Brillouin optical fiber sensor for cryogenic thermometry
a
Luc Thévenaz,
a
Alexandre Fellay,
a
Massimo Facchini,
b
Walter Scandale,
c
Marc Niklès,
a
Philippe A. Robert
a
EPFL Swiss Federal Institute of Technology, TOP-MET Laboratory of Metrology and Photonics,
CH-1015 Lausanne, Switzerland
b
CERN, LHC/MMS Division, CH-1211 Geneva 23, Switzerland
c
Omnisens SA, EPFL-PSE, CH-1015 Lausanne, Switzerland
ABSTRACT
Supraconductive installations are now commonly used in large facilities, such as power plants and particle accelerators.
This requires a permanent temperature control at very low temperature, but cryogenic temperature measurements in the
1-77K range requires expensive calibrated temperature probes.
We report here the possibility to use stimulated Brillouin scattering in optical fibres for temperature sensing down to
1K. Such a technique offers the additional advantage to make possible distributed measurement, so that very large
structures and systems can be controlled using a single fiber and a single analysing instrument. In addition only one by-
pass for the fiber is required as input to the cryogenic vessel, that is definitely a key advantage for the design and the
energy loss.
Brillouin scattering in optical fibers has never been investigated so far at temperature below 77K (nitrogen boiling
point). This absence of interest probably results from the constant decrease of scattering efficiency that was observed
while cooling the fiber down to 77K. Our measurements show the unexpected feature that scattering efficiency is
significantly raised below 50K and is even much better than observed at room temperature.
The relevance and the feasibility of the technique is demonstrated in real scale on the supraconductive magnets for the
future world largest particle accelerator, namely the large hadron collider (LHC) at CERN Laboratory in Geneva.
Keywords: optical fiber, cryogenic temperature, distributed sensor, Brillouin scattering.
1. INTRODUCTION
In the last twelve years, many papers dealing with Brillouin spectrum analysis for distributed strain or temperature
sensing in optical fibres have been published. Different operational set-ups have been proposed so far, some of them
being even commercially available. As far as temperature sensing is concerned, all these set-ups rely on the assumption
of a linear dependence of the measured Brillouin frequency shift on the temperature. This assumption – though
perfectly valid in the usual room temperature range – no longer holds in the domain discussed here.
Basically the Brillouin effect is a scattering of an incident lightwave by the acoustic phonons of a medium, the spectrum
of the scattered light containing key information about the vibrational properties of the considered medium. Practically
the centre of the Brillouin spectrum is directly proportional to the velocity of a vibration mode, while its linewidth is
related to its characteristic damping time. In the quasi-unidimensional geometry of single-mode optical fibres [1], the
Brillouin spectrum of the backscattered light is by far dominated by the resonance peak corresponding to the
fundamental longitudinal acoustic mode.
As mentioned above, in a fairly wide temperature range (-25°C - 80°C) covering most of the usual applications, the
Brillouin shift, that is the frequency difference between the incident and the scattered lightwaves, increases linearly,
with a slope coefficient around 1.36 MHz/°C at 1319 nm [2]. Over the same temperature range the resonance linewidth
steadily decreases.
As far as we know the low temperature domain has been much less studied by the fibre optics community.
Nevertheless, there are some large cryogenic installations where distributed temperature monitoring, and thus the use of
Brillouin effect in fibres, can be a valuable alternative. A particle accelerator, like the large hadron collider (LHC) under
Smart Structures and Materials 2002: Smart Sensor Technology and Measurement Systems
Daniele Inaudi, Eric Udd, Editors, Proceedings of SPIE Vol. 4694 (2002) © 2002
SPIE · 0277-786X/02/$15.00
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