| 1 | \section{Schedule}
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| 2 |
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| 3 | The following table presents an optimal schedule for the
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| 4 | European project taking into account the key date of the completion
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| 5 | of the new tunnel excavation around 2010. Soon after, CERN will have to decide
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| 6 | its post-LHC strategy, while nuclear physicists will hopefully choose CERN as
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| 7 | the host laboratory for the EURISOL project.
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| 8 | We would also like to stress that
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| 9 | the schedule of the neutrino beams from CERN is not constraining the
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| 10 | start of the other non accelerator items of research.
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| 11 | \begin{figure}[htb]
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| 12 | \vspace{4cm}
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| 13 | \epsfig{figure=./figures/sch_new.eps,width=\textwidth,angle=0}
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| 14 | %\epsfig{figure=./figures/sch.eps,width=0.6\textwidth,angle=-90}
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| 15 | \end{figure}
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| 16 |
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| 17 | \newpage
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| 18 | \section{Conclusions}
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| 19 | In conclusion a megaton scale
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| 20 | Water \v{C}erenkov detector at the Frejus site will address a series of
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| 21 | fundamental issues :
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| 22 | \begin{itemize}
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| 23 | \item explore the nucleon decay with a sensitivity an order of magnitude
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| 24 | better than current limits on different channels
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| 25 | \item in the case of a galactic or near galactic supernova explosion,
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| 26 | track the explosion in unprecedented detail providing at the same time
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| 27 | information on the third oscillation angle beyond what is currently
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| 28 | achievable in terrestrial experiments
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| 29 | \item provide a trigger for supernova explosions
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| 30 | for other astroparticle detectors for supernova exploding in a range of up to
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| 31 | 3 Mpc, knowing that 1 supernova explosion per year is expected
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| 32 | within a distance of
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| 33 | 10 Mpc
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| 34 | \item provide a 4 sigma detection of diffuse supernova
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| 35 | neutrinos after 2-3 years of operation
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| 36 | \item in association with a superbeam and betabeam from CERN
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| 37 | obtain a sensitivity to the third oscillation angle down to
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| 38 | $\sin^2(2\theta_{13}) \sim 10^{-4}$ and detect maximal CP violation at 3 sigmas
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| 39 | for $\sin^2(2\theta_{13})$ larger than $3\cdot 10^{-4}$
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| 40 | \end{itemize}
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| 41 | A series of other physics topics, not mentioned here, will also be adressed\,:
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| 42 | for instance neutrino physics, as well as
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| 43 | interdisciplinary topics in rock mechanics, geobiology, geochemistry,
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| 44 | geohydrology, geomechanics and geophysics that could benefit
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| 45 | from a large scale underground excavation.
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| 46 |
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| 47 | We believe that our project compares favorably with other similar
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| 48 | projects around the world, and should be seriously considered as a
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| 49 | very attractive major European project after the LHC. The proposed
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| 50 | strategy is thus the following: a megaton-scale detector could be
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| 51 | installed at Fr{\'e}jus and start physics in 2018. It would start
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| 52 | proton decay and supernova searches, which would last several
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| 53 | decades. As soon as the neutrino beam from SPL is available,
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| 54 | neutrino oscillation studies can start, and the advent of a beta beam
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| 55 | would increase significantly the performances of the detector.
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| 56 |
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| 57 | The signatories are eager to see the MEMPHYS project
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| 58 | come to life. They are aware that the actual location of a megaton detector
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| 59 | will depend on many issues, in particular the share of future big equipments
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| 60 | (such as linear colliders) worldwide. They are prepared to do the proposed
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| 61 | physics in any country, and have already set up collaborations with their
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| 62 | japanese and american colleagues. An inter-regional yearly (US-Europe-Japan)
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| 63 | workshop series NNN-XX (Next generation of Nucleon decay and Neutrino Physics
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| 64 | detectors) organizes and structures this convergence of interests.
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| 65 | The authors of this document hope however that Europe will not
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| 66 | miss a unique opportunity to keep a leading role in the underground physics,
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| 67 | complementary to the Gran Sasso.
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| 68 |
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| 69 | Furthermore, it is obvious that the current proposal is complementary
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| 70 | to other proposals for large undergrounds detectors using
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| 71 | liquid scintillator (LENA) or liquid argon technologies (GLACIER)
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| 72 | in order to pursue the same physics goals.
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| 73 | The advantage of the water \v{C}erenkov technique lies on the possibility
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| 74 | to instrument very large masses, while liquid argon detectors
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| 75 | can have an excellent resolution and liquid scintillators
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| 76 | very low detection thresholds for neutrino physics.
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| 77 | On the technology side the water \v{C}erenkov seems a straightforward
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| 78 | extension of the existing techniques while for instance the liquid argon
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| 79 | option presents daring technological challenges. The realisation of the
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| 80 | complementarities in physics potential and the common R\&D issues
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| 81 | (large underground caverns and containers: excavation issues and safety,
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| 82 | large area low cost photodetection and electronics,
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| 83 | purification and background issues, interdisciplinary issues, etc.)
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| 84 | prompted the proponents of the above solutions to start federating
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| 85 | their efforts in order to exploit the possible synergies in view of
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| 86 | common future proposals to the European Union ~\cite{Laguna}
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| 87 | and elsewhere.
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| 88 |
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| 89 |
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| 90 |
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| 91 | \section {Acknowledgements}
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| 92 |
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| 93 | The authors would like to thank the engineers of the IN2P3-CNRS laboratories,
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| 94 | especially Ch. de La Taille (LAL) and J. Pouthas (IPNO),
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| 95 | for their decisive contributions.
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| 96 |
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| 97 |
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