numerical modeling of flash and the european xfel · 2012-09-24 · igor zagorodnov | icap 2012|...

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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

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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?