Fabrication Tolerant Heterogeneously Integrated Lithium Niobate Modulator on Bi-Layer Silicon Nitride Using Micro Transfer Printing

The integration of Lithium Niobate (LN) on low-loss, CMOS-compatible SiN platforms combines the high Pockels effect of LN with SiN's low loss and CMOS compatibility, enabling efficient modulation and processing. Micro transfer printing (<tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mu$</tex> TP) facilitates the integration of functional materials such as LN, III-V, and BTO, enabling the creation of compact, multifunctional chips. LN-SiN Mach-Zehnder Modulators (MZMs) require long interaction lengths (in the cm range) for low-voltage operation, necessitating <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mu$</tex> TP of em-long LN coupons. These coupons should ideally cover the MZM arms, including signal and ground electrodes <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$(\sim 100\mu \mathrm{m}$</tex> wide). However, <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mu$</tex> TP of long coupons faces challenges such as limited rotational alignment accuracy, especially if the electrode incorporated on the LN coupon. Additionally, hybrid SiN-LN modulators encounter mode transition loss and reflections at the SiN-LN interface, which are typically mitigated with long tapers. However, tapering LN coupons for <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mu$</tex> TP often causes cracks and fabrication complexities [1]. This work presents design (Fig. 1(a)) and fabrication of LN-SiN modulator with simulated <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mathrm{V}\pi\mathrm{L}=3.6\mathrm{V}$</tex> -cm (Fig. 1(b)) and 3-dB bandwidth of over 100 GHz (Fig. 1(d)). The design features bi-layer SiN waveguides (750 nm and 200 nm thick) for adiabatic optical mode coupling [2], achieving ultra-low transition loss, and minimal reflection without LN tapers thereby alleviating the alignment accuracy requirement for <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mu$</tex> TP [3]. We also present the fabrication of the device, including the high-yield fabrication and <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mu$</tex> TP of LN coupons up to 1 cm long, 100 <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mu\mathrm{m}$</tex> wide.

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Published
2025-06-23
DOI
https://doi.org/10.1109/cleo/europe-eqec65582.2025.11109459
Primary Topic
Ferroelectric and Piezoelectric Materials
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article
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article

Fabrication Tolerant Heterogeneously Integrated Lithium Niobate Modulator on Bi-Layer Silicon Nitride Using Micro Transfer Printing

Kresten Yvind, Vahid Talebi, Marcello Girardi, Víctor Torres–Company et al.
Ferroelectric and Piezoelectric Materials
article

Fabrication Tolerant Heterogeneously Integrated Lithium Niobate Modulator on Bi-Layer Silicon Nitride Using Micro Transfer Printing

Kresten Yvind, Vahid Talebi, Marcello Girardi, Víctor Torres–Company, Minhao Pu, Yunhong Ding, Fabien Labbé, Yan Gao
article en

Abstract

The integration of Lithium Niobate (LN) on low-loss, CMOS-compatible SiN platforms combines the high Pockels effect of LN with SiN's low loss and CMOS compatibility, enabling efficient modulation and processing. Micro transfer printing (<tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mu$</tex> TP) facilitates the integration of functional materials such as LN, III-V, and BTO, enabling the creation of compact, multifunctional chips. LN-SiN Mach-Zehnder Modulators (MZMs) require long interaction lengths (in the cm range) for low-voltage operation, necessitating <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mu$</tex> TP of em-long LN coupons. These coupons should ideally cover the MZM arms, including signal and ground electrodes <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$(\sim 100\mu \mathrm{m}$</tex> wide). However, <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mu$</tex> TP of long coupons faces challenges such as limited rotational alignment accuracy, especially if the electrode incorporated on the LN coupon. Additionally, hybrid SiN-LN modulators encounter mode transition loss and reflections at the SiN-LN interface, which are typically mitigated with long tapers. However, tapering LN coupons for <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mu$</tex> TP often causes cracks and fabrication complexities [1]. This work presents design (Fig. 1(a)) and fabrication of LN-SiN modulator with simulated <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mathrm{V}\pi\mathrm{L}=3.6\mathrm{V}$</tex> -cm (Fig. 1(b)) and 3-dB bandwidth of over 100 GHz (Fig. 1(d)). The design features bi-layer SiN waveguides (750 nm and 200 nm thick) for adiabatic optical mode coupling [2], achieving ultra-low transition loss, and minimal reflection without LN tapers thereby alleviating the alignment accuracy requirement for <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mu$</tex> TP [3]. We also present the fabrication of the device, including the high-yield fabrication and <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mu$</tex> TP of LN coupons up to 1 cm long, 100 <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mu\mathrm{m}$</tex> wide.

Chalmers University of Technology (SE), Technical University of Denmark (DK)
Affordable and clean energy
Openalex Percentile: Top 84%
Ferroelectric and Piezoelectric Materials
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