2014
DOI: 10.1109/led.2014.2365216
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Composition- and Doping-Graded-Base InP/InGaAsSb Double Heterojunction Bipolar Transistors Exhibiting Simultaneous <inline-formula> <tex-math notation="TeX">\(f_{t}\) </tex-math></inline-formula> and <inline-formula> <tex-math notation="TeX">\(f_{\textrm {max}}\) </tex-math></inline-formula> of Over 500 GHz

Abstract: We demonstrate composition-and doping-gradedbase InP/InGaAsSb double heterojunction bipolar transistors (DHBTs) with a passivation ledge fabricated in a self-aligned process with i-line lithography. We obtained a high current gain of 52 and high breakdown voltage of 5 V for 0.2-µm-emitter DHBTs featuring 30-nm-thick composition-and doping-graded InGaAsSb base and 100-nm-thick InP collector. The HBTs exhibit an f t of 501 GHz and an f max of 503 GHz at a collector current density of 10.6 mA/µm 2 .

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Cited by 15 publications
(4 citation statements)
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“…However, the electron mobility of GaAsSb is lower than that of InGaAs, which limits f T [1]. Recently, we proposed a compositionally graded InGaAsSb base in order to boost electron mobility, and demonstrated simultaneous f T and f max of over 500 GHz [4]. The quaternary graded-base DHBTs with f T =f max ¼ 547=784 GHz have been also demonstrated [5] from a group of ETH-Zürich.…”
Section: Introductionmentioning
confidence: 99%
“…However, the electron mobility of GaAsSb is lower than that of InGaAs, which limits f T [1]. Recently, we proposed a compositionally graded InGaAsSb base in order to boost electron mobility, and demonstrated simultaneous f T and f max of over 500 GHz [4]. The quaternary graded-base DHBTs with f T =f max ¼ 547=784 GHz have been also demonstrated [5] from a group of ETH-Zürich.…”
Section: Introductionmentioning
confidence: 99%
“…The composition-graded layer was first proposed in the GaAs/AlGaAs system, which is known as a graded-index separate confinement heterostructure (GRIN SCH) and has been well developed in InP and GaN systems [10][11][12][13]. The composition-graded layer epitaxy technique provides more flexibility for semiconductor device designs, e.g., the modification of the builtin electric field, bandgap profile, and refractive index profile [14][15][16]. Further improving the performance of GaSb-based lasers requires addressing the series resistance caused by the abrupt interface between the waveguide layer and cladding layer, which remains a severe problem.…”
Section: Introductionmentioning
confidence: 99%
“…[3][4][5][6] Usually, heavily silicon-doped InGaAs cap layers have been used as contact layers to achieve low contact resistance fabricated by ex situ or in situ non-alloyed contacts in InP HEMTs [7][8][9] and HBTs. [10][11][12] The efficacy of high silicon-doping concentrations in InGaAs cap layers to obtain contact resistance of 4×10 −8 Ω•cm 2 has been demonstrated because the use of high semiconductor doping concentrations is known to promote current transport due to the tunneling effect. [13][14][15] However, it is difficult to further reduce the contact resistance by increasing the silicon-doping concentration in InGaAs, which can only be doped to the 19th power owing to the doping solubility limit.…”
Section: Introductionmentioning
confidence: 99%