Title: Villars 2004
1Villars 2004
- A Future Fixed Target Programme at
CERN?Conclusions of the SPSC Villars Meeting - 22nd-28th September 2004
- Ian C. Brock
- University of Bonn
2Outline
- Framework
- Machines and Beams
- Antiproton Physics
- Other Topics
- Flavour Physics
- Heavy Ions
- Soft and Hard Protons
- Neutrinos
3Charge
- to review present and future activities and
opportunities in fixed-target physics, and to
consider possibilities and options for a future
fixed target programme at CERN - globally important
- realistic (beams resources)
- short, intermediate, and long term
- From the Scientific Policy Committee
SPSC not in approval/rejection mode !
4Input and Timetable
- groups working on fixed target experiments at
CERN, and also groups which have in mind the
submission of proposals for such experiments, to
forward to the SPSC secretariat in due time a
short report indicating their ideas and plans for
the future - SPSC67 April 2004
- 11 submissions received
- COMPASS
- DIRAC Kp atoms
- CNGS
- September Villars
- December report to RB SPC
committed beyond 2005
5Programme
Date Morning Afternoon Afternoon
Wednesday Sept 22 CERN perspective accelerators MMWSPL HIF Heavy Ion 1
Thursday Sept 23 Heavy Ion 2 Neutrino 1 Neutrino 1
Friday Sept 24 Neutrino 2 Soft and hard hadron physics 1 Soft and hard hadron physics 1
Saturday Sept 25 Soft and hard hadron physics 2 Antiproton 1 Antiproton 1
Sunday Sept 26 Antiproton 2 HF 1 HF 1
Monday Sept 27 HF 2 Other Topics Discussion
Tuesday Sept 28 Summary, Discussion Conclusions
1 including presentations by convenors of
conclusions concerning physics directions
6Machines and Beams
7CERN 2004
8Users View of Future pre Villars04
? as heard by HIP from users
USER CERN COMMITMENT USERS WISHES USERS WISHES
USER Short term (low cost) Medium term (intermediate cost asap) Long term (high cost gt2013)
LHC Planned beams Ultimate luminosity Luminosity upgrades
FT (COMPASS) 7.2105 spills/y ? 7.2105 spills/y
CNGS 4.51019 p/year Upgrade 2
ISOLDE 1.92 mA Upgrade 5
Future n beams gt 2 GeV / 4 MW
EURISOL 1-2 GeV / 5 MW
Reference value for analysis
1350 pulses/h 3.21013 ppp
9Upgrades
- Beam loss irradiation _at_ high intensity
- multi-turn ejection from PS (island extraction)
- Period 0.6 s ? 0.9
s ? - gt cost gt
- worse PSB flexibility better
- Intensity/SPS pulse ? increase CNGS flux
- machine impedance (kickers, RF) ?
- injection energy ?
- bunching in the PS ?
only
10Fixed target ? CNGS
?FT CNGS share SPS cycles
CNGS request 4.5 1019 pot/year
FT request 7.2 105 spills/year
Without changes
Double batch Linac4
J
J
Double batch
?Impossible to meet FT CNGS demands
11Scope of Future Options
interest for interest for interest for interest for
LHC upgrade Neutrino physics beyond CNGS Radio-active ion beams (EURISOL) Others
Low energy 50 Hz RCS ( 400 MeV/2.5 GeV) Valuable Very interesting for super-beam beta-beam No ?
50 Hz SPL ( 2 GeV ) Valuable Very interesting for super-beam beta-beam Ideal Spare flux Þ possibility to serve more users
High energy 8 Hz RCS (30-50 GeV) Valuable Very interesting for neutrino factory No Valuable
New PS (30-50 GeV) Valuable No No Valuable
1 TeV LHC injector Very interesting for luminosity upgrade. Essential for LHC energyx2 No No Valuable
synergy
12Strategy (and action)
- Start 2004/5
- PS multi-turn ejection
- Increase SPS intensity (impacts all machines)
- 0.9s PSB repetition
- Linac 4 design
- ? construction decision _at_ end 2006
- Prepare decision on optimum future accelerator
- Study of a Superconducting Proton Linac (SPL)
- Alternative scenarios for the LHC upgrade
- Context for SPSC strategy and input
13Antiproton Physics
14AD
15Unique Ac Decelerator
16Unique Physics at CERN
- ASACUSA, ATRAP, ATHENA
- routine production of H
- antiprotonic He p e - ?
- Deceleration and capture of p
- Production of H and He
- yield !
- Spectroscopy ideally 1S 2S
- Present quantum states n30 !
