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Beamline-to-MICE Matching Ulisse Bravar University of Oxford 2 August 2004 MICE performance with ideal Gaussian beam JUNE04 beam from ISIS beamline (Kevin Tilley) Software, beam momentum and coil currents manipulation Results, cooling of the actual ISIS beam

Beamline-to-MICE Matching Ulisse Bravar University of Oxford 2 August 2004 MICE performance with ideal Gaussian beam JUNE04 beam from ISIS beamline (Kevin

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Page 1: Beamline-to-MICE Matching Ulisse Bravar University of Oxford 2 August 2004 MICE performance with ideal Gaussian beam JUNE04 beam from ISIS beamline (Kevin

Beamline-to-MICE Matching

Ulisse Bravar University of Oxford

2 August 2004 • MICE performance with ideal Gaussian beam• JUNE04 beam from ISIS beamline (Kevin Tilley)• Software, beam momentum and coil currents

manipulation • Results, cooling of the actual ISIS beam

Page 2: Beamline-to-MICE Matching Ulisse Bravar University of Oxford 2 August 2004 MICE performance with ideal Gaussian beam JUNE04 beam from ISIS beamline (Kevin

Cooling a Gaussian beam

• Beam in the middle of the upstream spectrometer: = 6 mm rad<p> = 200 MeV/c = 33 cm

• Gaussian distributions: x = 3.3 cm

px = 20 MeV/c

• Coils from Mice Note 49:about 15% cooling

LH

spectrometersz (m)

(

m r

ad)

Page 3: Beamline-to-MICE Matching Ulisse Bravar University of Oxford 2 August 2004 MICE performance with ideal Gaussian beam JUNE04 beam from ISIS beamline (Kevin

ISIS beam• Simulations of the MICE channel performed with ICOOL• Beamline designed by Kevin Tilley with TURTLE

• Latest beam design: JUNE04 • Pb diffuser is 8 mm thick

• Turtle-Icool interface planes: a) Middle of upstream spectrometerb) After Pb diffuser, prior to solenoidc) After Q9, prior to Pb and solenoid

• Work in progress:a) Interface Turtle-Icool midway between Q6-Q7 b) Simulate the entire beamline with Icool

Page 4: Beamline-to-MICE Matching Ulisse Bravar University of Oxford 2 August 2004 MICE performance with ideal Gaussian beam JUNE04 beam from ISIS beamline (Kevin

Beamline layout

• MICE beamline (NOT TO SCALE !!!)

Q7 Q8 Q9

Quadrupole triplet

Drift

Pb diffuser 0.8 cm

Solenoid & Spectrometer

LHFocus coil

TURTLE – ICOOL INTERFACES

Page 5: Beamline-to-MICE Matching Ulisse Bravar University of Oxford 2 August 2004 MICE performance with ideal Gaussian beam JUNE04 beam from ISIS beamline (Kevin

Beam design concept (1)MICE wants……

x/y

x’/y’

2. Particular input emittance RQD

qB

p

x

xxx

20

'max

max

1. Matched beam

…. at matching point (4T Spec Solenoid)

Page 6: Beamline-to-MICE Matching Ulisse Bravar University of Oxford 2 August 2004 MICE performance with ideal Gaussian beam JUNE04 beam from ISIS beamline (Kevin

Beam design concept (2)Scheme to provide simultaneously:-

This is the driving Design Concept in this design work:

To use ‘Beamsize’ & ‘Scatterer thickness’ to provide both beam matching, & required emittance generation.

200 2

1 RQD

0

00

0

00

1. Focus Beam with

x/y

x’/y’

MICE ACCEPTANCE A

0, 00 beamR

2. &

Matched after passing thru’ required scatterer

RQD 0, match

2

[Above figure illustrates case match region immediately follows scatterer]

Page 7: Beamline-to-MICE Matching Ulisse Bravar University of Oxford 2 August 2004 MICE performance with ideal Gaussian beam JUNE04 beam from ISIS beamline (Kevin

JUNE04 beam

• Beam is not cylindrically symmetric at Q9, far from Gaussian…

• Designed to achieve = 33 cm and = 0 in spectrometer solenoid

• Central momentum of ‘useful’ beam p = 236 MeV/c

• Design emittance y ONLY = 6 mm rad • This means:

(<pz> / mc) y y’ sqrt(1-r2) = 6 mm rad

Page 8: Beamline-to-MICE Matching Ulisse Bravar University of Oxford 2 August 2004 MICE performance with ideal Gaussian beam JUNE04 beam from ISIS beamline (Kevin

Beam at Q9 (1)

ptot (GeV/c)py (GeV/c)px (GeV/c)

x (m) y (m)

Page 9: Beamline-to-MICE Matching Ulisse Bravar University of Oxford 2 August 2004 MICE performance with ideal Gaussian beam JUNE04 beam from ISIS beamline (Kevin

