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dissociative dissociative recombination recombination CRP on Atomic and Molecular Data for Plasma CRP on Atomic and Molecular Data for Plasma Modelling Modelling Mats Larsson Department of Physics Stockholm University
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Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

Dec 28, 2015

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Page 1: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

Progress in measurements of Progress in measurements of dissociative recombinationdissociative recombination CRP on Atomic and Molecular Data for Plasma ModellingCRP on Atomic and Molecular Data for Plasma Modelling

Mats Larsson

Department of Physics

Stockholm University

Page 2: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

Task for Stockholm according Task for Stockholm according to minutes of 2005to minutes of 2005

BeH+ and BeH2+

Problem: The Manne Siegbahn Laboratory reluctant to deal with Be.

Page 3: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

Some pointsSome points

The Stockholm group has no national funding for fusion related research

The storage ring CRYRING is still in operation and beam time will be scheduled for the fall of 2007. The decision to shut down the lab was taken 2002, so the damage control has been quite successful!

Beam time during 2008 unclear

Page 4: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

ProgressProgress

Experiment on C4D2+

Results on CF2+ and CF3

+

The H3+ and its isotopologues

Development of data base for dissociative recombination

Page 5: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

Doubly excited neutral molecule

A2+B

AB+A

A+A+B

+

e-

DR of polyatomic ions

A2B+ + e- (Ee)

For example:

C2H+ + e- C2 + H + 6.60 eV

CH + C + 3.98 eV

C + C + H + 0.43 eV

3 possible DR -

channels

Page 6: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

Research programme

What do we measure?:

• Branching fractions of dissociative recombination• Thermal rate constants/Cross sections of dissociative recombination (energy/temperature – dependence)

Which ions do we study?:

- hydrocarbon ions (so far C2H+, C2H2+, C2H3

+, C2H4+, C2D5

+

C3H4+, C3H7

+, C4D9+, C4D2+), CFn+, H3

+

Page 7: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

Manne Siegbahn Laboratory

52 meters circumference

Page 8: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

ExperimentExperiment

• Long storage time – internal relaxation

• Multi-pass experiment

CRYRING Heavy Ion Storage Ring

electrons

neutrals

ions

Interaction - DR

ions

dipole magnet

SBD

• Electron cooling – well defined beam size

• Ions interact with electrons – dissociative recombination

• Well defined collision energies - velocity matched conditions

• Detect neutral fragments (from DR process)

Page 9: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

A2+ + e A + A; no grid

2A

Energy

Pulse height spectrum

Page 10: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

A2+ + e A + A; grid with 30% transmission

2A

A

Energy

Page 11: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

All fragment from one DR event hit the detector at the same time yield a pulse at an energy corresponding to full beam energy

Gives no information about

how the molecule breaks up

DR Branching DR Branching fractionfraction measurement measurement

C2H++e-

Page 12: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

Relate the fragments to different dissociation channels!

C2H++e-

2C

C+H

C

2C+H

DR Branching DR Branching ratioratio measurement measurement

C2H+ + e- C2

+ H

CH + C

C + C + H

e-

γN

βN

αN

T)-2T(1T)-T(10

T)(12TT)-T(10

T)-(1T0T)T(1

TTT

CN

HCN

2CN

H2CN

2

2

2

322

Page 13: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

DR Branching DR Branching ratiosratios – Hydrocarbon – Hydrocarbon ionsions

Products Ratio Products Ratio Products Ratio Products Ratio Products Ratio

C2+H 0.43 C2H+H 0.50 C2H2+H 0.29 C2H3+H 0.11 C2D4+D 0.12CH+C 0.39 C2+H2 0.02 C2H+H2 0.06 C2H2+H2 0.06 C2D3+D2 0.00C+C+H 0.18 C2+H+H 0.30 C2H+H+H 0.59 C2H2+H+H 0.66 C2D3+D+D 0.27

CH2+C 0.05 C2+H2+H 0.03 C2H+H2+H 0.10 C2D2+D2+D 0.28CH+CH 0.13 CH3+C 0.01 CH4+C 0.01 C2D2+D+D+D 0.13

CH2+CH 0.03 CH3+CH 0.02 C2D+D2+D2 0.00CH2+CH2 0.04 C2D+D2+D+D 0.00

CD4+CD 0.02CD3+CD2 0.17CD3+C+D2 0.00

C2D5+C2H

+ C2H2+ C2H3

+ C2H4+

Results have been compiled by Janev and Reiter (2002, 2004), and byFlorerscu-Mitchell and Mitchell (2006) and Adams, Poteryaand Babcock (2006)

Page 14: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

Viggiano et al. 2005

Page 15: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.
Page 16: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.
Page 17: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

CF2+ + e CF + F 714

CF3+ + e CF2 + F

8010Ehlerding et al. 2006

Page 18: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.
Page 19: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

New theory: PRL 90, 133201 (2003), PRA 68, 012703 (2003)

CRYRING

2000

Theory

ke[cm3s-1]

2003

AISA

Page 20: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

Kreckel et al., Phys. Rev. Lett. 95, 263201 (2005)

TSR

CRYRING

H3+

Page 21: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

H3+ D3

+

Page 22: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.
Page 23: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.
Page 24: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

D2H+ May 2007, CRYRING

Page 25: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.
Page 26: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.
Page 27: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

-900 V/ring

electrode

H2

para

Gas inlet/2 atm

Solenoid valve

Pinhole flange/ground

electrode

Insulating spacer

Skimmer

Page 28: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

Planned experimentPlanned experiment

Ion source will be characterised at the University of Illinois, in Ben McCall’s group with cavity ring-down spectroscopy; critical question: can we produce para-H3

+

using para-H2 as feed gas?

Experiment planned for September 2007, one week of beam time has been allocated

Page 29: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

Advanced Intergrated Stationary AfterglowGlosik et al. 2005

Page 30: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

Glosik et al. 2005

Page 31: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.

Summary HSummary H33++

Good agreement experiment-theory for dissociative recombination of H3

+, D3+ and H2D+

Several storage ring experiments agree with each other, but disagree with theory

Stationary afterglow experiments for H3+ give

almost factor 100 lower rate coefficient than storage rings and theory

Para-H3+ will be used in experiment in CRYRING

Page 32: Progress in measurements of dissociative recombination CRP on Atomic and Molecular Data for Plasma Modelling Mats Larsson Department of Physics Stockholm.