Research on a Micro-Nano Si/SiGe/Si Double Heterojunction Electro-Optic Modulation Structure

Feng, Song; Li, Lian-bi; Xue, Bin

doi:https://doi.org/10.1155/2018/8297650

Advances in Condensed Matter Physics

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Photonics and Optoelectronics of Low-Dimensional Materials

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Research Article | Open Access

Volume 2018 | Article ID 8297650 | https://doi.org/10.1155/2018/8297650

Research on a Micro-Nano Si/SiGe/Si Double Heterojunction Electro-Optic Modulation Structure

Song Feng,^1,2Lian-bi Li ,¹and Bin Xue¹

Academic Editor: Zaiquan Xu

Received26 Oct 2017

Accepted20 Mar 2018

Published02 May 2018

Abstract

The electro-optic modulator is a very important device in silicon photonics, which is responsible for the conversion of optical signals and electrical signals. For the electro-optic modulator, the carrier density of waveguide region is one of the key parameters. The traditional method of increasing carrier density is to increase the external modulation voltage, but this way will increase the modulation loss and also is not conducive to photonics integration. This paper presents a micro-nano Si/SiGe/Si double heterojunction electro-optic modulation structure. Based on the band theory of single heterojunction, the barrier heights are quantitatively calculated, and the carrier concentrations of heterojunction barrier are analyzed. The band and carrier injection characteristics of the double heterostructure structure are simulated, respectively, and the correctness of the theoretical analysis is demonstrated. The micro-nano Si/SiGe/Si double heterojunction electro-optic modulation is designed and tested, and comparison of testing results between the micro-nano Si/SiGe/Si double heterojunction micro-ring electro-optic modulation and the micro-nano Silicon-On-Insulator (SOI) micro-ring electro-optic modulation, Free Spectrum Range, 3 dB Bandwidth, value, extinction ratio, and other parameters of the micro-nano Si/SiGe/Si double heterojunction micro-ring electro-optic modulation are better than others, and the modulation voltage and the modulation loss are lower.

1. Introduction

With the rapid development of optoelectronic technology, optoelectronic devices have entered the nano era [1, 2], and many nanotechnology has been used in silicon photonics [3–5]. The reduced size of the device can improve the utilization rate of the chip area, but also the higher performance of the device is required, and the silicon epitaxial material is selected to make optoelectronic devices with higher performance. For example, the epitaxial InP material on silicon substrate is used to fabricate laser [6], the epitaxial Ge material is used to make detector [7], the epitaxial SiGe material is used to fabricate modulator [8], and so forth. In optoelectronic integration, the electro-optic modulator is a very important device, which is responsible for the conversion of optical signals and electrical signals [9, 10]. For the electro-optic modulator, the carrier density of waveguide region is one of the key parameters. When the injected carrier density of waveguide region is greater, the change of refractive index is greater, and also the modulator is more easily modulated [11, 12]. The traditional method of increasing carrier density is to increase the external modulation voltage, but this way will increase the modulation loss and also is not conducive to photonics integration [8, 13]. So SiGe technology is one way to solve this problem in silicon photonics. Photonics Electronics Technology Research Association (PETRA) and University of Tokyo have made a high-speed and highly efficient Si optical modulator with strained SiGe layer and demonstrated highly efficient modulations of 0.67 and 0.81 V·cm for VπL at dc reverse bias voltages of −0.5 and −2 , respectively, and also demonstrated a high-speed operation of 25 Gbps for the Si-MOD at a wavelength of around 1.3 μm [14]. University of Toronto has made SiGe BiCMOS linear modulator drivers, and the measured differential gain and bandwidth are over 20 dB and 70 GHz, respectively, and is −2.5 dBm [15]. Ghent University demonstrated single-wavelength, serial and real-time 100 GB/s NRZ-OOK transmission over 500 m SSMF with a GeSi EAM implemented on a silicon photonics platform. The device was driven with 2 Vpp without 50 Ω termination, allowing a low-complexity solution for 400 GbE short-reach optical interconnects [16].

