Superconducting
Quantum Interference Proximity Transistor
Francesco
Giazotto
NEST CNR-INFM and Scuola Normale Superiore, Piazza dei
Cavalieri 7, I-56126 Pisa, Italy
Proximity effect [1] is a phenomenon which can be described as the
induction of superconducting correlations into a normal-type conductor. One
striking consequence of this effect is the modification of the local density of
states (DOS) in the normal metal [2],
and the opening of a minigap whose amplitude can be
controlled by changing the macroscopic phase of the superconducting order
parameter [3]. Proximity effect was
experimentally demonstrated in mesoscopic hybrid
structures at milliKelvin
temperatures both in transport measurements [4]
as well as recently with scanning tunneling microscopy (STM) [5]. Here we
report the realization of a novel interferometer, the superconducting quantum
interference proximity transistor (SQUIPT), whose operation relies on the
modulation with the magnetic field of the DOS of a proximized
metal embedded in a superconducting loop. Flux sensitivities down to ~10-5
F0/Hz-1/2 (F0 » 2´10-15 Wb
is the flux quantum) can be achieved even for a non-optimized design, with an
intrinsic dissipation which is several orders of magnitude smaller than in
conventional superconducting interferometers. Optimizing the device parameters
promises to largely increase the sensitivity for the detection of tiny magnetic
fields. The SQUIPT has a number of
features which make it attractive for a variety of applications: (1) only a
simple DC read-out scheme is required, similarly to DC SQUIDs;
(2) either current- or voltage-biased measurement can be conceived depending on
the setup requirements; (3) a large flexibility in the fabrication parameters
and materials, such as semiconductors, carbon nanotubes
or grapheme instead of normal metals, is allowed to optimize the response and
the operating temperature; (4) ultralow dissipation (~1-100 fW)
which makes it ideal for nanoscale applications; (5)
ease of implementation in a series or parallel array for enhanced output; (6)
ease of integration with superconducting refrigerators [6]
to actively tune the device working temperature. This approach opens the way to
magnetic-field detection based on ``hybrid'' interferometers which take
advantage of the flexibility intrinsic to proximity metals.
References
[1] P. G. de Gennes, Superconductivity of Metals and Alloys
(W. A. Benjamin, New York, 1966).
[2] W. Belzig, C. Bruder, and G. Schön, Phys. Rev. B 54,
9443 (1996).
[3] W. Belzig, F. K.
Wilhelm, C. Bruder, G. Schön,
and A. D. Zaikin, Superlattices
Microstruct. 25, 1251 (1999).
[4] S. Guéron, H. Pothier, N. O. Birge, D. Esteve, and M. H. Devoret, Phys. Rev. Lett. 77, 3025 (1996).
[5] H. le Sueur, P. Joyez, H. Pothier, C. Urbina, and D. Esteve, Phys. Rev. Lett. 100,
197002 (2008).
[6] F. Giazotto, T. T. Heikkilä, A. Luukanen, A. M. Savin, and J. P. Pekola, Rev. Mod. Phys. 78,
217 (2006).