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High Transport Si/SiGe Heterostructures for CMOS Transistors with Orientation and Strain Enhanced Mobility

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SUMMARY We have demonstrated high mobility MOS transistors on high quality epitaxial SiGe films selectively grown on Si (100) substrates. The hole mobility enhancement afforded intrinsically by the SiGe channel (60%) is further increased by an optimized Si cap (40%) process, resulting in a combined∼100% enhancement over Si channels. Surface orienta-tion, channel direcorienta-tion, and uniaxial strain technologies for SiGe channels CMOS further enhance transistor performances. On a (110) surface, the hole mobility of SiGe pMOS is greater on a (110) surface than on a (100) surface. Both electron and hole mobility on SiGe (110) surfaces are further enhanced in a110 channel direction with appropriate uniaxial channel strain. We finally address low drive current issue of Ge-based nMOSFET. The poor electron transport property is primarily attributed to the intrinsi-cally low density of state and high conductivity effective masses. Results are supported by interface trap density (Dit) and specific contact resistivity

c).

key words: high transport, SiGe, orientation, strain, heterostructure

1.

Introduction

Strained Si channel CMOS technology has successfully

ex-tended device performance along the roadmap.

Enhance-ments have been more significant when combined with

high-k gate dielectric and metal gate technology. High

mo-bility alternative channels continue on the high performance

roadmap, where highly scaled Si channel CMOS has

limi-tations [1]–[3]. SiGe and other high mobility channels

po-tentially provide high injection velocity to achieve projected

high performance metrics.

Ge-based channel pMOSFETs fabricated on high

qual-ity epitaxial films selectively grown on Si (100) substrates

exhibit enhanced hole mobility. With a Si cap processed

on Ge channels, high-k gate dielectrics exhibited low C-V

hysteresis, interface trap density, and gate leakage current,

which are comparable to gate stack on Si channels [4]. The

mobility enhancement a

fforded intrinsically by the Ge

chan-nel is further increased by a Si cap process [5].

To enhance mobility in nMOS and pMOS, dual

chan-nel materials (Ge for pMOS or III-V for nMOS) or hybrid

Si surface orientation approaches have been demonstrated

[6]; however, they might increase integration complexity.

For a practical approach, the integration of high mobility

CMOS transistors on a single channel is preferable. While

Manuscript received September 1, 2010.

Manuscript revised December 28, 2010.

The authors are with SEMATECH, 2706 Montopolis Drive,

Austin TX 78741, USA.

††

The author is with Chungnam National University, Korea.

a) E-mail: [email protected]

DOI: 10.1587/transele.E94.C.712

Fig. 1 HR-XTEM of gate stack with Si cap, high-k, and metal gates on epitaxial Ge layers selectively grown on Si (100) substrates.

the mobility enhancement for Ge pMOSFETs has been well

reported, few studies have been able to improve Ge

nMOS-FET mobility after optimizing the gate stack and parasitic

resistance.

Recently, enhanced electron mobility of Ge

nMOSFETs was demonstrated in long channel transistors.

[7]–[9].

2.

Device Fabrication

High quality epitaxial SiGe channels are selectively grown

on shallow trench isolation-formed Si substrates. A Si cap

layer is deposited to improve the interface characteristics

and off-state current as shown in earlier report [10]. The

Si cap process mitigates the low potential barrier issues of

SiGe channels, which are major causes of the high off-state

current of small bandgap energy SiGe pMOSFETs. ALD

Hf-based gate oxide is deposited followed by the metal gate.

The TEM image (Fig. 1) shows a high-k gate dielectric and

metal gate fabricated on a SiGe-on-Si substrate.

3.

Results and Discussion

Figure 2 compares C-V curves of SiGe MOS capacitors

(25% and 40% Ge). EOT of 13.6 Å and 14.0 Å were

ex-tracted using CVC model from 25% and 40% Ge

capac-itors, respectively.

The physical thickness of HfSiO

2

is

40 Å. Minimal C-V hysteresis at 1 MHz was measured to

Copyright c

 2011 The Institute of Electronics, Information and Communication Engineers

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Fig. 2 C-V of SiGe MOS capacitors with low EOT and minimal hysteresis. Gate leakage current density (Jg) of HfSiO2dielectric on SiGe channel pMOSFETs.

Fig. 3 Gm enhancement afforded intrinsically by the SiGe channel (Ge=25%) is further increased by an optimized Si cap, resulting in a com-bined∼100% enhancement over Si channels.

be

10 mV (25% Ge) and ∼20 mV (40% Ge). Slightly high

C-V stretch-out was observed with 40% Ge, due to

inter-face charge density. Gate leakage current densities (J

g

) of

HfSiO

2

dielectrics on SiGe channels were lower than SiO

2

on Si channel devices by more than 3

× 10

2

times and

com-parable with optimized HfSiO

2

dielectrics on Si channels.