-
-
-
-
CPT matter-antimatter
17Improvements ATRAP
- Status 4.2K antiprotons are routinely
accumulated - Cooling through matter
- Improvements?
- Needed much lower temperatures
- Desired more antiprotons to speed data
accumulation - Desired more antiprotons to improve
spectroscopy - signal-to-noise
- Decelerator? RFQD? ELENA?
- Would give the much larger antiproton rate
desired - Small ring would fit in AD hall
- New beam lines would be needed
- Magnetic fields from experimental apparatus
- Substantial cost
? New experiments AEGIS ALPHA coming
18ELENA
- A small machine for deceleration and cooling of
antiprotons after AD to lower energies around 100
keV is feasible - One to two orders of magnitude more antiprotons
can be available for physics. - Main challenges for the low energy decelerator
like ultra low vacuum, beam diagnostics and
effective electron cooling can be solved, using
experience of AD and member-state laboratories
where similar low energy ion machines are
operational (ASTRID, Aarhus CRYring, Stockholm).
- The machine can be located inside of the AD Hall
with only minor modifications and reshuffling of
the present installation. - Machine assembling and commissioning can be done
without disturbing current AD operation
19SPSC Conclusions (1)
- Opportunity for fundamental physics in the CPT
violation sector using cold antiprotons - CERN is the only place in the world to explore it
and has attracted many external users - Important scientific and technological milestones
have been achieved - routine production of H
- anti-protonic He spectroscopy
- Strong recommendation to continue the AD program
after 2005 and to implement an improved beam
switching between experiments - Installation of the additional deceleration ring
ELENA would greatly increase the effectiveness of
current experiments and offer a long term program
using very cold intense anti proton beams
-
20SPSC Conclusions (2)
- Different potential signals of CPT violation
should be explored - A variety of approaches to trap ground state H
should continue to be pursued without
compromising the effective use of available
resources - Synergy between the different experiments is
strongly encouraged - A roadmap should be available in each
collaboration describing the medium and long term
future (with and without ELENA) towards the
important goal of H spectroscopy
-
-
21Other Projects
22SPSC Conclusions (1)
- Axions (CAST)
- The Collaboration has produced the best limits
to date on the production of axions. It is
interesting to note that an important and
substantial enhancement in sensitivity can be
achieved in the future by taking data with a 4He
and 3He gas fill. There are also interesting new
possibilities for developing further the
experimental techniques at CERN, in particular
associated with new developments concerned with
production of axions where a laser experiment is
claiming unexpected results. The SPSC encourages
the collaboration to continue to develop its
ideas and its methods. - AD4 p therapy
- The work continues to develop its understanding
of the details of the radiation damage of
biological matter. In particular the techniques
concerned with dosimetry and monitoring which are
used continue to be improved. The SPSC notes that
in the future the scope of the project could mean
that increased resources are necessary from CERN.
-
23SPSC Conclusions (2)
- Electrodynamics in Critical Crystalline Fields
- An interesting new proposal for a measurement of
trident production in a critical field was
presented. It was not clear to the SPSC quite how
the proposed measurement would contribute to the
understanding and exploitation of such physics in
the context of CERNs scientific programme. - (g-2)µ
- The SPSC considers that precision measurements of
(g-2)µ continue to be an important part of
understanding physics at the energy frontier.
Since the completion of the last (g-2)µ
experiment at BNL, which itself followed the
pioneering experiment at CERN, it is not yet
possible to foresee a new European initiative in
the immediate future. However, the SPSC notes
that the development of a major new programme of
muon and neutrino physics at CERN will make major
new opportunities possible.
Present CERN resource level appropriate
24Flavour Physics
25Flavour Physics (Kaon Physics)
- ?Precision measurements of rare flavour decays
probe the energy scale, and then flavour
structure, of new physics - - no SM tree
- - SM suppression
- - short distance dynamics
FCNC
?Experimental challenge BR 10-10 to 10-11
- ? 10 crucial for
- new LHC physics
26Landscape
27NA48/3
- 2004
- Launch GIGATRACKER RD
- Vacuum tests
- Evaluate straw tracker
- Start realistic cost estimation
- Complete analysis of beam-test data
- 2005
- Complete of the above
- Complete specifications
- Submit proposal to SPSC
- 2006-2008
- Construction, installation and beam-tests
- 2009-2010
- Data taking
p ? ion NA48/3 ? COMPASS
80 K ? p??
28SPSC Conclusions (1)
- There is a strong physics case for pursuing an
ambitious programme of kaon physics at CERN,
exploiting the high-energy proton beams available
at the SPS for decay-in-flight rare kaon decay
measurements. Building on its great expertise in
high-intensity neutral and charged kaon beams and
on the outstanding physics achievements of the
NA48, NA48/1 and NA48/2 experiments in the last
decade, CERN should remain in the future a major
laboratory for kaon physics at the sensitivity
frontier. - The SPSC welcomes the expression of interest for
a precise measurement of the K ? pvv
transition. According to present studies the
proposed experiment appears competitive in the
context of the worldwide kaon physics program.
