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(Hf,Zr)O2 offers considerable potential for next-generation semiconductor devices owing to its nonvolatile spontaneous polarization at the nanoscale. However, scaling this material to sub-5 nm thickness poses several challenges, including the formation of an interfacial layer and high trap concentration. In particular, a low-k SiO2 interfacial layer is naturally formed when (Hf,Zr)O2 films are directly grown on a Si substrate, leading to high depolarization fields and rapid reduction of the remanent polarization. To address these issues, we conducted a study to significantly improve ferroelectricity and switching endurance of (Hf,Zr)O2 films with sub-5 nm thicknesses by inserting a TiO2 interfacial layer. The deposition of a Ti film prior to Hf0.5Zr0.5O2 film deposition resulted in a high-k TiO2 interfacial layer and prevented the direct contact of Hf0.5Zr0.5O2 with Si. Our findings show that the high-k TiO2 interfacial layer can reduce the SiO2/Si interface trap density and the depolarization field, resulting in a switchable polarization of 60.2 μC/cm2 for a 5 nm thick Hf0.5Zr0.5O2 film. Therefore, we propose that inserting a high-k TiO2 interfacial layer between the Hf0.5Zr0.5O2 film and the Si substrate may offer a promising solution to enhancing the ferroelectricity and reliability of (Hf,Zr)O2 grown on the Si substrate and can pave the way for next-generation semiconductor devices with improved performance.


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Depolarization mitigated in ferroelectric Hf0.5Zr0.5O2 ultrathin films (< 5 nm) on Si substrate by interface engineering

Show Author's information Se Hyun Kim1,Younghwan Lee2,Dong Hyun Lee1,Geun Hyeong Park1Hyun Woo Jeong1Kun Yang1Yong Hyeon Cho1Young Yong Kim4Min Hyuk Park1,2,3( )
Department of Materials Science and Engineering, College of Engineering, Seoul National University, Seoul 08826, Republic of Korea
Research Institute of Advanced Materials, College of Engineering, Seoul National University, Seoul 08826, Republic of Korea
Inter-university Semiconductor Research Center, College of Engineering, Seoul National University, Seoul 08826, Republic of Korea
Pohang Accelerator Laboratory, Pohang University of Science & Technology, Pohang 790784, Republic of Korea

Se Hyun Kim, Younghwan Lee, and Dong Hyun Lee contributed equally to this work.

Abstract

(Hf,Zr)O2 offers considerable potential for next-generation semiconductor devices owing to its nonvolatile spontaneous polarization at the nanoscale. However, scaling this material to sub-5 nm thickness poses several challenges, including the formation of an interfacial layer and high trap concentration. In particular, a low-k SiO2 interfacial layer is naturally formed when (Hf,Zr)O2 films are directly grown on a Si substrate, leading to high depolarization fields and rapid reduction of the remanent polarization. To address these issues, we conducted a study to significantly improve ferroelectricity and switching endurance of (Hf,Zr)O2 films with sub-5 nm thicknesses by inserting a TiO2 interfacial layer. The deposition of a Ti film prior to Hf0.5Zr0.5O2 film deposition resulted in a high-k TiO2 interfacial layer and prevented the direct contact of Hf0.5Zr0.5O2 with Si. Our findings show that the high-k TiO2 interfacial layer can reduce the SiO2/Si interface trap density and the depolarization field, resulting in a switchable polarization of 60.2 μC/cm2 for a 5 nm thick Hf0.5Zr0.5O2 film. Therefore, we propose that inserting a high-k TiO2 interfacial layer between the Hf0.5Zr0.5O2 film and the Si substrate may offer a promising solution to enhancing the ferroelectricity and reliability of (Hf,Zr)O2 grown on the Si substrate and can pave the way for next-generation semiconductor devices with improved performance.

Keywords: ferroelectric, charge trapping, hafnia, depolarization

References(67)

[1]

Park GH, Lee DH, Choi H, et al. Emerging fluorite-structured antiferroelectrics and their semiconductor applications. ACS Appl Electron Mater 2023, 5: 642–663.

[2]

Park MH. A perspective on the physical scaling down of hafnia-based ferroelectrics. Nanotechnology 2023, 34: 202001.

[3]

Yang K, Kim SH, Jeong HW, et al. Perspective on ferroelectric devices: Lessons from interfacial chemistry. Chem Mater 2023, 35: 2219–2237.

[4]

Müller M, Efe I, Sarott MF, et al. Ferroelectric thin films for oxide electronics. ACS Appl Electron Mater 2023, 5: 1314–1334.

[5]

Noheda B, Nukala P, Acuautla M. Lessons from hafnium dioxide-based ferroelectrics. Nat Mater 2023, 22: 562–569.

