486 research outputs found
Investigation of the determination of optical properties with the use of integrating spheres and an inverse adding doubling algorithm
Direct demonstration of circulating currents in a controllable -SQUID generated by a 0 to transition of the weak links
A controllable -SQUID is a DC SQUID with two controllable
-junctions as weak links. A controllable -junction consists of a
superconducting - normal metal - superconducting Josephson junction with two
additional contacts to the normal region of the junction. By applying a voltage
over these contacts it is possible to control the sate of the junction,
i.e. a conventional (0) state or a -state, depending on the magnitude of
. We demonstrate experimentally that, by putting one junction into a
-state, a screening current is generated around the SQUID loop at integer
external flux. To be able to do this, we have fabricated controllable
-junctions, based on Cu-Nb or Ag-Nb, in a new geometry. We show that at
1.4 K only the Nb-Ag device shows the transition to a -state as a function
of consistent with theoretical predictions. In a controllable SQUID
based on Nb-Ag we observe, a part from a screening current at integer external
flux, a phase shift of of the oscillations under suitable
current bias, depending on the magnitude of .Comment: 11 pages, 12 figures, subm. to Phys. Rev.
The controllable pi - SQUID
We have fabricated and studied a new kind of DC SQUID in which the magnitude
and sign of the critical current of the individual Josephson junctions can be
controlled by additional voltage probes connected to the junctions. We show
that the amplitude of the voltage oscillations of the SQUID as a function of
the applied magnetic field can be tuned and that the phase of the oscillations
can be switched between 0 and in the temperature range of 0.1 - 4.2 K
using a suitable control voltage. This is equivalent to the external
application of (n+1/2) flux quantum.Comment: 3 Figures, submitted to Applied Physics Letter
Terahertz hot electron bolometer waveguide mixers for GREAT
Supplementing the publications based on the first-light observations with the
German Receiver for Astronomy at Terahertz frequencies (GREAT) on SOFIA, we
present background information on the underlying heterodyne detector
technology. We describe the superconducting hot electron bolometer (HEB)
detectors that are used as frequency mixers in the L1 (1400 GHz), L2 (1900
GHz), and M (2500 GHz) channels of GREAT. Measured performance of the detectors
is presented and background information on their operation in GREAT is given.
Our mixer units are waveguide-based and couple to free-space radiation via a
feedhorn antenna. The HEB mixers are designed, fabricated, characterized, and
flight-qualified in-house. We are able to use the full intermediate frequency
bandwidth of the mixers using silicon-germanium multi-octave cryogenic
low-noise amplifiers with very low input return loss. Superconducting HEB
mixers have proven to be practical and sensitive detectors for high-resolution
THz frequency spectroscopy on SOFIA. We show that our niobium-titanium-nitride
(NbTiN) material HEBs on silicon nitride (SiN) membrane substrates have an
intermediate frequency (IF) noise roll-off frequency above 2.8 GHz, which does
not limit the current receiver IF bandwidth. Our mixer technology development
efforts culminate in the first successful operation of a waveguide-based HEB
mixer at 2.5 THz and deployment for radioastronomy. A significant contribution
to the success of GREAT is made by technological development, thorough
characterization and performance optimization of the mixer and its IF interface
for receiver operation on SOFIA. In particular, the development of an optimized
mixer IF interface contributes to the low passband ripple and excellent
stability, which GREAT demonstrated during its initial successful astronomical
observation runs.Comment: Accepted for publication in A&A (SOFIA/GREAT special issue
Fluctuations in the electron system of a superconductor exposed to a photon flux
We report on fluctuations in the electron system, Cooper pairs and
quasiparticles, of a superconducting aluminium film. The superconductor is
exposed to pair-breaking photons (1.54 THz), which are coupled through an
antenna. The change in the complex conductivity of the superconductor upon a
change in the quasiparticle number is read out by a microwave resonator. A
large range in radiation power can be chosen by carefully filtering the
radiation from a blackbody source. We identify two regimes. At high radiation
power, fluctuations in the electron system caused by the random arrival rate of
the photons are resolved, giving a straightforward measure of the optical
efficiency (48%). At low radiation power fluctuations are dominated by excess
quasiparticles, the number of which is measured through their recombination
lifetime
Ballistic reflection at a side-gate in a superconductor-semiconductor-superconductor structure
We have fabricated a sub-micron-sized structure consisting of an InAs-based
2DEG, two narrow Nb leads and a gate, where the indirect ballistic transport
between the non-oppositely superconducting contacts can be controlled by the
voltage applied to the gate. This new kind of tuneable junction can be used for
applications and allows several fundamental questions related to the transport
mechanism to be studied. First results of experiments carried out in this
respect are presented.Comment: 6 pages, 4 eps-figure
Microwave-induced excess quasiparticles in superconducting resonators measured through correlated conductivity fluctuations
We have measured the number of quasiparticles and their lifetime in aluminium
superconducting microwave resonators. The number of excess quasiparticles below
160 mK decreases from 72 to 17 m with a 6 dB decrease of the
microwave power. The quasiparticle lifetime increases accordingly from 1.4 to
3.5 ms. These properties of the superconductor were measured through the
spectrum of correlated fluctuations in the quasiparticle system and condensate
of the superconductor, which show up in the resonator amplitude and phase
respectively. Because uncorrelated noise sources vanish, fluctuations in the
superconductor can be studied with a sensitivity close to the vacuum noise
- …