X-Ray Transport, Diagnostic, & Commissioning Plans. LCLS Diagnostics and Commissioning Workshop

Size: px
Start display at page:

Download "X-Ray Transport, Diagnostic, & Commissioning Plans. LCLS Diagnostics and Commissioning Workshop"

Transcription

1 X-Ray Transport, Diagnostic, & Commissioning Plans LCLS Diagnostics and Commissioning Workshop *This work was performed under the auspices of the U.S. Department of Energy by the University of California, Lawrence Livermore National Laboratory under contract No. W-745-Eng-48 and by Stanford University, Stanford Linear Accelerator Center under contract No. DE-AC3-76SF515. September 22, 24 UCRL-PRES-26663

2 XTOD Layout Outline FEL parameters along Beam line XTOD Diagnostics and Front-End Optics Spontaneous Radiation Model Spontaneous and FEL signals in Direct Imager Diagnostic Spontaneous Reflection in Undulator Vacuum Chamber Conclusions September 22, 24 UCRL-PRES-26663

3 Diagnostics and Front-End Layout

4 1.5 Scope: Front End Enclosure/ Near Experimental Hall 4' Muon shield NEH PPS PPS Front End Enclosure Photon Beam Slit A 83 m Solid Attenuator 112 m Slit B Gas Attenuator Direct Imager Indirect Imager Flipper Mirror Comissioning: Spectrometer, Total Energy Electron Beam Fast close valve 13' Muon shield Electron Dump September 22, 24 UCRL-PRES-26663

5 Diagnostics for Commissioning 83 m from end of undulator 112 m from end of undulator Front End Enclosure Near Hall Hutch 1 Slits Gas Attenuator Solid Slits Attenuator Imaging Systems Calorimeter or spectrometer Muon Shield Muon Shield September 22, 24 UCRL-PRES-26663

6 FEL parameters along Beam line F = A e 2 x 2 + y w 2 2

7 FEL Parameters at KeV Z, m A, γ/nm 2 W, µm Dose Be Dose Si Dose Mo Slit Solid Atten Slit Hutch Flipper mirror Far Hall September 22, 24 UCRL-PRES-26663

8 Dose to melt for various materials Z Melt dose ev/atom Dose in NEH Hutch 1 1 kev 8 kev Beryllium Diamond Aluminum Silicon Copper Molybdenum Tin Tungsten Lead Doses should be compared to dose needed to melt September 22, 24 UCRL-PRES-26663

9 FEL Parameters at 4. KeV Z, m A, γ/nm 2 W, µm Dose Be Dose Si Dose Mo Slit Solid Atten Slit Hutch Flipper mirror Far Hall September 22, 24 UCRL-PRES-26663

10 FEL Parameters at.826 KeV Z, m A, γ/nm 2 W, µm Dose Be Dose Si Dose Mo Slit Solid Atten Slit Hutch Flipper mirror Far Hall September 22, 24 UCRL-PRES-26663

11 Material suitability a strong function of photon energy Fluence to Melt NEH Peak Fluence at entrance Low Z materials such as Be, C, B 4 C and Si will survive at least > 1 shot in the NEH Melts in NEH September 22, 24 UCRL-PRES-26663

12 Diagnostics and Front-End Optics

13 Gas and Solid Attenuators Gas Attenuator stage 2 Gas Attenuator stage 1 Gas Attenuator high pressure vesssel Slit B Autocad Solid Attenuator September 22, 24 UCRL-PRES-26663

14 Solid Be likely to survive at 88 m Xray Dose* Dose* Dose* Dose* Ephoton Li Be B4C C ev ev/atom ev/atom ev/atom ev/atom Be <.1 ev/atom for all photon energies September 22, 24 UCRL-PRES-26663

15 Pressure or thickness for 1-4 attenuation Use Gas Use Solids * 6 m of gas at pressure September 22, 24 UCRL-PRES-26663

16 Gas Attenuator Prototype Design and Analyses Will Validate Concepts 1 DP-Vacuum + Conductance Intermediate Flow Modeled C = C (1.114 P t m avg ( P d Fg + ( P avg avg d F ) g d F ) g Torr Time (s) Chamber Stage 2 Stage 4 September 22, 24 UCRL-PRES-26663

17 NEH Hutch 1 Diagnostic systems Direct Imager Indirect Imager Comissioning Tank September 22, 24 UCRL-PRES-26663

18 Star Cell Imaging Detector Tank Be Isolation valve Direct Imager (Placed directly in beam) Indirect Imager (Sees only a low intensity reflection) varian VA R Turbo pump September 22, 24 UCRL-PRES-26663

19 Imaging detector head prototype CCD Camera Microscope Objective X-ray beam LSO or YAG:Ce crystal prism assembly September 22, 24 UCRL-PRES-26663

20 Direct imager issues Vacuum Operation Low Photon Energy Performance 12 Hz Readout Afterglow in LSO High Energy Spontaneous Background Damage threshold September 22, 24 UCRL-PRES-26663

21 Indirect Imager reflects small amount of FEL into camera, avoiding damage Be Mirror Reflectivity at 8 KeV Be Mirror E-1 Be Mirror Reflectivity 1.E E-2.1 R.1 1.E-3 1.E-4 1.E-5 1.E-6 Be Mirror angle provides "gain" adjustment over several orders of magnitude and discriminates against high energy spontaneous background 1.E-7 1.E-8 Angle (degrees) September 22, 24 UCRL-PRES-26663

22 Minimum mirror reflectivity needed to fill CCD well Objective mag Solid Angle Optical efficiency Scintillator Sensitivity CCD QE 2.5 x 1.88E γ/mev.67 1 kev 4 kev 8 kev Photons / nm Photoelectrons 2. x x x 1 8 Full Well / PE 2.5 x x x 1-3 September 22, 24 UCRL-PRES-26663

23 Indirect imager issues Calibration Mirror roughness Tight camera geometry Compton background Vacuum θ 2θ mechanics Making mirror thin enough for maximum transmission Ceramic multilayers? Use as an Imaging Monochrometer September 22, 24 UCRL-PRES-26663

24 Commissioning strategy Start with Low Power Spontaneous Saturate Direct Imagers, measure linearity with solid attenuators Raise power, Measure linearity of Calorimeter and Indirect imager. Cross calibrate Test Gas Attenuator Raise Power, Look for FEL in Direct Imager Verify linearity with attenuators switch to Indirect Imager if scintilator damages September 22, 24 UCRL-PRES-26663

25 Spontaneous Radiation Model

26 Spontaneous Data Chain UCLA Near-Field Calculator ~2 Gbyte HDF5 HDF5 to Paradox Converter (x,y,e,p) Paradox format, 4 X 1 GByte ReBinner Coarser Energy Bins (159) (x,y,e,p) Paradox format, 35 MByte Blob DB Converter faster to read (E,P[x,y]) Paradox, 5 MBytes y Viewer x E September 22, 24 UCRL-PRES-26663

27 Spontaneous Fluence at NEH Hutch 1 Fluence 6 F x, y = P ( E) E E x, y 4 Y, mm X, mm Te = 4.5 GeV Z = 243 m x = 1. mm y =.3 mm 1.85 mj 4 2 Y, mm Fluence -2 X, mm Te = 14.5 GeV Z = 243 m x =.3 mm y =.1 mm 18.2 mj September 22, 24 UCRL-PRES-26663