[6]

Kim IJ, Lee JS. Ferroelectric transistors for memory and neuromorphic device applications. Adv Mater 2023, 35: 2206864.

[7]

Park MH, Kwon D, Schroeder U, et al. Binary ferroelectric oxides for future computing paradigms. MRS Bull 2021, 46: 1071–1079.

[8]

Mikolajick T, Slesazeck S, Park MH, et al. Ferroelectric hafnium oxide for ferroelectric random-access memories and ferroelectric field-effect transistors. MRS Bull 2018, 43: 340–346.

[9]

Mulaosmanovic H, Breyer ET, Dünkel S, et al. Ferroelectric field-effect transistors based on HfO2: A review. Nanotechnology 2021, 32: 502002.

[10]

Khan AI, Keshavarzi A, Datta S. The future of ferroelectric field-effect transistor technology. Nat Electron 2020, 3: 588–597.

[11]

Böscke TS, Müller J, Bräuhaus D, et al. Ferroelectricity in hafnium oxide thin films. Appl Phys Lett 2011, 99: 102903.

[12]

Park MH, Lee YH, Kim HJ, et al. Ferroelectricity and antiferroelectricity of doped thin HfO2-based films. Adv Mater 2015, 27: 1811–1831.

[13]

Schroeder U, Park MH, Mikolajick T, et al. The fundamentals and applications of ferroelectric HfO2. Nat Rev Mater 2022, 7: 653–669.

[14]

Park JY, Yang K, Lee DH, et al. A perspective on semiconductor devices based on fluorite-structured ferroelectrics from the materials-device integration perspective. J Appl Phys 2020, 128: 240904.

[15]

Park MH, Lee YH, Mikolajick T, et al. Review and perspective on ferroelectric HfO2-based thin films for memory applications. MRS Commun 2018, 8: 795–808.

[16]

Cheynet MC, Pokrant S, Tichelaar FD, et al. Crystal structure and band gap determination of HfO2 thin films. J Appl Phys 2007, 101: 54101.

[17]

Wilk GD, Wallace RM, Anthony JM. High-κ gate dielectrics: Current status and materials properties considerations. J Appl Phys 2001, 89: 5243–5275.

[18]
Strkalj N, Gattinoni C, Vogel A, et al. In-situ monitoring of interface proximity effects in ultrathin ferroelectrics. Nat Commun 2020, 11 : 5815.
DOI
[19]

Kuk SH, Han SM, Kim BH, et al. An investigation of HZO-based n/p-FeFET operation mechanism and improved device performance by the electron detrapping mode. IEEE Trans Electron Devices 2022, 69: 2080–2087.

[20]
Kuk SH, Han SM, Kim BH, et al. Comprehensive understanding of the HZO-based n/pFeFET operation and device performance enhancement Strategy. In: Proceedings of the 2021 IEEE International Electron Devices Meeting, 2021.
DOI
[21]

Li YL, Zhu H, Liu X, et al. Trap characteristics of hafnium oxide-based ferroelectric field-effect transistors measured by using a current transient method. Appl Phys Lett 2023, 122: 112905.

[22]

Toprasertpong K, Tahara K, Takenaka M, et al. Evaluation of polarization characteristics in metal/ferroelectric/semiconductor capacitors and ferroelectric field-effect transistors. Appl Phys Lett 2020, 116: 242903.

[23]

Gong NB, Ma TP. Why is FE–HfO2 More suitable than PZT or SBT for scaled nonvolatile 1-T memory cell. A retention perspective. IEEE Electron Device Lett 2016, 37: 1123–1126.

[24]

Pan X, Ma TP. Retention mechanism study of the ferroelectric field effect transistor. Appl Phys Lett 2011, 99: 013505.

[25]

Gong NB, Ma TP. A study of endurance issues in HfO2-based ferroelectric field effect transistors: Charge trapping and trap generation. IEEE Electron Device Lett 2018, 39: 15–18.

[26]

Chen KT, Chen HY, Liao CY, et al. Non-volatile ferroelectric FETs using 5-nm Hf0.5Zr0.5O2 with high data retention and read endurance for 1T memory applications. IEEE Electron Device Lett 2019, 40: 399–402.

[27]

Tan AJ, Liao YH, Wang LC, et al. Ferroelectric HfO2 memory transistors with high- κ interfacial layer and write endurance exceeding 1010 cycles. IEEE Electron Device Lett 2021, 42: 994–997.