This paper presents a micro-nano Si/SiGe/Si double heterojunction electro-optic modulation structure, which can greatly improve the carrier injection concentration and decrease modulation voltage and loss. It is an ideal electro-optic modulator, which is conducive to the photonics integrated circuit miniaturization and integration and also provides a new way for the research of micro-nano optoelectronic devices based on silicon.

2. Structure and Energy Band

Based on the SOI PIN electro-optic modulation structure, a micro-nano Si/SiGe/Si double heterojunction electro-optic modulation structure is presented, which is abbreviated as Silicon/Silicon Germanium/Silicon-On-Insulator (Si/SiGe/Si-OI) structure, as shown in Figure 1. The bottom of the structure is On-Insulator (OI) material, the P+ and N+ regions in the top layer are silicon materials, and the I region is SiGe material in Figure 1. P+ region is doped by B element, and the doping concentration is 1 × 10¹⁹ cm⁻³. N+ region is doped by P element, and the doping concentration is also 1 × 10¹⁹ cm⁻³. I region is N type intrinsic SiGe, and the doping concentration is 1 × 10¹⁵ cm⁻³. In Figure 1, structure parameters are H = 220 nm, h = 50 nm, W = 400~600 nm, and the width between active region and waveguide is a variable value.

In order to facilitate comparison and analysis, two kinds of PIN modulation structures with Si and SiGe materials are established. One is the PIN modulation structure with Si based on the SOI PIN structure, which is abbreviated as SOI structure, as shown in Figure 2(a). The other is the PIN modulation structure with SiGe based on the Silicon Germanium-On-Insulator (SiGe-OI) PIN structure, which is abbreviated as SiGe-OI structure, as shown in Figure 2(b). The doping concentration and structure parameters of two structures are the same as Si/SiGe/Si double heterojunction electro-optic modulation structure.

(a)

(b)

Si/SiGe/Si-OI structure is composed of P type Si with the high doping concentration, N type SiGe with the low doping concentration, and N type Si with the high doping concentration. Capital P and N represent Wide Band Gap Semiconductor, and lowercase n represents Narrow Band Gap Semiconductor. So the PIN structure can be equivalent as a Pn heterojunction and a nN heterojunction structure, and the band diagram is shown in Figure 3 under the equilibrium state.

When the PIN structure is working, the main carriers of n region are composed of electron from the P region and hole from the N region, and the barrier height is a key parameter who can influence injection efficiency of electron and hole. After heterojunction band of Si/SiGe/Si-OI structure is analyzed, the hole barrier height of Pn heterojunction of the Si/SiGe/Si-OI structure is represented by the following formula [17]:where is the barrier height, is the Boltzmann constant, is the absolute temperature, is the intrinsic carrier concentration of silicon, is the intrinsic carrier concentration of Silicon Germanium, is the doping concentration of n region, is the doping concentration of P region, is the Ge content. Formula (1) indicates that the hole barrier height of Pn heterojunction is related to the doping concentration of P region and n region, the band gap of materials, the temperature, and the Ge content. When the temperature is constant, the lower the doping concentration of P region and n region, the lower the hole barrier height. The narrower the band gap, the higher the intrinsic carrier concentration, and the lower the hole barrier height. The bigger the Ge content, the lower the hole barrier height.

Assuming that , , and the Ge content is 0.2, so the hole barrier height of Pn heterojunction can be calculated equal to at room temperature. For SOI structure and SiGe-OI structure, the Pn junction is homojunction, and the hole barrier height can be analyzed according to the following formula [17]:where is the Fermi level of the P region and is the Fermi level of the n region. The hole barrier height of Pn homojunctions of the SOI structure can be calculated equal to , and the hole barrier height of Pn homojunctions of the SiGe-OI structure can be calculated equal to . In the same conditions, the hole barrier height of the Si/SiGe/Si-OI structure is lowest, and the hole barrier height of the SOI structure is highest. This result can be verified by Silvaco CAD software, as shown in Figure 4 [17].

