Unfortunately for me, the 1 Dimensional Luttinger Bose-Einstein Condensate
seems to have already been proposed, but as far as I can tell, not as an
explanation of cold fusion:
***Also perhaps here.

New Journal of Physics <http://iopscience.iop.org/1367-2630/> Volume 10
<http://iopscience.iop.org/1367-2630/10> April 2008
<http://iopscience.iop.org/1367-2630/10/4>

R Citro *et al* 2008 *New J. Phys.* *10* 045011
doi:10.1088/1367-2630/10/4/045011<http://dx.doi.org/10.1088/1367-2630/10/4/045011>
 Luttinger hydrodynamics of confined one-dimensional Bose gases with
dipolar interactions Focus on Quantum Correlations in Tailored
Matter<http://iopscience.iop.org/1367-2630/10/4/045001>

R Citro1, S De Palo2, E Orignac3, P Pedri4,5 and M-L Chiofalo6
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 Abstract <http://iopscience.iop.org/1367-2630/10/4/045011>
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Part of Focus on Quantum Correlations in Tailored
Matter<http://iopscience.iop.org/1367-2630/10/4/045001>

Ultracold bosonic and fermionic quantum gases confined to
quasi-one-dimensional (1D) geometry are promising candidates for probing
fundamental concepts of Luttinger liquid (LL) physics. They can also be
exploited for devising applications in quantum information processing and
precision measurements. Here, we focus on 1D dipolar Bose gases, where
evidence of super-strong coupling behavior has been demonstrated by
analyzing the low-energy static and dynamical structures of the fluid at
zero temperature by a combined reptation quantum Monte Carlo (RQMC) and
bosonization approach. Fingerprints of LL behavior emerge in the whole
crossover from the already strongly interacting Tonks-Girardeau at low
density to a dipolar density wave regime at high density. We have also
shown that a LL framework can be effectively set up and utilized to
describe this strongly correlated crossover physics in the case of confined
1D geometries after using the results for the homogeneous system in LL
hydrodynamic equations within a local density approximation. This leads to
the prediction of observable quantities such as the frequencies of the
collective modes of the trapped dipolar gas under the more realistic
conditions that could be found in ongoing experiments. The present paper
provides a description of the theoretical framework in which the above
results have been worked out, making available all the detailed derivations
of the hydrodynamic Luttinger equations for the inhomogeneous trapped gas
and of the correlation functions for the homogeneous system.

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