28 Energy Slices Near-Field calculation 88 m from End-of-Undulator, Sven Richie, UCLA 2 mm 2 mm Far-Field calculation 4 m from Center-of-Undulator, Roman Tatchyn, SSRL < E < 1 kev 7.6 < E < 9. kev 1 < E < 2 kev 2 < E < 27 kev September 22, 24 UCRL-PRES-26663

29 LCLS beam footprint Expected LCLS beam profile contains FEL and Spontaneous halo 2-3 mj FEL 3 mj High energy core Eγ > 4 kev 2 mj Spontaneous At entrance to NEH, FEL tuned to 8261 ev Fundamental September 22, 24 UCRL-PRES-26663

30 Spontaneous and FEL signals in the Direct Imager Diagnostic

31 Camera Image Calculator Chain Spontaneous DB (E,P[x,y]) Spontaneous + ε x FEL Absorbed in 25 µm LSO Photoelectrons in Camera (2.5 x Zeiss + SITEC CCD) x ε y x E FEL Transmitted by Material September 22, 24 UCRL-PRES-26663

32 14.5 GeV Spontaneous, NEH H1 Y, mm Fluence -2 X, mm 2 All photons 4 6 Number / kev 8,,, 7,,, 6,,, 5,,, 4,,, 3,,, 2,,, 1,,, Photon Energy Spectra 2 4 E, kev 6 8 Y, mm Fluence -2 X, mm Stops in 25 µm LSO Number / kev 8,,, 7,,, 6,,, 5,,, 4,,, 3,,, 2,,, 1,,, Photon Energy Spectra 2 4 E, kev 6 8 September 22, 24 UCRL-PRES-26663

33 14.5 GeV Spontaneous Direct Imager Signal Photons Energy All photons Stops in 25 µm LSO CCD photoelectron levels < 15K e - Full well (16 bit) 327K e - so this is ½ scale on CCD readout (X-Ray resolution 3 x 1 µm) September 22, 24 PhotoElectrons/Pixel 15, 1, 5, -5 UCRL-PRES Photoelectrons/Pixel Horizontal LineOut X, mm

34 14.5 GeV Spontaneous + FEL Photons Energy All photons Stops in 25 µm LSO Y, mm Fluence -1 X, mm PhotoElectrons/Pixel 1,,, 5,, Photoelectrons/Pixel Horizontal LineOut (X-Ray resolution 3 x 1 µm) Need attenuation of 2.4 x 1-4 for CCD full well -4-2 X, mm September 22, 24 UCRL-PRES-26663

35 Use of 16.9 mm B 4 C Attenuator Raw photon spectra of FEL + Spontaneous Spectra of FEL + Spontaneous after B4C Photons/keV Spectra of photons stopping in LSO September 22, 24 UCRL-PRES-26663

36 Direct Imager Image 14.5 GeV 1% FEL + Spontaneous through 16.8 mm B 4 C into 25 mm LSO Y, mm Fluence -2 X, mm PhotoElectrons/Pixel 1, 5, Horizontal LineOut X, mm Good FEL signal at ½ CCD Full Scale but increased background in image (X-Ray resolution 3 x 1 µm) September 22, 24 UCRL-PRES-26663

37 Y, mm How faint can FEL be? 14.5 GeV 1% FEL + Spontaneous directly into 25 mm LSO Fluence -2 X, mm PhotoElectrons/Pixel 3,, 25,, 2,, 15,, 1,, 5,, Horizontal LineOut -4-2 X, mm (X-Ray resolution 3 x 1 µm) Y, mm Fluence.1% FEL + Spontaneous into Horizontal 25 mm LineOut LSO X, mm PhotoElectrons/Pixel 4, 3, 2, 1, X, mm September 22, 24 UCRL-PRES-26663

38 Y, mm Y, mm GeV Spontaneous, NEH H1 All photons -1 Fluence X, mm mj x 1 11 Stops in 25 Fluence µm LSO 1.25 mj , -2 1, , X, mm (X-Ray resolution 1 x 3 µm) PhotoElectrons/Pixel Direct Imager Photoelectrons Photons / kev Direct Imager Horizontal LineOut Photoelectrons X, mm September 22, 24 UCRL-PRES-26663

39 4.5 GeV Spontaneous + ε x FEL Direct Imager Image Direct Imager Photoelectrons 1 % FEL Y, mm Fluence X, mm 1 2 PhotoElectrons/Pixel 5,, 4,, 3,, 2,, 1,, Horizontal LineOut X, mm % FEL Y, mm Fluence X, mm September 22, PhotoElectrons/Pixel (X-Ray resolution 1 x 3 µm) UCRL-PRES , 2, 15, 1, 5, Horizontal LineOut X, mm

40 Commissioning with Direct Imager Direct Imager will see spontaneous on a single shot at GeV Direct Imager will need 1-4 attenuation for on scale operation at full FEL power, which increases background. These calculations show a factor of ~5-1 margin. Without attenuator, Direct Imager will see FEL at.1% power at 4.5 GeV and significantly <.1% at 14.5 GeV September 22, 24 UCRL-PRES-26663

41 Spontaneous Reflection in Undulator Vacuum Chamber

42 Spontaneous Monte Carlo Chain Spontaneous Blob DB (E,P[x,y]) Paradox, 5 Mbytes Inject FEL (E,P[x,y]) Paradox, 5 Mbytes Cumulative DB (x,y,f[e]) Paradox, 5 Mbytes ( E) Photon MC Generator creates random photons according to cumulative distribution (x,y,z,vx,vy,vz,e) of individual photons F x, y = E P P x, y x, y ( E) de ( E) de September 22, 24 UCRL-PRES-26663

43 Spontaneous Monte Carlo Simulation Source spatial distribution 2 1 Photon starting angles generated to give calculated spontaneous spatial distribution y, mm x, mm Photon starting x, y matches electron distribution, a Gaussian with σ = 3 µm 1 2 Events / 2 meter 15, 1, 5, Initial Z 1 z, meter 2 Photon starting z is uniform along undulator (from < z < 13 m) September 22, 24 UCRL-PRES-26663

44 Each photon final x, y has its own cumulative energy distribution Calculated far-field energy spectrum y Source Energy Distribution Events / 1 KeV 9, 8, 7, 6, 5, 4, 3, 2, 1, 5 E, K ev 1 x E September 22, 24 Monte Carlo Energy Distribution UCRL-PRES-26663

45 Simulated spatial distributions agree with far-field calculation Final y, mm Final position All Photons Final x, mm Final y, mm Final Position 1st harmonic Final x, mm Monte Carlo 465 m from beginning of undulator Far-Field Calculation 4 m from center of undulator September 22, 24 UCRL-PRES-26663

46 Simulated spatial distributions agree with far-field calculation higher orders Final y, mm Final position, 2nd harmonic Final y, mm Final Position, 3rd harmonic Final y, mm Final position, E> 4 KeV Final x, mm Final x, mm Final x, mm September 22, 24 UCRL-PRES-26663

47 Spontaneous Emission Angle Below Critical Angle 13 m 243 m 6-2 mm Θ min =.2.8 mrad Θ max = mrad Cu 8261 ev Cu 826 ev 1 1 R.5 R mrad Angle, mrad September 22, 24 UCRL-PRES-26663

48 Vacuum Pipe Simulation 14.5 GeV Without pipe With pipe 2 Final position 2 Final position Final y, mm 5-5 Final y, mm Final x, mm Final x, mm September 22, 24 UCRL-PRES-26663

