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CRYSTAL COLLIMATION EXPERIMENT AT THE TEVATRON Nikolai Mokhov Fermilab

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Title: CRYSTAL COLLIMATION EXPERIMENT AT THE TEVATRON Nikolai Mokhov Fermilab


1
CRYSTAL COLLIMATION EXPERIMENTAT THE TEVATRON
Nikolai MokhovFermilab
US LHC Accelerator Research Program
bnl - fnal- lbnl - slac
LARP Collaboration Meeting SLAC October 17-19,
2007
2
OUTLINE
  • Introduction
  • Mission Statement
  • Crystal Collimation
  • Studies at Tevatron
  • Proposal for Experiment
  • Tevatron Study Plan
  • Deliverables
  • Collaboration, LOI and Meeting at Fermilab

See also next talks by Dean on measurements and
findings at Tevatron, and by NM on status of the
proposal and contributions
3
INTRODUCTION
  • The promise of bent crystal channeling technique
    for beam halo collimation at high-energy
    colliders was recognized at the SSC in 1991. A
    bent crystal, serving as a primary element,
    coherently bends halo particles onto a secondary
    collimator. First successful measurements were
    performed at IHEP in 1998 for 1 to 70 GeV
    protons. Crystal collimation was studied at RHIC
    in 2003. Experiments by IHEP, CERN, BNL and FNAL
    have shown that crystals are heat- and
    radiation-resistant. Deflection efficiency
    deteriorates at about 6/1020 p/cm2 rate.
  • Based on realistic modeling (1999, 2003), it was
    proposed to implement a bent crystal into the
    Tevatron collimation system. First measurements
    (2005-2006) were quite encouraging.

4
MISSION STATEMENT

We propose an experiment at Fermilabs Tevatron
to measure the predicted improvement in
collimation efficiency that could be obtained by
replacing amorphous primary collimators with bent
crystals. Considering the unique possibility
provided by the Tevatron Collider, and having
already established fruitful collaborative
efforts on crystal characterization, tests and
use for collimation, we propose to test and
confirm models of multi-turn dynamics with
crystals by exploiting channeling and newly
understood phenomena such as volume reflection as
well as to further study collimation.
5
MISSION STATEMENT (contd)

In our view, this is a necessary first step to
being able to evaluate an engineering
implementation of this technique in LHC that - if
proven - promises an enhanced performance of the
LHC collimation system with a reduced impedance
and easier implementation for heavy-ion beam halo
cleaning. There is also an interest in crystal
channeling from the ILC and Muon Collider
communities.
Collimation including crystal channeling is
the first item on Oliver Brunings Accelerator
Physics wish list for LARP
6
Two-Stage Collimation with Target and Crystal
Courtesy R. Assmann
7
BENT CRYSTAL FOR TEVATRON COLLIMATION
  • We have shown (PAC99) and later confirmed (2003)
    that implementation of a silicon bent crystal
    instead of amorphous primary collimators
    (targets), can improve the Tevatron collimation
    efficiency defined then as a reduction of beam
    loss in CDF - by a factor of
  • 2 with one (horizontal) target replaced, and with
    contribution from beam-gas scattering
    unsuppressed
  • 3 with one (horizontal) target replaced, and with
    contribution from beam-gas scattering suppressed
  • up to a factor of 4 to 6 for the 2-plane
    collimation.

8
REPLACING PRIMARY COLLIMATOR WITH CRYSTAL AT 5 s
(2005)
The primary H-collimator (D49 tungsten L-shaped
target) is before the dog-leg at bH96 m, D2.3
m. The crystal is in the dog-leg at bH73 m,
D2.5 m, about the same phase advance wrt
secondary collimators.
O-shaped 110 Si-crystal 5-mm L, 5 mm H, 1mm
V critical angle 5 mrad bending angle 439
mrad miscut angle 465 mrad
9
980-GEV BEAM CHANNELING DATA vs THEORY
Oct. 6, 2005 By Dean Still
Jan. 31, 2006
With E03H out, LE033C BLM is proportional
to nuclear interact. rate in crystal
Channeled beam peak width is 224 mrad (rms)
10
COMPARING EFFECTS OF PROTON HALO LOSSES FOR BENT
CRYSTAL AND TUNGSTEN TARGET
Crystal aligned at peak (118 mrad)
CDF
E03 BLM
PIN
11
OUTCOME OF 2005-2006 MEASUREMENTS
  • When using the crystal
  • A factor of 2 is achieved in better reduction of
    CDF losses a half a ring or three kilometers
    downstream (in agreement with modeling).
  • The secondary collimator could remain further (1
    mm or so) from the beam thus reducing impedance.
  • Nuclear interaction rate in the crystal was 2 to
    3 times lower compared to the amorphous target,
    reducing proportionally irradiation of the
    downstream components.

