| [387] | 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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