Drew Rotunno Mentor: Dr. Itzik Ben-Itzhak, Bethany Joachim Bethany Joachim.

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Fast beams of neutral molecules – the next generation of laser induced molecular dissociation imaging Drew Rotunno Mentor: Dr. Itzik Ben- Itzhak, Bethany Joachim

Transcript of Drew Rotunno Mentor: Dr. Itzik Ben-Itzhak, Bethany Joachim Bethany Joachim.

Page 1: Drew Rotunno Mentor: Dr. Itzik Ben-Itzhak, Bethany Joachim Bethany Joachim.

Fast beams of neutral molecules – the next generation of laser induced molecular

dissociation imagingDrew Rotunno

Mentor: Dr. Itzik Ben-Itzhak,

Bethany Joachim

Page 2: Drew Rotunno Mentor: Dr. Itzik Ben-Itzhak, Bethany Joachim Bethany Joachim.

Motivations

AMO – Atomic and Molecular Collisions

DETEC

TO

R

Page 3: Drew Rotunno Mentor: Dr. Itzik Ben-Itzhak, Bethany Joachim Bethany Joachim.

Motivations

AMO – Femtosecond laser pulses Laser-induced molecular dissociation imaging

DETEC

TO

R

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Motivations

Laser + Target Neutrals Not enough energy to detect

DETEC

TO

RD

ETEC

TO

R

E

Page 5: Drew Rotunno Mentor: Dr. Itzik Ben-Itzhak, Bethany Joachim Bethany Joachim.

Motivations

Laser + Fast Neutrals

DETEC

TO

R

Page 6: Drew Rotunno Mentor: Dr. Itzik Ben-Itzhak, Bethany Joachim Bethany Joachim.

Motivations

Q: How do we get fast neutrals?

A: Neutralize fast ions

Page 7: Drew Rotunno Mentor: Dr. Itzik Ben-Itzhak, Bethany Joachim Bethany Joachim.

Remove an electron from a negatively charged ion

Add an electron to a positively charged ion

How do we neutralize?

e

Page 8: Drew Rotunno Mentor: Dr. Itzik Ben-Itzhak, Bethany Joachim Bethany Joachim.

Target Choice

NOBLE GASSES

Argon (jet, cell)

Ionization energy ~15eV / atom vs. Alkali ~5eV

Very cheap and available and safe

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The Theory

H2+

Ar

H+

H2+

H2(H2

*)

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Cross sections

Collision probability, reinterpreted as area

Depends on species, both target and projectile

Depends on Beam energy

Page 11: Drew Rotunno Mentor: Dr. Itzik Ben-Itzhak, Bethany Joachim Bethany Joachim.

Measurements of Cross sections

H2+ + Ar, separated by product Charge transfer from Cs, by projectile

A.V. Phelps (1992) F.W. Meyer et al. (1977)

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Conversion rates

𝑌𝑁 𝑃

=𝑛𝑇 ∙𝑙𝑇 ∙𝜎Yield(H2)

Number of incoming particles

(H2+)Target particles per unit volume

Length

Cross Section

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Conversion rates

𝑌𝑁 𝑃

=𝑛𝑇 ∙𝑙𝑇 ∙𝜎

Solving for target density shows we need about At STP, this means we need 1 mTorr = .001 mmHg of pressure

~ 3 cm for few keV H2+ on Ar

Want 10%

?

Page 14: Drew Rotunno Mentor: Dr. Itzik Ben-Itzhak, Bethany Joachim Bethany Joachim.

The Theory

H2+

Ar

H+

H2+

H2(H2

*)

Page 15: Drew Rotunno Mentor: Dr. Itzik Ben-Itzhak, Bethany Joachim Bethany Joachim.

The Piece

diameter ~ 2 inches

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The Cut-away

Argon gas in

MicroChannel Plate

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The Microchannel Plate

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The Cut-away

Argon gas in

MicroChannel Plate

“Gas Mask”

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Fluid Flow Through Tubes

Higher length/radius ratio leads to more directed flow

Preserves vacuum

Ours: L/R ~ 80

W. Steckelmacher et al. (1978)

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Test Beamline

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Next Step - Testing

Measuring conversion factor How much H2 do we get? ( H fragments

too) Maximize

Fast feedback to optimize pressure▪ Too high – double collisions, more H

fragments States of molecules

Populations of ground vs. excited states▪ Hard to determine, but interesting to study

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End

Thanks KSU, Dr. Itzik Ben-Itzhak, IBI Group,National Science Foundation