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Eric Prebys |
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FNAL Beams Division |
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One of two electrostatic pre-accs accelerates H-
ions to 750 keV. |
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The linac accelerates these ions to 400 MeV |
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The ions are injected over several (up to 12)
turns into the booster, and passed through a foil to strip off the
electrons. |
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The booster accelerates the protons from 400 MeV
to 8 GeV. |
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The booster lattice is in an offset 15 Hz
(line/4) resonant circuit. This
sets an overall quantum of time for the whole accelerator (“tick”, “click”,
“clink”). |
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Instantaneous 15 Hz rep rate routinely achieved. |
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Average rep rate limited by |
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Power dissipation of ramped elements |
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Above ground radiation (safety issues) |
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Below ground radiation (activation issues) |
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Some numbers: |
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Historical high*: 3E12 ppp @2.5 Hz (3E16 pph) |
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Run II needs: 5E12 ppp @.7 Hz (1.3E16 pph) |
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BooNE+Run II: 5E12 ppp @5.7 Hz (1E17 pph) |
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NuMI + Run II: 5E12 ppp @3.2 Hz (6E16 pph) |
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Linac chopper: 15 Hz |
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ORBUMP Magnets: 7.5 Hz (lots of work to go to
15Hz) |
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Booster RF: 7.5 Hz (Maybe go to 15 if we use
existing cooling lines). |
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BEXBMP: 15 Hz |
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Extraction kickers: 15 Hz |
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MP02 extraction septum: 2.5 Hz (New PS -> 5
Hz, New magnet + PS -> 7.5Hz, + more cables -> 15 Hz. ~6/2002) |
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-> We currently take 7.5 Hz as a practical
limit for BooNE and beyond. |
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Radiation Limitations |
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Above ground (want to avoid turning towers into
controlled access area). |
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Shielding |
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Reduce beam losses |
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Below ground (must avoid making booster elements
too hot to handle). |
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Reduce beam losses |
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The Booster uses multi-turn injection, resulting
in a continuous beam around the ring. |
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If beam is passing through the extraction septum
while it is ramping, some of it will be steered into beam elements. |
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This is the single largest source of radiation
resulting from the booster. |
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Solution:
Early in the cycle, the old extraction kicker is pulsed, blowing a
“notch” in the beam. Extraction is
timed to coincide with the notch. |
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Problem:
although it’s a factor of 20 better to lose the beam early in the
cycle, it’s still not negligible (more in a minute) |
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It looks like with a combination of shielding
and careful beam handling, we should be able to keep above ground radiation
to acceptable levels, even at BooNE+Run II intensities. |
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In order to reduce the uncontrolled beam loss
when creating the notch, the idea is to excite a resonant instability and
then scrape the beam away at a well-positioned collimator. |
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Collimators have been commissioned, but
unfortunately didn’t make it in time for this shutdown. |
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Most of the prep work has been done, so
installing the collimators should be able to be done in about a day, and
will probably get done before BooNE. |
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The main beam elements ramp with the momentum,
but up until now, the corrector elements have been operated DC |
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Beam can “wander” by up to a few cm’s during
ramp. |
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Ramping control cards were installed during the
shutdown. |
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Closure control program almost ready. Still
needs to be tested. |
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Correctors not powerful enough to steer the beam
all the way through the cycle. Still,
should help. |
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Injection Line diagnostics upgraded
substantially during shutdown. |
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Space charge studies underway. |
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Transition revisited? |
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The main injector circumference is exactly 7
times the booster circumference, so there’s room for 7 booster batches. |
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BUT, one slot must remain empty to allow the
injection kicker to ramp down. -> max 6 booster batches/M.I. Cycle
(unless we do slipstacking…) |
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Everything measured in 15 Hz “clicks” |
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Minimum M.I. Ramp = 22 clicks = 1.4 s |
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MiniBoone batches “don’t count”. |
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Cycle times of interest |
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Stack cycle: 1 inj + 22 MI ramp = 23 clicks =
1.5 s |
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NuMI cycle: 6 inj + 22 MI ramp = 28 clicks = 1.9
s |
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Full Slipstack cycle (total 11 batches): |
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6
inject
+ 2 capture (6 -> 3)
+ 2 inject
+ 2 capture (2 -> 1)
+ 2 inject
+ 2 capture (2 -> 1)
+ 1 inject
+ 22 M.I. Ramp
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39 clicks = 2.6 s |
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In order to Reduce radiation, a “notch” is made
in the beam early in the booster cycle. |
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Currently, the extraction time is based on the
counted number of revolutions (RF buckets) of the Booster. This ensures
that the notch is in the right place. |
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The actual time can vary by > 5 usec! |
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This is not a problem if booster sets the
timing, but it’s incompatible with multi-bunch running. |
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We must be able to fix this total time so we can
synchronize to the M.I. orbit. |
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This is called “beam cogging”. |
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Detect slippage of notch relative to nominal and
adjust radius of beam to compensate. |
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Early losses are extremely non-linear with
number of turns of injection. |
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Space charge effects are typically blamed, but
the details are not well understood. |
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A study group is working on this. |
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Too late for BooNE, by maybe NuMI? |
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Increasing the ppp would allow you to almost
double your total protons before hitting the BooNE rad limits!! |
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Reasonable booster assumptions: |
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5E12 ppp |
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Ave 7.5 Hz rep rate |
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Up to 1E17 pph w/o tripping rad alarm (BooNE
needs) |
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Assuming BooNE runs as planned, the one
NuMI-specific booster issue is that of beam cogging! |
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With those limits, NuMI can expect 2.7E20 p/year |
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Slipstacking (if it worked perfectly!) would
increase this by about 30%. |
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Increasing the ppp could increase NuMI’s
delivered protons. |
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