49 Line outs through center Without pipe With pipe September 22, 24 UCRL-PRES-26663

50 Final y, mm Y, mm Final y, mm Flux Reflection at higher orders UCLA Calculation, without pipe -2 X, mm 2 Final Position 1st harmonic Final x, mm Final Position 1st harmonic Y, mm Final y, mm Monte Carlo, with pipe Final y, mm Monte Carlo, without pipe Final position, 2nd harmonic -4 Flux -2 X, mm Final x, mm Final position, 2nd harmonic Y, mm Final y, mm 6 Final y, mm Final Position, 3rd harmonic -4 Flux -2 X, mm Final x, mm Final Position, 3rd harmonic Final x, mm Final x, mm Final x, mm 4 6 < E < 1 kev 1 < E < 2 kev 2 < E < 3 kev September 22, 24 UCRL-PRES-26663

51 Photon Energies > 4 KeV 2 Final position, E> 4 KeV Final y, mm 1-1 Without pipe Final x, mm Final position, E> 4 KeV Final y, mm 1-1 With pipe Final x, mm September 22, 24 UCRL-PRES-26663

52 Reflection in pipe at 4.5 GeV Final position Final y, mm Final x, mm Final position 5 Final y, mm Final x, mm September 22, 24 UCRL-PRES-26663

53 Tilted pipe at 14.5 GeV Final y, mm F in a l p o s it io n Pipe parallel to beam F in a l x, m m Final y, mm Final position -1 1 Final x, mm Pipe tilted 19 µr, raised.9 mm, and shifted to the right.9 mm September 22, 24 UCRL-PRES-26663

54 Vacuum chamber reflections We will see a lot of reflection of the spontaneous off of the tube. The reflection will increase the spontaneous background in the center by x 3 to 4. Twists and tilts in the vaccum chamber will make it hard(er) to interpret the observed spontaneous radiation pattern September 22, 24 UCRL-PRES-26663

55 Future work and conclusions

56 Near term activities planned Modeling and Simulation - during CR Spontaneous / FEL simulations Calculate Beam sizes at Gas Attenuator, Cameras, etc. with apertures Re-sampling for true response at 14.5 GeV Simulations of Camera response to mix of Spontaneous and FEL with optimum attenuators and scintillator Decide on the apertures! Pipes, Muon shield, Component R&D - after CR Spectrometer, Total Energy, Damage Mechanical & Vacuum - after CR Decide on the apertures! Pipes, Muon shield, Gas Attenuator Calculations and Prototype Beam Line Layout / Standardization / Detailed Specifications September 22, 24 UCRL-PRES-26663

57 Layout geometry is set Summary Beam modeling codes in place Reflection off of undulator vacuum chamber seriously distorts the spontaneous radiation pattern Direct imager model in progress to specify scintillator and attenuator thickness, and CCD gain parameters. Need similar model for Indirect Imager, and Calorimeter. Modeling of other diagnostics will proceed in FY5 September 22, 24 UCRL-PRES-26663

X-ray Transport Optics and Diagnostics Commissioning Report

X-ray Transport Optics and Diagnostics Commissioning Report LCLS-TN-4-15 UCRL-PROC-27494 X-ray Transport Optics and Diagnostics Commissioning Report Richard M. Bionta, Lawrence Livermore National Laboratory. October 23, 24 LCLS Diagnostics and Commissioning Workshop,

More information

XTOD Layout and Diagnostic Systems. Facility Advisory Committee Meeting October 12-13, 2004

XTOD Layout and Diagnostic Systems. Facility Advisory Committee Meeting October 12-13, 2004 Facility Advisory Committee Meeting October 12-13, 24 This work was performed under the auspices of the U.S. Department of Energy by the University of California, Lawrence Livermore National Laboratory

More information

LCLS project update. John Arthur. LCLS Photon Systems Manager

LCLS project update. John Arthur. LCLS Photon Systems Manager LCLS project update LCLS Photon Systems Manager LCLS major construction nearly finished Technical systems turning on with good performance Experimental instruments Expectations for early operation First

More information

Today s Outline - January 25, C. Segre (IIT) PHYS Spring 2018 January 25, / 26

Today s Outline - January 25, C. Segre (IIT) PHYS Spring 2018 January 25, / 26 Today s Outline - January 25, 2018 C. Segre (IIT) PHYS 570 - Spring 2018 January 25, 2018 1 / 26 Today s Outline - January 25, 2018 HW #2 C. Segre (IIT) PHYS 570 - Spring 2018 January 25, 2018 1 / 26 Today

More information

Check the LCLS Project website to verify 2 of 7 that this is the correct version prior to use.

Check the LCLS Project website to verify 2 of 7 that this is the correct version prior to use. 1. Introduction: The XTOD Offset System (OMS) is designed to direct the LCLS FEL beam to the instruments and experimental stations, while substantially reducing the flux of unwanted radiation which accompanies

More information

Photon Diagnostics. FLASH User Workshop 08.

Photon Diagnostics. FLASH User Workshop 08. Photon Diagnostics FLASH User Workshop 08 Kai.Tiedtke@desy.de Outline What kind of diagnostic tools do user need to make efficient use of FLASH? intensity (New GMD) beam position intensity profile on the

More information

ABSTRACT. Supported by U.S. DoE grant No. DE-FG02-96ER54375

ABSTRACT. Supported by U.S. DoE grant No. DE-FG02-96ER54375 ABSTRACT A CCD imaging system is currently being developed for T e (,t) and bolometric measurements on the Pegasus Toroidal Experiment. Soft X-rays (E

More information

Photon Beamlines and Diagnostics at LCLS

Photon Beamlines and Diagnostics at LCLS SLAC-PUB-14348 Photon Beamlines and Diagnostics at LCLS S. Moeller¹*, J. Arthur¹, A. Brachmann¹, R. Coffee¹, F.-J. Decker¹, Y. Ding¹, D. Dowell¹, S. Edstrom¹, P. Emma¹, Y. Feng¹, A. Fisher¹, J. Frisch¹,

More information

Status of the PRad Experiment (E )

Status of the PRad Experiment (E ) Status of the PRad Experiment (E12-11-106) NC A&T State University Outline Experimental apparatus, current status Installation plan Draft run plan Summary PRad Experimental Setup Main detectors and elements:

More information

Yiping FENG DCO

Yiping FENG DCO LUSI Diagnostics and Common Optics Pop-in Profile/Wavefront Monitors Optics Review [sp39100004-1_xrpopinprofmon-prd] Yiping Feng LUSI Instrument Scientist February 10, 2009 Outline Introduction Performance

More information

NIST EUVL Metrology Programs

NIST EUVL Metrology Programs NIST EUVL Metrology Programs S.Grantham, C. Tarrio, R.E. Vest, Y. Barad, S. Kulin, K. Liu and T.B. Lucatorto National Institute of Standards and Technology (NIST) Gaithersburg, MD USA L. Klebanoff and

More information

Electron Beam Diagnosis Using K-edge Absorp8on of Laser-Compton Photons

Electron Beam Diagnosis Using K-edge Absorp8on of Laser-Compton Photons LLNL-PRES-740689 Electron Beam Diagnosis Using K-edge Absorp8on of Laser-Compton Photons Y. Hwang 1, D. J. Gibson 2, R. A. Marsh 2, T. Tajima 1, C. P. J. Barty 1 1 University of California, Irvine 2 Lawrence

More information

Pixel hybrid photon detectors

Pixel hybrid photon detectors Pixel hybrid photon detectors for the LHCb-RICH system Ken Wyllie On behalf of the LHCb-RICH group CERN, Geneva, Switzerland 1 Outline of the talk Introduction The LHCb detector The RICH 2 counter Overall