The goal is to detect more than 100 signal events
over two years starting in 2009. A major upgrade
of the present NA48/2 setup is necessary and the
needed RD and detector developments should be
supported.
29SPSC Conclusions (2)
- In a longer term future CERN could aim at
precision measurements in the neutral channels,
K0L ? p0ee- and K0L ? p0vv, which by then may
have been observed elsewhere. - The SPSC takes note of the extended, compelling
and competitive kaon program that could be made
possible by a new high-intensity (MMW)
high-energy proton machine.
30SPSC Conclusions (3)
- The NA60 Collaboration has developed over the
years a high-precision detector, comprising a
muon spectrometer coupled with a silicon-pixel
vertex telescope, capable of handling large track
multiplicities. The SPSC takes note of the
opportunity of exploiting the excellent di-muon
mass and vertex position resolution of the NA60
detector to search for rare open charm decays in
p-U collisions, including the highly-suppressed
D0 ? µµ- decay. The feasibility of observing or
setting a competitive limit for this decay with
the proposed experiment still needs to be
demonstrated.
31Heavy Ions
32SPbS Panorama
? expt _at_ SPbS theory ? QGP
B. Mueller
33Chromodynamic Phase Equilibria
? SPS _at_ phase transition
34Critical Point
? theoretical guidance model dependent
Stephanov
35North Area Heavy Ions gt2005
After the long shut-down ions will be injected
into the SPS via LEIR. The LEIR project has been
launched for filling the LHC with ions. Filling
the SPS instead will require more resources.
If the ions are required for the SPS fixed target
program and if the required resources are made
available, one might expect to get
- Lead ions from 2009 (after PS-SPS-LHC ions
running-in) - Other (lighter) ions depending on LHC ion
physics program.
It should be noted that many relevant
non-radioactive ion species are possible in
principle, but with significant preparation time
and effort. Note that North Area and LHC ions are
exclusive if not the same ion
Possible intensities are up to 109 Pb54 from
LEIR per transfer (3.6 sec). They can be limited
in LEIR with an interlock based on a BCT
measurement. Limitation of flux in EHN1 requires
new TAX blocks (up to 300 kCHF/beam).
36Low Mass Dileptons
? Excess dileptons thermal radiation ?
s
400 GeV
NA60
CERES/NA45
Mee
Mµµ
37Input Elements for SPSC Conclusions
- The CERN fixed target programme with heavy ions
has, by any measure, been a spectacular success.
CERN results have contributed to the development
of theoretical interpretations of the
measurements in terms of a phase change in
hadronic matter to quark-gluon, coloured, degrees
of freedom. - Recent developments confirm that heavy ion beams
at the CERN SPS energies and luminosity remain an
ideal tool to observe the features of the phase
transition whereas higher energy machines are
better suited to study the properties of this new
state of matter.
38- NA49
- High pT suppression, a potential signature of jet
quenching in the QGP, is a highlight of the RHIC
heavy ion results. It has not yet been properly
addressed at SPS energies. - In light of this, the NA49 Pb-Pb data should be
reanalysed. Only then could a proton run for
reference data be considered. These data would
clarify the interplay between the Cronin effect
and high pT suppression.
- NA60
- Steady developments in radiation hard detectors
have resulted in more refined measurements. In
particular, recent results from NA60 show the
improvements that can be made using a pixel
vertex telescope. - The p and In data from NA60 should provide
answers to a set of open questions (open charm,
rho mass shift, thermal radiation) arising from
previous experimental CERN results. - Their requested Pb-Pb data would extend the
measurements to the highest energy densities
available at the SPS
39SPSC General Recommendations
- A major step in the field would certainly be
achieved through the challenging observation of
the critical point of the QCD phase transition.
