Network


Latest external collaboration on country level. Dive into details by clicking on the dots.

Hotspot


Dive into the research topics where John L. Reno is active.

Publication


Featured researches published by John L. Reno.


Optics Express | 2005

Operation of terahertz quantum-cascade lasers at 164 K in pulsed mode and at 117 K in continuous-wave mode.

Benjamin S. Williams; Sushil Kumar; Qing Hu; John L. Reno

We report the demonstration of a terahertz quantum-cascade laser that operates up to 164 K in pulsed mode and 117 K in continuous-wave mode at approximately 3.0 THz. The active region was based on a resonant-phonon depopulation scheme and a metal-metal waveguide was used for modal confinement. Copper to copper thermocompression wafer bonding was used to fabricate the waveguide, which displayed improved thermal properties compared to a previous indium-gold bonding method.


Applied Physics Letters | 2003

3.4-THz quantum cascade laser based on longitudinal-optical-phonon scattering for depopulation

Benjamin S. Williams; Hans Callebaut; Sushil Kumar; Qing Hu; John L. Reno

We report the development of a quantum cascade laser, at λ=87.2 μm, corresponding to 3.44 THz or 14.2 meV photon energy. The GaAs/Al0.15Ga0.85As laser structure utilizes longitudinal-optical (LO) phonon scattering for electron depopulation. Laser action is obtained in pulsed mode at temperatures up to 65 K, and at 50% duty cycle up to 29 K. Operating at 5 K in pulsed mode, the threshold current density is 840 A/cm2, and the peak power is approximately 2.5 mW. Based on the relatively high operating temperatures and duty cycles, we propose that direct LO-phonon-based depopulation is a robust method for achieving quantum cascade lasers at long-wavelength THz frequencies.


Applied Physics Letters | 2009

186 K operation of terahertz quantum-cascade lasers based on a diagonal design

Sushil Kumar; Qing Hu; John L. Reno

Resonant-phonon terahertz quantum-cascade lasers operating up to a heat-sink temperature of 186 K are demonstrated. This record temperature performance is achieved based on a diagonal design, with the objective to increase the upper-state lifetime and therefore the gain at elevated temperatures. The increased diagonality also lowers the operating current densities by limiting the flow of parasitic leakage current. Quantitatively, the diagonality is characterized by a radiative oscillator strength that is smaller by a factor of two from the least of any previously published designs. At the lasing frequency of 3.9 THz, 63 mW of peak optical power was measured at 5 K, and approximately 5 mW could still be detected at 180 K.


Applied Physics Letters | 2002

Terahertz photoconductivity and plasmon modes in double-quantum-well field-effect transistors

Xomalin G. Peralta; S. J. Allen; Michael C. Wanke; N.E. Harff; Jerry A. Simmons; M. P. Lilly; John L. Reno; Peter John Burke; J. P. Eisenstein

Double-quantum-well field-effect transistors with a grating gate exhibit a sharply resonant, voltage tuned terahertz photoconductivity. The voltage tuned resonance is determined by the plasma oscillations of the composite structure. The resonant photoconductivity requires a double-quantum well but the mechanism whereby plasma oscillations produce changes in device conductance is not understood. The phenomenon is potentially important for fast, tunable terahertz detectors.


Applied Physics Letters | 2003

Terahertz quantum-cascade laser at λ≈100 μm using metal waveguide for mode confinement

Benjamin S. Williams; Sushil Kumar; Hans Callebaut; Qing Hu; John L. Reno

We report lasing at ∼3.0 THz (λ≈98–102 μm) in a quantum-cascade structure in which mode confinement is provided by a double-sided metal waveguide. The depopulation mechanism is based on resonant phonon scattering, as in our previous work. Lasing takes place in pulsed mode up to a heat-sink temperature of 77 K. The waveguide consists of metallic films placed above and below the 10-μm-thick multiple-quantum-well gain region, which gives low losses and a modal confinement factor of nearly unity. Fabrication takes place via low-temperature metallic wafer bonding and subsequent substrate removal using selective etching. This type of waveguide is expected to be increasingly advantageous at even longer wavelengths.


Applied Physics Letters | 2006

Real-time terahertz imaging over a standoff distance (>25meters)

Alan W. M. Lee; Qi Qin; Sushil Kumar; Benjamin S. Williams; Qing Hu; John L. Reno

The authors demonstrate the use of a terahertz quantum cascade laser (QCL) for real-time imaging in transmission mode at a standoff distance of 25meters. Lasing frequency was selected for optimum transmission within an atmospheric window at ∼4.9THz. Coarse frequency selection was made by design of the QCL gain medium. Finer selection (to within 0.1THz) was made by judicious choice of laser cavity length to adjust facet losses and therefore lasing threshold bias, in order to overlap the peak frequency of the Stark-shifted gain spectrum with the atmospheric window. Images are shown using an uncooled 320×240 microbolometer camera.