(a)

(b)

(c)

The electron barrier height of nN heterojunction of the Si/SiGe/Si-OI structure can be represented by the following formula [17]:where is the carrier concentration of N region and is the carrier concentration of n region. Formula (3) indicates that the electron barrier height of the nN heterojunction of Si/SiGe/Si-OI structure is also related to the doping concentration of N region and n region, the band gap of materials, the temperature, and the Ge content. When the temperature is constant, the lower the doping concentration of N region, the lower the hole barrier height. The higher the doping concentration of n region, the lower the hole barrier height. The wider band gap of n region, the lower the intrinsic carrier concentration, and the lower the hole barrier height. The narrower the band gap of N region, the higher the intrinsic carrier concentration, and the lower the hole barrier height. The smaller the Ge content, the lower the hole barrier height.

Assuming that , , and the Ge content is 0.2, so the electron barrier height of nN heterojunction can be calculated equal to at room temperature. For SOI structure and SiGe-OI structure, the nN junction is homojunction, and the electron barrier height can be analyzed according to the following formula [17]:

The electron barrier height of nN homojunctions of the SOI structure can be calculated equal to , and the electron barrier height of nN homojunctions of the SiGe-OI structure can be calculated equal to . In the same conditions, the electron barrier height of the Si/SiGe/Si-OI structure is lowest, and the electron barrier height of the SOI structure is highest. This result can be verified by Silvaco CAD software, as shown in Figure 4.

When the forward bias voltage is set between P region and N region, the original balance between carrier diffusion motion and drift motion is broken, and the PIN device is under nonequilibrium state. Because the doping concentration of the I region is very small, the resistance is very large. The doping concentration of the P region and the N region is very large, and the resistance is very small, so the external positive bias voltage is basically born in the I region. The forward bias voltage produces an electric field opposite to the Built-in Electric Field in the I region, which weakens the intensity of the electric field in the I region and reduces the space charge, so the barrier height decreases. Because the hole barrier height of Pn heterojunction and the electron barrier height of nN heterojunction of Si/SiGe/Si-OI structure all are lower than the barrier height of SiGe-OI structure and SOI structure, so the band of Si/SiGe/Si-OI structure is flattened first under the forward bias voltage. In other words, the Si/SiGe/Si-OI structure has the higher carrier injection at the same forward bias voltage. At 1 V forward voltage, the band simulations of three type modulation structures are shown in Figure 5 [17].

(a)

(b)

(c)

3. Result Analysis

In order to verify that the Si/SiGe/Si-OI structure has better characteristics, the carrier concentration of the SOI structure, the SiGe-OI structure, and the Si/SiGe/Si-OI structure are shown in Figure 6. Figure 6(a) shows the relationship between the electron concentration and modulation voltage for three structures, and Figure 6(b) shows the relationship between the hole concentration and modulation voltage. It can be seen from Figure 6 that, with the increase of modulation voltage, the carrier concentration of three kinds of modulation structure all are gradually increased. When the modulation voltage exceeds 0.6 V, the carrier concentration of the Si/SiGe/Si-OI structure is significantly greater than the carrier concentration of the SOI structure; when the modulation voltage is greater than 0.75 V, the carrier concentration of the Si/SiGe/Si-OI structure is significantly greater than the carrier concentration of SiGe-OI structure; when the modulation voltage is up to 0.9 V, the carrier concentration of the Si/SiGe/Si-OI structure is 6 × 10¹⁸ cm⁻³, but the SOI structure and the SiGe-OI structure reach the same carrier concentration at 2 V modulation voltage; when the modulation voltage reaches 2 V, the carrier concentration of the Si/SiGe/Si-OI structure could increase to 1.5 × 10¹⁹ cm⁻³. Assuming the SOI structure and the SiGe-OI structure all work at 2 V modulation voltage, so the Si/SiGe/Si-OI structure can work only at 0.9 V modulation voltage. From that we can see the modulation voltage of electro-optic modulator effectively is reduced, and the injection efficiency of electro-optic modulator effectively is improved for the Si/SiGe/Si-OI structure.

