TY - JOUR
T1 - InAlAs/InAs/InGaAs pseudomorphic high electron mobility transistors exhibiting ultra-fast optical response
AU - Taguchi, Hirohisa
AU - Wakimura, Nobuhito
AU - Nakagawa, Yugo
AU - Iida, Tsutomu
AU - Takanashi, Yoshifumi
PY - 2009
Y1 - 2009
N2 - High electron mobility transistors with a pseudomorphically strained InAs channel (InAs-PHEMTs) have superior electron-transport properties and high electron density, which are due to a large conduction-band discontinuity. In this work, we demonstrate that InAs-PHEMTs have an additional property: they exhibit an ultra-fast optical response with a timeconstant of 3.5 x10 -11 s. By irradiating the optical signal onto the InAs-PHEMTs, hole-electron pairs are created in the channel layer. Holes accumulated in the source region of the channel layer recombine immediately with 2DEG due to an Auger recombination mechanism. Holes generated in the region outside the gate also recombine immediately with the 2DEG due to the Auger recombination mechanism before they drift or diffuse toward the gate region. This is why the optical response time of an InAs-PHEMT is extremely small and it is restricted by the time for holes to transit across the gate region. A circuit incorporating an InAs-PHEMT as a transistor and an InAlAs/InAs/InGaAs MSM photodiode that has the same structure as an InAs-PHEMT as an optical detector has the potential to be applied as an ultra-fast receiver optoelectronic integrated circuit.
AB - High electron mobility transistors with a pseudomorphically strained InAs channel (InAs-PHEMTs) have superior electron-transport properties and high electron density, which are due to a large conduction-band discontinuity. In this work, we demonstrate that InAs-PHEMTs have an additional property: they exhibit an ultra-fast optical response with a timeconstant of 3.5 x10 -11 s. By irradiating the optical signal onto the InAs-PHEMTs, hole-electron pairs are created in the channel layer. Holes accumulated in the source region of the channel layer recombine immediately with 2DEG due to an Auger recombination mechanism. Holes generated in the region outside the gate also recombine immediately with the 2DEG due to the Auger recombination mechanism before they drift or diffuse toward the gate region. This is why the optical response time of an InAs-PHEMT is extremely small and it is restricted by the time for holes to transit across the gate region. A circuit incorporating an InAs-PHEMT as a transistor and an InAlAs/InAs/InGaAs MSM photodiode that has the same structure as an InAs-PHEMT as an optical detector has the potential to be applied as an ultra-fast receiver optoelectronic integrated circuit.
UR - http://www.scopus.com/inward/record.url?scp=70349416724&partnerID=8YFLogxK
U2 - 10.1002/pssc.200881510
DO - 10.1002/pssc.200881510
M3 - Conference article
AN - SCOPUS:70349416724
SN - 1862-6351
VL - 6
SP - 1386
EP - 1389
JO - Physica Status Solidi (C) Current Topics in Solid State Physics
JF - Physica Status Solidi (C) Current Topics in Solid State Physics
IS - 6
T2 - 35th International Symposium on Compound Semiconductors, ISCS 2008
Y2 - 21 September 2008 through 24 September 2008
ER -