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MATS/LaSpec MATS/LaSpec

MATS/LaSpec - PowerPoint Presentation

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MATS/LaSpec - PPT Presentation

Status report Alexander Herlert FAIR GmbH o n behalf of the MATS and LaSpec Collaborations Thanks to W Nörtershäuser D Rodríguez P Campell I Moore and G Neyens for providing slidesmaterial ID: 362942

mats ion trap laspec ion mats laspec trap amp penning laser ugr detection tof rfq beam ugw design triga

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Slide1

MATS/LaSpecStatus report

Alexander HerlertFAIR GmbHon behalf of the MATS and LaSpec Collaborations

Thanks to W. Nörtershäuser, D. Rodríguez, P. Campell, I. Moore, and G. Neyens for providing slides/material

NuSTAR Week 2011, Bucharest, October 17-21, 2011Slide2

Precise M

easurements on very short-lived nuclei using an Advanced Trapping System

Laser Spectroscopy on very short-lived nuclei

MATS &

LaSpec

stands for

10

countries,

24 institutes

, 87 members

8

countries,

13 institutes

, 34 membersSlide3

RFQ cooler & buncher

MR-TOF

MATS

EBIT

Laser Spectroscopy

Dipole magnet

Gas cell

for more information see: Technical Design Report of MATS & LaSpec:

D. Rodriguez, K. Blaum, W. Nörtershäuser et al.EPJ Special Topics 183 (2010) 1-123

MATS &

LaSpec

at the LEB/FAIRSlide4

Technical Design Report of MATS & LaSpec:

D. Rodriguez, K. Blaum, W. Nörtershäuser et al.EPJ Special Topics 183 (2010) 1-123

RFQ: JYFL

ß-NMR: Leuven

Collinear Ion Beamline:

Manchester

Collinear Atom Beamline + Optical Pumping: Mainz

MATS &

LaSpec

at the LEB/FAIRSlide5

Turbo

Simulation results: Emittance ~6π

mm mrad, Δ

E~ 3 eV,

δ

T ~3

m

s for 2 keV pulse of ejected

133Cs

+ when using buffer gas at 80 K. 80% injection efficiency, when assuming parallel beam d=4 mm, (40 kV) before deceleration

Electrode design similar to ISCOOL

Valve

Deceleration

QP deflector

+einzel

Insulator

Turbo

Valve

Mini RFQ

RFQ trap

He in (0.04 mbar)

Drift tube & acceleration

Turbo

3-stage

rf

cooler for MATS and

LaSpecSlide6

Mass measurements have been already performed

Important work going on the ion source (helios) in order to make

practicable more elements from the californium source

K. Blaum,

W. Nörtershäuser et al (MPIK)

Layout of the TRIGA-Spec experimentSlide7

common

beamline

Recently added:

RFQ cooler and buncher

(COLETTE)

Prototyping &

Development @ TRIGA-SpecSlide8

Status of the LASPEC Prototype at the TRIGA-Reactor in Mainz

D. Lunney, NIM A598 (2009) 379-387

beam diagnostics for MATS and LASPEC

(MCP and imaging optics for beam profile control)

build and testing

laser spectroscopy on praseodymium

(preparatory work under realistic conditions for on-line runs, e.g. at ISOLDE)

successfully tested

RFQ cooler and buncher

(in preparation for on-line coupling to the reactor)

currently comissioning

ISOLDE, CERN

TRIGA,

Mainz

Titelmasterformat durch Klicken bearbeiten

Laser

SpHERe

Laser

Sp

ectroscopy of

H

ighly Charged Ions and

E

xotic

R

adioactive Nucl

e

i

Status of the LASPEC Prototype at the TRIGA-Reactor in MainzSlide9

Optical pumping & Conetraps

P. Reinhed et al., NIM A621 (2010) 83

Use intra cooler optical pumping to selectively populate desired ionic state

Greatly enhanced efficiencies and spectroscopic access to previously “impossible” elements

-Can be used in electrostatic traps which double as “energy elevators” in LaSpecSlide10

A new optical detection region for Collinear Laser Spectroscopy

Optical detection efficiency improved by factor 10 + background photon detection reduced by 50% !

