Facilities

 

 

 

 

 

New Single Shot Frequency Monitor

By using a static THz interferometer the frequency of the free electron laser (FEL) can be precisely measured in a single shot. In the left is shown an interference pattern produced by the interferometer for the FEL operating at 0.59 THz. Not only the laser frequency, but the whole spectrum in the range 0.1 – 4 THz can be obtained using this so called holographic Fourier transform spectrometer.
 
 

Semiconductor Processing

UCSB is a world leader in III-V semiconductor processing and molecular beam epitaxy (MBE). The state-of-the-art Nanofabrication Facility, one of the premier university cleanroom facilities in the country, was recently augmented by the engineering sciences cleanroom--occupying the entire first floor of a brand new 90,000 sq. ft. building. In addition the CNSI building (under construction) will have its fourth floor as a dedicated cleanroom, with areas for biological as well as chemical experiments.

Terahertz Sources - all in one convenient location

Central to our experimental facilities are the free-electron lasers or FELs (0.5-5 THz, 50-1000 µm, 5 kW peak power, 10 µs pulses) at the Center for Terahertz Science and Technology. These are the world's premier sources for intense, coherent terahertz radiation. At the output of the FEL is a pulse-slicer, capable of slicing short pulses (adjustable from 10 ps - 100 ns) out of the main FEL microsecond pulse.
CW Virginia Diodes coherent sources: 240 GHz 1 THz These sources made by Virginia Diodes multiply a 13 GHz coherent microwave source up to 240 GHz in one source and 1 THz in the second source. These sources are tunable around these central frequencies.

Terahertz Spectrometers

THz time domain systems: ASOPS: THz-TDS fiber laser based system with no mechanical delay line, capable of 500ns/spectrum Traditional THz-TDS system
Bruker FTIR spectrometer spectrometer (Michelson interferometer w/ coherent broadband source) 240 GHz pulsed ESR spectrometer

Terahertz Optics - unique expertise

Wire-grid polarizers Variable retardation plates Large off-axis parabolic mirrors and elliptical mirrors TPX THz lenses

Optical sources, detectors

Doubled] Mode-locked Ti:S laser ([350-400nm], 700-800nm, 150 fs pulses)
Regenerative Ti:S amplifier (10 mJ per pulse)
CW Tunable Ti:S laser (700-1000nm, 1 W cw)
Doubled Nd:YAG (532nm, 10 mJ per pulse)
Ar ion laser (488nm, 5 W cw)
TE-cooled GaAs photon-counting PMT (Hamamatsu 943-02) (160-930nm) and Several other PMT's
TE-cooled MCP intensified CCD (400-900nm)
0.85m SPEX double-grating Raman spectrometer
Acton grating spectrometers: 0.75m, 0.5m, 0.15m (2)
Princeton Instruments back-illuminated, deep-depletion CCD
New Focus Fizeau wavelength meter
New Focus External Cavity Tunable Diode Laser
Several CW diode and HeNe lasers

Terahertz Detectors

Liquid He cooled Si bolometer (thermal-limit, 100 ms response)
Liquid He cooled InSb bolometer (200ns response)
Fast Ga:Ge photoconductor (moderate-sensitivity, 1 ns response)
Pyroelectric detectors (low-sensitivity, 1 ns response)
Thomas Keating absolute calibrated detector
TACIT detector (under development, currently <1ns response) Cryogenics
8 Tesla Oxford superconducting optical cryostat
8 Tesla Oxford spectromag split-coil superconducting magnet
12 Tesla Oxford spectromag split-coil superconducting magnet
Several liquid helium flow cryostats with optical access
Several liquid nitrogen cooled detector housings

Lab Locations

Free Electron Laser Facility (1300 series rooms): Access to the FEL is through Broida Hall room 1357, located at the east end of the Broida Hall first floor south-facing outdoor walkway. Keypad entry is not required during business hours. See the CTST site for a map of the FEL including conference room and FEL user lab locations. Telephone numbers are Dave Enyeart's office: 893-3390, THz source and Detector Lab (1380B): 893-4707 (collaborative lab with Allen group), Quantum Control Lab (1380C): 893-2423 (collaborative lab with Awschalom group), Pulse Slicer Lab (1380D): 893-8396, THz Spin lab (1380E--coming soon) 893-8396. FTIR lab: Broida Hall room 1215 (first floor, south-facing outdoor walkway opposite the temporary office space). Houses Bruker and Bomem FTIR instruments, flow cryostats (one sample-in-vacuum, one sample-in-vapor), bolometers and optical/NIR spectroscopy equipment. Telephone: 893-2132. THz spectroscopy lab: Broida Hall room 1217, access via FTIR lab. Includes clean bench, chemical hood, network analyzer and (coming soon) CW multiplied solid-state THz source.