[28]
Tan AJ, Pesic M, Larcher L, et al. Hot electrons as the dominant source of degradation for sub-5nm HZO FeFETs. In: Proceedings of the 2020 IEEE Symposium on VLSI Technology, 2020.
DOI
[29]

Liang YK, Wu JS, Teng CY, et al. Demonstration of highly robust 5 nm Hf0.5Zr0.5O₂ ultra-thin ferroelectric capacitor by improving interface quality. IEEE Electron Device Lett 2021, 42: 1299–1302.

[30]
Chen KT, Lee MH, Liao CY, et al. Improvement on ferroelectricity and endurance of ultra-thin HfZrO2 capacitor with molybdenum capping electrode. In: Proceedings of the 2019 Electron Devices Technology and Manufacturing Conference, 2019.
DOI
[31]

Goh Y, Hwang J, Lee YS, et al. Ultra-thin Hf0.5Zr0.5O2 thin-film-based ferroelectric tunnel junction via stress induced crystallization. Appl Phys Lett 2020, 117: 242901.

[32]

Yadav M, Kashir A, Oh S, et al. High polarization and wake-up free ferroelectric characteristics in ultrathin Hf0.5Zr0.5O2 devices by control of oxygen-deficient layer. Nanotechnology 2021, 33: 085206.

[33]

Gao ZM, Luo YB, Lyu SX, et al. Identification of ferroelectricity in a capacitor with ultra-thin (1.5-nm) Hf0.5Zr0.5O2 film. IEEE Electron Device Lett 2021, 42: 1303–1306.

[34]

Tian X, Shibayama S, Nishimura T, et al. Evolution of ferroelectric HfO2 in ultrathin region down to 3 nm. Appl Phys Lett 2018, 112: 102902.

[35]

Li T, Dong JC, Zhang N, et al. Interface control of tetragonal ferroelectric phase in ultrathin Si-doped HfO2 epitaxial films. Acta Mater 2021, 207: 116696.

[36]

Walters G, Shekhawat A, Rudawski NG, et al. Tiered deposition of sub-5 nm ferroelectric Hf1− x Zr x O2 films on metal and semiconductor substrates. Appl Phys Lett 2018, 112: 192901.

[37]

McBriarty ME, Narasimhan VK, Weeks SL, et al. Crystal phase distribution and ferroelectricity in ultrathin HfO2–ZrO2 bilayers. Phys Status Solidi B 2020, 257: 1900285.

[38]

Cheema SS, Kwon D, Shanker N, et al. Enhanced ferroelectricity in ultrathin films grown directly on silicon. Nature 2020, 580: 478–482.

[39]

Cheema SS, Shanker N, Hsu SL, et al. Emergent ferroelectricity in subnanometer binary oxide films on silicon. Science 2022, 376: 648–652.

[40]

Kim SH, Yu GT, Park GH, et al. Interfacial engineering of a Mo/Hf0.3Zr0.7O2/Si capacitor using the direct scavenging effect of a thin Ti layer. Chem Commun 2021, 57: 12452–12455.

[41]
Wagner C, Naumkin A, Kraut-Vass A, et al. NIST X-ray Photoelectron Spectroscopy Database. US Department of Commerce, 2003.
[42]

Slink WE, DeGroot PB. Vanadium–titanium oxide catalysts for oxidation of butene to acetic acid. J Catal 1981, 68: 423–432.

[43]
Moulder JF, Stickle WF, Sobol PE, et al. Handbook of X-ray Photoelectron Spectroscopy. Eden Prairie (USA): Perkin-Elmer Corporation, 1992.
[44]

Sittig C, Textor M, Spencer ND, et al. Surface characterization. J Mater Sci Mater Med 1999, 10: 35–46.

[45]

Luo XG, Li Y, Yang H, et al. Investigation of HfO2 thin films on Si by X-ray photoelectron spectroscopy, Rutherford backscattering, grazing incidence X-ray diffraction and variable angle spectroscopic ellipsometry. Crystals 2018, 8: 248.

[46]

Landers AT, Koshy DM, Lee SH, et al. A refraction correction for buried interfaces applied to in situ grazing-incidence X-ray diffraction studies on Pd electrodes. J Synchrotron Radiat 2021, 28: 919–923.

[47]

Sang XH, Grimley ED, Schenk T, et al. On the structural origins of ferroelectricity in HfO2 thin films. Appl Phys Lett 2015, 106: 162905.

[48]

Park MH, Schenk T, Fancher CM, et al. A comprehensive study on the structural evolution of HfO2 thin films doped with various dopants. J Mater Chem C 2017, 5: 4677–4690.

[49]

Lee Y, Alex Hsain H, Fields SS, et al. Unexpectedly large remanent polarization of Hf0.5Zr0.5O2 metal–ferroelectric–metal capacitor fabricated without breaking vacuum. Appl Phys Lett 2021, 118: 012903.

