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Showing posts with label Arthur C. Gossard. Show all posts
Showing posts with label Arthur C. Gossard. Show all posts
Friday, March 15, 2019
Abstract-Picosecond-scale Terahertz pulse characterization with field-effect transistors
Stefan Regensburger, Stephan Winnerl, J. Michael Klopf, Hong Lu, Arthur C. Gossard, Sascha Preu
https://ieeexplore.ieee.org/document/8662700
Precise real-time detection of Terahertz pulses is a key requirement for characterization of pulsed Terahertz sources and non-destructive testing applications. We experimentally evaluate the speed limits of Terahertz rectification in field-effect transistors using the example of pulses from a free-electron laser. We develop an improved model for the description of these Terahertz pulses and demonstrate its validity experimentally by comparison to spectroscopic data as well as to expectation values calculated from free-electron laser physics. The model in conjunction with the high speed of the detectors permits the detection of an exponential rise time of the pulses as short as 5 ps despite a Gaussian post detection time constant of 11 and 14 ps for a large area and an antenna-coupled detector, respectively. This proves that field-effect transistors are excellent compact, room-temperature Terahertz detectors for applications that require an intermediate frequency bandwidth of several tens of GHz.
Saturday, December 2, 2017
Abstract-Dynamical Birefringence: Electron-Hole Recollisions as Probes of Berry Curvature
Hunter B. Banks, Qile Wu, Darren C. Valovcin, Shawn Mack, Arthur C. Gossard, Loren Pfeiffer, Ren-Bao Liu, and Mark S. Sherwin
The direct measurement of Berry phases is still a great challenge in condensed-matter systems. The bottleneck has been the ability to adiabatically drive an electron coherently across a large portion of the Brillouin zone in a solid where the scattering is strong and complicated. We break through this bottleneck and show that high-order sideband generation (HSG) in semiconductors is intimately affected by Berry phases. Electron-hole recollisions and HSG occur when a near-band-gap laser beam excites a semiconductor that is driven by sufficiently strong terahertz-frequency electric fields. We carry out experimental and theoretical studies of HSG from three GaAs/AlGaAs quantum wells. The observed HSG spectra contain sidebands up to the 90th order, to our knowledge the highest-order optical nonlinearity reported in solids. The highest-order sidebands are associated with electron-hole pairs driven coherently across roughly 10% of the Brillouin zone around the Γ point. The principal experimental claim is a dynamical birefringence: the intensity and polarization of the sidebands depend on the relative polarization of the exciting near-infrared (NIR) and the THz electric fields, as well as on the relative orientation of the laser fields with the crystal. We explain dynamical birefringence by generalizing the three-step model for high-order harmonic generation. The hole accumulates Berry phases due to variation of its internal state as the quasimomentum changes under the THz field. Dynamical birefringence arises from quantum interference between time-reversed pairs of electron-hole recollision pathways. We propose a method to use dynamical birefringence to measure Berry curvature in solids.
Friday, March 20, 2015
Erbium Modified III-V Semiconductors as Photoconductors in the Terahertz Region
http://techtransfer.universityofcalifornia.edu/NCD/24909.html
Brief Description
A composite material system with embedded Erbium-Arsenic (ErAs) nanostructures for 1030nm operation with higher dark resistance and ultrafast carrier lifetime.
Background
Spectroscopic applications in the terahertz (THz) region are used in broadband imaging and in the detection of chemical and biological hazards. Photoconductors are the most frequently used devices for THz generation and detection in the terahertz region. The terahertz region is located between the infrared and microwave wavelengths on the electromagnetic spectrum, and requires that spectroscopic devices have ultrafast carrier lifetime and high electrical resistance in the dark. Spectroscopic applications have been achieved for 800nm wavelength operation, but fiber-laser comparable systems that operate at a higher wavelength have not been explored.