Mobility enhancement was supported in the

transcon-ductance (Gm) results in Fig. 3. SiGe channels (Ge=25%)

without a Si cap (EOT=14.1) exhibited ∼60% Gm

enhance-ment over the Si channels (EOT=13.2). After applying the

Si cap process (deleted) on SiGe channel (EOT

=13.4), Gm

was further enhanced by

∼40%. Therefore, a ∼100%

en-hancement was achieved by the combined SiGe channel and

Si cap processing.

For further hole mobility enhancement, we have

in-troduced a SiGe (110) surface orientation, varying

chan-nel direction, and uniaxial strain to boost the performance

of pMOS and nMOS simultaneously [11], [12].

Fig. 4

shows the available channel directions:

110, 100 for a

(100) surface; and

110, 111, 100 for a (110) surface.

It also shows MOSFETs with varying channel directions:

0

(conventional), 45

, 90

, and 135

.

For the pMOS on (100) surface (Fig. 5), the

100

di-rection enhances Gm in Si (8%) and in SiGe (18%) as

com-pared to the

110 direction. This enhancement factor

be-comes more significant for SiGe pMOS on (110) surfaces

where the

110 direction enhances Gm 60% more than

100 direction.

Finally, we address low drive current issue of Ge-based

nMOSFET. The poor electron transport property is

primar-ily attributed to high interface trap density near the

conduc-tion band edge and high series S/D resistance. In this work,

we propose the intrinsically low density of state and high

conductivity effective masses [13]. Results are supported

by interface trap density (Dit) and specific contact

resistiv-ity (ρ

c

). Figure 6. compares transconductance (Gm) of Si

and Ge channels. For Ge pMOSFETs, I

d

increases as Ge

% increases in the channel due to enhanced hole mobility

as previously reported. For Ge nMOSFETs, however, I

d

de-creases dramatically as Ge % inde-creases.

It is likely that most electrons populate the L valleys

for a (001) [110] Ge nMOSFET channel direction (Fig. 7).

Effective masses projected on the (100) plane are strongly

a

ffected by L valleys in a way that is consistent with the

Schrodinger equation. Effective masses of electrons, which

populate L valleys are large for conductivity and small for

the density of states in conventional (100) [110] channel

di-rections, resulting in low electron mobility and carrier

con-centration in Ge-based nMOSFETs.

The large conductivity effective mass and low

den-sity of state effective mass of L valleys compromise carrier

mobility and carrier concentration and, therefore, degrades

transport characteristics of (001) [110] Ge nMOSFETs The

small electron population in

Γ valleys with very small

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ef-Fig. 4 Channel directions and rotated (0◦∼135◦) MOSFETs;110 and 100 for a (100) surface and 110, 111, and 100 for a (110) surface. 2D sub-band energy diagrams: (b) SiGe (100) and (c) SiGe (110) surface.

Fig. 5 100 enhances pMOS Gm in both Si (8%) and SiGe (18%) than

110 on (100) surface. More significant gain (60%) is achieved for SiGe pMOS on (110)110.

fective mass 0.044 m

0

that contributes to bulk Ge electron

mobility may accounts for the low inversion electron

mobil-ity of Ge nMOSFETs.

The relative performance of Si and Ge MOSFETs is

in good agreement with total on-resistance (R

total

) vs. gate

length (L

g

) results. For nMOSFETs, R

total

of the Ge channel

is higher than the Si channel, resulting in low drain current

in Ge nMOSFETs. For pMOSFETs, R

total

of the Ge channel

is lower than the Si channel and enhanced transport

charac-teristics were obtained.

4.

Conclusions

Optimized Si caps reduced interface trap density and

showed minimal C-V hysteresis. Si cap processing

effec-tively suppressed the off-state current of SiGe pMOSFETs

by providing better gate control over the channel, while

en-hancing hole mobility by 40% in the SiGe channel, which

Fig. 6 ID-VGcurves of Si and Ge CMOS. Enhanced drain current of Ge

pMOSFETs. Low drain current of Ge nMOSFETs.

Fig. 7 Schematic diagram of energy valleys and constant-energy ellip-soids in (001) Ge conduction band, showing channel direction [110], [010], and [100].

resulted in a

∼100% mobility enhancement over Si

chan-nels. Carrier mobility is enhanced on a SiGe (110) surface

orientation with additive gains in the

110 channel

direc-tion. Further mobility enhancement is achieved with

uni-axial strain, suggesting sustainable process-induced strain

technology as a SiGe (110) CMOS performance booster.