12
VOLUME REFLECTION
This work at RHIC/FNAL uncovered the importance
of the long neglected coherent crystal effect
predicted at Tomsk two decades ago, volume
reflection.
  • Contrary to channeling, which is extremely
    sensitive to beam-crystal alignment (10-mrad
    level in Tevatron), VR is a much higher
    acceptance effect promising as a collimation
    tool for TeV beams as well as for Recycler
    (Project X) and a muon collider!
  • The IHEP/PNPI/RHIC/FNAL investigation has helped
    to spark interest in the volume reflection
    process including a fast track investigation in
    the H8 400-GeV p beam at the CERN SPS in the fall
    of 2006 (W. Scandale et al.). That precision
    investigation has produced a spectacular
    confirmation of volume reflection (97
    efficiency) and also developed tools to
    characterize crystals that could potentially
    serve as LHC collimators.

13
Towards Crystal Collimation Collaboration
  • Encouraged by these results and recent crystal
    developments, and aiming at a high-performance
    collimation vital for the LHC, crystal
    collimation collaboration has non-formally
    started in December 2005
  • Better crystals characterized mechanically,
    optically and with beams
  • Beam tests at the SPS extracted beams (400 GeV)
  • Crystal collimation experiment in the SPS ring
  • Support crystal collimation expt at Tevatron to
    guarantee its success
  • In Dec. 2005, consensus on the Tevatron
    experiment was reached
  • The old crystal needs to be replaced with the
    optimal characterized one with a bending angle of
    about 0.15 mrad.
  • Dedicated beam diagnostics must be implemented to
    see the deflected beam (phosphorous screen,
    crawling wire, etc.), in addition to excellent
    global beam instrumentation in Tevatron.
  • The characterization and knowledge of the
    additional crystal parameters (miscut angle,
    surface perfection) are vital for success of the
    studies. The crystal preparation, etching,
    characterization and beam tests will be done with
    INFN and INTAS money.

14
INSTALLING NEW CRYSTAL IN TEVATRON (1)

It turned out that the parameters of the BNLs
crystal used in the first studies were not
optimal for the Tevatron conditions. Express
simulations by V. Biryukov, have shown that the
collimation efficiency can be noticeably improved
by replacing the original 5-mm long crystal with
a shorter one which has a smaller bending angle.
Of course, the optimal parameters depend on
details of the lattice, collimation system
configuration and beam loss region layout, but
the trends shown convinced us to replace the
original crystal with a new shorter one.
Moreover, we also wanted to investigate a new
technology developed to improve crystal
performance. A custom crystal was prepared and
characterized at Protvino and Ferrara 3-mm L,
1-mm W, 150 mrad bending angle, strip, chemical
etching. It replaced the old one during the 2006
Tevatron long shutdown.
15
INSTALLING NEW CRYSTAL IN TEVATRON (2)

16
PROBLEMS IDENTIFIED IN 2007
  1. Angular reproducibility of inchworm mechanics
  2. Noise in the PIN and BLM detectors
  3. Beam diagnostics is insufficient to measure
    channeled and volume reflected beams
  4. Need full realistic multi-turn simulations for
    the current lattice and crystal/collimator
    configuration to confirm 1999-2003 results,
    justify a choice of a short crystal and identify
    locations for comprehensive beam diagnostics
    (single particle tracking capability?) and second
    (vertical) crystal/goniometer

In next talk, Dean will give you details on
(1)-(3) as well as on room in the Tevatron for
installation of new hardware in 2008
17
PROPOSAL FOR EXPERIMENT AT TEVATRON IN 2008-2009

Aiming at the high-performance collimation vital
for the LHC, considering a unique possibility
provided by the Tevatron collider (before its
shutdown for collider physics), and having
already established fruitful collaborative
efforts on crystal characterization, tests and
use for collimation, we propose an experiment at
the Tevatron to test and confirm models of
multi-turn dynamics with crystals by exploiting
channeling and volume reflection.
18
TEVATRON MEASUREMENT GOALS
  • Channeled beam
  • Volume-reflected beam
  • Beam loss and radiation levels downstream of the
    crystal setup
  • Beam loss rate in the B0 (CDF beam-halo monitors)
    for 1- and 2-plane collimation
  • Possible deformation of the crystal or crystal
    holder during a vacuum baking process.
  • Attempt to study crystal damage shock and
    integrated dose.
  • () Add dedicated beam diagnostics
  • Quantitative measure of collimation efficiency
    improvement is reduction of (3) primary LHC
    concern and (4).
  • We are going to simulate the deflected beam loss
    in the Tevatron and LHC (in collaboration with
    IHEP and CERN colleagues). Consistency with the
    current secondary collimator and absorber layout
    is of a concern here need simulations and
    optimizations.