Description
Researchers at UC Santa Barbara have developed a composite material system with embedded Erbium-Arsenic (ErAs) nanostructures for 1030nm operation with higher dark resistance and ultrafast carrier lifetime. The system utilizes a rare earth (RE) element, Erbium, to create a III-V semiconductor with the desired bandgaps. When the solubility limit of the RE element is reached, RE-V nanostructures are formed within the III-V semiconductor matrix. These nanostructures trap photo-carriers to reach ultrashort lifetimes and the Fermi levels of the RE-V compounds pin somewhere within the III-V bandgaps to help increase the dark resistance.
Advantages
- Reduced cost of photoconductor materials and THz system overall
- Compact fiber lasers allow for reduced THz system size
- Increased dark resistance
Applications
- Photoconductors
- Broadband imaging
- Detection of chemical & biological hazards
Inventors
- Gossard, Arthur C.
- Lu, Hong
- Palmstrom, Christopher J.
Other Information
Categorized As
Related cases
2015-332-0
Keywords
terahertz, III-V, photoconductor
Contact
Meaghan A. Shaw / shaw@tia.ucsb.edu / tel: View Phone Number. Please reference Tech ID #24909.
Saturday, July 26, 2014
Abstract-Plasmonics enhanced photomixing for generating quasi-continuous-wave frequency-tunable terahertz radiation
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Christopher W. Berry, Mohammad R. Hashemi, Sascha Preu, Hong Lu, Arthur C. Gossard, and Mona Jarrahi »View Author Affiliations
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Optics Letters, Vol. 39, Issue 15, pp. 4522-4524 (2014)
http://dx.doi.org/10.1364/OL.39.004522
http://dx.doi.org/10.1364/OL.39.004522
We experimentally demonstrate an order of magnitude enhancement in the quasi-continuous-wave radiated power from a photomixer with plasmonic contact electrodes in comparison with an analogous conventional photomixer without plasmonic contact electrodes in the 0.25–2.5 THz frequency range when pumped at an optical wavelength of 1550 nm. The significant efficiency enhancement results from the unique capability of the plasmonic contact electrodes to reduce the average transport path of photocarriers to the device contact electrodes, increasing the ultrafast photocurrent that drives the terahertz antenna.
Monday, March 3, 2014
Novel quantum dot laser paves the way for lower-cost photonics
http://phys.org/news/2014-03-quantum-dot-laser-paves-lower-cost.html
With the
explosive growth of bandwidth demand in telecommunications networks, experts
are continually seeking new ways to transmit increasingly large amounts of data
in the quickest and cheapest ways possible. Photonic devices—which convert
light to electricity and vice versa—offer an energy-efficient alternative to
traditional copper network links for information transmission. Unfortunately,
these devices are also almost always prohibitively pricey.
One way to bring those costs down is to make photonics compatible with the existing silicon microelectronics industry. A promising way to do that is by growing "quantum dot" lasers directly on silicon substrates, according to graduate student Alan Y. Liu of theUniversity of California at Santa Barbara (UCSB) and
his colleagues, who include UCSB professors John E. Bowers and Arthur C.
Gossard. Although such quantum dot lasers have been grown on silicon before,
their performance has not equaled that of quantum dot lasers grown on their
native substrates, which are platforms made of similar materials as the quantum
dot lasers themselves.
One way to bring those costs down is to make photonics compatible with the existing silicon microelectronics industry. A promising way to do that is by growing "quantum dot" lasers directly on silicon substrates, according to graduate student Alan Y. Liu of the
Now Liu and his collaborators
in Bowers and Gossard's groups have demonstrated a novel quantum dot laser that
not only is grown on silicon but that performs as well as similar lasers grown
on their native substrates. The team will discuss its record-breaking results
achieved using such lasers at this year's OFC Conference and Exposition, being
held March 9-13 in San Francisco, Calif., USA.
The researchers believe the
work is an important step towards large-scale photonic integration in an ultra
low-cost platform.