Large conductivity and small density of state effective

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masses of (001) [110] Ge sub-valleys cause low mobility

and carrier concentration, resulting in low on-state current

of Ge-based nMOSFETs.

References

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[2] N. Taoka, W. Mizubayashi, Y. Morita, S. Migita, H. Ota, and S. Takagi, “Physical origins of mobility enhancement of Ge pMISFETs with Si passivation layers,” VLSI Technology, pp.80–81, 2009. [3] J. Mitard, C. Shea, B. DeJaeger, A. Pristera, G. Wang, M. Houssa, G.

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[4] J. Oh, P. Majhi, R. Jammy, R. Joe, A. Dip, T. Sugawara, Y. Akasaka, T. Kaitsuka, T. Arikado, and M. Tomoyasu, “Additive mobility en-hancement and off-state current reduction in SiGe channel pMOS-FETs with optimized Si cap and high-k metal gate stacks,” Interna-tional Symposium on VLSI-TSA, April 2009.

[5] J. Oh, P. Majhi, C.Y. Kang, and R. Jammy, “High mobility SiGe channel pMOSFETs epitaxially grown on Si (100) substrates with HfSiO2high-k dielectric and metal gate,” International Conference

on Solid State Devices and Materials (SSDM), pp.702–703, 2008. [6] M. Yang, V.W.C. Chan, K.K. Chan, L. Shi, D.M. Fried, J.H. Stathis,

A.I. Chou, E. Gusev, J.A. Ott, L.E. Burns, M.V. Fischetti, and M. Ieong “Hybrid-orientation technology (HOT): Opportunities and challenges,” IEEE Trans. Electron Devices, vol.53, p.965, 2006. [7] K. Morii, T. Iwasaki, R. Nakane, M. Takenaka, and S. Takagi,

“High performance GeO2/Ge nMOSFETs with source/drain

junc-tions formed by gas phase doping,” IEDM Tech. Dig., p.681, 2009. [8] D. Kuzum, T. Krishnamohan, A. Nainani, Y. Sun, P.A. Pianetta,

H.S.-P. Wong, and K. Saraswat, “Experimental demonstration of high mobility Ge NMOS,” IEDM Tech. Dig., p.455, 2009. [9] C.H. Lee, T. Nishimura, N. Saido, K. Nagashio, K. Kita, and A.

Toriumi, “Record-high electron mobility in Ge n-MOSFETs exceed-ing Si universality,” IEDM Tech. Dig., p.457, 2009.

[10] J. Huang, P.D. Kirsch, J. Oh, S.H. Lee, P. Majhi, H.R. Harris, D.C. Gilmer, G. Bersuker, D. Heh, C.S. Park, C. Park, H.-H. Tseng, and R. Jammy, “Mechanisms limiting EOT scaling and gate leakage cur-rents of high-k/metal gate stacks directly on SiGe,” IEEE Electron Device Lett., vol.30, no.3, pp.285–287, March 2009.

[11] J. Oh, S.-H. Lee, K.-S. Min, J. Huang, B.G. Min, B. Sassman, K. Jeon, W.-Y. Loh, J. Barnett, I. Ok, C.-Y. Kang, C. Smith, D.-H. Ko, P.D. Kirsch, and R. Jammy, “SiGe CMOS on (110) channel orienta-tion with mobility boosters: Surface orientaorienta-tion, channel direcorienta-tions, and uniaxial strain,” VLSI Technology, pp.39–40, June 2010. [12] S.E. Thompson, M. Armstrong, C. Auth, S. Cea, R. Chau, G. Glass,

T. Hoffman, J. Klaus, Z. Ma, B. Mcintyre, A. Murthy, B. Obradovic, L. Shifren, S. Sivakumar, S. Tyagi, T. Ghani, K. Mistry, M. Bohr, and Y. El-Mansy, “A logic nanotechnology featuring strained-silicon,” IEEE Electron Device Lett., vol.25, pp.191–193, 2004.

[13] J. Oh, I. Ok, C.-Y. Kang, M. Jamil, S.-H. Lee, W.-Y. Loh, J. Huang, B. Sassman, L. Smith, S. Parthasarathy, B.E. Coss, W.-H. Choi, H.-D. Lee, M. Cho, S.K. Banerjee, P. Majhi, P.H.-D. Kirsch, H.-H. Tseng, and R. Jammy, “Mechanisms for low on-state current of Ge (SiGe) nMOSFETs: A comparative study on gate stack, resistance, and orientation-dependent effective masses,” VLSI Technology, pp.238– 239, 2009.