More information

Monte Carlo Simulation of the PRad Experiment at JLab 1

Monte Carlo Simulation of the PRad Experiment at JLab 1 Monte Carlo Simulation of the PRad Experiment at JLab 1 Li Ye Mississippi State University for the PRad collaboration 1.This work is supported in part by NSF MRI award PHY-1229153, the U.S. Department

More information

x-ray Beam Size Monitor

x-ray Beam Size Monitor x-ray Beam Size Monitor J. Alexander, N. Eggert, J. Flanagan, W. Hopkins, B. Kreis, M. McDonald, D. Peterson, N. Rider Goals: 2 products: tuning tool with rapid feedback of beam height during LET measurements

More information

RANDY W. ALKIRE, GEROLD ROSENBAUM AND GWYNDAF EVANS

RANDY W. ALKIRE, GEROLD ROSENBAUM AND GWYNDAF EVANS S-94,316 PATENTS-US-A96698 BEAM POSITION MONITOR RANDY W. ALKIRE, GEROLD ROSENBAUM AND GWYNDAF EVANS CONTRACTUAL ORIGIN OF THE INVENTION The United States Government has rights in this invention pursuant

More information

THz Pump Beam for LCLS. Henrik Loos. LCLS Hard X-Ray Upgrade Workshop July 29-31, 2009

THz Pump Beam for LCLS. Henrik Loos. LCLS Hard X-Ray Upgrade Workshop July 29-31, 2009 Beam for LCLS Henrik Loos Workshop July 29-31, 29 1 1 Henrik Loos Overview Coherent Radiation Sources Timing THz Source Performance 2 2 Henrik Loos LCLS Layout 6 MeV 135 MeV 25 MeV 4.3 GeV 13.6 GeV σ z.83

More information

Measurements of MeV Photon Flashes in Petawatt Laser Experiments

Measurements of MeV Photon Flashes in Petawatt Laser Experiments UCRL-JC-131359 PREPRINT Measurements of MeV Photon Flashes in Petawatt Laser Experiments M. J. Moran, C. G. Brown, T. Cowan, S. Hatchett, A. Hunt, M. Key, D.M. Pennington, M. D. Perry, T. Phillips, C.

More information

LUSI Pulse Picker System

LUSI Pulse Picker System ENGINEERING SPECIFICATION DOCUMENT (ESD) Doc. No. SP-391-001-50 R0 LUSI SUB-SYSTEM DCO LUSI Pulse Picker System Rick Jackson Design Engineer, Author Signature Date Marc Campell DCO Design Engineer Signature

More information

Upgrade of the ultra-small-angle scattering (USAXS) beamline BW4

Upgrade of the ultra-small-angle scattering (USAXS) beamline BW4 Upgrade of the ultra-small-angle scattering (USAXS) beamline BW4 S.V. Roth, R. Döhrmann, M. Dommach, I. Kröger, T. Schubert, R. Gehrke Definition of the upgrade The wiggler beamline BW4 is dedicated to

More information

Undulator K-Parameter Measurements at LCLS

Undulator K-Parameter Measurements at LCLS Undulator K-Parameter Measurements at LCLS J. Welch, A. Brachmann, F-J. Decker, Y. Ding, P. Emma, A. Fisher, J. Frisch, Z. Huang, R. Iverson, H. Loos, H-D. Nuhn, P. Stefan, D. Ratner, J. Turner, J. Wu,

More information

LCLS-II-HE Instrumentation

LCLS-II-HE Instrumentation LCLS-II-HE Instrumentation Average Brightness (ph/s/mm 2 /mrad 2 /0.1%BW) LCLS-II-HE: Enabling New Experimental Capabilities Structural Dynamics at the Atomic Scale Expand the photon energy reach of LCLS-II

More information

MC SIMULATION OF SCATTER INTENSITIES IN A CONE-BEAM CT SYSTEM EMPLOYING A 450 kv X-RAY TUBE

MC SIMULATION OF SCATTER INTENSITIES IN A CONE-BEAM CT SYSTEM EMPLOYING A 450 kv X-RAY TUBE MC SIMULATION OF SCATTER INTENSITIES IN A CONE-BEAM CT SYSTEM EMPLOYING A 450 kv X-RAY TUBE A. Miceli ab, R. Thierry a, A. Flisch a, U. Sennhauser a, F. Casali b a Empa - Swiss Federal Laboratories for

More information

Infrared Single Shot Diagnostics for the Longitudinal. Profile of the Electron Bunches at FLASH. Disputation

Infrared Single Shot Diagnostics for the Longitudinal. Profile of the Electron Bunches at FLASH. Disputation Infrared Single Shot Diagnostics for the Longitudinal Profile of the Electron Bunches at FLASH Disputation Hossein Delsim-Hashemi Tuesday 22 July 2008 7/23/2008 2/ 35 Introduction m eb c 2 3 2 γ ω = +

More information

Status of the LHCb Experiment

Status of the LHCb Experiment Status of the LHCb Experiment Werner Witzeling CERN, Geneva, Switzerland On behalf of the LHCb Collaboration Introduction The LHCb experiment aims to investigate CP violation in the B meson decays at LHC

More information

MPI Halbleiterlabor. MPI Semiconductor Laboratory. MPI mf

MPI Halbleiterlabor. MPI Semiconductor Laboratory. MPI mf MPI Halbleiterlabor MPI Semiconductor Laboratory MPI mf LCLS User Workshop, SLAC, Menlo Park, 18. 10. 2008 Lothar Strüder, MPI Halbleiterlabor and Universität Siegen 1 Prepared by 1. MPI-HLL (MPE and MPP)

More information

CESRTA Low Emittance Tuning Instrumentation: x-ray Beam Size Monitor

CESRTA Low Emittance Tuning Instrumentation: x-ray Beam Size Monitor CESRTA Low Emittance Tuning Instrumentation: x-ray Beam Size Monitor xbsm group: (those who sit in the tunnel) J. Alexander, N. Eggert, J. Flanagan, W. Hopkins, B. Kreis, M. McDonald, D. Peterson, N. Rider

More information

Nonintercepting Diagnostics for Transverse Beam Properties: from Rings to ERLs

Nonintercepting Diagnostics for Transverse Beam Properties: from Rings to ERLs Nonintercepting Diagnostics for Transverse Beam Properties: from Rings to ERLs Alex H. Lumpkin Accelerator Operations Division Advanced Photon Source Presented at Jefferson National Accelerator Laboratory

More information

BL39XU Magnetic Materials

BL39XU Magnetic Materials BL39XU Magnetic Materials BL39XU is an undulator beamline that is dedicated to hard X-ray spectroscopy and diffractometry requiring control of the X-ray polarization state. The major applications of the

More information

On-line spectrometer for FEL radiation at

On-line spectrometer for FEL radiation at On-line spectrometer for FEL radiation at FERMI@ELETTRA Fabio Frassetto 1, Luca Poletto 1, Daniele Cocco 2, Marco Zangrando 3 1 CNR/INFM Laboratory for Ultraviolet and X-Ray Optical Research & Department

More information

VUV-FEL User workshop, August 23-24, 2004

VUV-FEL User workshop, August 23-24, 2004 Layout of the user facility Kai Tiedtke Kai Tiedtke, HASYLAB@ VUV-FEL User workshop, August 23-24, 2004 Kai.Tiedtke@desy.de Kai Tiedtke, HASYLAB@ Outline Photon beam transport Layout of the experimental

