Abstract

Thin avalanche layers have been adopted to achieve low excess noise and high-gain bandwidth products in InP and InAlAs avalanche photodiodes. In this paper, we report the excess noise characterization in a series of $\text{Al}_{\mathbf{1{-}}{\boldsymbol x}}$ Ga $_{\boldsymbol{x}}$ As $_{\mathbf{0.56}}$ Sb $_{\mathbf{0.44}}$ ( $x\,= \,0,\,0.05$ , 0.1, 0.15) diodes with avalanche layer thickness of 110–116 nm. These alloys, lattice matched to InP, showed lower excess noise than InP and InAlAs. Dark current, most probably originating from surface leakage, was observed to be lower in composition with higher Ga concentration. Avalanche gain and excess noise measurements using lasers of 543 and 633 nm wavelengths indicated that at a given electric field, the electron ionization coefficient is larger than the hole ionization coefficient. Using the 543 nm laser, low excess noise data corresponding to an effective ionization coefficient ratio of $k\,= \,0.1$ in the conventional excess noise theory was measured in $\text{Al}_{\mathbf{1{-}}{\boldsymbol x}}$ Ga $_{\boldsymbol{x}}$ As $_{\mathbf{0.56}}$ Sb $_{\mathbf{0.44}}$ ( $x\,= \,0.05$ , 0.1, 0.15), although pure electron injection was not achieved. Our results demonstrated the potential of using $\text{Al}_{\mathbf{1{-}}{\boldsymbol x}}$ Ga $_{\boldsymbol{x}}$ As $_{\mathbf{0.56}}$ Sb $_{\mathbf{0.44}}$ ( $x\,= \,0.05$ , 0.1, 0.15) as replacement for InP and InAlAs for high speed and low excess noise avalanche photodiodes. The data reported in this paper is available from the ORDA digital repository ( https://doi.org/10.15131/shef.data.5155822 ).

Highlights

  • High-speed avalanche photodiodes (APDs) are key components in long-haul high bit rate optical communication systems because they exploit internal gain to provide higher sensitivity than a conventional p+in+ photodiode

  • The measured capacitance is < 30 pF, confirming the devices are suitable for excess noise measurements

  • Increases when the laser wavelength decreases, i.e. when the carrier injection profile approaches pure electron injection with fewer electron-hole pairs generated in the i-layer and fewer holes injected from the n+ layer. This suggests that, in the Al1-xGaxAs0.56Sb0.44 (x = 0 to 0.15), the electron ionization coefficient is higher than the hole ionization coefficient, i.e

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Summary

INTRODUCTION

High-speed avalanche photodiodes (APDs) are key components in long-haul high bit rate optical communication systems because they exploit internal gain to provide higher sensitivity than a conventional p+in+ photodiode. Low excess noise and high gain-bandwidth product (GBP) are crucial for achieving high bit rate optical communication systems. Even higher GBP (340 GHz) was demonstrated by Ge/Si APDs, with Si avalanche region and Ge absorption region [12], their dark current and quantum efficiency are not comparable to those of InGaAs/InP or InGaAs/InAlAs APDs. researchers continue to investigate other materials as alternative avalanche layer materials. Having demonstrated a high GBP of 424 GHz with an InGaAs/Al0.85Ga0.15As0.56Sb0.44 APD for 1550 nm wavelength light [17], excess noise factors and ionization coefficients of the alloy Al1-xGaxAs0.56Sb0.44 are the remaining APD-related characteristics that have not been investigated.

EXPERIMENTAL DETAILS
RESULTS AND DISCUSSION
10 AlAsSb 1
CONCLUSION
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