(a)

(b)

In order to verify the correctness of the theoretical analysis and simulation results, we have made the micro-nano Si/SiGe/Si double heterojunction electro-optic modulation, as shown in Figure 7. For the modulation of the optical part, the micro-ring modulation structure is selected. Figure 7(a) shows schematic diagram of the micro-nano Si/SiGe/Si double heterojunction micro-ring electro-optic modulation, Figure 7(b) shows Laser Scanning Confocal Microscopy (LSCM) picture of device by LEXT-OLS4000, Figure 7(c) shows Scanning Electron Microscope (SEM) picture of micro-ring structure by JSM-6700F, and Figure 7(d) shows SEM of device. The waveguide width is 450 nm, the ridge waveguide height is 220 nm, the planar waveguide height is 50 nm, the gap between waveguide and micro-ring is 200 nm, the micro-ring radius is 10 μm, the doping concentration of P+ region is 1 × 10¹⁹ cm⁻³, the doping concentration of N+ region is 1 × 10¹⁹ cm⁻³, and the doping concentration of I region is 1 × 10¹⁵ cm⁻³. At the same processing conditions and device parameters, the micro-nano SOI micro-ring electro-optic modulation is also made for testing comparison.

(a)

(b)

(c)

(d)

The transmission spectrum of the micro-nano Si/SiGe/Si double heterojunction micro-ring electro-optic modulation has been tested, as shown in Figure 8. From that we can see the Free Spectrum Range (FSR) is 9.44 nm, and the 3 dB Bandwidth of the resonant peak is 0.12 nm, near the 1549 nm. The corresponding value is 12900, and the extinction ratio of the resonant peak is 11.2 dB.

At the same testing conditions, the transmission spectrum of the micro-nano SOI micro-ring electro-optic modulation has also been tested, as shown in Figure 9. From that we can see the Free Spectrum Range (FSR) is 9.41 nm, and the 3 dB Bandwidth of the resonant peak is 0.13 nm, near the 1548 nm. The corresponding value is 11900, and the extinction ratio of the resonant peak is 7.0 dB.

From the comparison of testing results between the micro-nano Si/SiGe/Si double heterojunction micro-ring electro-optic modulation and the micro-nano SOI micro-ring electro-optic modulation, we can see that Free Spectrum Range, 3 dB Bandwidth, value, extinction ratio, and other parameters of the micro-nano Si/SiGe/Si double heterojunction micro-ring electro-optic modulation are better than that of the micro-nano SOI micro-ring electro-optic modulation, and value and the extinction ratio are especially greater than that of the micro-nano SOI micro-ring electro-optic modulation.

The test result of the micro-nano Si/SiGe/Si double heterojunction micro-ring electro-optic modulation is shown in Figure 10. The forward bias voltages are 0, 1, 1.1, 1.2 V, respectively. From that we can see the resonant peak has obviously been blue-shifted after the forward bias voltage is set. When the forward bias voltage is 1 V, the value of blue-shift is 0.71 nm.

When the forward bias voltages are 0, 1.5, 1.8, 2 V, respectively, the transmission spectrum of the micro-nano SOI micro-ring electro-optic modulation has been tested, as shown in Figure 11. From that we can see the resonant peak has also obviously been blue-shifted after the forward bias voltage is set, but the modulation effect is worse than Si/SiGe/Si modulation. Only when the forward bias voltage is up to 2 V, the value of blue-shift is 0.71 nm.