IEEE Photonics Technology Letters | 2006

Real-time imaging using a 4.3-THz quantum cascade laser and a 320 /spl times/ 240 microbolometer focal-plane array

Alan W. M. Lee; Benjamin S. Williams; Sushil Kumar; Qing Hu; John L. Reno

We report the use of a ~50-mW peak power 4.3-THz quantum cascade laser (QCL) as an illumination source for real-time imaging with a 320 times 240 element room-temperature microbolometer focal-plane array detector. The QCL is modulated synchronously with the focal-plane array for differential imaging. Signal-to-noise ratios of ~340 are achieved at a 20-frame/s acquisition rate, and the optical noise equivalent power of the detector array at 4.3 THz is estimated to be ~320 pW/radicHz. Both reflection and transmission mode imaging are demonstrated


Applied Physics Letters | 2005

Terahertz heterodyne receiver based on a quantum cascade laser and a superconducting bolometer

J. R. Gao; J. N. Hovenier; Z.Q. Yang; J.J.A. Baselmans; A. Baryshev; M. Hajenius; T. M. Klapwijk; A. J. L. Adam; T.O. Klaassen; Benjamin S. Williams; Satyendra Kumar; Qing Hu; John L. Reno

We report the first demonstration of an all solid-state heterodyne receiver that can be used for high-resolution spectroscopy above 2THz suitable for space-based observatories. The receiver uses a NbN superconducting hot-electron bolometer as mixer and a quantum cascade laser operating at 2.8THz as local oscillator. We measure a double sideband receiver noise temperature of 1400K at 2.8THz and 4.2K, and find that the free-running QCL has sufficient power stability for a practical receiver, demonstrating an unprecedented combination of sensitivity and stability.


Applied Physics Letters | 2004

Continuous-wave operation of terahertz quantum-cascade lasers above liquid-nitrogen temperature

Sushil Kumar; Benjamin S. Williams; Stephen Kohen; Qing Hu; John L. Reno

We report cw operation of a quantum-cascade laser at 3.2 THz (λ≈94 μm) up to a heat-sink temperature of 93 K. Resonant longitudinal-optical phonon scattering is used to depopulate the lower radiative state and a low-loss metal–metal waveguide is used to provide high modal confinement. Optical powers of ∼1.8 mW at 10 K and ∼400 μW at 78 K are observed from a single facet of a 40-μm-wide and 1.35-mm-long laser device. A threshold current density of 432 A/cm2 at 10 K and 552 A/cm2 at 78 K was obtained in cw mode. The same device lased up to 129 K in pulsed mode with a threshold current density of 419 A/cm2 at 5 K.


Optics Express | 2007

Surface-emitting distributed feedback terahertz quantum-cascade lasers in metal-metal waveguides

Sushil Kumar; Benjamin S. Williams; Qi Qin; Alan W. M. Lee; Qing Hu; John L. Reno

Single-mode surface-emitting distributed feedback terahertz quantum-cascade lasers operating around 2.9 THz are developed in metal-metal waveguides. A combination of techniques including precise control of phase of reflection at the facets, and use of metal on the sidewalls to eliminate higher-order lateral modes allow robust single-mode operation over a range of approximately 0.35 THz. Single-lobed far-field radiation pattern is obtained using a pi phase-shift in center of the second-order Bragg grating. A grating device operating at 2.93 THz lased up to 149 K in pulsed mode and a temperature tuning of 19.7 GHz was observed from 5 K to 147 K. The same device lased up to 78 K in continuous-wave (cw) mode emitting more than 6 mW of cw power at 5 K. In general, maximum temperature of pulsed operation for grating devices was within a few Kelvin of that of multi-mode Fabry-Perot ridge lasers.

Collaboration


Dive into the John L. Reno's collaboration.

Top Co-Authors

Avatar

Qing Hu

Massachusetts Institute of Technology

View shared research outputs
Top Co-Authors

Avatar
Top Co-Authors

Avatar

Sushil Kumar

University of the South Pacific

View shared research outputs
Top Co-Authors

Avatar

Igal Brener

Sandia National Laboratories

View shared research outputs
Top Co-Authors

Avatar

Jerry A. Simmons

Sandia National Laboratories

View shared research outputs
Top Co-Authors

Avatar

Eric A. Shaner

Sandia National Laboratories

View shared research outputs
Top Co-Authors

Avatar

Albert D. Grine

Sandia National Laboratories

View shared research outputs
Top Co-Authors

Avatar

J. P. Bird

State University of New York System

View shared research outputs
Top Co-Authors

Avatar

M. P. Lilly

Sandia National Laboratories

View shared research outputs
Top Co-Authors

Avatar

Michael C. Wanke

Sandia National Laboratories

View shared research outputs
Researchain Logo
Decentralizing Knowledge