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p-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay introduction and concept p-bar d-cel simulations ISOLTRAP@ISOLDE consequences on GBAR layout With crucial help from: V. Manea, S. Cabaret, P. Dupré, S. Dephine (C and Robert Wolf (U. Greifswald)

P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay introduction and concept p-bar d-cel simulations

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Page 1: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

p-bar d-cel:keV antiproton pulses

David LunneyCSNSM (IN2P3-CNRS)

Université de Paris Sud, Orsay

introduction and concept p-bar d-cel simulations ISOLTRAP@ISOLDE consequences on GBAR layout

With crucial help from:V. Manea, S. Cabaret, P. Dupré, S. Dephine (CSNSM)and Robert Wolf (U. Greifswald)

Page 2: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

From ELENA:100 keV p pulse300 ns (1.3 m)4 mm mrad

deceleration and pulsed drift tube: concept

- 99 kV

1 keV0.2 m40 mm mrad

drift tube

- 99 kV

1-keVp pulse

Page 3: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

SIMION simulations by Vladimir Manea

deceleration and pulsed drift tube: simulation

Page 4: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

Transport from decelerator to reaction chamber (GIOS)

Page 5: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

Full simulations of antiproton deceleration and focusing

• One single simulation of the 3 m path of the ions from the entrance to the deceleration setup to the injection into the positronium chamber.

• Optimization of the deceleration and focusing voltages, as well as of the setup geometry, for a maximum transport efficiency through the positronium chamber (preliminary value 15%).

Deceleration

Focusing

SIMION simulations by Vladimir Manea

Page 6: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations
Page 7: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

prototype instrumentat the CSNSM, Orsay (March 2012)

Page 8: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

8

5-10ms

100-3000ms

0.001-1000ms

100-500ms

1-30ms

ISOLTRAP spectrometer at ISOLDE (2 Penning, 1 Paul, 1 MR-tof trap)ISOLTRAP spectrometer at ISOLDE (2 Penning, 1 Paul, 1 MR-tof trap)

60-kV, 1-kHz pulsed drift-tube switch

Page 9: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

Exotic nuclides and anti-mattermajor difference: buffer gas!

Page 10: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

16/02/2012 ISOLTRAP Collaboration meeting 2011

HV-switch circuitHV-switch circuit

10

200M500nF

5k

75→175

t

U

τ=1.1us

t=11us τ=40ns

t=400ns

Heinzinger PNChp ±60kV, 10mAdU<10-5Unom/8h; dUrf,pp<10-5Unom ; dUtemp<10-5Unom/Kcommunication: GPIB, RS232, analog

220pF

Behlke HTS 651-10-GSM, 65kV, 100Apk

dVdrop < 30V @ 60kV

Page 11: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

16/02/2012 ISOLTRAP Collaboration meeting 2011

New HV-switch partsNew HV-switch parts

11

Behlke HTS 651-10-GSM+ direct liquid cooling (DLC)*

Switch

Radiator

Pump

Buffer capacitor andRF-sealed copper housing

500nF60kV900J

*GALDEN HT135

Heinzinger PNChp 60kV, 10mA

200MOhm resistor

Page 12: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

16/02/2012 ISOLTRAP Collaboration meeting 2011

HV-switch present status and performanceHV-switch present status and performance

12

Power dissipation and load capacitance extrapolated to 60kV @ 200Hz

Maximum power dissipation at around 1200Hz switching frequency

Page 13: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

16/02/2012 ISOLTRAP Collaboration meeting 2011

HV-switch present status and performanceHV-switch present status and performance

13

peak shape with old setup peak shape with new setuptaken from Zn run

large tail

close to gaussian shape

80Rb

80Zn

no tail

Page 14: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

16/02/2012 ISOLTRAP Collaboration meeting 2011

HV-switch present status and performanceHV-switch present status and performance

14

under-critical damping:increasing resistance necessary 75 Ohm → 175 Ohm

Page 15: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

16/02/2012 ISOLTRAP Collaboration meeting 2011

HV cage reassemblyHV cage reassembly

15

Alkaliion

source

Alkaliion

sourceHV switch

setup

HV switch setup

RFQBuncher

HVpd

60kVFUGHVcage

Page 16: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

16/02/2012 ISOLTRAP Collaboration meeting 2011

HV cage reassemblyHV cage reassembly

16

Alkaliion

source

Alkaliion

sourceHV switch

setup

HV switch setup

RFQBuncher

60kVFUGHVcage

60kVHeinzingerHVpd

dU via CS class*

* by Christopher

Page 17: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

HV-switch SafetyHV-switch Safety

Dividing the HV cages demands a separate safety installation for the HV-switch cage: If VETO is set, LOW status is active -> HVpd=0V

switch and cooling controller

Trigger & Vetoterminal

Control System TPG 300pressure

Center 3pressure

p Buncher p drift tubetrigger

Behlke switch

Cooling system

Tacho Pump and Fan speedsTemp.: Fore, Back, Pump

Pump and Fan statustrigger IN VETO 1-4 optional:

trigger optical OUTand trigger TTL OUT

(manual reset button)

trigger optical INtrigger TTL IN

direct triggertrigger IN

status OUT: Temp, Freq., DCswitch status optical

5V DC power supply5V DC IN

9V DC power supply

switch status monitor

24V DC power supply

Line

vol

tage

attached to cooper box grounding16/02/2012 17

Page 18: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

GBAR layout issues

Page 19: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations
Page 20: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

Extraction from ELENA in a short straight section

25 January 2012 CERN Transfer line WS / Pavel Belochitskii

20

Page 21: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations
Page 22: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

beam transportenergy: 60 keV

Page 23: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations
Page 24: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations
Page 25: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations
Page 26: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

H+ Production

SiO2 coatin

gfast extraction from trap

Ortho-positronium

Page 27: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

GBAR – reaction chamber trajectories

p

p

H

H+

e

e

?

?

?

Page 28: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations
Page 29: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

AD1-5?

Page 30: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

AD1-5?

Page 31: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

AD1-5?

Page 32: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

16/02/2012 ISOLTRAP Collaboration meeting 2011

SummarySummary

32

Decelerator•Pulsed drift scheme: start from working instrument (60 kV)•First simulations show phase space conserved •transmission not disastrous (35%)

Layout issues•Question: are H+, p-, e+ beams interesting for others?•Extraction and transport part of ELENA (i.e. resp. CERN)?•Positioning of equipment…

different extraction segment?rotating ELENA?increasing ELENA kicker-bender angle?adding multipoles?

Page 33: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations
Page 34: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations
Page 35: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

AD1-5?

Page 36: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations
Page 37: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

ELENA layout in AD Hall

25 January 2012 CERN Transfer line WS / Pavel Belochitskii

Page 38: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations
Page 39: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations
Page 40: P-bar d-cel: keV antiproton pulses David Lunney CSNSM (IN2P3-CNRS) Université de Paris Sud, Orsay  introduction and concept  p-bar d-cel simulations

16/02/2012 ISOLTRAP Collaboration meeting 2011

HV-switch modificationHV-switch modification

40

old circuit: new circuit:

Design objectives: Repetition rate up to 1kHz @ 60kV Stable high-voltage potential Safety, ReliabilityChallenges: Power dissipation: up to 600W RF-noise

Drawbacks: Repetition rate max. 3Hz dropping HVcage potential (Leakage current issue)