From the comparison of testing results between the micro-nano Si/SiGe/Si double heterojunction micro-ring electro-optic modulation and the micro-nano SOI micro-ring electro-optic modulation, we can see that the modulation efficiency of the micro-nano Si/SiGe/Si double heterojunction micro-ring electro-optic modulation is better than that of the micro-nano SOI micro-ring electro-optic modulation at the same processing conditions and testing conditions. In other words, the modulation voltage of the micro-nano Si/SiGe/Si double heterojunction micro-ring electro-optic modulation is lower than that of the micro-nano SOI micro-ring electro-optic modulation, and the modulation power of the micro-nano Si/SiGe/Si double heterojunction micro-ring electro-optic modulation is lower too. So the testing results are consistent with previous theoretical analysis and simulation results.

4. Conclusions

This paper presents a micro-nano Si/SiGe/Si double heterojunction electro-optic modulation structure. Based on the band theory of single heterojunction, the barrier height of the new structure is quantitatively analyzed, and the formulas of barrier height are gotten using the numerical calculus and derivation. The reason of carrier injection enhancement in the new structure is analyzed. On the simulation platform, the new structure, SiGe-OI structure, and SOI structure are simulated. From the comparison of simulation results, when the modulation voltage is up to 0.9 V, the carrier concentration of the new structure is 6 × 10¹⁸ cm⁻³, but the SOI structure and the SiGe-OI structure reach the same carrier concentration at 2 V modulation voltage. Finally, the micro-nano Si/SiGe/Si double heterojunction electro-optic modulation is made and tested. Comparison of testing results between the micro-nano Si/SiGe/Si double heterojunction micro-ring electro-optic modulation and the micro-nano SOI micro-ring electro-optic modulation, Free Spectrum Range, 3 dB Bandwidth, value, extinction ratio, and other parameters of the micro-nano Si/SiGe/Si double heterojunction micro-ring electro-optic modulation are better than others, and the modulation voltage and the modulation power are lower. So, the micro-nano Si/SiGe/Si double heterojunction electro-optic modulation structure is an ideal device structure to replace the traditional SOI and SiGe-OI electro-optic modulators structure.

Conflicts of Interest

The authors declare that they have no conflicts of interest.

Acknowledgments

This work was financially supported by National Natural Science Foundation of China (Grant no. 61204080), Natural Science Foundation of Shaanxi Province of China (Grant no. 2017JM6075), Foundation of Shaanxi Provincial Education Department (Grant no. 17JK0335), State Key Laboratory of Functional Materials for Informatics (Grant no. SKL201804), and Shaanxi Province Ordinary University Key Disciplines Construction Projects of Special Funds (Grant no. (2008)169).

