SEMICONDUCTOR DEVICES

BE-SONOS flash memory along with metal gate and high-k dielectrics in tunnel barrier and its impact on charge retention dynamics

Sonal Jain1, Deepika Gupta2, Vaibhav Neema1 and Santosh Vishwakarma2

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 Corresponding author: Vaibhav Neema, Email: vaibhav.neema@gmail.com

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Abstract: We investigate the effect of a high-k dielectric in the tunnel layer to improve the erase speed-retention trade-off. Here, the proposed stack in the tunnel layer is AlLaO3/HfAlO/SiO2. These proposed materials possess low valence band offset with high permittivity to improve both the erase speed and retention time in barrier engineered silicon-oxide-nitride-oxide-silicon(BE-SONOS). In the proposed structure HfAlO and AlLaO3 replace Si3N4 and the top SiO2 layer in a conventional oxide/nitride/oxide(ONO) tunnel stack. Due to the lower conduction band offset(CBO) and high permittivity of the proposed material in the tunnel layer, it offers better program/erase(P/E) speed and retention time. In this work the gate length is also scaled down from 220 to 55 nm to observe the effect of high-k materials while scaling, for the same equivalent oxide thickness(EOT). We found that the scaling down of the gate length has a negligible impact on the memory window of the devices. Hence, various investigated tunnel oxide stacks possess a good memory window with a charge retained up to 87.4%(at room temperature) after a period of ten years. We also examine the use of a metal gate instead of a polysilicon gate, which shows improved P/E speed and retention time.

Key words: high-k dielectric materialsnonvolatile memorytunnel barrierretentionendurance and bandgap-engineered



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Fig. 1.  Schematics of (a) BE-SON(ONO)S,(b) BE-SON(AHO)S,(c) BE-MON(AHO)S. Work function of TiN gate and P$^{+}$-polygate are 4.7 eV and 4.4 eV,respectively.

Fig. 2.  (Color online) $I_{\rm d}$-$V_{\rm g}$ curves for BE-SON(ONO)S,BE-SON(AHO)S and BE-MON(AHO)S with gate voltage for programming and erasing condition are $+19$ V and $-18$ V respectively. Work function of polysilicon gate and TiN gate are 4.4 eV and 4.7 eV respectively.

Fig. 3.  (Color online) (a) Programming characteristics of BE-SON(ONO)S,BE-SON(AHO)S,and BE-MON(AHO)S. (b) Erasing characteristics of BE-SON(ONO)S,BE-SON(AHO)S,and BE-MON(AHO)S. Programming voltage $V_{\rm g}$ $=$ 19 V and erasing voltage $V_{\rm g}$ $=$ $-18$ V at gate length $=$ 220 nm.

Fig. 4.  (Color online) $I_{\rm d}$-$V_{\rm g}$ curves of the following engineered tunnel stacks (for 110 nm and 55 nm gate length). (a) BE-MON(AHO)S. (b) BE-SON(AHO)S. (c) BE-SON(ONO)S. Programming voltage $V_{\rm g}$ $=$ 19 V and erasing voltage $V_{\rm g}$ $=$ $-18$ V work function of polysilicon gate and TiN gate are 4.4 eV and 4.7 eV respectively.

Fig. 5.  (Color online) (a) Programming characteristics of BE-SON(ONO)S,BE-SON(AHO)S and BE-MON(AHO)S. (b) Erasing characteristics of BE-SON(ONO)S,BE-SON(AHO)S and BE-MON(AHO)S. Programming voltage applied $V_{\rm g}$ $=$ $+19$ V and erasing voltage $V_{\rm g}$ $=$ $-18$ V at scaled gate length $=$ 55 nm along with the polysilicon control gate whose work function P$^{+}$-poly $=$ 4.4 eV and metal gate TiN $=$ 4.7 eV respectively.

Fig. 6.  (Color online) Charge retention characteristics. (a) BE-SON(ONO)S,BE-SON(HNO)S,BE-SON(AHO)S at RT after 10 years for 220 nm gate length. (b) BE-SON(AHO)S at room temperature after 10 years for 110 nm and 55 nm.

Table 1.   Tunnel dielectric parameters of different high $k$ materials used in our simulation.

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Table 2.   Typical parameters of the P-channel BE-SONOS.

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    Received: 08 July 2015 Revised: Online: Published: 01 March 2016

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      Sonal Jain, Deepika Gupta, Vaibhav Neema, Santosh Vishwakarma. BE-SONOS flash memory along with metal gate and high-k dielectrics in tunnel barrier and its impact on charge retention dynamics[J]. Journal of Semiconductors, 2016, 37(3): 034002. doi: 10.1088/1674-4926/37/3/034002 S Jain, D Gupta, V Neema, S Vishwakarma. BE-SONOS flash memory along with metal gate and high-k dielectrics in tunnel barrier and its impact on charge retention dynamics[J]. J. Semicond., 2016, 37(3): 034002. doi: 10.1088/1674-4926/37/3/034002.Export: BibTex EndNote
      Citation:
      Sonal Jain, Deepika Gupta, Vaibhav Neema, Santosh Vishwakarma. BE-SONOS flash memory along with metal gate and high-k dielectrics in tunnel barrier and its impact on charge retention dynamics[J]. Journal of Semiconductors, 2016, 37(3): 034002. doi: 10.1088/1674-4926/37/3/034002

      S Jain, D Gupta, V Neema, S Vishwakarma. BE-SONOS flash memory along with metal gate and high-k dielectrics in tunnel barrier and its impact on charge retention dynamics[J]. J. Semicond., 2016, 37(3): 034002. doi: 10.1088/1674-4926/37/3/034002.
      Export: BibTex EndNote

      BE-SONOS flash memory along with metal gate and high-k dielectrics in tunnel barrier and its impact on charge retention dynamics

      doi: 10.1088/1674-4926/37/3/034002
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      • Corresponding author: Vaibhav Neema, Email: vaibhav.neema@gmail.com
      • Received Date: 2015-07-08
      • Accepted Date: 2015-08-27
      • Published Date: 2016-01-25

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