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Nuclear Physics Type talks 1) Adriana Gagyi- Palffy 2) Ken Ledingham 3) Fred Hartmann 4) Silvia Cipiccia

Nuclear Physics Type talks 1) Adriana Gagyi-Palffy 2) Ken Ledingham 3) Fred Hartmann 4) Silvia Cipiccia 5) Chris Murphy

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Page 1: Nuclear Physics Type talks 1) Adriana Gagyi-Palffy 2) Ken Ledingham 3) Fred Hartmann 4) Silvia Cipiccia 5) Chris Murphy

Nuclear Physics Type talks

1) Adriana Gagyi-Palffy2) Ken Ledingham3) Fred Hartmann4) Silvia Cipiccia5) Chris Murphy

Page 2: Nuclear Physics Type talks 1) Adriana Gagyi-Palffy 2) Ken Ledingham 3) Fred Hartmann 4) Silvia Cipiccia 5) Chris Murphy

Quantum Control of Nuclei with Coherent x-

ray light

Adriana Palffy

Page 3: Nuclear Physics Type talks 1) Adriana Gagyi-Palffy 2) Ken Ledingham 3) Fred Hartmann 4) Silvia Cipiccia 5) Chris Murphy

Doppler shift

0 keV

50.1 keV

223Ra

3/2-

3/2+

bridge the gap between nuclear excitation and photon energies...

T. Bürvenich, J. Evers and C. H. Keitel, PRL 96, 142501 (2006)

Nuclear excitations and the XFEL XFEL

Page 4: Nuclear Physics Type talks 1) Adriana Gagyi-Palffy 2) Ken Ledingham 3) Fred Hartmann 4) Silvia Cipiccia 5) Chris Murphy

What about the Petawatt laser?

Create the dense plasma for NEEC/NEET?

NEEC: to compare advantages of a dedicated electron target!

Help have an ion accelerator and XFEL at the same spot?

Will ELI provide ion accelerationand coherent x-rays or gamma-rays?

If yes, good enough for nuclear applications?

NIF? Plenty of electrons, photons, neutrons.

Can we model/analyze what is going on?

PW laser

Page 5: Nuclear Physics Type talks 1) Adriana Gagyi-Palffy 2) Ken Ledingham 3) Fred Hartmann 4) Silvia Cipiccia 5) Chris Murphy

Nuclear quantum optics applications for XFEL light

Coherent control of nuclei in a three-level system

triggering level

isomer

ground state

Conclusions

Combination of nuclear excitations in plasmas: trade-off between control and efficiency?

Driving of nuclear transitions via electrons or photons

NEECNEET

Isomer depletion – nuclear batteries?

STIRAP with nuclei

Page 6: Nuclear Physics Type talks 1) Adriana Gagyi-Palffy 2) Ken Ledingham 3) Fred Hartmann 4) Silvia Cipiccia 5) Chris Murphy

Cartoon of NEET/NEECKritcher et al LLNL

Page 7: Nuclear Physics Type talks 1) Adriana Gagyi-Palffy 2) Ken Ledingham 3) Fred Hartmann 4) Silvia Cipiccia 5) Chris Murphy

The theory is now sufficiently well understood that competing nuclear excitation by scattered electrons and direct photons can easily be calculated leaving NEET/NEEC experimental comparisons with theory meaningful

Page 8: Nuclear Physics Type talks 1) Adriana Gagyi-Palffy 2) Ken Ledingham 3) Fred Hartmann 4) Silvia Cipiccia 5) Chris Murphy

Sylvia talked about about electron acceleration up to about GeV in Wakefield acceleration and when coupled to either undulators or Betatron Emission mode promised monochromatic photons up to MeV levels

Page 9: Nuclear Physics Type talks 1) Adriana Gagyi-Palffy 2) Ken Ledingham 3) Fred Hartmann 4) Silvia Cipiccia 5) Chris Murphy

Peak brilliance of light sources with star of GRLS at 1MeV 15 orders of magnitude greater than all synchrotrons and FELS

Page 10: Nuclear Physics Type talks 1) Adriana Gagyi-Palffy 2) Ken Ledingham 3) Fred Hartmann 4) Silvia Cipiccia 5) Chris Murphy

Strathclyde/Jena Laser Wakefield Radiation Source

(Nature Physics, 2007)

~70 MeV electron bunch generates optical photons

Page 11: Nuclear Physics Type talks 1) Adriana Gagyi-Palffy 2) Ken Ledingham 3) Fred Hartmann 4) Silvia Cipiccia 5) Chris Murphy

Toward LWFA driven FEL: undulator VUV radiation measurements at Strathclyde

Compact radiation sources based on laser-plasma wakefield accelerators

Betatron radiation: a promising compact tuneable x- gamma-ray femtosecond source

The Scottish Centre for the Application of Plasma Based Accelerators. SCAPA 200-300TW laser for applications: nuclear physics, health sciences, plasma physics

Page 12: Nuclear Physics Type talks 1) Adriana Gagyi-Palffy 2) Ken Ledingham 3) Fred Hartmann 4) Silvia Cipiccia 5) Chris Murphy

Overview of High Brightness Gamma-Ray Light Source – Nuclear Photonics –Nuclear Fluorescence Resonance

Fred Hartemann

Page 13: Nuclear Physics Type talks 1) Adriana Gagyi-Palffy 2) Ken Ledingham 3) Fred Hartmann 4) Silvia Cipiccia 5) Chris Murphy

GRLS)

Gamma ray resonant fluorescence

Mainland security

Nuclear waste reclassification

Page 14: Nuclear Physics Type talks 1) Adriana Gagyi-Palffy 2) Ken Ledingham 3) Fred Hartmann 4) Silvia Cipiccia 5) Chris Murphy

Storing radioactive waste at power stations

There are hundreds of thousands of such barrels world wide with very little knowledge of the contents. GRLSs would enable certifiable classification of the waste contents

Page 15: Nuclear Physics Type talks 1) Adriana Gagyi-Palffy 2) Ken Ledingham 3) Fred Hartmann 4) Silvia Cipiccia 5) Chris Murphy

Depository of hundreds of drums of radioactive waste

Page 16: Nuclear Physics Type talks 1) Adriana Gagyi-Palffy 2) Ken Ledingham 3) Fred Hartmann 4) Silvia Cipiccia 5) Chris Murphy

Antimatter creation (Positrons) using

Intense lasersVia

Bethe Heitler Process Z+e- =Z+2e- + e+

Trident Process Z+γ = Z+e- + e +

Using different thicknesses of targets

Page 17: Nuclear Physics Type talks 1) Adriana Gagyi-Palffy 2) Ken Ledingham 3) Fred Hartmann 4) Silvia Cipiccia 5) Chris Murphy

Although laser created positrons have been seen before Chris indicated that programs on

VULCAN and Gemini had not been successful. However what had

been learned could eventually lead to successful results in the future

with the counter-propogating beams in vacuum leading to

creation of antimatter