19
FROM ONE-PLANE TO FULL COLLIMATION

The first system collimated only in the
horizontal plane. A comprehensive system would
also collimate in the vertical plane as well as
in dispersion for off-momentum particles. These
results are multiplicative, so the halo scraping
could be improved by up to a factor of eight, as
shown in early simulations. We aim at the full
system in Phase II of this proposal.
20
TASKS End of 2007 (TeV study time 4 hrs)
  1. Decide on a need to replace the goniometer and
    existing crystal with the ST4 crystal that was
    characterized in the September 2006 H8 experiment
    at CERN.
  2. Perform EOS studies in early December.
  3. Initiate detailed simulations of collimation
    system performance with a single strip crystal in
    the realistic Tevatron lattice for both channeled
    and volume-reflected beams.
  4. Work out a plan on beam diagnostics improvement
    and specify new goniometer for 2009 beam studies.

21
TASKS-2008 (three TeV study sessions)
  1. Build improved beam diagnostics system and new
    Ferrara goniometer.
  2. Develop new strip and multistrip crystals.
  3. Complete EOS and proton-only store angular scans
    with the crystal chosen in 2007.
  4. Perform detailed simulations for a complete
    two-plane crystal-based Tevatron collimation
    system.
  5. Initiate tests to provide information about the
    possible deformation of the crystal or crystal
    holder during a vacuum baking process (up to 200
    degrees).
  6. Investigate the possibility of a crystal damage
    experiment where crystals and instrumentation for
    assessing dose rates could be placed in the
    Fermilab beams. Once enough beam is integrated on
    one crystal, it should be moved back to CERN for
    H8 beam line characterization.

22
GOAL-2009
  • Demonstrate efficiency of a well-prepared bent
    crystal collimation system for 2 planes with
    channeled and volume-reflected 1-TeV beams at
    least for two crystal types (single and
    multi-layer) in comparison with tungsten target
    results.
  • This plan will be adjusted based on 2007-2008
    measurements.

23
TASKS-2009 (TeV study time 6 shifts 48 hrs)
  • Install New Hardware
  • Remove E01 collimator to replace with vertical
    crystal assembly
  • Crystal, goniometer, instrumentation tunnel
    installation
  • 2. 150-GeV Beam Tests (1.25 shifts)
  • Test BLM response, inchworm and channel the beam
  • Debug all motion control and instrumentation
  • 3. 980-GeV End-of-Store Beam Studies (4.75
    shifts)
  • Find and characterize channeling (V-plane)
  • Collimate channeled beam (V, H)
  • Collimate volume-reflected beam (V, H)
  • Attempt full channeled collimation (VH)
  • Attempt full volume-reflected collimation (VH)
  • Repeat with another crystal type

24
DELIVERABLES
  • Realistic simulations of multi-turn dynamics with
    crystals by exploiting channeling and volume
    reflection, benchmarked in measurements at the
    Tevatron.
  • Conclusive data and directly relevant input for
    decisions on a possible upgrade path for LHC
    collimation improved collimation efficiency,
    reduced impedance and irradiation of downstream
    components in a quantitative agreement with
    corresponding calculations, and quantitative
    answers to the questions on damage limits and
    sensitivity analyses.
  • 3. Crystal technology, process, hardware
    (goniometer etc.) instrumentation most suitable
    for 2-plane collimation of LHC beams, transferred
    to CERN.

25
COLLABORATION, LOI AND MEETING ON DEC. 6-7
We received a very encouraging support from the
LARP, Fermilab, CERN and INFN management, and
also from the August Accelerator Advisory
Committee at Fermilab (see my next talk). It was
proposed that we prepare a Letter-of-Intent
(LOI), Crystal Collimation Experiment at the
Tevatron and form an official collaboration. A
zero-order draft Discussion Document can be
downloaded. 15 Institutions expressed an interest
to join with quite substantial contributions in
some cases. We are planning a first organizing
meeting at Fermilab on December 6-7, 2007, with a
complete LOI draft and organizational proposals
distributed before that.
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