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Primary Proton Plug MC Study

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Kaon absorption in plug is not high since kaons may decay before reaching the plug. In plug, kaon creation is greater than kaon absorption. Plug position ... – PowerPoint PPT presentation

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Title: Primary Proton Plug MC Study


1
Primary Proton Plug MC Study
  • Joshua Spitz
  • Construction meeting 6/30/05

2
What does a plug do?
  • When JPARC increases from .5MW to 4MW, the beam
    dump may be in trouble.
  • High energy protons irradiating the beam dump.
  • A graphite cylinder in the beamline will absorb
    some of these primary protons.
  • Potential pion absorption at the plug.
  • Loss of neutrino flux.

3
What I have studied
  • MC simulation using JNUBEAM.
  • Plug geometry optimization (radius and length).
  • Minimizing neutrino flux loss
  • Maximizing primary proton absorption
  • Figure of meritprotons with Pgt35GeV/c
  • Plug position optimization
  • Where between horn 2 and 3?
  • Parent pion and background creation at plug

4
Proton profile without plug in place
At beam dump
P gt 35 GeV/c
P lt 35 GeV/c
About 15.5 of primary protons make it to the
beam dump without a plug in place.
5
Basic effect of a plug
2cm radius, 60cm length plug in place
No plug in place
At beam dump
6
Basic effect of a plug part 2
At beam dump
2cm radius, 60cm length plug in place
No plug in place
Pgt 35 GeV/c
7
Plug geometry optimization
  • Proton stopping power has an upper limit in terms
    of plug length.
  • Plug radius of 3cm is too large for maintaining
    nu-mu flux.

8
Plug geometry optimization part 2
X(top) and Y(bottom) position of protons with
Pgt35GeV/c at beam dump. Black is without plug,
red is with plug. On left plug with 2cm radius,
40cm length. On right plug with 2cm radius,
120cm length. 106 POT.
9
Plug geometry optimization part 3
  • Geometry optimization was completed with plug
    about halfway in between horn 2 and 3.
  • Longer plugs are better.
  • Upper limit to plug length, beyond which more
    plug is unnecessary.
  • The best plug radius is between 1cm and 2cm.
  • Up to 60 primary proton absorption with a plug
    in place with negligible neutrino flux loss.
  • Possibly 65-70 primary proton absorption with
    plug very close to downstream horn 2.
  • Very low(1) increase in secondary protons.

10
Nu-mu and background with a plug
  • Why is there no loss in neutrino flux with a
    1-2cm radius plug?
  • Parent pion creation in plug can contribute to as
    much as 2.5 of total nu-mu flux.
  • Pion absorptionpion creation
  • All background particles increase with a plug in
    place.
  • Parent creation at plug.
  • Little kaon absorption (compared to pion).
  • Kaons often decay before reaching the plug.

11
Nu-mu from parent created at plug
Black is total flux. Red is flux from parent
created at plug(2cm radius, 40cm length).
12
Background and the plug
  • Kaon absorption in plug is not high since kaons
    may decay before reaching the plug.
  • In plug, kaon creation is greater than kaon
    absorption.

13
Plug position
  • Most of this study was completed with the plug
    about half way between horn 2 and 3.
  • However, basic simulations were completed to
    study the optimal position of a plug.
  • A plug as close as possible to downstream of horn
    2 is best for proton absorption.
  • Neutrino flux does not suffer.
  • Primary proton cone is smaller.
  • Maximizes proton absorption.

14
Nu-mu-bar beam and the plug
  • Nu-mu is a large background source for a
    nu-mu-bar beam.
  • With a plug in place, the nu-mu background will
    increase by 10-15 (depending on radius and
    length).

15
Plug advantages/disadvantages
  • Advantages
  • upwards of 65 primary proton stopping power
  • zero neutrino flux loss
  • Disadvantages
  • increase in background rates
  • 5 increase in nu-e flux.
  • Larger increases for nu-bar background.
  • increase in background rates with nu-mu-bar beam
  • 10-15 increase in background nu-mu flux
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