Currently, so-called
"quantum well" lasers are used for data transmission. They consist of
nanometers-thick layers of light-emitting material, representing the quantum
well, sandwiched between other materials that serve to guide both the injected
electrical current as well as the output light. A quantum dot laser is similar
in design, but the sheets of quantum well materials are replaced with a high
density of smaller dots, each a few nanometers high and tens of nanometers
across. To put it in perspective, 50 billion of them would fit onto one side of
a penny.
"Quantum wells are
continuous in two dimensions, so imperfections in one part of the well can
affect the entire layer. Quantum dots, however, are independent of each other,
and as such they are less sensitive to the crystal imperfections resulting from
the growth of laser material on silicon," Liu said.
"Because of this, we can
grow these lasers on larger and cheaper silicon substrates. And because of
their small size," Liu added, "they require less power to operate
than quantum well lasers while outputting more light, so they would enable
low-cost silicon photonics."
In their new work, the team
grew quantum dots directly on silicon substrates using a technique known as
molecular beam epitaxy, or MBE ("epitaxy" refers to the process of
growing one crystal on top of another, with the orientation of the top layer
determined by that of the bottom).
"The major advantage of
epitaxial growth is that it enables us to exploit the existing economies of
scale for silicon, which would drive down cost," Liu said. He added that
"MBE is the best method for creating high-quality quantum dots that
are suitable for use in lasers" and that "the entire laser can be
grown continuously in a single run, which minimizes potential
contamination."
More information: Presentation W4C.5. titled "High
Performance 1.3μm InAs Quantum Dot Lasers Epitaxially Grown on Silicon"
will take place Wednesday, March 12 at 5:00 p.m. in room 121 of the Moscone Center . (www.ofcconference.org/)
This work was recently
published in Applied
Physics Letters: Liu, A. Y., et al. "High performance
continuous wave 1.3 μm quantum dot lasers on silicon." Applied Physics Letters,
104, 041104 (2014)
Journal
reference: Applied Physics Letters

Provided
by Optical Society of America 
Monday, December 2, 2013
Abstract-Terahertz electron-hole recollisions in GaAs/AlGaAs quantum wells: Robustness to scattering by optical phonons and thermal fluctuations
My Note: I have reposted this abstract as it was found online. Please excuse any errors.
Hunter Banks, Ben Zaks, Fan Yang, Shawn Mack, Arthur C. Gossard, Renbao Liu, and Mark S. Sherwin
Accepted
Electron-hole recollisions are induced by resonantly injecting excitons with a near-IR laser at frequency $f_{\text{NIR}}$ into quantum wells driven by a ~10 kV/cm field oscillating at $f_{\text{THz}} = 0.57$ THz. At $T=12$ K, up to 18 sidebands are observed at frequencies $f_{\text{Sideband}}=f_{\text{NIR}}+2n f_{\text{THz}}$, with $-8 \le 2n \le 28$. Electrons and holes recollide with total kinetic energies up to 57 meV, well above the $E_{\text{LO}} = 36$ meV threshold for longitudinal optical (LO) phonon emission. Sidebands with order up to $2n=22$ persist up to room temperature. A simple model shows that LO phonon scattering suppresses but does not eliminate sidebands associated with kinetic energies above $E_{\text{LO}}$.
Friday, September 13, 2013
Abstract-Terahertz electron-hole recollisions in GaAs/AlGaAs quantum wells: robustness to scattering by optical phonons and thermal fluctuations
Electron-hole recollisions are induced by resonantly injecting excitons with a near-IR laser at frequency $f_$ into quantum wells driven by a ~10 kV/cm field oscillating at $f_= 0.57$ THz. At $T=12$ K, up to 18 sidebands are observed at frequencies $f_=f_+2n f_$, with $-8 \le 2n \le 28$. Electrons and holes recollide with total kinetic energies up to 57 meV, well above the $E_} = 36$ meV threshold for longitudinal optical (LO) phonon emission. Sidebands with order up to $2n=22$ persist up to room temperature. A simple model shows that LO phonon scattering suppresses but does not eliminate sidebands associated with kinetic energies above $E_
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