Vitali Khachatryan, Arthur Tarloyan, Vahe Sahakyan, V. Tsakanov

Slides:



Advertisements
Similar presentations
X-ray Free Electron lasers Zhirong Huang. Lecture Outline XFEL basics XFEL basics XFEL projects and R&D areas XFEL projects and R&D areas Questions and.
Advertisements

1 Optimal focusing lattice for XFEL undulators: Numerical simulations Vitali Khachatryan, Artur Tarloyan CANDLE, DESY/MPY
Undulator Physics April 29, 2004 Heinz-Dieter Nuhn, SLAC / SSRL Facility Advisory Committee Meeting Undulator Physics Diagnostics.
Performance Analysis Using Genesis 1.3 Sven Reiche LCLS Undulator Parameter Workshop Argonne National Laboratory 10/24/03.
Undulator Physics Update October 12, 2004 Heinz-Dieter Nuhn, SLAC / LCLS Facility Advisory Committee Meeting Undulator Physics Update.
Recirculating pass optics V.Ptitsyn, D.Trbojevic, N.Tsoupas.
GINGER Results for the NEW LCLS Undulator Configuration William M. Fawley Lawrence Berkeley National Laboratory Presented to LCLS Undulator Parameter Workshop.
Undulator Gap Increase Linac Coherent Light Source Stanford Synchrotron Radiation Laboratory Stanford Linear Accelerator Center.
Overview of Proposed Parameter Changes Linac Coherent Light Source Stanford Synchrotron Radiation Laboratory Stanford Linear Accelerator.
Undulator Specifications Linac Coherent Light Source Stanford Synchrotron Radiation Laboratory Stanford Linear Accelerator Center.
J. Pflüger / DESY - Radiation Damage Workshop Stanford June 19, 2008 Radiation Damage Study at FLASH using the Diagnostic Undulator J. Pflüger, J. Skupin,
The impact of undulators in an ERL Jim Clarke ASTeC, STFC Daresbury Laboratory FLS 2012, March 2012.
Undulator parameters choice/wish based on a simplified XFEL cost model Jürgen Pfingstner 29 st of July 2015.
Operated by the Jefferson Science Associates for the U.S. Depart. Of Energy Thomas Jefferson National Accelerator Facility Alex Bogacz, Dogbone RLA – Design.
B. FaatzS2E workshop, August 18-22, XFEL simulations with GENESIS Outline: Undulator layout (real/simulated) Matching Genesis.
Beam Dynamics and FEL Simulations for FLASH Igor Zagorodnov and Martin Dohlus Beam Dynamics Meeting, DESY.
Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.
28-May-2008Non-linear Beam Dynamics WS1 On Injection Beam Loss at the SPring-8 Storage Ring Masaru TAKAO & J. Schimizu, K. Soutome, and H. Tanaka JASRI.
Max Cornacchia, SLAC LCLS Project Overview BESAC, Feb , 2001 LCLS Project Overview What is the LCLS ? Transition from 3 rd generation light sources.
1 Alternative Bunch Compressor 30 th Sep KNU Eun-San Kim.
Basic Energy Sciences Advisory Committee MeetingLCLS February 26, 2001 J. Hastings Brookhaven National Laboratory LCLS Scientific Program X-Ray Laser Physics:
HYBRID WARM-COLD SYNCHROTRON FOR THE MUON COLLIDER Al Garren July 28, 2011.
Kiyoshi Kubo Electron beam in undulators of e+ source - Emittance and orbit angle with quad misalignment and corrections - Effect of beam pipe.
NON-WIGGLER-AVERAGED START-TO-END SIMULATIONS OF HIGH-GAIN FREE- ELECTRON LASERS H.P. Freund Science Applications International Corp. McLean, Virginia.
DESY Deutsches Electron Synchrotron Shima Bayesteh.
PEP-X Ultra Low Emittance Storage Ring Design at SLAC Lattice Design and Optimization Min-Huey Wang SLAC National Accelerator Laboratory With contributions.
Design Considerations of table-top FELs laser-plasma accelerators principal possibility of table-top FELs possible VUV and X-ray scenarios new experimental.
Transverse Gradient Undulator and its applications to Plasma-Accelerator Based FELs Zhirong Huang (SLAC) Introduction TGU concept, theory, technology Soft.
Operated by the Southeastern Universities Research Association for the U.S. Depart. Of Energy Thomas Jefferson National Accelerator Facility Alex Bogacz,
Lattice design for FCC-ee Bastian Haerer (CERN BE-ABP-LAT, Karlsruhe Institute of Technology (KIT)) 1 8 th Gentner Day, 28 October 2015.
1 BROOKHAVEN SCIENCE ASSOCIATES 1 NSLS-II Lattice Design 1.TBA-24 Lattice Design - Advantages and shortcomings Low emittance -> high chromaticity -> small.
Parameter scan for the CLIC damping rings July 23rd, 2008 Y. Papaphilippou Thanks to H. Braun, M. Korostelev and D. Schulte.
What did we learn from TTF1 FEL? P. Castro (DESY).
1 Project X Workshop November 21-22, 2008 Richard York Chris Compton Walter Hartung Xiaoyu Wu Michigan State University.
HF2014 Workshop, Beijing, China 9-12 October 2014 Challenges and Status of the FCC-ee lattice design Bastian Haerer Challenges.
Harmonic lasing in the LCLSII SXR beamline G. Marcus, Y. Ding, Z. Huang 11/21/2013.
Simulations of X-ray production for different undulator options 19 th of March 2015 Juergen Pfingstner.
Operated by JSA for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Alex Bogacz IDS- NF Acceleration Meeting, Jefferson Lab,
Some Simulations for the Proposed Hard X-Ray Self- Seeding on LCLS J. Wu J. Wu et al. Feb. 25, 2011.
From Beam Dynamics K. Kubo
Seeding in the presence of microbunching
Eduard Prat / Sven Reiche :: Paul Scherrer Institute
EUPRAXIA-PISA JUNE 2016 e-Beam-Laser
Beam Dynamics in Curved ILC Main Linac (following earth curvature)
NSLS-II Lattice Design Strategies Weiming Guo 07/10/08
Paul Scherrer Institut
Yuhui Li How to edit the title slide
Limitations of Electron Beam Conditioning in Free-Electron Lasers
Free Electron Lasers (FEL’s)
F. Villa Laboratori Nazionali di Frascati - LNF On behalf of Sparc_lab
Progress activities in short bunch compressors
LHC (SSC) Byung Yunn CASA.
Two-bunch self-seeding for narrow-bandwidth hard x-ray FELs
XFEL Simulations with SIMPLEX and GENESIS (Some preliminary results)
Design of an ECHO-seeded FEL at nm wavelength
SASE FEL PULSE DURATION ANALYSIS FROM SPECTRAL CORRELATION FUNCTION
Status of FEL Physics Research Worldwide  Claudio Pellegrini, UCLA April 23, 2002 Review of Basic FEL physical properties and definition of important.
Gain Computation Sven Reiche, UCLA April 24, 2002
LCLS FEL Parameters Heinz-Dieter Nuhn, SLAC / SSRL April 23, 2002
Achieving Required Peak Spectral Brightness Relative Performance for Four Undulator Technologies Neil Thompson WP5 – 20/03/19.
Undulator Physics Diagnostics / Commissioning Strategy Heinz-Dieter Nuhn, SLAC / SSRL August 11, 2004 Undulator Overview FEL Parameters Diagnostics and.
Coupler Effects in High Energy Part of XFEL Linac
XFEL Beam Dynamics Activity at CANDLE
BEAM REALISTIC ERROR ORBIT IMPACT ON SASE PERFORMANCE
Linear beam dynamics simulations for XFEL beam distribution system
Progress on Non-linear Beam Dynamic Study
Fanglei Lin, Yuhong Zhang JLEIC R&D Meeting, March 10, 2016
Fanglei Lin MEIC R&D Meeting, JLab, July 16, 2015
Fanglei Lin JLEIC R&D Meeting, August 4, 2016
3.2 km FODO lattice for 10 Hz operation (DMC4)
Presentation transcript:

