Optimal excess noise reduction in thin heterojunction Al/sub 0.6/Ga/sub 0.4/As-GaAs avalanche photodiodes

It has been recently found that the initial-energy effect, which is associated with the finite initial energy of carriers entering the multiplication region of an avalanche photodiode (APD), can be tailored to reduce the excess noise well beyond the previously known limits for thin APDs. However, the control of the initial energy of injected carriers can be difficult in practice for an APD with a single multiplication layer. In this paper, the dead-space multiplication recurrence theory is used to show that the low noise characteristics associated with the initial-energy effect can be achieved by utilizing a two-layer multiplication region. As an example, a high bandgap Al/sub 0.6/Ga/sub 0.4/As material, termed the energy-buildup layer, is used to elevate the energy of injected carriers without incurring significant multiplication events, while a second GaAs layer with a lower bandgap energy is used as the primary carrier multiplication layer. Computations show that devices can be optimally designed through judicious choice of the charge-layer width to produce excess noise factor levels that are comparable to those corresponding to homojunction APDs benefiting from a maximal initial-energy effect. A structure is presented to achieve precisely that.

[1]  Jeremy Allam,et al.  Role of satellite valleys in ionisation rate enhancement in multiple quantum well avalanche photodiodes , 1990 .

[2]  Bahaa E. A. Saleh,et al.  Effect of dead space on gain and noise double-carrier-multiplication avalanche photodiodes , 1992, Optical Society of America Annual Meeting.

[3]  J.C. Campbell,et al.  Avalanche photodiodes with an impact-ionization-engineered multiplication region , 2000, IEEE Photonics Technology Letters.

[4]  A. Holmes,et al.  Monte Carlo simulation of low-noise avalanche photodiodes with heterojunctions , 2002 .

[5]  M. Teich,et al.  Impact-ionization and noise characteristics of thin III-V avalanche photodiodes , 2001 .

[6]  John P. R. David,et al.  Avalanche multiplication noise characteristics in thin GaAs p/sup +/-i-n/sup +/ diodes , 1998 .

[7]  Bahaa E. A. Saleh,et al.  Effect of dead space on the excess noise factor and time response of avalanche photodiodes , 1990 .

[8]  J. David,et al.  A Monte Carlo investigation of multiplication noise in thin p/sup +/-i-n/sup +/ GaAs avalanche photodiodes , 1998 .

[9]  J. Campbell,et al.  Calculation of gain and noise with dead space for GaAs and Al/sub x/Ga/sub 1-x/As avalanche photodiode , 2002 .

[10]  Bahaa E. A. Saleh,et al.  Breakdown voltage in thin III–V avalanche photodiodes , 2001 .

[11]  J. Campbell,et al.  Calculation of Gain and Noise With Dead Space for GaAs and Al Ga As Avalanche Photodiode , 2002 .

[12]  Joe C. Campbell,et al.  Ultra-low noise avalanche photodiodes with a "centered-well" multiplication region , 2003 .

[13]  J. David,et al.  Avalanche multiplication in Al/sub x/Ga/sub 1-x/As (x=0 to 0.60) , 2000 .

[14]  X. Li,et al.  Low-noise avalanche photodiodes with graded impact-ionization-engineered multiplication region , 2001, IEEE Photonics Technology Letters.

[15]  Bahaa E. A. Saleh,et al.  Dead-space-based theory correctly predicts excess noise factor for thin GaAs and AlGaAs avalanche photodiodes , 2000 .

[16]  R. J. McIntyre,et al.  A new look at impact ionization-Part I: A theory of gain, noise, breakdown probability, and frequency response , 1999 .

[17]  Bahaa E. A. Saleh,et al.  Boundary effects on multiplication noise in thin heterostructure avalanche photodiodes: theory and experiment [Al/sub 0.6/Ga/sub 0.4/As/GaAs] , 2002 .

[18]  A. Lacaita,et al.  Dead space approximation for impact ionization in silicon , 1996 .

[19]  C. Hu,et al.  A new look at impact ionization-Part II: Gain and noise in short avalanche photodiodes , 1999 .

[20]  F. Capasso,et al.  The graded bandgap multilayer avalanche photodiode: A new low-noise detector , 1982, IEEE Electron Device Letters.

[21]  Bahaa E. A. Saleh,et al.  Effect of dead space on gain and noise in Si and GaAs avalanche photodiodes , 1992 .

[22]  J. David,et al.  Avalanche multiplication in submicron AlxGa1−xAs/GaAs multilayer structures , 2000 .

[23]  J.C. Campbell,et al.  Impact ionization characteristics of III-V semiconductors for a wide range of multiplication region thicknesses , 2000, IEEE Journal of Quantum Electronics.

[24]  R. C. Tozer,et al.  Treatment of soft threshold in impact ionization , 2001 .