More information

Breakout Session 3: Mirror Update. 2007/4/ /22 Peter M. Stefan LCLS Facility Advisory Committee (FAC) Meeting

Breakout Session 3: Mirror Update. 2007/4/ /22 Peter M. Stefan LCLS Facility Advisory Committee (FAC) Meeting Breakout Session 3: Mirror Update 2007/4/16-17 1/22 Peter M. Stefan LCLS Facility Advisory Committee (FAC) Meeting stefan@slac.stanford.edu Breakout Session 3: Mirror Update Overall Offset Mirror System

More information

Demonstration of exponential growth and saturation at VUV wavelengths at the TESLA Test Facility Free-Electron Laser. P. Castro for the TTF-FEL team

Demonstration of exponential growth and saturation at VUV wavelengths at the TESLA Test Facility Free-Electron Laser. P. Castro for the TTF-FEL team Demonstration of exponential growth and saturation at VUV wavelengths at the TESLA Test Facility Free-Electron Laser P. Castro for the TTF-FEL team 100 nm 1 Å FEL radiation TESLA Test Facility at DESY

More information

Performance of 8-stage Multianode Photomultipliers

Performance of 8-stage Multianode Photomultipliers Performance of 8-stage Multianode Photomultipliers Introduction requirements by LHCb MaPMT characteristics System integration Test beam and Lab results Conclusions MaPMT Beetle1.2 9 th Topical Seminar

More information

LCLS Injector Diagnostics. Henrik Loos. Diagnostics overview Transverse Beam Properties Longitudinal Beam Properties

LCLS Injector Diagnostics. Henrik Loos. Diagnostics overview Transverse Beam Properties Longitudinal Beam Properties Diagnostics overview Transverse Beam Properties Longitudinal Beam Properties LCLS Diagnostics Tasks Charge Toroids (Gun, Inj, BC, Und) Faraday cups (Gun & Inj) Trajectory & energy Stripline BPMs (Gun,

More information

Air Bearing Monochromator at APS 13-ID-E (GSECARS)

Air Bearing Monochromator at APS 13-ID-E (GSECARS) Air Bearing Monochromator at APS 13-ID-E (GSECARS) Matt Newville, Peter Eng, Mark Rivers, GSECARS, U Chicago Paul Murray, IDT Upgraded Canted Beamline at GSECARS Air-bearing monochromator Performance and

More information

FLASH 2. FEL seminar. Charge: 0.5 nc. Juliane Rönsch-Schulenburg Overview of FLASH 2 Hamburg,

FLASH 2. FEL seminar. Charge: 0.5 nc. Juliane Rönsch-Schulenburg Overview of FLASH 2 Hamburg, FLASH 2 FEL seminar Juliane Rönsch-Schulenburg Overview of FLASH 2 Hamburg, 2016-03-22 Charge: 0.5 nc Overview 1. FLASH 2 Overview 1.Layout parameters 2. Operation FLASH2. 1.Lasing at wavelengths between

More information

Optics for next generation light sources

Optics for next generation light sources Optics for next generation light sources Anton Barty Centre for Free Electron Laser Science Hamburg, Germany Key issues Optical specifications Metrology (mirror surfaces) Metrology (wavefront, focal spot)

More information

Optimization of Energy Modulation Filter for Dual Energy CBCT Using Geant4 Monte-Carlo Simulation

Optimization of Energy Modulation Filter for Dual Energy CBCT Using Geant4 Monte-Carlo Simulation Original Article PROGRESS in MEDICAL PHYSICS 27(3), Sept. 2016 http://dx.doi.org/10.14316/pmp.2016.27.3.125 pissn 2508-4445, eissn 2508-4453 Optimization of Energy Modulation Filter for Dual Energy CBCT

More information

Water-Window Microscope Based on Nitrogen Plasma Capillary Discharge Source

Water-Window Microscope Based on Nitrogen Plasma Capillary Discharge Source 2015 International Workshop on EUV and Soft X-Ray Sources Water-Window Microscope Based on Nitrogen Plasma Capillary Discharge Source T. Parkman 1, M. F. Nawaz 2, M. Nevrkla 2, M. Vrbova 1, A. Jancarek

More information

Wir schaffen Wissen heute für morgen

Wir schaffen Wissen heute für morgen Analyzing Wavefront and Spectrum of Hard X-ray Free-Electron Laser Radiation SLS (since 2001) Wir schaffen Wissen heute für morgen PSI: SLAC: SACLA: EuroXFEL: C. David, S. Rutishauser, P. Karvinen, I.

More information

Advanced Beam Instrumentation and Diagnostics for FELs

Advanced Beam Instrumentation and Diagnostics for FELs Advanced Beam Instrumentation and Diagnostics for FELs P. Evtushenko, Jefferson Lab with help and insights from many others: S. Benson, D. Douglas, Jefferson Lab T. Maxwell, P. Krejcik, SLAC S. Wesch,

More information

High granularity scintillating fiber trackers based on Silicon Photomultiplier

High granularity scintillating fiber trackers based on Silicon Photomultiplier High granularity scintillating fiber trackers based on Silicon Photomultiplier A. Papa Paul Scherrer Institut, Villigen, Switzerland E-mail: angela.papa@psi.ch Istituto Nazionale di Fisica Nucleare Sez.

More information

FIRST INDIRECT X-RAY IMAGING TESTS WITH AN 88-mm DIAMETER SINGLE CRYSTAL

FIRST INDIRECT X-RAY IMAGING TESTS WITH AN 88-mm DIAMETER SINGLE CRYSTAL FERMILAB-CONF-16-641-AD-E ACCEPTED FIRST INDIRECT X-RAY IMAGING TESTS WITH AN 88-mm DIAMETER SINGLE CRYSTAL A.H. Lumpkin 1 and A.T. Macrander 2 1 Fermi National Accelerator Laboratory, Batavia, IL 60510

More information

Partial Replication of Storms/Scanlan Glow Discharge Radiation

Partial Replication of Storms/Scanlan Glow Discharge Radiation Partial Replication of Storms/Scanlan Glow Discharge Radiation Rick Cantwell and Matt McConnell Coolescence, LLC March 2008 Introduction The Storms/Scanlan paper 1 presented at the 8 th international workshop

More information

Yasar Onel, University of Iowa; Dave Winn, Fairfield Univ. 1/20/2005

Yasar Onel, University of Iowa; Dave Winn, Fairfield Univ. 1/20/2005 Project name R&D for luminosity monitor Classification (accelerator: subsystem) IPBI / Accelerator Institution(s) and personnel University of Iowa, Department of Physics and Astronomy: Yasar Onel (professor)

More information

X-ray generation by femtosecond laser pulses and its application to soft X-ray imaging microscope

X-ray generation by femtosecond laser pulses and its application to soft X-ray imaging microscope X-ray generation by femtosecond laser pulses and its application to soft X-ray imaging microscope Kenichi Ikeda 1, Hideyuki Kotaki 1 ' 2 and Kazuhisa Nakajima 1 ' 2 ' 3 1 Graduate University for Advanced

More information

Radiographic sensitivity improved by optimized high resolution X -ray detector design.

