 B8 B9 B10 B11 B12 B13 B14 B15 B16 B17 B18 B19 B20 B21 B22 B23 B24 B25 B26 B27 B28 2 11 12 13 14 15 12 13 14 15 11 11 11 11 11 11 A1 A2 A3 A4 A5 A6 A7 A8 A9 A10 A11 A12 11 A13 12 A14 13 A15 14 A16 11 A17 12 A18 13 A19 14 A20 A21 A22 A23 A24 A25 A26 A27 D1 D2 D3 D4 D5 D6 D7 D8 D9 D10 D11 D12 D13 D14 D15 D16 D17 D18 D19 D20 D21 D22 D23 D24 D25 D26 1.41599179 77 Appendix B2 B3 B4 B5 B6 B7 B8 B9 B10 B11 B12 B13 B14 B15 B16 B17 B18 B19 B20 B21 B22 B23 B24 B25 B26 B27 B28 A1 A2 A3 A4 A5 A6 A7 A8 A9 A10 A11 A12 A13 A14 A15 A16 A17 A18 1.40933633 1.34808555 1.38275648 1.34673396 1.07000000 1.07000000 1.07000000 1.07000000 1.54917500 1.54908678 1.34836666 1.40932652 1.41571386 1.40772943 1.34676157 1.07000000 1.07000000 1.07000000 1.07000000 1.54000000 1.07000000 1.07000000 1.07000000 1.54000000 1.07000000 1.07000000 1.07000000 119.95949109 117.97713873 121.82355726 122.64069850 120.08189758 120.02028014 121.01126546 121.13321491 127.83451227 102.14986896 127.90370453 118.03427609 119.96756946 119.81908807 117.74579678 120.98279976 120.01620358 120.09044570 78 Appendix A19 A20 A21 A22 A23 A24 A25 A26 A27 D1 D2 D3 D4 D5 D6 D7 D8 D9 D10 D11 D12 D13 D14 D15 D16 D17 D18 D19 D20 D21 D22 D23 D24 D25 D26 121.12677974 112.58384395 109.47122063 109.47122063 109.47122063 109.37364076 109.47122063 109.47122063 109.47122063 -0.19890558 1.55475744 -2.14654149 179.42512220 179.39131399 179.92028971 -178.91478709 -179.34776797 -177.50951102 -177.32764828 178.62623598 -0.67896547 -0.77035771 0.38458418 -1.48734971 179.31256956 179.33975438 -179.49226204 63.68542824 176.71105879 -63.28894121 56.71105879 -61.12263941 64.64922488 -175.35077512 -55.35077512 1.5 1.5 1.0 1.5 1.0 2.0 1.0 1.5 11 1.0 2.0 17 1.0 10 1.0 79 Appendix 10 11 12 1.0 22 1.0 26 1.0 12 13 2.0 17 1.5 13 14 1.5 18 1.0 14 15 1.5 19 1.0 15 16 1.5 20 1.0 16 17 2.0 21 1.0 17 18 19 20 21 22 23 1.0 24 1.0 25 1.0 23 24 25 26 27 1.0 28 1.0 29 1.0 27 28 29 80 [...]... the memory device will change its state from state ‘0’ to state ‘1’ Depending on its storage mechanisms and electrical characteristics, memory devices can generally be classified into 2 types: non- volatile and volatile memory Figure 1.1 shows the hierarchy of the memory system 1 In non volatile memory devices, information stored can still be retained even when no external power is applied Non volatile. .. present silicon- based floating gate memory is elaborated, with the pros and cons of the device performance highlighted Polymer 10 memory device is subsequently introduced as a replacement to silicon- based floating gate memory It also presents the different types of memory device currently in the market The common performance indicators of the memory devices will be highlighted and discussed in proper... to non- volatile memories, volatile memories require power in order to retain the stored information It can also be further classified into dynamic random access memory (DRAM) or static random access memory (SRAM) In DRAMs, the written data can only be maintained by refreshing pulses applied periodically When external stimulus is removed, the DRAM will lose its data over time In SRAMs, the memory device... Figure 2.4: Molecular structure of PF8Eu [8] 16 Chapter 2 Literature Review Figure 2.5: Device structure of fabricated memory device [8] The switching performance of the device is shown in Figure 2.6 Initially, the current increases with voltage At around +3V, a sudden increase in current density indicates switching After switching, it is found that the device can retain its ON state Applying a negative... project Being novel devices in the market, a number of polymer memory research works are covered and categorized accordingly A summary table is provided to consolidate the research findings to provide a better understanding of present state of art of polymer memory Chapter 3 concentrates on the prospect of building a polymer memory device based on silicon substrates The motivation of using an organic-inorganic... These are stated in the International Technology Roadmap for Semiconductors (ITRS)2 to ensure the continuity of Moore’s law by realizing the roadmap and specifications As such, the current CMOS technology in memory device should reach a bottleneck stage and alternatives need to be explored 4 1.3 Conventional floating gate memory The conventional floating gate memory device is based on silicon substrates... dependent on them In these digital devices, the key feature which governs its functionality is its memory component Put it simply, a memory device, is an electronic holding place for instructions and data where more than one conductivity state can be assessed In its pristine state (no information is stored), the memory component can be conventionally referred to as in state ‘0’ Once information is inputted... endurance/performance etc In polymer memory devices, data is stored based on the polymer’s electronic and chemical properties Most of the polymer devices reported are mainly two-terminal devices It has a simple integration scheme, flexible, with good scalability, low cost potential and low operating voltage Besides, high density can be achieved mainly due to the simple structure of device In the various proposed memory. .. on organic materials have been reported,3,4 including rewritable type and write-once-read-many-times (WORM) type memory devices Polymer memory could potentially store far more data than other non- volatile alternatives Several advanced deposition methods have been proposed in the field of polymer memory, such as ink-jet printing, which is capable of forming micro-meter high polymer wall with good precision... conventional floating gate memory structure 9 Thus, it is of immense value to explore the potential of forming passive matrix circuits by incorporating polymer film with silicon substrate for memory devices with rectifying properties The polymer material role is to achieve bistable states under external stimulus while the silicon substrate serves to achieve the rectifying I-V characteristics Thus, the main challenge ...Spine NON- VOLATILE MOLECULAR MEMORY IN SILICON IC APPLICATION TAN YOKE PING 2007 NON- VOLATILE MOLECULAR MEMORY IN SILICON IC APPLICATION TAN YOKE PING ( B.Eng (Hons.), NUS... novel memory device structure incorporating polymer film as the switching medium in memory devices, contrary to the conventional floating gate memory In my work, an attempt was made to fabricate memory. .. Conventional floating gate memory The conventional floating gate memory device is based on silicon substrates It comprises of a floating gate (made of polysilicon) sandwiched between two silicon dioxide

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