Beam at Q9 (2)

• Beam is everything but Gaussian

• Top: x – pz correlation

• Bottom:a) <x> is not 0

b) px is asymmetric

x (m)

x (m) px (GeV/c)

pz (GeV/c)

Page 10: Beamline-to-MICE Matching Ulisse Bravar University of Oxford 2 August 2004 MICE performance with ideal Gaussian beam JUNE04 beam from ISIS beamline (Kevin

x – pz correlation

• Correlation after Q9• Disappears after Pb

scatterer and inside spectrometer

265 MeV/c

x (m)

p z (

GeV

/c)

Page 11: Beamline-to-MICE Matching Ulisse Bravar University of Oxford 2 August 2004 MICE performance with ideal Gaussian beam JUNE04 beam from ISIS beamline (Kevin

Cooling (1)

• Ideal Gaussian beam• JUNE04 beam

Designed assuming that the optics of the cooling channel were optimised for a central momentum of:<p> = 200 MeV/c

• Interface Turtle – Icool: centre of upstream solenoid

• Transmission = 80% • COOLING = ???

z (m)

(

m r

ad)

Page 12: Beamline-to-MICE Matching Ulisse Bravar University of Oxford 2 August 2004 MICE performance with ideal Gaussian beam JUNE04 beam from ISIS beamline (Kevin

A few steps

• MICE channel designed for pcentral = 200 MeV/c

• Beam at Q9 designed to provide <p> = 236 MeV/c, due to A2 – p correlation

Steps:• Scale ALL coil currents in the

MICE channel by 236/207• Include Pb diffuser in Icool• Propagate Turtle beam from

Q9 into centre of spectrometer • Inside upstream spectrometer,

select ONLY events with ptot within 5% of 236 MeV/c

ptot

CUT

ptot (GeV/c)

Page 13: Beamline-to-MICE Matching Ulisse Bravar University of Oxford 2 August 2004 MICE performance with ideal Gaussian beam JUNE04 beam from ISIS beamline (Kevin

B-field in Icool

• Fringe field from Q9 not included in Icool simulation

• Bz from solenoid ‘almost’ zero at Q9

• Pb scatterer inside fringe field from solenoid

• Bz in solenoid >> 4 T

Q9

Pb

z (m)

Bz

(T)

Page 14: Beamline-to-MICE Matching Ulisse Bravar University of Oxford 2 August 2004 MICE performance with ideal Gaussian beam JUNE04 beam from ISIS beamline (Kevin

Icool vs. Turtle

• ptot in the centre of the upstream spectrometer:

a) Icool

b) Turtle

Note: Turtle uses thin lens approximation for solenoid fringe field

ptot (GeV/c)

Page 15: Beamline-to-MICE Matching Ulisse Bravar University of Oxford 2 August 2004 MICE performance with ideal Gaussian beam JUNE04 beam from ISIS beamline (Kevin

Longitudinal momentum

• JUNE04 beam, all events

• JUNE04 beam with ptot cut

z (m)

<p z

> (

GeV

/c)

Page 16: Beamline-to-MICE Matching Ulisse Bravar University of Oxford 2 August 2004 MICE performance with ideal Gaussian beam JUNE04 beam from ISIS beamline (Kevin

Cooling (2)

• JUNE04 beam, all events

• JUNE04 beam with ptot cut

z (m)

(

m r

ad)

Page 17: Beamline-to-MICE Matching Ulisse Bravar University of Oxford 2 August 2004 MICE performance with ideal Gaussian beam JUNE04 beam from ISIS beamline (Kevin

Cooling (3)• Ideal Gaussian beam = 15.8%

Transmission = 98.6%

• JUNE04 beam = 11.1%

Transmission = 72.8%

• 7,075 after Q9• 5,412 total in upstream

spectrometer• Of these, 1,543 pass the cut

on ptot• 1,124 left in downstream

spectrometer z (m)

(

m r

ad)

Page 18: Beamline-to-MICE Matching Ulisse Bravar University of Oxford 2 August 2004 MICE performance with ideal Gaussian beam JUNE04 beam from ISIS beamline (Kevin

Beta functions

• Gaussian beam, starting in upstream solenoid

• JUNE04 beam, all events

• JUNE04 beam with ptot cut

z (m)

(

m)

Page 19: Beamline-to-MICE Matching Ulisse Bravar University of Oxford 2 August 2004 MICE performance with ideal Gaussian beam JUNE04 beam from ISIS beamline (Kevin

Conclusions• MICE coils and JUNE04 beam need some more work

• We have an actual beam + cooling channel design that works !!!

• Beamline: a) Reduce central momentum to

<p> = 207 MeV/cb) Have central momentum in the centre

of the ptot distribution, not in the tailc) More interface planes Turtle-Icool

• Keep an eye on event rate: 1,124 + / 7,075 + = 15.9% !!!