MAP MDI at SLAC
Thomas Markiewicz, SLAC Muon Collider Higgs Factory Workshop, UCLA March 22, 2013
Muon Accelerator Program (MAP) MDI
In 2013 SLAC submitted an MDI-focused work package to MAP mgmt. for funding Scope:
• Concentrate on the Higgs Factory (1st) and 3 TeV collider (2nd) • Develop a realistic implementation of a detector with IR magnets and local shielding • Characterize performance
To better understand and control the background source terms, a small group of mostly volunteers has:
• Acquired the current (preliminary) HF lattice • Begun to study the lattice with rapid tracking tools: (Decay)Turtle, DIMAD & Transport
- Uli Wienands & Lew Keller • Created a FLUKA model of the lattice to understand “front end” issues of significance to
the detector: Takashi Maruyama - Energy deposition in local masking, etc.
• Communicate regularly with MAP MDI & Physics/Detector groups
Not yet begun • Look at files of background in an SiD inspired detector in the LCSIM environment
- Norman Graf et al 2
3
Introduction to Muon Colliders: First Principles
Input: • Neuffer’s talk at MAP 2012 Winter meeting at SLAC • Lattice: Alexahin (preliminary) v8.2
Muon lifetime = 1300 revolutions in 300m ring at 62.5 GeV Fill = 1000 turns= 1msec Fill frequency =15 Hz, 1 bunch/beam, 2E12 muons/bunch At injection
• 20 kJoules/beam, 300 kW/beam Decay electrons:
• Peak decay rate = 5.1E6/m/beam • Average electron energy in lab = 22 GeV • Average electron angle in lab w.r.to muon = 1.7 mrad • Peak e- power lost to ring = 5.4 MW/beam • Average e- power lost to ring = 56.4 kW/beam • Average e- power density =188 W/m/beam
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Decay Electron Kinematics
Elab (GeV)
Theta_lab (rad.)
Theta_lab (rad.)
Ela
b (G
eV)
Muon Collider Geometry in FLUKA Takashi Maruyama
Alexahin’s MAD deck • Use MAD survey file
Wrote a program to read the survey file and generate FLUKA input.
• Primitive geometry definitions • Region definitions • Material definitions • Magnetic field type (bends, quads, sexts)
and strength Collider parameters are arbitrarily chosen, but can be changed easily.
• Tunnel radius (2 m) • Tunnel wall thickness (50 cm) • Magnet shape and size (Bend: 2 m x 1 m) • Beampipe thickness (1 mm) • Beampipe radius (10 cm)
5
Steel
Concrete
Air
Dirt
Study #1 Backgrounds crossing scoring plane at 5m from source points
Scoring plane
- decays
Tunnel filling concrete shield added
6 Takashi Maruyama/SLAC
An example: Decays at z=22.7m without tunnel filling concrete shield
7 Takashi Maruyama/SLAC
Particle flux reaching the IR
10-2
10-1
100
101
102
103
104
105
106
107
Par
ticle
s / 5
mill
ion
deca
ys
3025201510
Distance from IP (m)
e- e+ photon neutron muon pion
8 Takashi Maruyama/SLAC
Decays at s = 6.4 m
X (cm)
Y (c
m)
e+/e-
X (cm)
Neutrons
9
Takashi Maruyama/SLAC
Tunnel
Decays at s = 22.7 m
X (cm)
Y (c
m)
Neutrons Muons
X (cm) 10
Takashi Maruyama/SLAC
- +
General Comments on background type & location
e+/e- and • Inside beam pipe and magnet bore
Neutrons • Magnet bore • More diffuse over tunnel
Muons • Bend magnets sweep muons and Magnet body acts like a
shield • ~50 muons/meter
Hadrons • Smaller flux and easier to shield
11 Takashi Maruyama/SLAC
12
Study 2: IP Conic Mask Study Vary thickness at tip and look at particles penetrating the mask
• Inspired by Mokhov 1.5 TeV design • Use large apertures specified in Alexahin
lattice for IP magnets • Maintain 6cm long beampipe at IP • Scale beampipe radius to 4cm radius based
on 13.5cm to 1.78 cm radii of apertures of first quad in 1.5 TeV versus HF lattices
0
50
100
150
200
250
300
350
400
450
500
0 2000 4000 6000 8000 10000 12000
Masks & Final Focus
M1_Cone
M1_Barrel
M2_Cone
QLB1
QLB2
QLB2
QLB3
Quad
r=22cm r=23cm
Quad Combined Function
IR Mask
Varied the thickness at tip from 5-75mm
2 × 107 decays between 0 and 4 m.
Count particles
3 Tesla Solenoid
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5E6 decays/m rate x 4m => results absolutely normalized Sig_x = Sig_y = 5cm at 1st quad
Takashi Maruyama/SLAC
Particle flux leaving beampipe and mask vs. Mask thickness
e+/e- 0.5 cm 1.5 cm 3.5 cm 7.5 cm
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e+/e
-/100
0/cm
Pho
tons
/100
0/cm
Takashi Maruyama/SLAC
Particle flux vs. Mask thickness
Neutrons 0.5 cm 1.5 cm 3.5 cm 7.5 cm
15
Neu
trons
/cm
Takashi Maruyama/SLAC
16
Comments
Need a HF reference design with agreed to parameters: • Emittances, beam sizes, etc. • Beam pipe radii, apertures, VXD length, …
Designs too immature to invest vast computing resources (and time) • Rapid prototyping tools & investigation of parameter space
preferable We at SLAC look forward to continuing this work if MAP
decides it is worth it