Results with ISCOOL a new Radio Frequency Quadrupole Cooler and Buncher at ISOLDE

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ISOLDE WS 2007 Results with ISCOOL a new Radio Frequency Quadrupole Cooler and Buncher at ISOLDE P. Delahaye, H. Frånberg, AB-OP-PSB, ISCOOL, COLLAPS, ISOLDE collaboration

description

Results with ISCOOL a new Radio Frequency Quadrupole Cooler and Buncher at ISOLDE. P. Delahaye, H. Fr å nberg, AB-OP-PSB, ISCOOL, COLLAPS, ISOLDE collaboration. Where at ISOLDE. ISCOOL. Installation in pictures. INSTALLATION. Implementation of the RFQ into the ISOLDE vacuum system. - PowerPoint PPT Presentation

Transcript of Results with ISCOOL a new Radio Frequency Quadrupole Cooler and Buncher at ISOLDE

Page 1: Results with ISCOOL a new Radio Frequency Quadrupole Cooler and Buncher at ISOLDE

ISOLDE WS 2007

Results with ISCOOL a new Radio Frequency

Quadrupole Cooler and Buncher at ISOLDE

P. Delahaye, H. Frånberg,

AB-OP-PSB, ISCOOL, COLLAPS, ISOLDE collaboration

Page 2: Results with ISCOOL a new Radio Frequency Quadrupole Cooler and Buncher at ISOLDE

ISOLDE WS 2007

ISCOOL

Where at ISOLDE

Page 3: Results with ISCOOL a new Radio Frequency Quadrupole Cooler and Buncher at ISOLDE

ISOLDE WS 2007

Installation in pictures

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ISOLDE WS 2007

INSTALLATIONImplementation of the RFQ into the ISOLDE

vacuum system.Construction of HV platform and HV cage of

the RFQ. Standard controls in the working sets: QP

arrays for the RFQ and for the beam tuning after the cooler.– RF and gas still on LabVIEW.

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ISOLDE WS 2007

OPERATION OF ISCOOL

• Set-up by the ISOLDE operators.

• Improved transmission past the switchyard Improved (faster and easier) set-up for the beam

to the experiments

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ISOLDE WS 2007

Principle

RFV

Three elements:RF quadrupolar fieldRadial confinement

DC potentialsExtracting ion in bunches or in continuous mode

Buffer gas Ion motion cooling

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Transmissions

• Potentials along the axis

Transmission dependence on the emittance of the ISOLDE ion sources.ISOLDE on-line surface ion sources has smaller emittance than ISOLDE FEBIAD ion sources (<25 π·mm mrad). The off-line tests were performed with an ion source with ε = 35π mm mrad

80eV

5-2V/cm

~1E-2 mbar 4He10-2mbar l/s

EXTRACTIONINJECTION

50V (30V enough)

TRAPPING

0 20 40 60 80 100 120 1400

20

40

60

80

100

Mass

Tra

nsm

issi

on

on-line surface ionsourceon-line plasma ionsourceoff-line surface ionsource

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ISOLDE WS 2007

Bunching mode

30-60 keV

80eV5-2V/cm

~1E-2 mbar 4He10-2mbar l/s EXTRACTIONINJECTION

50V (30V enough)

TRAPPING

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ISOLDE WS 2007

Cooling time• TOF < 1ms from the

entrance to the exit of the RFQ– No losses for short

lived ions.

• 1 passage is enough to get a cold beam – as measured off-line,

and other labs as predicted by simulations for other systems

-200 0 200 400 600 800 1000 1200 1400 1600 1800-1

0

1

2

3

4

4.0x10-4

6.0x10-4

8.0x10-4

1.0x10-3

1.2x10-3

1.4x10-3

1.6x10-3

Bea

m g

ate

Time [s]

MC

P

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ISOLDE WS 2007

Emittance measurements (off-line)~35·mm·mrad 95% emittance

~2.2·mm·mrad 95% emittance

• 10 x decrease of the beam emittance– The worst case scenario

at ISOLDE is the FEBIAD ion source with >25 p·mm·mrad emmittance.

• Injection efficiency into the cooler is depending on the beam emittance from the ISOLDE target and ion source unit.

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ISOLDE WS 2007

0.00E+000 4.00E+008 8.00E+008 1.20E+009-2.00E+007

0.00E+000

2.00E+007

4.00E+007

6.00E+007

8.00E+007

1.00E+008

1.20E+008

1.40E+008

1.60E+008

Ext

ract

ed

ion

s

Injected ions

Space charge limits

• Up to 108/s!! As measured with FC (data under analysis with MCP)

0 1x109 2x109 3x109 4x109 5x109

0.0

2.0x107

4.0x107

6.0x107

8.0x107

1.0x108

1.2x108

1.4x108

Ext

ract

ed io

ns

Injected ions

39K, Collection time=10 ms–1 secExtraction time 150 us

85Rb

0.0 5.0x107 1.0x108 1.5x108 2.0x108 2.5x108

0.0

2.0x106

4.0x106

6.0x106

8.0x106

1.0x107

1.2x107

1.4x107

Ext

ract

ed io

ns

Injected ions

23Na

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Bunch width

Depends on the space charge and cooling time

-40 -20 0 20 40 60 80 100 120 140

-8x10-3

-7x10-3

-6x10-3

-5x10-3

-4x10-3

-3x10-3

-2x10-3

-1x10-3

0

1x10-3

2x10-3

MC

P s

igna

l

Time [s]

10 ms 100 ms 1000 ms

Collection time=cooling time

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Yield measurements

• 26Na T1/2=1.07 s

• 48K T1/2=6.8 s

• Yields in continuous mode: – 26Na :1.2e6 at/uC– 48K: 2.2e4 at/uC

• Yields in bunched mode – analysis under progress

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HOT SPOTS

0.5 µSv/h15 µSv/h

10 µSv/h

3 µSv/h

10 µSv/h

15 µSv/h

5 µSv/h5 µSv/h

0.5 µSv/h

Beam direction

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Results

• High transmission efficiencies

• Easy beam tuning to experiments

• Yield measurements continuous vs. bunched mode

• Losses due to trapping time (analysis in progress

• First measurements with radioactive isotopes performed together with COLLAPS (see next talk)

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ISOLDE HRS + Cooled beams

HRSIS

COO

L

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OutlookUp to October 2007:

From Nov. 2007:

Next step:

Upgrade of HRS Mag 90:

EURISOL HIE Isolde:

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ISOLDE WS 2007

Thanks to:

• AB-OP-PSB-iso team: Pascal, Erwin, Magnus, Emiliano and Tim.

• AB/ATB

• AB/CO

• AB/PO

• AB/VAC

• SC/RP

• ISOLDE collaboration

• COLLAPS collaboration

• ISCOOL collaboration

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ISOLDE WS 2007

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ISCOOL tests with COLLAPS46K Beam 1E5 ions/s after the cooler. Collection time 20 minutes, with 300ms bunching and a 12us

gate and 2mW of laser power.

-7 -6 -5 -4 -3 -2 -1

0

20

40

60

80

100

120

140

160

180

200

Gat

ed c

ount

s

Tuning voltage

-7 -6 -5 -4 -3 -2 -1

490000

492000

494000

496000

498000

500000

502000

To

tal c

oun

ts

Tuning volts

Singles (continuous counting)Bunched:12us gated spectra

Background suppression factor~1E4