Techniques

Our experimental expertise is in special techniques for the terahertz frequency range. These involve a combination of far-infrared, near-infrared, ultrafast, and RF techniques at low temperature.

Terahertz pulse slicing

The output pulses of the UCSB Free Electron Laser have a duration of roughlyone microsecond. For many experiments, however, it is desirable to have precisecontrol over a wide range of pulse widths. The Pulse Slicer operated by the SherwinGroup extracts THz radiation pulses from the FEL output that can be varied between10 ps and 100 ns in duration. An intense optical pulse from a regeneratively-amplifiedTi:S laser excites free carriers in silicon wafers. Thethickness of these wafers is precisely tuned so that they become efficientmirrors for THz radiation upon exposure to the intense optical pulse. The FELmicrosecond THz pulse is passed through two reflection switches made of the siliconwafers, which defines the beginning of a short pulse. The end of the pulse isdefined by an optical delay stage that controls the time before a transmissionswitch (silicon wafer) cuts off the outgoing THz pulse. This control over THzpulse width has made it possible to demonstrate such phenomena as Rabi Oscillationof electrons bound to shallow donors in GaAs.

Terahertz photoconductivity

An intense terahertz pulse from the pulse slicer drives electrons in the devicefrom localized to extended states. This results in a change in the conductivityin the RF frequency range. Coherent terahertz oscillations of electrons can bemapped out stroboscopically by measuring the photoconductivity vs. terahertzpulse length or delay.

Optically-detected terahertz spectroscopy

In optically detected THz experiments, changes in the optical absorption, photoluminesence, or resonant scattering due to THz irradation aremeasured. We have used this technique to investigate collectivedynamics of electrons in quantum wells, and recently, as a technique forreading out the quantum state of shallowdonors in GaAs.

Terahertz Time-Domain Spectroscopy

Broadband THz radiation with time duration on the order of a picosecond is generated in a semoconductor wafer by incident near-infrared (NIR) 150fs laser pulses. The THz is created by either difference frequency mixing of the NIR in a semiconductor with a second-order susceptiblity nonlinearity, or by photo-created electrons accelerating across the surface depletion fields of a doped semiconductor.

The THz is collimated, and sent collinearly with a probe beam from the femtosecond laser pulse through an electro-optic ZnTe crystal. The THz electric field rotates the polarization probe pulse via the Pockels effect. The rotation of the probe pulse is detected by a balanced optical bridge. The rotation is proportional to the magnitude of the THz electric field. By varying the time delay with of the probe pulse, the electric field of the THz can be measured. The THz spectrum is found by Fourier transforming the electric field and taking the square modulus.

THz transmission or reflection can be measured by placing a sample in the path of the terahertz and comparing the measured spectrum with a reference spectrum taken with no sample.

Terahertz-optical mixing spectroscopy

Anintense terahertz field (FEL beam) modulates an optical beam as it passes througha device. The modulation results in sidebands on the optical beam, separatedfrom the fundamental by an integer number of terahertz photons. As a magneticor electric field tunes the sample through a terahertz resonance, the sidebandpeaks. Recently, this technique was used to observe, for the first time, Autler-Townessplitting in a quantum well.

Fourier-Transform Infrared Spectroscopy (FTIR)

The FTIR is a Michelson interferometer used to measure infrared absorption of a sample. Our Bruker IFS 66v can be used in the near, mid and far IR, providing absorption spectra over an extremely wide spectral range (1-500um), using a combination of alkakli-halide and mylar beam splitters and InSb, HgCdTe (MCT), and bolometer detectors for detection.

The FTIR sends a collimated thermal source with a broad emmision spectrum through a sample and into a Michelson interferometer. The instrument sweeps the mirror in one arm of the interfermeter at a constant rate. An interferogram is produced by measuring the intensity at the output of the interferemeter as a function of time. For low-light measurements the interferogram can be built up by repeatedly stepping the mirror and collecting a single data point.

The frequency spectrum is obtained by taking the Fourier transform of the interferogram and subtracting it from a reference spectrum taken with no sample. Our FTIR is mainly used to measure FIR intraband absorption spectra of coupled quantum well and dots, but we can also use it to measure the thickness of wafers by measuring the spacing between Fabry-Perot fringes.

There are many tips and tricks on our particular machine, a Bruker IFS 66v.

Fabrication

The devices used in our experiments range from unprocessed bulkor expitaxial semiconductors to more complex structures involving multiple gates,ohmic contacts, anti-reflection coatings, waveguides, and antennas.