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Dive into the research topics where Sarath D. Gunapala is active.

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Featured researches published by Sarath D. Gunapala.


Applied Physics Letters | 2009

A high-performance long wavelength superlattice complementary barrier infrared detector

David Z. Ting; Cory J. Hill; Alexander Soibel; Sam A. Keo; Jason M. Mumolo; Jean Nguyen; Sarath D. Gunapala

We describe a long wavelength infrared detector where an InAs/GaSb superlattice absorber is surrounded by a pair of electron-blocking and hole-blocking unipolar barriers. A 9.9 μm cutoff device without antireflection coating based on this complementary barrier infrared detector design exhibits a responsivity of 1.5 A/W and a dark current density of 0.99×10−5 A/cm2 at 77 K under 0.2 V bias. The detector reaches 300 K background limited infrared photodetection (BLIP) operation at 87 K, with a black-body BLIP D∗ value of 1.1×1011 cm Hz1/2/W for f/2 optics under 0.2 V bias.


IEEE Photonics Technology Letters | 2004

High-temperature operation of InAs-GaAs quantum-dot infrared photodetectors with large responsivity and detectivity

S. Chakrabarti; Adrienne D. Stiff-Roberts; P. Bhattacharya; Sarath D. Gunapala; S. Bandara; Sir B. Rafol; S. W. Kennerly

We have optimized the growth of multiple (40-70) layers of self-organized InAs quantum dots separated by GaAs barrier layers in order to enhance the absorption of quantum-dot infrared photodetectors (QDIPs). In devices with 70 quantum-dot layers, at relatively large operating biases (/spl les/-1.0 V), the dark current density is as low as 10/sup -5/ A/cm/sup 2/ and the peak responsivity ranges from /spl sim/0.1 to 0.3 A/W for temperatures T=150 K-175 K. The peak detectivity corresponding to these low dark currents and high responsivities varies in the range 6/spl times/10/sup 9//spl les/D/sup */(cm/spl middot/Hz/sup 1/2//W)/spl les/10/sup 11/ for temperatures 100/spl les/T(K)/spl les/200. These performance characteristics represent the state-of-the-art for QDIPs and indicate that this device heterostructure is appropriate for incorporation into focal plane arrays.


IEEE Transactions on Electron Devices | 2000

640/spl times/486 long-wavelength two-color GaAs/AlGaAs quantum well infrared photodetector (QWIP) focal plane array camera

Sarath D. Gunapala; Sumith V. Bandara; A. Singh; John K. Liu; B. Rafol; E.M. Luong; Jason M. Mumolo; N.Q. Tran; David Z. Ting; J.D. Vincent; C. A. Shott; J. Long; P.D. LeVan

We have designed and fabricated an optimized long-wavelength/very-long wavelength two-color quantum well infrared photodetector (QWIP) device structure. The device structure was grown on a 3-in semi-insulating GaAs substrate by molecular beam epitaxy (MBE). The wafer was processed into several 640/spl times/486 format monolithically integrated 8-9 and 14-15 /spl mu/m two-color (or dual wavelength) QWIP focal plane arrays (FPAs). These FPAs were then hybridized to 640/spl times/486 silicon CMOS readout multiplexers. A thinned (i.e., substrate removed) FPA hybrid was integrated into a liquid helium cooled dewar for electrical and optical characterization and to demonstrate simultaneous two-color imagery. The 8-9 /spl mu/m detectors in the FPA have shown background limited performance (BLIP) at 70 K operating temperature for 300 K background with f/2 cold stop. The 14-15 /spl mu/m detectors of the FPA reaches BLIP at 40 K operating temperature under the same background conditions. In this paper we discuss the performance of this long-wavelength dualband QWIP FPA in terms of quantum efficiency, detectivity, noise equivalent temperature difference (NE/spl Delta/T), uniformity, and operability.


IEEE Journal of Quantum Electronics | 2007

640

Sarath D. Gunapala; Sumith V. Bandara; Cory J. Hill; David Z. Ting; John K. Liu; B. Rafol; E.R. Blazejewski; Jason M. Mumolo; Sam A. Keo; Sanjay Krishna; Y.-C. Chang; C.A. Shott

Epitaxially grown self-assembled InAs-InGaAs-GaAs quantum dots (QDs) are exploited for the development of large-format long-wavelength infrared focal plane arrays (FPAs). The dot-in-a-well (DWELL) structures were experimentally shown to absorb both 45deg and normal incident light, therefore, a reflection grating structure was used to enhance the quantum efficiency. The devices exhibit peak responsivity out to 8.1 mum, with peak detectivity reaching ~1times1010 Jones at 77 K. The devices were fabricated into the first long-wavelength 640times512 pixel QD infrared photodetector imaging FPA, which has produced excellent infrared imagery with noise equivalent temperature difference of 40 mK at 60-K operating temperature


Semiconductor Science and Technology | 2005

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Sarath D. Gunapala; Sumith V. Bandara; John K. Liu; Cory J. Hill; Sir B. Rafol; Jason M. Mumolo; J.T. Trinh; Meimei Z. Tidrow; Paul D. LeVan

Mid-wavelength infrared (MWIR) and long-wavelength infrared (LWIR) 1024 × 1024 pixel quantum well infrared photodetector (QWIP) focal planes have been demonstrated with excellent imaging performance. The MWIR QWIP detector array has demonstrated a noise equivalent differential temperature (NEΔT) of 17 mK at a 95 K operating temperature with f/2.5 optics at 300 K background and the LWIR detector array has demonstrated a NEΔT of 13 mK at a 70 K operating temperature with the same optical and background conditions as the MWIR detector array after the subtraction of system noise. Both MWIR and LWIR focal planes have shown background limited performance (BLIP) at 90 K and 70 K operating temperatures respectively, with similar optical and background conditions. In this paper, we will discuss the performance in terms of quantum efficiency, NEΔT, uniformity, operability and modulation transfer functions.


