Ge GAA FETs and TMD FinFETs for the Applications Beyond Si—A Review

Yao‐Jen Lee, Guang-Li Luo, Fu-Ju Hou, Min‐Cheng Chen, Chih-Chao Yang, Chang‐Hong Shen, Wen-Fa Wu, Jia‐Min Shieh, Wen‐Kuan Yeh

IEEE Journal of the Electron Devices Society · 2016 · 31 citations · 21 references

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Abstract

Two parts of work are included in this paper. In the first part, the novel Ge gate-all-around field effect transistors (GAA FETs) are introduced and discussed. Fabrication of Ge GAA FETs requires only simple top-down dry etching and blanket Ge epitaxy techniques readily available in mass production. First, a novel process to etch away the defective Ge near Ge/Si interface from epitaxial Ge grown on SOI achieves a nearly defect-free channel, good gate control triangular gate, larger effective width than rectangular fin, and have low punch-through current through the Si substrate. By dislocation removal, the defect-free Ge channel can be formed on nothing. The p-channel triangular Ge GAA FET with fin width (W <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">fin</sub> ) of 52 nm and Lg of 183 nm has I <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">on</sub> /I <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">off</sub> = 10 <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">5</sup> , SS = 130 mV/dec, and Ion = 235 μA/μm at -1 V. Next, due to the highest electron mobility (2200 cm <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sup> /Vs) on (111) Ge surface, the n-channel triangular Ge GAA FET with (111) sidewalls on Si and Lg = 350 nm shows 2 times enhanced Ion with respect to the devices with near (110) sidewalls. Electrostatic control of SS = 94 mV/dec (at 1 V) can be further improved if superior gate stack than EOT = 5.5 nm and Dit = 1×10 <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">12</sup> cm <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">-2</sup> ·eV <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">-1</sup> is used. The Ion can be further enhanced if the line edge roughness (LER) can be reduced. Second, a feasible pathway to scale the Ge MOSFET technology by using a novel diamond-shaped Ge GAA FET with four {111} facets is also reviewed. The proposed dry etching process involves three isotropic/anisotropic etching steps with different Cl <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> /HBr ratios for forming the suspended diamond-shaped channel. Taking advantages of the GAA configuration, favorable carrier mobility of the {111} surface, and nearly defect-free suspended channel, nFET and pFET with excellent performance have been demonstrated, including an I <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">on</sub> /I <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">off</sub> ratio exceeding 10 <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">8</sup> , the highest ever reported for Ge-based pFETs. The TMD FinFET devices are reviewed in the second part of this paper. The TMD FinFET channel is deposited by CVD. MoS <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> covered on Si fin and nanowire resulted in improved (+25%) I <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">on</sub> of the FinFET and nanowire FET. The PFETs also operated effectively and the N/P device V <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">th</sub> are low and matched perfectly. The proposed heterogeneous Si/TMD 3DFETs can be useful in future electronics. Furthermore, a 4 nm thin transition-metal dichalcogenide (TMD) body FinFET with back gate control is also proposed and reviewed. Hydrogen plasma treatment of TMD is employed to lower the series resistance. The 2 nm thin back gate oxide enables 0.5 V of V <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">th</sub> shift with 1.2 V change in back bias for correcting device variations and dynamically configuring a device as a high performance or low leakage device. TMD can potentially provide sub-nm thin monolayer body needed for 2 nm node FinFET.

References

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