In addition, QCD lattice calculations are
expected to constrain better its position in the
next few years - Signatures have to be refined and quantified and
the corresponding experimental signal, or
signals, have to be understood theoretically. In
addition, the experimental sensitivity for such
measurements must be optimised - The opportunity to pursue a heavy ion physics
program at the CERN SPS within the framework and
constraints imposed by the LHC should be
preserved. Once the LHC has been commissioned
with ions, an SPS programme aimed at the study of
rare process signatures and important specific
issues such as the identification of the critical
point as well as the study of its properties
would be possible
40Soft and Hard Hadron Physics
41Hadron Physics
H1 ZEUS - DESY
- Energy frontier
- Colliders
- Precision frontier
- Colliders FT
- Intensity frontier
- Theoretical symbiosis
- Lattice
- ChPT
- pQCD
GSI
? CDF D0 - FNAL
? BABAR - SLAC
42COMPASS
- 1996 Proposal
- 1997 Conditional approval
- 1999 2000 Construction and installation
- 2001 Commissioning run
- 2002 -2004 Data taking µp and µp
- Precision hadron structure
- nucleon spin structure (valence ? sea)
- Precision hadron dynamics
- pQCD ? n-pQCD (Q2, pT2)
- resonant phenomena
- Into the future GPDs and precision structure
functions
? ?
? ??
approved
gluons
43COMPASS ?G/G
?Finding charm
c
s(?G/G) proposal 0.14
c
200234 s(?G/G) 0.24
??G/G from high pT hadrons pairs
-
44DIRAC
?pp and Kp atoms - scattering lengths
- ?PT
? Ke decay
? excess at very small pL and pT
atomic pairs
? data 2001 2003 (PS) ? setting up 2006 (PS) ?
running 2007/8 (PS) ? planning gt 2008 (SPS ?)
free pairs
? experimental theoretical uncertainty _at_ SPS
45SPSC Conclusions (1)
- The PS/SPS facility is competitive worldwide,
even with the advent of new machines. It allows
CERN to have significant impact in the
understanding of the strong interaction in low
and high energy domains (Lattice QCD, ChPT and
pQCD). - The COMPASS experiment plays an important role in
the CERN fixed target program with the SPS beam.
The experiment should complete in the medium term
their original proposal (especially ?G/G, as well
as transversity, polarisabilities and hadron
spectroscopy). The SPSC is concerned about a
possible shortage of protons, and thus encourages
the collaboration to prioritise their physics
program. - In the longer term, a new programme of
measurements is proposed. The GPD determinations
would be in a unique kinematical domain. The
remaining part of the programme concerns
structure function measurements using lepton DIS
and Drell Yan.
46SPSC Conclusions (2)
- The physics case for the DIRAC experiment,
including its extension at the PS which has
already been recommended for approval by the
SPSC, is important. For the longer term, with
installation of the existing set-up at the SPS,
it would be possible to reach a precision
matching the theoretical predictions. - The SPSC took note of an Expression of Interest
to measure lepton flavor violation in the µ-t
sector(µN ? t N) using the SPS. - The SPSC is not convinced that the part of the
conceivedp-A NA49 program related to the
pentaquark search can lead to a significant
advance.
47SPSC Conclusions (3)
- In 2006, until OPERA is ready to take physics
data with its nominal target mass, it is
important to take advantage of the opportunity to
complete as much as possible of the remaining
approved COMPASS physics programme. To this end,
it is important that beam delivery starts as
early as possible in 2006. At the same time, it
is also important that COMPASS optimise its
overall physics efficiency. Beyond 2006, the SPSC
encourages solutions allowing the delivery and
use of the maximum numbers of protons to satisfy
the completion of physics experiments using the
SPS/PS beams. - In the longer term future, it is interesting to
note that any high intensity facility at CERN
will make possible new opportunities for hadron
physics using neutrino and muon beams.
48Neutrinos
49?-oscillations
50Hierarchy
Solar KamLAND
Super-K
51CERN ? LNGS CNGS
52CERN ? LNGS CNGS
CERN Commitment 5 x 4.5 1019 protons on target
53OPERA
? Ready end 2006
2 kTon (Pb) 0.04 kTon emulsion
56 emulsion films / brick
- for the full detector
- 2 supermodules
- 31 walls / supermodule
- 52 x 64 bricks /wall
- 200 000 bricks
9 kt-yr
?m21.2x10-3 eV2 2.7 events ?m22.4x10-3 eV2 11
events ?m25.4x10-3 eV2 54 events
54ICARUS
1.8kT ready end 2007? Statistics and background
with 3kT similar to OPERA
LAr drift
n
muon spectrometer 2 kton Fe B1.8 T
3m
55Next ?
56 T2K
57Strategy
- High statistics by high intensity n beam
- Tune En at oscillation maximum
- Sub-GeV n beam
- Low particle multiplicity suited for Water
Cherenkov - Good En resolution dominated by nm n? m p
- Narrow band beam to reduce BG
0.75MW 50GeV-PS
Off-Axis n beam
Super-Kamiokande
58Slide from M. Lindroos
59Megatonne ?