IEEE Transactions on Electron Devices | 1997

512 Pixels Long-Wavelength Infrared (LWIR) Quantum-Dot Infrared Photodetector (QDIP) Imaging Focal Plane Array

Sarath D. Gunapala; John K. Liu; Jin Suk Park; Mani Sundaram; C. A. Shott; Theodore R. Hoelter; T. L. Lin; S. T. Massie; Paul D. Maker; Richard E. Muller; Gabby Sarusi

A 9-/spl mu/m cutoff 256/spl times/256 hand-held quantum well infrared photodetector (QWIP) camera has been demonstrated. Excellent imagery, with a noise equivalent differential temperature (NE/spl Delta/T) of 26 mK has been achieved. In this paper, we discuss the development of this very sensitive long wavelength infrared (LWIR) camera based on a GaAs/AlGaAs QWIP focal plane array and its performance in quantum efficiency, NE/spl Delta/T, minimum resolvable temperature (MRTD), uniformity, and operability.


IEEE Transactions on Electron Devices | 1998

1024 × 1024 pixel mid-wavelength and long-wavelength infrared QWIP focal plane arrays for imaging applications

Sarath D. Gunapala; S.V. Bundara; John K. Liu; Winn Hong; Mani Sundaram; Paul D. Maker; Richard E. Muller; C. A. Shott; Ronald J. Carralejo

A 9-/spl mu/m cutoff 640/spl times/486 snap-shot quantum well infrared photodetector (QWIP) camera has been demonstrated. The performance of this QWIP camera is reported including indoor and outdoor imaging. The noise equivalent differential temperature (NE/spl Delta/T) of 36 mK has been achieved at 300 K background with f/2 optics. This is in good agreement with expected focal plane array sensitivity due to the practical limitations on charge handling capacity of the multiplexer, read noise, bias voltage, and operating temperature.


IEEE Transactions on Electron Devices | 1997

9-/spl mu/m cutoff 256/spl times/256 GaAs/Al/sub x/Ga/sub 1-x/As quantum well infrared photodetector hand-held camera

Sarath D. Gunapala; John K. Liu; Jin S. Park

A 9-/spl mu/m cutoff 256/spl times/256 hand-held quantum well infrared photodetector (QWIP) camera has been demonstrated. Excellent imagery, with a noise equivalent differential temperature (NE/spl Delta/T) of 26 mK has been achieved. In this paper, we discuss the development of this very sensitive long wavelength infrared (LWIR) camera based on a GaAs/AlGaAs QWIP focal plane array and its performance in quantum efficiency, NE/spl Delta/T, minimum resolvable temperature (MRTD), uniformity, and operability.


Semiconductors and Semimetals | 2011

Long-wavelength 640/spl times/486 GaAs-AlGaAs quantum well infrared photodetector snap-shot camera

David Z. Ting; Alexander Soibel; Linda Höglund; Jean Nguyen; Cory J. Hill; Arezou Khoshakhlagh; Sarath D. Gunapala

Publisher Summary This chapter provides an overview of type-II superlattice infrared detectors. The type-II InAs/GaSb superlattices have several fundamental properties that make them suitable for infrared detection: (1) their band gaps can be made arbitrarily small by design, (2) they are more immune to band-to-band tunneling compared with bulk material, (3) the judicious use of strain in type-II InAs/GaInSb strained layer superlattice (SLS) can enhance its absorption strength over that of the type-II InAs/GaSb superlattice to a level comparable with HgVdTe (MCT), and (4) type-II InAs/Ga(In)Sb superlattices also reduce Auger recombination. In addition, the dark current characteristics of type-II superlattice-based single element long-wavelength infrared (LWIR) detectors are currently approaching state-of-the-art MCT detector. Noise measurements highlight the need for surface leakage suppression, which can be tackled by improved etching, passivation, and device design. The chapter also describes the principles behind advanced superlattice infrared detectors based on heterostructure designs. It also explores some aspects of device fabrication and characterization.


IEEE Transactions on Electron Devices | 1997

9-{micro}m cutoff 256 x 256 GaAs/Al{sub x}Ga{sub 1{minus}x}As quantum well infrared photodetector hand-held camera

Sarath D. Gunapala; Jin S. Park; Gabby Sarusi; True-Lon Lin; John K. Liu; Paul D. Maker; Richard E. Muller; C. A. Shott; Ted Hoelter

In this paper, we discuss the development of very sensitive, very long wavelength infrared GaAs/Al/sub x/Ga/sub 1-x/As quantum well infrared photodetectors (QWIPs) based on bound-to-quasi-bound intersubband transition, fabrication of random reflectors for efficient light coupling, and the demonstration of a 15-/spl mu/m cutoff 128/spl times/128 focal plane array imaging camera. Excellent imagery, with a noise equivalent differential temperature (NE/spl Delta/T) of 30 mK has been achieved.

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John K. Liu

California Institute of Technology

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David Z. Ting

California Institute of Technology

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Jason M. Mumolo

California Institute of Technology

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Sumith V. Bandara

California Institute of Technology

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Cory J. Hill

Jet Propulsion Laboratory

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Alexander Soibel

California Institute of Technology

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Sam A. Keo

Jet Propulsion Laboratory

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Jean Nguyen

Jet Propulsion Laboratory

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Sir B. Rafol

California Institute of Technology

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