Vitali Khachatryan, Arthur Tarloyan, Vahe Sahakyan, V. Tsakanov XFEL Simulation Results for various Focusing Lattices Vitali Khachatryan, Arthur Tarloyan, Vahe Sahakyan, V. Tsakanov CANDLE XFEL Beam Dynamics Group Meeting, 31 March 2008

Contents Introduction SASE1 simulations SASE2 simulations Summary The purpose of the simulation study: the investigation of the impact of focusing lattice various arrangements with the reduced number of the quadrupole magnets on the SASE FEL performance.

Introduction Wavelength Beta-average Phase Adv. Ncell SASE1 λ=0.1 nm β=32m μ=22.4° 17 SASE2 λ=0.1 nm β=46m μ=15° 24 SASE2 λ=0.4 nm β=15m μ=54° 24 SASE3 λ=0.4-1.6 nm β=15m μ=54° 11

The purpose of the simulation study: the investigation of the impact of focusing lattice various arrangements with the reduced number of the quadrupole magnets on the SASE FEL performance. Undul Undul F D Lcell=12.2 Focusing lattice -design Reduction of quadrupole fields Reduction of quadrupole misalignment effects

(Time-dependent simulation with the GENESIS). SASE1 Simulations Dependence of the normalized radiation parameters on the number of quadrupole magnets and the average beta function (Time-dependent simulation with the GENESIS). Number of Quads Beta function [m] Maximal Power Spacial size Divergence Bandwidth Brilliance 34 32 1 18 0.91 1.05 1.03 1.04 0.745 64 0.971 1.07 0.855 1.02 1.14 128 0.557 1.33 0.64 0.716 10 0.624 1.23 0.608

SASE2 Simulations The study was conducted for the two extreme values of the wavelength range 0.1nm and 0.4nm. Dependence on mean beta function of the saturation length and radiation brightness for the two different arrangements of the focusing lattice was investigated.

Current design

SASE2 Simulations – 0.1 -0.4 nm (in process) Figure 1. Beta function in x and y direction for XFEL lattices.

SASE3 Simulations SASE3 FEL GENESIS Steady State Simulation Results; Power growth curves for focusing lattice arrangements with quadrupole magnets number equal to 22, 12 and 6. Wavelength is 1.6nm (the highest value for 17.5 GeV beam energy).

SASE3 FEL simulations N quads 22 12 Rad. Power at Saturation (GW) 280 207 Saturation length (m) 65.5 87 Pirce param. (x10**-3) 1.76 1.4 Brightness 1 1.3

Intermediate Summary SASE 1 Reduction of FODO cells by factor of 2 and beta 64 m Brightness increase– 14% Decrease of Power – 3% SASE 2 - Reduction of FODO cells by factor of 2 and beta 70m. Brightness increase - 10% Saturation length increase – 2.7% SASE 2 Reduction of FODO cells by 2 and beta 35m Brightness decrease - 10% Saturation length increase – 17% (247m) SASE 3 - With reduced number of quadrupoles by factor 2 Brightness increase - 30% Saturation length increase -32%