欢迎登录材料期刊网

材料期刊网

高级检索

采用射频磁控溅射法制备Ti金属薄膜作为反应电极,结合脉冲激光沉积法在Pt/Ti/Si衬底上制备了Ti/非晶-SrTiO3-δ (STO)/Pt结构的阻变存储器件单元.器件的有效开关次数可达200次以上.利用5 mV的小电压测量处于高低阻态的器件电阻,发现在经过3.1 ×105 s以后,两种阻态的电阻值均没有明显的变化,说明器件具有较好的保持特性.器件处于高阻态和低阻态的电阻比值可达100倍以上.在9mA的限制电流下,器件的低阻态为500 Ω,有利于降低电路的功耗.氧离子和氧空位的迁移在阻变开关中起到重要的作用,界面层TiOx发挥着氧离子库的作用.阻变开关机制归因为导电细丝(Filaments)的某些部分出现氧化或者还原现象,造成导电细丝的形成和断开.

参考文献

[1] Waser R;Aono M .Nanoionics-Based Resistive Switching Memory[J].Nature Materials,2007,6:833-840.
[2] Akihito Sawa .Resistive switching in transition metal oxides[J].Materials Today,2008(6):28-36.
[3] G. I. Meijer .Who Wins the Nonvolatile Memory Race?[J].Science,2008(5870):1625-1626.
[4] Simmons J;Verderber R .New Conduction and Reversible Memory Phenomena in Thin Insulating Films[J].Proceedings of the Royal Society Series A Mathematical Physical and Engineering Sciences,1967,301(1464):77-102.
[5] Dearnaley G;Stoneham A M;Morgan D V .Electrical Phenomena in Amorphous Oxide Films[J].Reports on Progress in Physics,1970,33:1129-1191.
[6] Xia YD;He WY;Chen L;Meng XK;Liu ZG .Field-induced resistive switching based on space-charge-limited current[J].Applied physics letters,2007(2):22907-1-22907-3-0.
[7] Seo S;Lee MJ;Seo DH;Choi SK;Suh DS;Joung YS;Yoo IK;Byun IS;Hwang IR;Kim SH .Conductivity switching characteristics and reset currents in NiO films[J].Applied physics letters,2005(9):3509-1-3509-3-0.
[8] 赵冬月,刘保亭,郭哲,李曼,陈剑辉,代鹏超,韦梦祎.非晶 Ti-Al 过渡层对 Pt/Ba0.6Sr0.4TiO3/Pt电容器结构和性能的影响[J].人工晶体学报,2011(01):161-165.
[9] KRZYSZTOF SZOT;WOLFGANG SPEIER;GUSTAV BIHLMAYER;RAINER WASER .Switching the electrical resistance of individual dislocations in single-crystalline SrTiO_3[J].Nature materials,2006(4):312-320.
[10] Choi D;Lee D;Sim H et al.Reversible Resistive Switching of SrTiOx Thin Films for Nonvolatile Memory Applications[J].Applied Physics Letters,2006,88:082904.
[11] Ni M C;Guo S M;Tian H F et al.Resistive Switching Effect in SrTiO3-δ/Nb-doped SrTiO3 Heterojunction[J].Applied Physics Letters,2007,91:183502.
[12] Yan X B;Li K;Yin J et al.The Resistive Switching Mechanism of Ag/SrTiO3/Pt Memory Cells[J].Electrochemical and Solid State Letters,2010,133:H87-H89.
[13] Yan X B;Xia Y D;Xu H N et al.Effects of the Electroforming Polarity on Bipolar Resistive Switching Characteristics of SrTiO3-δ Films[J].Applied Physics Letters,2010,97:112101.
[14] Li K;Xia Y;Xu B et al.Conduction Behavior Change in Amorphous LaLuO3 Dielectrics Based on Correlated Barrier Hopping Theory[J].Applied Physics Letters,2010,96:182904.
[15] Lin CY;Wu CY;Wu CY;Tseng TY;Hu CM .Modified resistive switching behavior of ZrO2 memory films based on the interface layer formed by using Ti top electrode[J].Journal of Applied Physics,2007(9):94101-1-94101-5-0.
[16] Yang M K;Park J W;Ko T-K et al.Bipolar Resistive Switching Behavior in Ti/MnO/Pt Structure for Nonvolatile Memory Devices[J].Applied Physics Letters,2009,95:042105.
[17] Li S L;Shang D S;Li J et al.Resistive Switching Properties in Oxygen-Deficient Pr0.7Ca0.3MnO3 Junctions with Active Al Top Electrodes[J].Journal of Applied Physics,2009,105:033710.
[18] Harada T;Ohkubo I;Tsubouchi K et al.Trap-Controlled Space-Charge-Limited Current Mechanism in Resistance Switching at Al/Pr0.7 Ca0 3 MnO3 Interface[J].Applied Physics Letters,2008,92:222113.
[19] Yasushi Ogimoto;Yukio Tamai;Masashi Kawasaki;Yoshinori Tokura .Resistance switching memory device with a nanoscale confined current path[J].Applied physics letters,2007(14):143515-1-143515-3-0.
[20] Moos R;Hárdtl K H .Defect Chemistry of Donor-Doped and Undoped Strontium Titanate Ceramics between 1000 ℃ and 1400 ℃[J].Journal of the American Ceramic Society,1997,80:2549.
[21] Ikeda J A S;Chiang Y M .Space Charge Segregation at Grain Boundaries in Titanium Dioxide:I,Relationship between Lattice Defect Chemistry and Space Charge Potential[J].Journal of the American Ceramic Society,1993,76:2437.
[22] Guan W;Liu M;Long S et al.On the Resistive Switching Mechanisms of Cu/ZrO2:Cu/Pt[J].Applied Physics Letters,2008,93:223-506.
上一张 下一张
上一张 下一张
计量
  • 下载量()
  • 访问量()
文章评分
  • 您的评分:
  • 1
    0%
  • 2
    0%
  • 3
    0%
  • 4
    0%
  • 5
    0%