[50]

Lee Y, Broughton RA, Hsain HA, et al. The influence of crystallographic texture on structural and electrical properties in ferroelectric Hf0.5Zr0.5O2. J Appl Phys 2022, 132: 244103.

[51]

Hsain HA, Lee Y, Lomenzo PD, et al. Wake-up free ferroelectric hafnia–zirconia capacitors fabricated via vacuum-maintaining atomic layer deposition. J Appl Phys 2023, 133: 225304.

[52]

Engel-Herbert R, Hwang Y, Stemmer S. Comparison of methods to quantify interface trap densities at dielectric/III–V semiconductor interfaces. J Appl Phys 2010, 108: 124101.

[53]
Nicollian E, Brews J. MOS (Metal Oxide Semiconductor) Physics and Technology. John Wiley &amp; Sons, 2002.
[54]

Stancu A, Ricinschi D, Mitoseriu L, et al. First-order reversal curves diagrams for the characterization of ferroelectric switching. Appl Phys Lett 2003, 83: 3767–3769.

[55]

Mitoseriu L, Stoleriu L, Stancu A, et al. First order reversal curves diagrams for describing ferroelectric switching characteristics. Process Appl Ceram 2009, 3: 3–7.

[56]

Schenk T, Hoffmann M, Ocker J, et al. Complex internal bias fields in ferroelectric hafnium oxide. ACS Appl Mater Interfaces 2015, 7: 20224–20233.

[57]

Lomenzo PD, Richter C, Mikolajick T, et al. Depolarization as driving force in antiferroelectric hafnia and ferroelectric wake-up. ACS Appl Electron Mater 2020, 2: 1583–1595.

[58]

Toprasertpong K, Tahara K, Hikosaka Y, et al. Low operating voltage, improved breakdown tolerance, and high endurance in Hf0.5Zr0.5O2 ferroelectric capacitors achieved by thickness scaling down to 4 nm for embedded ferroelectric memory. ACS Appl Mater Interfaces 2022, 14: 51137–51148.

[59]

Park MH, Kim HJ, Kim YJ, et al. Study on the size effect in Hf0.5Zr0.5O2 films thinner than 8 nm before and after wake-up field cycling. Appl Phys Lett 2015, 107: 192907.

[60]

Zacharias M, Streitenberger P. Crystallization of amorphous superlattices in the limit of ultrathin films with oxide interfaces. Phys Rev B 2000, 62: 8391–8396.

[61]
Ma TP, Gong NB. Retention and endurance of FeFET memory cells. In: Proceedings of the 2019 IEEE 11th International Memory Workshop, 2019.
DOI
[62]

Ma TP, Han JP. Why is nonvolatile ferroelectric memory field-effect transistor still elusive. IEEE Electron Device Lett 2002, 23: 386–388.

[63]

Zaumseil P. High-resolution characterization of the forbidden Si200 and Si222 reflections. J Appl Crystallogr 2015, 48: 528–532.

[64]

Park MH, Lee YH, Kim HJ, et al. Surface and grain boundary energy as the key enabler of ferroelectricity in nanoscale hafnia-zirconia: A comparison of model and experiment. Nanoscale 2017, 9: 9973–9986.

[65]

Li T, Ye M, Sun ZZ, et al. Origin of ferroelectricity in epitaxial Si-doped HfO2 films. ACS Appl Mater Interfaces 2019, 11: 4139–4144.

[66]

Nguyen MC, Kim S, Lee K, et al. Wakeup-free and endurance-robust ferroelectric field-effect transistor memory using high pressure annealing. IEEE Electron Device Lett 2021, 42: 1295–1298.

[67]

Lyu JK, Song TF, Fina I, et al. High polarization, endurance and retention in sub-5 nm Hf0.5Zr0.5O2 films. Nanoscale 2020, 12: 11280–11287.

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Received: 29 April 2023
Revised: 20 December 2023
Accepted: 16 January 2024
Published: 13 March 2024
Issue date: March 2024

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© The Author(s) 2024.

Acknowledgements

Acknowledgements

This study was supported by the National Research Foundation (NRF) grant, funded by the Ministry of Science and Information and Communication Technology of Korea (MSIT) (Nos. 2022M3F3A2A01073562, 2020R1C1C1008193, and 2021M3F3A2A02037889). Younghwan Lee acknowledges support from the NRF grant, funded by the MSIT (No. NRF-2022R1A6A3A01086832). We would like to thank Editage (www.editage.co.kr) for editing and reviewing the English language in the manuscript. Experiments at PLS-II were supported in part by the Korean government MSIT and POSTECH.

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This is an open access article under the terms of the Creative Commons Attribution 4.0 International License (CC BY 4.0, http://creativecommons.org/licenses/by/4.0/).

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