Radiographic sensitivity improved by optimized high resolution X -ray detector design. DIR 2007 - International Symposium on Digital industrial Radiology and Computed Tomography, June 25-27, 2007, Lyon, France Radiographic sensitivity improved by optimized high resolution X -ray detector

More information

New fabrication and packaging technologies for CMOS pixel sensors: closing gap between hybrid and monolithic

New fabrication and packaging technologies for CMOS pixel sensors: closing gap between hybrid and monolithic New fabrication and packaging technologies for CMOS pixel sensors: closing gap between hybrid and monolithic Outline Short history of MAPS development at IPHC Results from TowerJazz CIS test sensor Ultra-thin

More information

Outline of the proposed JLAMP VUV/soft X-ray FEL and the challenges for the photon beamlines and optics

Outline of the proposed JLAMP VUV/soft X-ray FEL and the challenges for the photon beamlines and optics Outline of the proposed JLAMP VUV/soft X-ray FEL and the challenges for the photon beamlines and optics J. Michael Klopf Jefferson Lab - Free Electron Laser Division Workshop on Future Light Sources SLAC

More information

Phase 1 upgrade of the CMS pixel detector

Phase 1 upgrade of the CMS pixel detector Phase 1 upgrade of the CMS pixel detector, INFN & University of Perugia, On behalf of the CMS Collaboration. IPRD conference, Siena, Italy. Oct 05, 2016 1 Outline The performance of the present CMS pixel

More information

Circumference 187 m (bending radius = 8.66 m)

Circumference 187 m (bending radius = 8.66 m) 4. Specifications of the Accelerators Table 1. General parameters of the PF storage ring. Energy 2.5 GeV (max 3.0 GeV) Initial stored current multi-bunch 450 ma (max 500 ma at 2.5GeV) single bunch 70 ma

More information

OPERATION OF A SINGLE PASS, BUNCH-BY-BUNCH X-RAY BEAM SIZE MONITOR FOR THE CESR TEST ACCELERATOR RESEARCH PROGRAM*

OPERATION OF A SINGLE PASS, BUNCH-BY-BUNCH X-RAY BEAM SIZE MONITOR FOR THE CESR TEST ACCELERATOR RESEARCH PROGRAM* OPERATION OF A SINGLE PASS, BUNCH-BY-BUNCH X-RAY BEAM SIZE MONITOR FOR THE CESR TEST ACCELERATOR RESEARCH PROGRAM* N.T. Rider, M. G. Billing, M.P. Ehrlichman, D.P. Peterson, D. Rubin, J.P. Shanks, K. G.

More information

The Henryk Niewodniczański INSTITUTE OF NUCLEAR PHYSICS Polish Academy of Sciences ul. Radzikowskiego 152, Kraków, Poland.

The Henryk Niewodniczański INSTITUTE OF NUCLEAR PHYSICS Polish Academy of Sciences ul. Radzikowskiego 152, Kraków, Poland. The Henryk Niewodniczański INSTITUTE OF NUCLEAR PHYSICS Polish Academy of Sciences ul. Radzikowskiego 152, 31-342 Kraków, Poland. www.ifj.edu.pl/reports/2003.html Kraków, grudzień 2003 Report No 1931/PH

More information

Design of Photon Beamlines at the European XFEL

Design of Photon Beamlines at the European XFEL Design of Photon Beamlines at the European XFEL Harald Sinn (THOCI1) FEL 2010 Malmö August 26, 2010 Construction progress at the European XFEL www.xfel.eu Experimental Hall in Schenefeld Injector building

More information

CXRS-edge Diagnostic in the Harsh ITER Environment

CXRS-edge Diagnostic in the Harsh ITER Environment 1 FIP/P4-17 CXRS-edge Diagnostic in the Harsh ITER Environment A.Zvonkov 1, M.De Bock 2, V.Serov 1, S.Tugarinov 1 1 Project Center ITER, Kurchatov sq.1, Building 3, 123182 Moscow, Russia 2 ITER Organization,

More information

DALLA LUCE VISIBILE AI RAGGI X: NUOVI RIVELATORI DI IMMAGINI PER RAGGI X A DISCRIMINAZIONE IN ENERGIA ED APPLICAZIONI

DALLA LUCE VISIBILE AI RAGGI X: NUOVI RIVELATORI DI IMMAGINI PER RAGGI X A DISCRIMINAZIONE IN ENERGIA ED APPLICAZIONI DALLA LUCE VISIBILE AI RAGGI X: NUOVI RIVELATORI DI IMMAGINI PER RAGGI X A DISCRIMINAZIONE IN ENERGIA ED APPLICAZIONI D. Pacella ENEA - Frascati LIMS, Frascati 14-15 ottobre 2015 Come per la fotografia:

More information

Commissioning of Thomson Scattering on the Pegasus Toroidal Experiment

Commissioning of Thomson Scattering on the Pegasus Toroidal Experiment Commissioning of Thomson Scattering on the Pegasus Toroidal Experiment D.J. Schlossberg, R.J. Fonck, L.M. Peguero, G.R. Winz University of Wisconsin-Madison 55 th Annual Meeting of the APS Division of

More information

membrane sample EUV characterization

membrane sample EUV characterization membrane sample EUV characterization Christian Laubis, PTB Outline PTB's synchrotron radiation lab Scatter from structures Scatter from random rough surfaces Measurement geometries SAXS Lifetime testing

More information

X-rays. X-rays are produced when electrons are accelerated and collide with a target. X-rays are sometimes characterized by the generating voltage

X-rays. X-rays are produced when electrons are accelerated and collide with a target. X-rays are sometimes characterized by the generating voltage X-rays Ouch! 1 X-rays X-rays are produced when electrons are accelerated and collide with a target Bremsstrahlung x-rays Characteristic x-rays X-rays are sometimes characterized by the generating voltage

More information

Detection and application of Doppler and motional Stark features in the DNB emission spectrum in the high magnetic field of the Alcator C-Mod tokamak

Detection and application of Doppler and motional Stark features in the DNB emission spectrum in the high magnetic field of the Alcator C-Mod tokamak Detection and application of Doppler and motional Stark features in the DNB emission spectrum in the high magnetic field of the Alcator C-Mod tokamak I. O. Bespamyatnov a, W. L. Rowan a, K. T. Liao a,

More information

A Parallel Radial Mirror Energy Analyzer Attachment for the Scanning Electron Microscope

A Parallel Radial Mirror Energy Analyzer Attachment for the Scanning Electron Microscope 142 doi:10.1017/s1431927615013288 Microscopy Society of America 2015 A Parallel Radial Mirror Energy Analyzer Attachment for the Scanning Electron Microscope Kang Hao Cheong, Weiding Han, Anjam Khursheed

More information

P61 BEAMLINE. Calculations of beamline characteristics Version 2.3

P61 BEAMLINE. Calculations of beamline characteristics Version 2.3 P61 BEAMLINE 31-1-18 Calculations of beamline characteristics Version.3 PHOTON FLUX FROM WIGGLERS FOR P61 1E+13 13 5 15 1.E+13 1 mm x 1 mm aperture Flux (ph/s/.1%b.w.) 1E+1 1 1.E+1 P61A (m) 1E+11 11 1E+

More information

X-ray Detectors: What are the Needs?

X-ray Detectors: What are the Needs? X-ray Detectors: What are the Needs? Sol M. Gruner Physics Dept. & Cornell High Energy Synchrotron Source (CHESS) Ithaca, NY 14853 smg26@cornell.edu 1 simplified view of the Evolution of Imaging Synchrotron

More information

Advances in X-Ray Scintillator Technology Roger D. Durst Bruker AXS Inc.