100 mm Ø aspheric lenses

Electron Tubes 9658B

2” PMT , S20 IR sensitive photocathode

Laser / K beam

detected region

Simulated efficiency of new and previous set-up: gain ≈

14x

Mark Bissell et al., NIM, in preparation

(Design: M.L. Bissell, K.U. Leuven, Belgium)

Use refrigerant circulator FP40-MC to cool photocathode to -30

C

via Cu heat exchanger. Slide11

Experimental

sequence for MATSGas catcher

RFQ

buncher

MR-TOF-MS

Preparation

Penning trap

EBIT

Measurement

Penning

trap

Detector

trapSlide12

MR-TOF-MS (

UGießen)

10

-8

mbar

Kinetic Energy

1.5 keV

Curved

RFQs

Differential

Pumping

Section

Injection

Trap System

Time-of-Flight

Analyzer

10

-4

mbar

10

-2

mbar

Energy

Buncher

Ion Gate

Isochronous

SEM

Post-Analyzer

Reflector

Gate Detectors

Internal

Ion Source

10

-6

mbar

Ions

Separated

Ions

Mass Measurement

Aux. Detector

133

Cs

+

12 ms TOF

Mass resolving power

(FWHM)

m/

m

=

1

00,000

(

5 ms TOF

)

Isobar separation

Demonstrated for C

6

H

6

and

13

C

12

C

5

H

5

(Intensity ratio 170:1,

m = 4 MeV)

Ion capacity

> 10

4

per cycle and >10

6

per second

W. R. Plass et alSlide13

Test for the LEB: MR-TOF-MS at the FRS Ion Catcher

MR-TOF-MS was commissioned successfully at the FRS Ion Catcher in the S411 experiment (07.10. - 12.10.2011)!

(See talk by H. Geissel)

W.R. Plaß et al., GSI Scientific Report 2010, p. 137 (2011)Slide14

High electron current up to 2000 mA.

High ion densities: 106 to 1010 ions/cm3

6 keV, 2 A electron beam. Current density 1400 A/cm

2

, background pressure 10

-10

mbar (H

2

), ion temperature 300 eV. The calculation includes radiative recombination and charge exchange.

EBIT (MPIK Heidelberg)

(Courtesy of J.R. Crespo)

(EBIT at TRIUMF)

J. R. Crespo et al (MPIK)Slide15

Penning traps (UGW, MPIK Heidelberg, GSI, UGR

)

(Courtesy of J.R. Crespo)

Study of the injection of ions into the field of a 12 T Magnet (UGW)

Design of an alignment support for the trap (UGW)

(Superconducting magnet at UGW )

(L. Schweikhard, G. Marx et al)Slide16

Ion detection for the Penning traps (UGR, MPIK, UGW)

Cryogenic environment and UHV.Broad-band mass identification

Detection in the preparation Penning trap

The detection in the measurement

Penning trap:

FT-ICR for single ion sensitivity

C. Weber

PhD Thesis (UM)

R. Ferrer, PhD Thesis (UM)

Amplifier in vacuum (UGR)

D. Rodríguez et al

Amplifier in air (UGR)

Coil for single ion

D

etection

(UGR)

Technical drawing of the setup at UGR for FT-ICR tests

J. M. Cornejo, Master thesis (UGR)Slide17

The

Detector Trap (LMU Munich)

mock-

up:

detector

carrier boards

between trap

electrodes

cryotest

:

lN

2

temperature, selection

of groove dimensions

Characteristics:

Replace

inner Penning trap electrode by cubic setup of

4

Si-strip detectors

U

se

detector bias for trapping potential

Penning trap

electrodes

:

D

etector

dimensions given by: space in magnet bore,

required position resolution

, efficiency

optimization

D

etectors

need to comply with UHV and cryogenic conditions

strip detector

(P. Thirolf et al)

Developments also carried out at PNPI

A

n funding has been receivedSlide18

Off-line ion source (PNPI)

Y. Nu. N

ovikiov et alSlide19

Funding ID (Preconstruction-MoU)Slide20

Status and perspectives

FAIR will offer unique opportunities with RIBMATS & LaSpec will incorporate the most advanced technical developments on ion traps, lasers and beam preparation

The Technical Design Report was approved in May 2010Several groups have received funding to start the construction of the different components

A large number of laser and Penning trap setups at different European institutes, universities and RIB facilities can be used for developing very advanced components (MPI-K, JYFL, ISOLDE, KVI, GSI, TRIGA, UGR, UGW, UG, SPIRAL2...)

MATS can be tested and can be ready before FAIR is in operation

Unfortunately, the first stage of the modularized start version of FAIR does not include the low energy beam line where MATS & LaSpec will be placed