Jungwoo Oh holds a doctorate in materi-als science and engineering from the University of Texas at Austin. He earned a master’s de-gree in materials science and engineering from POSTECH and a bachelor’s degree from Yon-sei University in Korea. He works as a Member Technical Staff within SEMATECH’s Materials & Emerging Technology Division. Dr. Oh is conducting nanoscale advanced CMOS devices using a variety of semiconductor materials and processing. Dr. Oh’s research includes system on chip integration of III-V-on-Si photonics and electronics for display, telecommunication, and energy devices.

Jeff Huang was born in Taiwan in 1975. He received the M.S. and Ph.D. degrees in the elec-tronics engineering from National Chiao Tung University, Taiwan in 2001 and 2006, respec-tively. He joined SEMATECH, Texas, USA in 2006, where he worked on the development of Front End CMOS process. He is an author or coauthor of more than 60 publications.

Injo Ok received the B.S. and M.S. de-grees in Electrical Engineering from Changwon National University, Changwon, Korea in 2000 and 2002, respectively and the Ph.D. degree in Electrical and Computer Engineering at the Uni-versity of Texas, Austin. In April 2008, he joined Sematech at Albany, Albany, NY, where he works on fabrication and characterization of III-V and SiGe FinFET transistors for 22-nm node and beyond. He has authored or coau-thored more than 47 technical papers.

Se-Hoon Lee (S’06) was born in Seoul, Korea. He received the B.S. degree in electri-cal engineering from Seoul National University, Seoul, Korea, in 2004 and the M.S. degree in electrical and computer engineering from The University of Texas at Austin, Austin, in 2007, where he is currently working toward the Ph.D. degree. From 2006 to 2010, he was a Device In-tern and a visiting Research Student with SEmi-conductor MAnufacturing TECHnology (SE-MATECH) Inc., Austin. His research interest includes heteroepitaxy of group IV semiconductor materials by chemical vapor deposition, fabrication of scaled high-mobility channel MOSFETs, and electrical characterizations on carrier transport properties and reliabil-ity of MOSFETs.

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Rajarao “Raj” Jammy graduated with a doctoral degree in Electrical Engineering from Northwestern University in November 1996. He then joined IBM’s Semiconductor Research and Development Center in East Fishkill, NY, where he worked on development of ultra-thin di-electrics, advanced doping techniques and other front end of line technologies for deep trench DRAMs. In January 2001 he was appointed as Manager of the Thermal Processes, and Surface Preparation group with additional responsibili-ties in CMP, Thin Films and Metallization in the DRAM development organization. He moved to IBM T. J. Watson Research Center in York-town Heights, NY in June 2002 to manage IBM’s efforts on high k gate dielectrics and metal gates. Between June 2005 and June 2008 he was an IBM assignee to SEMATECH as the Director of the Front End Processes Division in Austin, TX. In June 2008 he joined SEMATECH staff after the completion of his assignment from IBM. As SEMATECH staff his respon-sibilities were expanded, and he currently serves as the Vice President of Emerging Technologies. He holds more than 50 patents and is an author /co-author of over 125 publications/presentations.

Hi-Deok Lee received the B.S., M.S., and Ph.D. degrees in electrical engineering from the Korea Advanced Institute of Science and Tech-nology, Daejeon, Korea, in 1990, 1992, and 1996, respectively. In 1996, he joined the LG Semicon Company, Ltd. (currently Hynix Semi-conductor Ltd.), Chongju, Choongbuk, Korea, where he has been involved in the development of 0.35-, 0.25-, and 0.18-μm CMOS technolo-gies, respectively. He was also responsible for the development of 0.15- and 0.13-μm CMOS technologies. Since 2001, he has been with Chungnam National University, Daejeon, Korea, and now is a Professor with the Department of Electron-ics Engineering. From 2006 to 2008, he was with the University of Texas, Austin, and SEMATECH, Austin, as a Visiting Scholar. His research in-terests are in the areas of nanoscale CMOS technology and analog MOS-FET technology and their reliability physics, analysis and modeling of low frequency noise, silicide/germanide technology, and Test Element Group design. His research interests also include RF CMOS device modeling, circuit design, crosstalk, and time delay modeling of interconnection lines. Dr. Lee is a member of the Institute of Electronics Engineers of Korea.

Fig. 1 HR-XTEM of gate stack with Si cap, high-k, and metal gates on epitaxial Ge layers selectively grown on Si (100) substrates.
Fig. 2 C-V of SiGe MOS capacitors with low EOT and minimal hysteresis. Gate leakage current density (J g ) of HfSiO 2 dielectric on SiGe channel pMOSFETs.
Fig. 6 I D -V G curves of Si and Ge CMOS. Enhanced drain current of Ge pMOSFETs. Low drain current of Ge nMOSFETs.

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