Advances in X-Ray Scintillator Technology Roger D. Durst Bruker AXS Inc. Advances in X-Ray Scintillator Technology Roger D. Durst Inc. Acknowledgements T. Thorson, Y. Diawara, E. Westbrook, MBC J. Morse, ESRF C. Summers, Georgia Tech/PTCE B. Wagner, Georgia Tech/PTCE V. Valdna,

More information

ANALYTICAL MICRO X-RAY FLUORESCENCE SPECTROMETER

ANALYTICAL MICRO X-RAY FLUORESCENCE SPECTROMETER Copyright(c)JCPDS-International Centre for Diffraction Data 2001,Advances in X-ray Analysis,Vol.44 325 ANALYTICAL MICRO X-RAY FLUORESCENCE SPECTROMETER ABSTRACT William Chang, Jonathan Kerner, and Edward

More information

Muon Collider background rejection in ILCroot Si VXD and Tracker detectors

Muon Collider background rejection in ILCroot Si VXD and Tracker detectors Muon Collider background rejection in ILCroot Si VXD and Tracker detectors N. Terentiev (Carnegie Mellon U./Fermilab) MAP 2014 Winter Collaboration Meeting Dec. 3-7, 2014 SLAC New MARS 1.5 TeV Muon Collider

More information

NIF Neutron Bang Time Detector Development on OMEGA

NIF Neutron Bang Time Detector Development on OMEGA NIF Neutron Bang Time Detector Development on OMEGA 2400 2200 NBT2 scintillator bang time (ps) 2000 1800 1600 1400 1200 rms = 54 ps 1000 1000 1200 1400 1600 1800 2000 2200 2400 V. Yu. Glebov University

More information

SIMULATION OF A SIGNAL IN THE BEAM LOSS

SIMULATION OF A SIGNAL IN THE BEAM LOSS RADIATION ASPECTS OF LHC SIMULATION OF A SIGNAL IN THE BEAM LOSS MONITORS OF THE MOMENTUM CLEANING INSERTION FOR THE NEW COLLIMATOR JAWS DESIGN IHEP, Protvino, Russia Summary of the presentation Page 1

More information

VELA PHOTOINJECTOR LASER. E.W. Snedden, Lasers and Diagnostics Group

VELA PHOTOINJECTOR LASER. E.W. Snedden, Lasers and Diagnostics Group VELA PHOTOINJECTOR LASER E.W. Snedden, Lasers and Diagnostics Group Contents Introduction PI laser step-by-step: Ti:Sapphire oscillator Regenerative amplifier Single-pass amplifier Frequency mixing Emphasis

More information

Workshop IGLEX Andromède & ThomX 23 June 2016, LAL Orsay. The X-line of ThomX.

Workshop IGLEX Andromède & ThomX 23 June 2016, LAL Orsay. The X-line of ThomX. Workshop IGLEX Andromède & ThomX 23 June 2016, LAL Orsay The X-line of ThomX jerome.lacipiere@neel.cnrs.fr mjacquet@lal.in2p3.fr Brightness panorama of X-ray (10-100 kev) sources Synchrotron : not very

More information

MICRO XRF OF LIGHT ELEMENTS USING A POLYCAPILLARY LENS AND AN ULTRA THIN WINDOW SILICON DRIFT DETECTOR INSIDE A VACUUM CHAMBER

MICRO XRF OF LIGHT ELEMENTS USING A POLYCAPILLARY LENS AND AN ULTRA THIN WINDOW SILICON DRIFT DETECTOR INSIDE A VACUUM CHAMBER Copyright JCPDS - International Centre for Diffraction Data 2005, Advances in X-ray Analysis, Volume 48. 229 MICRO XRF OF LIGHT ELEMENTS USING A POLYCAPILLARY LENS AND AN ULTRA THIN WINDOW SILICON DRIFT

More information

Status of the PRad Experiment (E )

Status of the PRad Experiment (E ) Status of the PRad Experiment (E12-11-106) NC A&T State University for the PRad collaboration Outline PRad Physics goals Experimental setup Current status Summary The Proton Charge Radius Puzzle New high

More information

Change History Log. Rev Revision Sections Affected Description of Change /25/08 All Initial Version

Change History Log. Rev Revision Sections Affected Description of Change /25/08 All Initial Version Change History Log Rev Revision Sections Affected Description of Change Number Date 000 2/25/08 All Initial Version 2 of 20 that this is the correct version prior to use. Introduction: The AMO instrument

More information

Physics Laboratory Scattering of Photons from Electrons: Compton Scattering

Physics Laboratory Scattering of Photons from Electrons: Compton Scattering RR Oct 2001 SS Dec 2001 MJ Oct 2009 Physics 34000 Laboratory Scattering of Photons from Electrons: Compton Scattering Objective: To measure the energy of high energy photons scattered from electrons in

More information

Radiological Safety Analysis Document for the CLAS12 Engineering and the first physics run of Run Group A

Radiological Safety Analysis Document for the CLAS12 Engineering and the first physics run of Run Group A Radiological Safety Analysis Document for the CLAS12 Engineering and the first physics run of Run Group A This Radiological Safety Analysis Document (RSAD) will identify the general conditions associated

More information

3 General layout of the XFEL Facility

3 General layout of the XFEL Facility 3 General layout of the XFEL Facility 3.1 Introduction The present chapter provides an overview of the whole European X-Ray Free-Electron Laser (XFEL) Facility layout, enumerating its main components and

More information

Operation of a Single Pass, Bunch-by-bunch x-ray Beam Size Monitor for the CESR Test Accelerator Research Program. October 3, 2012

Operation of a Single Pass, Bunch-by-bunch x-ray Beam Size Monitor for the CESR Test Accelerator Research Program. October 3, 2012 Operation of a Single Pass, Bunch-by-bunch x-ray Beam Size Monitor for the CESR Test Accelerator Research Program October 3, 2012 Goals Goals For This Presentation: 1.Provide an overview of the efforts

More information

Roman Pots. Marco Oriunno SLAC, PPA. M.Oriunno, SLAC

Roman Pots. Marco Oriunno SLAC, PPA. M.Oriunno, SLAC Roman Pots Marco Oriunno SLAC, PPA The Roman Pot technique 1. The Roman Pot, an historically successful technique for near beam physics: ISR, SPS, TEVATRON, RICH, DESY 2. A CERN in-house technology: ISR,

More information

Components of Optical Instruments

Components of Optical Instruments Components of Optical Instruments General Design of Optical Instruments Sources of Radiation Wavelength Selectors (Filters, Monochromators, Interferometers) Sample Containers Radiation Transducers (Detectors)

More information

The CMS Outer HCAL SiPM Upgrade.

The CMS Outer HCAL SiPM Upgrade. The CMS Outer HCAL SiPM Upgrade. Artur Lobanov on behalf of the CMS collaboration DESY Hamburg CALOR 2014, Gießen, 7th April 2014 Outline > CMS Hadron Outer Calorimeter > Commissioning > Cosmic data Artur

More information

The HPD DETECTOR. Michele Giunta. VLVnT Workshop "Technical Aspects of a Very Large Volume Neutrino Telescope in the Mediterranean Sea"

The HPD DETECTOR. Michele Giunta. VLVnT Workshop Technical Aspects of a Very Large Volume Neutrino Telescope in the Mediterranean Sea The HPD DETECTOR VLVnT Workshop "Technical Aspects of a Very Large Volume Neutrino Telescope in the Mediterranean Sea" In this presentation: The HPD working principles The HPD production CLUE Experiment

More information

Red Laser for Monitoring Light Source

Red Laser for Monitoring Light Source Red Laser for Monitoring Light Source Liyuan Zhang, Kejun Zhu and Ren-yuan Zhu Caltech Duncan Liu JPL CMS ECAL Week, CERN April 16, 22 A Brief History. Red Laser Specification. Result of Market Survey.