60Towards Neutrino Factory Horizon
?13
CP sensitivity
61SPL Proposed Roadmap
- Consistent with the content of a talk by L.
Maiani at the Celebration of the Discovery of
the W and Z bosons. Contribution to a document
to be submitted to the December Council (CERN
Future Projects and Associated RD). - Assumptions
- construction of Linac4 in 2007/10 (with
complementary resources, before end of LHC
payment) - construction of SPL in 2008/15 (after end of LHC
payments)
Linac 4 approval
SPL approval
LHC upgrade
Warning Compressor ring and detector (8 years)
are not quoted Protons from the SPL ready
in 2015
62Proton Driver ? ?
Mezzetto
? expensive ? likelihood improves with
synergy ? ? beam RD for new technology -
target - cooling (MICE) ? ?e - ß beam ?µ -
superbeam ? ? Fact
63CNGS Proton Budget
- CERN committed to delivering 5x4.51019 p.o.t. to
CNGS aimed at uniquely demonstrating t
appearance. The physics case remains as valid as
it was at the time of approval, and therefore
CERN should make every reasonable effort to
fulfill this commitment. However, no compelling
scientific case has been offered for CERN to
increase the scope of this commitment. - It appears that with the current machine
performance it is not possible to simultaneously
satisfy CNGS and COMPASS. We therefore consider
it very important that efforts continue to
achieve more available p.o.t., including the
earliest practicable implementation of multi-turn
extraction. The experiments should be prepared
for a longer running period than originally
planned to achieve their allocation of p.o.t. - On current schedule the full OPERA detector will
not be completely ready in early 2006, implying
that the most efficient use of the available
p.o.t. will be for the COMPASS programme until
OPERA is fully constructed later in 2006. - NEW 60 of ICARUS could be ready at end of 2007
64CERN participation in the development of future
neutrino facilities
- Future neutrino facilities offer great promise
for fundamental discoveries (such as CP
violation) in neutrino physics, and a post-LHC
construction window may exist for a facility to
be sited at CERN. - CERN should arrange a budget and personnel to
enhance its participation in further developing
the physics case and the technologies necessary
for the realization of such facilities. This
would allow CERN to play a significant role in
such projects wherever they are sited. - A high-power proton driver is a main building
block of future projects, and is therefore
required. - A direct superbeam from a 2.2 GeV SPL does not
appear to be the most attractive option for a
future CERN neutrino experiment as it does not
produce a significant advance on T2K. - We welcome the effort, partly funded by the EU,
concerned with the conceptual design of a beta
beam. At the same time CERN should support the
European neutrino factory initiative in its
conceptual design.
65CERN participation in the development of future
neutrino facilities
- Detectors new detector technologies are
necessary to take full advantage of the physics
capabilities of future neutrino facilities. - Examples of needed advances are cheaper, higher
efficiency, large-area, light sensors and
magnetized detectors capable of distinguishing
electrons from positrons. - Given its central role as Europes particle
physics laboratory, CERN should support,
participate, and coordinate such technical
developments.
We did not discuss CLICCERN has to decide on
relative priorities forCLIC and/or Neutrino
Factory
66Other Experiments
- Hadron Production
- Further hadron production experiments
specifically designed to meet the needs of
neutrino experiments are essential. - There are several existing CERN detectors which
could, with some modifications, fulfill this
requirement. This would be a scientifically
important and cost-effective use of CERN
resources. - C2GT
- This is an interesting idea which would require
substantial technical development before its
feasibility could be demonstrated. It also
requires modifications to the CNGS beamline. No
such modifications should be made until CERNs
existing commitment to the CNGS programme has
been met. By that time C2GTs competitiveness
would be doubtful.
67Fixed target physics at CERN? (1)
- 2011 Physics vibrant, important, leading
- SPS p.o.t ?
- schedule/prioritise/improve
- Completion of hadron program essential
- CNGS window before T2K
- Hadron production for ? physics
- ionion 2009 (synergy with LHC)
- Rare flavour 2009 (synergy with LHC)
- Fundamental physics with p atoms (medical)
-
increasing p.o.t
68Fixed target physics at CERN? (2)
- gt2011 Physics must be vibrant, important,
leading - ionion 2009 (synergy with LHC)
- Rare flavour 2009 (synergy with LHC)
- Fundamental physics with p atoms
- Hadron structure GPDs
- dynamics low energy, resonance
- ? physics evaluation RD _at_ CERN
- p-driver ? superbeam ? detector
- global context ? NF
-
if appropriate ?
synergies with other science? SPL?
All but HI benefit from/require high
intensity RCPSB RCPS