Large ferroelectric polarization of TiN/Hf0.5Zr0.5O2/TiN ...

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1 [Supplementary material] Large ferroelectric polarization of TiN/Hf 0.5 Zr 0.5 O 2 /TiN capacitors due to stress-induced crystallization at low thermal budget Si Joon Kim 1 , Dushyant Narayan 1 , Jae-Gil Lee 1 , Jaidah Mohan 1 , Joy S. Lee 1 , Jaebeom Lee 1 , Harrison S. Kim 1 , Young-Chul Byun 1 , Antonio T. Lucero 1 , Chadwin D. Young 1 , Scott R. Summerfelt 2 , Tamer San 2 , Luigi Colombo 2 , and Jiyoung Kim 1,* 1 Department of Materials Science and Engineering, The University of Texas at Dallas, 800 West Campbell Road, Richardson, Texas 75080, United States 2 Texas Instruments, 13121 TI Blvd, Dallas, Texas 75243, United States Keywords Ferroelectric random access memory, Hf0.5Zr0.5O2, Atomic layer deposition, Stress-induced crystallization, Low thermal budget process *Electronic mail: [email protected]

Transcript of Large ferroelectric polarization of TiN/Hf0.5Zr0.5O2/TiN ...

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[Supplementary material]

Large ferroelectric polarization of TiN/Hf0.5Zr0.5O2/TiN capacitors due to

stress-induced crystallization at low thermal budget

Si Joon Kim1, Dushyant Narayan1, Jae-Gil Lee1, Jaidah Mohan1, Joy S. Lee1, Jaebeom Lee1,

Harrison S. Kim1, Young-Chul Byun1, Antonio T. Lucero1, Chadwin D. Young1, Scott R.

Summerfelt2, Tamer San2, Luigi Colombo2, and Jiyoung Kim1,*

1Department of Materials Science and Engineering, The University of Texas at Dallas,

800 West Campbell Road, Richardson, Texas 75080, United States

2Texas Instruments,

13121 TI Blvd, Dallas, Texas 75243, United States

Keywords

Ferroelectric random access memory, Hf0.5Zr0.5O2, Atomic layer deposition, Stress-induced

crystallization, Low thermal budget process

*Electronic mail: [email protected]

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For the pulse write/read measurement (see Fig. S1(a)),1 a series of write and read trapezoidal

voltage pulses with a pulse width of 4 μs, a rising/falling time of 1 μs, and a delay time of 10 μs

were applied to the Hf0.5Zr0.5O2 (HZO) samples using a pulse generator (Agilent 81110A). The

subsequent voltage drop on the internal resistor of 50Ω (shunt resistor) was measured using an

oscilloscope (Tektronix DPO7104). The load current was calculated from the load voltage using

Ohm's law and the load current of each pulse was integrated over time to extract the polarization.

Figure S1(b) and (c) show an example of the pulse write/read result of the HZO sample

according to the pulse sequence.

In the write/read sequence, the write pulse is applied such that the switching and non-

switching polarization can be extracted from the read pulse. For example, applying +2.5 V write

pulse and -2.0 V read pulse can help us extract the switching polarization at -2.0 V from the read

pulse. Similarly, applying -2.5 V write pulse and -2.0 V read pulse can help us extract the non-

switching polarization at -2.0 V from the read pulse. Hence, the applied write voltage was fixed

at ±2.5 V and the read voltage varied from -2.5 V to 2.5 V with 0.1 V step as shown in Fig. S1(c).

It takes around 5 s to initialize the pulse generator and the oscilloscope between each write/read

sequence, which gives the domains sufficient time to relax. By subtracting the integrated current

values of the switching and non-switching read pulses, the real ferroelectric switching

polarization (Psw) were extracted. The slope of the integrated current values of non-switching

read pulses can be also used to extract the dielectric constant of the HZO sample as shown in Fig.

S1 and Fig. S2(a).

We can see two different slope regions in non-switching pulse write/read results (see Fig.

S2(a) inset). Therefore, two dielectric constants in two different read voltage operation regions

are extracted from non-switching pulse write/read results, respectively. The dielectric constant in

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the first region (when read voltage is much lower than coercive voltage) and the second region

(when read voltage is coercive voltage or higher) are about 45.3 and 67.2, respectively. The

dielectric constant extracted from the first region is similar to the dielectric constant obtained

from the small signal capacitance-voltage (C-V) measurement at 2.5 MV/cm (higher than

coercive field) where the ferroelectric switching effect is minimized (at a frequency of 10 kHz

with an amplitude of 50 mV using an Agilent 4284A) as shown in Fig. S2(b). Meanwhile, the

extracted dielectric constant at or above the coercive voltage is close to the maximum dielectric

constant in small signal C-V measurement at the coercive voltage. These extracted values are

shown in Table I of the manuscript.

[1] S. J. Kim, D. Narayan, J.-G. Lee, J. Mohan, J. S. Lee, J. Lee, C. D. Young, J. Kim, S. R.

Summerfelt, T. San, and L. Colombo, in Proc. 9th IEEE International Memory Workshop

(IMW), (2017).

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FIG. S1. (a) Schematic diagram of pulse write/read measurement. (b) Pulse write/read result of

the HZO sample annealed at 400°C after TiN TE deposition. (c) The sequence of pulse

write/read measurement: for example, the write voltage was fixed at ±2.5 V and the read voltage

varied (-2.0 V, -1.5 V, -0.5 V, 0.5 V, 1.5 V, and 2.0 V).

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FIG. S2. The extracted dielectric constant of the HZO sample annealed at 400°C after TiN TE

deposition from (a) non-switching pulse write/read result and (b) small signal C-V measurement.