More information

Calibration of KAP meters

Calibration of KAP meters Calibration of KAP meters Alexandr Malusek! Division of Radiological Sciences Department of Medical and Health Sciences Linköping University! 2014-04-15 1 Outline 1. KAP meter construction 2. Air kerma-area

More information

pcvd diamond beam position monitors for PETRA III

pcvd diamond beam position monitors for PETRA III pcvd diamond beam position monitors for PETRA III Eckhard Wörner Diamond Materials GmbH Tullastraße 72, 79108 Freiburg, Germany CARAT workshop 13-15.12.09 1/39 Outline Some news about Diamond Materials

More information

Initial Results from a Cryogenic Proton Irradiation of a p-channel CCD

Initial Results from a Cryogenic Proton Irradiation of a p-channel CCD Centre for Electronic Imaging Initial Results from a Cryogenic Proton Irradiation of a p-channel CCD Jason Gow Daniel Wood, David Hall, Ben Dryer, Simeon Barber, Andrew Holland and Neil Murray Jason P.

More information

Supplementary Information

Supplementary Information Supplementary Information Supplementary Figure 1. Modal simulation and frequency response of a high- frequency (75- khz) MEMS. a, Modal frequency of the device was simulated using Coventorware and shows

More information

High Rep-Rate KrF Laser Development and Intense Pulse Interaction Experiments for IFE*

High Rep-Rate KrF Laser Development and Intense Pulse Interaction Experiments for IFE* High Rep-Rate KrF Laser Development and Intense Pulse Interaction Experiments for IFE* Y. Owadano, E. Takahashi, I. Okuda, I. Matsushima, Y. Matsumoto, S. Kato, E. Miura and H.Yashiro 1), K. Kuwahara 2)

More information

MEC Laser Systems. Bill White LCLS Laser Group Leader April 13, Bill White. MEC Laser Systems. MEC Workshop.

MEC Laser Systems. Bill White LCLS Laser Group Leader April 13, Bill White. MEC Laser Systems. MEC Workshop. Bill White LCLS Laser Group Leader April 13, 2009 1 1 Bill White Outline Laser Requirements / Wish List Energy vs. Rep Rate Trade-offs Baseline ns laser fs laser Layout in Hutch 6 Other possibilities Helen

More information

The SIRAD irradiation facility at the INFN - Legnaro National Laboratory

The SIRAD irradiation facility at the INFN - Legnaro National Laboratory The SIRAD irradiation facility at the INFN - Legnaro National Laboratory I. Introduction 2 The INFN - Legnaro National Laboratory (LNL) SIRAD beamline http://www.lnl.infn.it 3 What is SIRAD? SIRAD is the

More information

Introduction to X-ray Detectors for Synchrotron Radiation Applications

Introduction to X-ray Detectors for Synchrotron Radiation Applications Introduction to X-ray Detectors for Synchrotron Radiation Applications Pablo Fajardo Instrumentation Services and Development Division ESRF, Grenoble EIROforum School on Instrumentation (ESI 2011) Outline

More information

NORMAL-INCIDENCE MULTILAYER MIRROR X-RAY MICROSCOPE

NORMAL-INCIDENCE MULTILAYER MIRROR X-RAY MICROSCOPE NORMAL-NCDENCE MULTLAYER MRROR X-RAY MCROSCOPE FNAL REPORT FG03-93SF20141 DSCLAMER Thii report was prepared as an account of work sponsored by an agency of the United States Government. Neither the United

More information

Beam Diagnostics, Low Level RF and Feedback for Room Temperature FELs. Josef Frisch Pohang, March 14, 2011

Beam Diagnostics, Low Level RF and Feedback for Room Temperature FELs. Josef Frisch Pohang, March 14, 2011 Beam Diagnostics, Low Level RF and Feedback for Room Temperature FELs Josef Frisch Pohang, March 14, 2011 Room Temperature / Superconducting Very different pulse structures RT: single bunch or short bursts

More information

A Measurement of the Photon Detection Efficiency of Silicon Photomultipliers

A Measurement of the Photon Detection Efficiency of Silicon Photomultipliers A Measurement of the Photon Detection Efficiency of Silicon Photomultipliers A. N. Otte a,, J. Hose a,r.mirzoyan a, A. Romaszkiewicz a, M. Teshima a, A. Thea a,b a Max Planck Institute for Physics, Föhringer

More information

RF Time Measuring Technique With Picosecond Resolution and Its Possible Applications at JLab. A. Margaryan

RF Time Measuring Technique With Picosecond Resolution and Its Possible Applications at JLab. A. Margaryan RF Time Measuring Technique With Picosecond Resolution and Its Possible Applications at JLab A. Margaryan 1 Contents Introduction RF time measuring technique: Principles and experimental results of recent

More information

I. PERFORMANCE OF X-RAY PRODUCTION COMPONENTS FLUOROSCOPIC ACCEPTANCE TESTING: TEST PROCEDURES & PERFORMANCE CRITERIA

I. PERFORMANCE OF X-RAY PRODUCTION COMPONENTS FLUOROSCOPIC ACCEPTANCE TESTING: TEST PROCEDURES & PERFORMANCE CRITERIA FLUOROSCOPIC ACCEPTANCE TESTING: TEST PROCEDURES & PERFORMANCE CRITERIA EDWARD L. NICKOLOFF DEPARTMENT OF RADIOLOGY COLUMBIA UNIVERSITY NEW YORK, NY ACCEPTANCE TESTING GOALS PRIOR TO 1st CLINICAL USAGE

More information

Shintake Monitor Nanometer Beam Size Measurement and Beam Tuning

Shintake Monitor Nanometer Beam Size Measurement and Beam Tuning Shintake Monitor Nanometer Beam Size Measurement and Beam Tuning Technology and Instrumentation in Particle Physics 2011 Chicago, June 11 Jacqueline Yan, M.Oroku, Y. Yamaguchi T. Yamanaka, Y. Kamiya, T.

More information

Hadron Calorimeter for Hall A (HCAL-J)

Hadron Calorimeter for Hall A (HCAL-J) Hadron Calorimeter for Hall A (HCAL-J) Status report 7/11/12 G.B. Franklin, Carnegie Mellon JLAB/ CMU/ JINR/INFN-CT Collaboration Based on JINR design used at COMPASS 1 JINR (DUBNA) produced 9 HCAL modules

More information

Introduction. Chapter 16 Diagnostic Radiology. Primary radiological image. Primary radiological image

Introduction. Chapter 16 Diagnostic Radiology. Primary radiological image. Primary radiological image Introduction Chapter 16 Diagnostic Radiology Radiation Dosimetry I Text: H.E Johns and J.R. Cunningham, The physics of radiology, 4 th ed. http://www.utoledo.edu/med/depts/radther In diagnostic radiology

More information

The CMS ECAL Laser Monitoring System

The CMS ECAL Laser Monitoring System The CMS ECAL Laser Monitoring System CALOR 2006 XII INTERNATIONAL CONFERENCE on CALORIMETRY in HIGH ENERGY PHYSICS Adi Bornheim California Institute of Technology Chicago, June 8, 2006 Introduction CMS

More information