References

K. Singh and D. Kaur, “Vertically arrays of Si-LaNiO3/BiFeO3/Au core-shell nano-capacitors for prominent coupled electro-optic effect,” Journal of Applied Physics, vol. 121, no. 11, Article ID 114103, 2017.
View at: Publisher Site | Google Scholar
K. Nozaki, S. Matsuo, T. Fujii et al., “Photonic-crystal nano-photodetector with ultrasmall capacitance for on-chip light-to-voltage conversion without an amplifier,” Optica, vol. 3, no. 5, pp. 483–492, 2016.
View at: Publisher Site | Google Scholar
Q. Fang, J. Song, X. Luo et al., “Low Loss Fiber-to-Waveguide Converter with a 3-D Functional Taper for Silicon Photonics,” IEEE Photonics Technology Letters, vol. 28, no. 22, pp. 2533–2536, 2016.
View at: Publisher Site | Google Scholar
Z. Zhang, J. Hu, H. Chen et al., “Low-crosstalk silicon photonics arrayed waveguide grating,” Chinese Optics Letters, vol. 15, no. 4, Article ID 041301, 2017.
View at: Publisher Site | Google Scholar
Q. Fang, J. Hu, Z. Zhang et al., “A ring-mirrors-integrated silicon photonics arrayed waveguide grating,” in Proceedings of the 2017 Conference on Lasers and Electro-Optics Pacific Rim (CLEO-PR), pp. 1-2, Singapore, July 2017.
View at: Publisher Site | Google Scholar
J. Bowers, M. Davenport, and S. Liu, “A 20 GHz colliding pulse mode-locked heterogeneous InP-silicon laser,” Cleo: Science Innovations, vol. SW4C.5, 2017.
View at: Google Scholar
W. Hua and S.-X. Liu, “Nonlinear resonance phenomenon of one-dimensional Bose - Einstein condensate under periodic modulation,” Chinese Physics B, vol. 23, no. 2, Article ID 020309, 2014.
View at: Publisher Site | Google Scholar
S. Akiyama, M. Imai, T. Baba et al., “Compact PIN-diode-based silicon modulator using side-wall-grating waveguide,” IEEE Journal of Selected Topics in Quantum Electronics, vol. 19, no. 6, pp. 74–84, 2013.
View at: Publisher Site | Google Scholar
H. Zwickel, S. Wolf, C. Kieninger et al., “Silicon-organic hybrid (SOH) modulators for intensity-modulation / direct-detection links with line rates of up to 120 Gbit/s,” Optics Express, vol. 25, no. 20, pp. 23784–23800, 2017.
View at: Publisher Site | Google Scholar
S. Heidmann, G. Ulliac, N. Courjal, and G. Martin, “Characterization and control of the electro-optic phase dispersion in lithium niobate modulators for wide spectral band interferometry applications in the mid-infrared,” Applied Optics, vol. 56, no. 14, pp. 4153–4157, 2017.
View at: Publisher Site | Google Scholar
N. Hoppe, C. Rothe, A. Celik et al., “Single waveguide silicon-organic hybrid modulator,” Advances in Radio Science, vol. 15, pp. 141–147, 2017.
View at: Publisher Site | Google Scholar
M. Lauermann, S. Wolf, P. C. Schindler et al., “40 GBd 16QAM signaling at 160 Gb/s in a silicon-organic hybrid modulator,” Journal of Lightwave Technology, vol. 33, no. 6, Article ID 7015552, pp. 1210–1216, 2015.
View at: Publisher Site | Google Scholar
M. Streshinsky, R. Ding, A. Novack et al., “50 Gb/s silicon traveling wave Mach-Zehnder modulator near 1300 nm,” in Proceedings of the Optical Fiber Communications Conference and Exhibition, vol. 14560428:1-3, 2014.
View at: Publisher Site | Google Scholar
J. Fujikata, M. Noguchi, Y. Kim et al., “High-speed and highly efficient Si optical modulator with strained SiGe layer,” Applied Physics Express, vol. 11, no. 3, p. 032201, 2018.
View at: Publisher Site | Google Scholar
R. J. A. Baker, J. Hoffman, P. Schvan, and S. P. Voinigescu, “SiGe BiCMOS linear modulator drivers with 4.8-Vpp differential output swing for 120-GBaud applications,” in Proceedings of the 2017 IEEE Radio Frequency Integrated Circuits Symposium, RFIC 2017, pp. 260–263, USA, June 2017.
View at: Publisher Site | Google Scholar
J. Verbist, M. Verplaetse, S. A. Srinivasan et al., “Real-Time 100 Gb/s NRZ-OOK transmission with a silicon photonics GeSi electro-Absorption modulator,” in Proceedings of the 6th IEEE Photonics Society Optical Interconnects Conference, OI 2017, pp. 29-30, USA, June 2017.
View at: Publisher Site | Google Scholar
S. Feng, B. Xue, LB. Li et al., “Analysis of Si/SiGe/Si double heterojunction band about a noval structure of PIN electronic modulation,” Acta Physica Sinica, vol. 65, no. 5, article 054201, Article ID 054201, 2016.
View at: Google Scholar

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Copyright © 2018 Song Feng et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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