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Start-to-End Simulations Numerical Modeling of FLASH and the European XFEL Igor Zagorodnov Deutsches Elektronen Synchrotron, Hamburg, Germany S2E Meeting, DESY 24. September 2012

Numerical Modeling of FLASH and the European XFEL · 2012-09-24 · Igor Zagorodnov | ICAP 2012| 22. August 2012 | Seite 3 Motivation to verify the facility design and to improve

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Page 1: Numerical Modeling of FLASH and the European XFEL · 2012-09-24 · Igor Zagorodnov | ICAP 2012| 22. August 2012 | Seite 3 Motivation to verify the facility design and to improve

Start-to-End Simulations

Numerical Modeling of FLASH and the European XFEL

Igor Zagorodnov

Deutsches Elektronen Synchrotron,Hamburg, Germany

S2E Meeting, DESY24. September 2012

Page 2: Numerical Modeling of FLASH and the European XFEL · 2012-09-24 · Igor Zagorodnov | ICAP 2012| 22. August 2012 | Seite 3 Motivation to verify the facility design and to improve

Igor Zagorodnov| ICAP 2012| 22. August 2012 | Seite 2

Content

� motivation

� FLASH simulations

� XFEL simulations

� tools, internet presence and publications

� challenges

Page 3: Numerical Modeling of FLASH and the European XFEL · 2012-09-24 · Igor Zagorodnov | ICAP 2012| 22. August 2012 | Seite 3 Motivation to verify the facility design and to improve

Igor Zagorodnov| ICAP 2012| 22. August 2012 | Seite 3

Motivation

�to verify the facility design and to improve it�to explain facility performance and to improve it�to develop new ideas, facilities etc.

Why do we need S2E simulations?

accelerator undulator

laser light

Page 4: Numerical Modeling of FLASH and the European XFEL · 2012-09-24 · Igor Zagorodnov | ICAP 2012| 22. August 2012 | Seite 3 Motivation to verify the facility design and to improve

Igor Zagorodnov| ICAP 2012| 22. August 2012 | Seite 4

Motivation

�to reproduce the measurements�to predict the measurements

Can we trust the S2E simulations?

Yes! If we are able

Page 5: Numerical Modeling of FLASH and the European XFEL · 2012-09-24 · Igor Zagorodnov | ICAP 2012| 22. August 2012 | Seite 3 Motivation to verify the facility design and to improve

Igor Zagorodnov| ICAP 2012| 22. August 2012 | Seite 5

FLASH Simulations

gun accelerator undulator laboratory

Page 6: Numerical Modeling of FLASH and the European XFEL · 2012-09-24 · Igor Zagorodnov | ICAP 2012| 22. August 2012 | Seite 3 Motivation to verify the facility design and to improve

Igor Zagorodnov| ICAP 2012| 22. August 2012 | Seite 6

FLASH Simulations

�detailed simulation of the whole facility�simulation of experiments (triangular profile)�simulations of measurements (weak

compression, spike mode)� longitudinal wakes are included�BBA, microbunching, trajectory jitter etc?

Already done

Page 7: Numerical Modeling of FLASH and the European XFEL · 2012-09-24 · Igor Zagorodnov | ICAP 2012| 22. August 2012 | Seite 3 Motivation to verify the facility design and to improve

Igor Zagorodnov| ICAP 2012| 22. August 2012 | Seite 7

FLASH Simulations

�more accurate simulations without suspicious steps (matching, shifting of slice centers etc.)

�to reproduce the LOLA measurements at FLASH for average and strong compression

�to explain the SASE dependence on ACC1 gradient

�to include the transverse wakes

Has to be done (short term)

Page 8: Numerical Modeling of FLASH and the European XFEL · 2012-09-24 · Igor Zagorodnov | ICAP 2012| 22. August 2012 | Seite 3 Motivation to verify the facility design and to improve

Igor Zagorodnov| ICAP 2012| 22. August 2012 | Seite 8

XFEL Simulations

Layout

1 130MeVE =1,1M

Gun

1,3M

2M 3M 4M

LH

DL 1BC 2BC 3BC2 700MeVE = 3 2400 MeVE = 4 14 /17.5GeVE =

Page 9: Numerical Modeling of FLASH and the European XFEL · 2012-09-24 · Igor Zagorodnov | ICAP 2012| 22. August 2012 | Seite 3 Motivation to verify the facility design and to improve

Igor Zagorodnov| ICAP 2012| 22. August 2012 | Seite 9

XFEL Simulations

�detailed simulation of the facility up to the collimation section

�simulation of different compression scenarious

� longitudinal wakes partially included�BBA, microbunching, quad errors, etc?

Already done

Page 10: Numerical Modeling of FLASH and the European XFEL · 2012-09-24 · Igor Zagorodnov | ICAP 2012| 22. August 2012 | Seite 3 Motivation to verify the facility design and to improve

Igor Zagorodnov| ICAP 2012| 22. August 2012 | Seite 10

XFEL Simulations

�simulations of the whole facility�more accurate simulations without suspicious

steps (matching, shifting of slice centers etc.)�simulations of non-standart scenarious

(different charges in the train etc.)�tollerance studies

Has to be done (short term)

Page 11: Numerical Modeling of FLASH and the European XFEL · 2012-09-24 · Igor Zagorodnov | ICAP 2012| 22. August 2012 | Seite 3 Motivation to verify the facility design and to improve

Igor Zagorodnov| ICAP 2012| 22. August 2012 | Seite 11

Tools, Internet Presence and Publications

�convertors�fast trackers�manuals, tests, examples

Tools

�tools �results documented�reproducibility of the results

Internet Presence

� internal reports� in referred journals

Publications

Page 12: Numerical Modeling of FLASH and the European XFEL · 2012-09-24 · Igor Zagorodnov | ICAP 2012| 22. August 2012 | Seite 3 Motivation to verify the facility design and to improve

Igor Zagorodnov| ICAP 2012| 22. August 2012 | Seite 12

Challenges

� simulation of FLASH II� simulation and explanation of XFEL performance� plasma experiments at FLASH

� the simulations has to checked through experiments� we have to be able to reproduce the measurements� we have to be able to predict the measurements

We have to continue the accelerator code development!

Page 13: Numerical Modeling of FLASH and the European XFEL · 2012-09-24 · Igor Zagorodnov | ICAP 2012| 22. August 2012 | Seite 3 Motivation to verify the facility design and to improve

Igor Zagorodnov| ICAP 2012| 22. August 2012 | Seite 13

Challenges

The European XFEL Machine FAQ?

https://slacportal.slac.stanford.edu/sites/lclscore_public/Lists/LCLS_FAQ/FAQ.aspx

See, for example, LCLS Machine FAQ

� What is the photon energy range and how long does it take to switch?� What is the highest pulse energy available (number of photons in the

pulse) and how does it vary with photon energy and pulse length?� What is the x-ray pulse length, how long does it take to change it, and

how does the pulse energy and peak power vary with pulse length?� How does the x-ray transverse beam size vary with photon energy and

electron peak current settings?� What are the temporal characteristics of the x-ray pulse, including

number of spikes, spike duration, peak power in each spike, and how does this vary with photon energy and peak current?