2
A.Shapovalov ([email protected]) for the BIW2010, Santa Fee, New Mexico, USA Emittance Measurement Wizard at PITZ. Abstract The Photo Injector Test Facility at DESY, Zeuthen site (PITZ) develops electron sources of high brightness beams, required for linac based free electron lasers (FELs) like FLASH or the European XFEL. One of the key issues in electron beam optimization is the minimization of the transverse emittance. The main method to measure emittance at PITZ is a single slit scan technique, implying local beam divergence measurement by insertion of the slit mask at a definite location within the beam and measurements of the transmitted beamlet profile downstream of the slit station. “Emittance Measurement Wizard” (EMWiz) is the program used by PITZ operators for automated emittance measurements. EMWiz combines an acquisition program for beam and beamlet image recording and a postprocessing tool for the analysis of the measured transverse phase space of the electron beam. It provides a way to execute the difficult emittance measurements in an automatic mode and to get a calculated emittance result. Photo Injector Test facility at DESY, Zeuthen site (PITZ) Three EMSY stations are located in the current setup. The first EMSY station (EMSY1) behind the exit of the booster cavity is used in the standard emittance measurement procedure. It is at 5.74 m downstream the photocathode corresponding to the expected minimum emittance location. Emittance Measurement at PITZ Transverse emittance measurement using slit scan technique For this technique, the local divergence is estimated by transversely cutting the electron beam into thin slices. Then, the size of the beamlets created by the slits is measured at the YAG screen at some distance downstream the EMSY station. The 10 m slit and a distance between the slit mask and the beamlet observation screen of 2.64 m are used in the standard emittance measurement. In the emittance measurement setup and procedure, intrinsic cuts have been minimized by e.g. using highly sensitive screens, a 12 bit signal resolution CCD-camera and a large area of interest to cover the whole beam distribution. Therefore, emittance value is called 100% rms emittance. The momenta of the beam after the gun and the booster acceleration are measured using spectrometers with screen stations in the dispersive arm downstream the RF-gun and in the first dispersive arm downstream the booster cavity. The normalized rms emittance is calculated using the formula: 2 2 2 2 x x x x x x n EMSY1 (z = 5.74 mm) beamlet screen 2.64 m Schematic representation of the single slit scan technique. Measurement results in summer 2009 0.3 0.5 0.7 0.9 1.1 1.3 377 379 381 383 385 387 389 main solenoid current, A rms beam size, mm Xrms Yrms XYrms a) b) c) Measured beam size (top) and normalized projected emittance (bottom) vs. main solenoid current at EMSY1 station for a gun phase of +6 degree off-crest and booster phase on-crest (opened symbols for fast scan and solid symbols for detailed scan). 0.8 1.0 1.2 1.4 1.6 1.8 2.0 377 379 381 383 385 387 389 main solenoid current, A emittance, mm mrad Ex Ey Exy Ex Ey Exy Transverse distribution (a), horizontal (b), and vertical (c) phase space of the best emittance point at the solenoid current ~383.5 A. The Emittance Measurement SYstem (EMSY) consists of horizontal and vertical actuators. Stepper motors are provided to move separately each one of the four axes of EMSY which give the precise spatial positioning and orientation of the components. On each of the actuators, either a YAG or OTR screen is mounted to observe the beam distribution. A single and a multi slit masks are mounted consecutive to take samples from the transverse phase space of the electron beam. A CCD camera is used to observe the screens. ID: TUPSM057 is the Lorentz factor corresponding to the beam energy. and are the second central moments of the electron beam distribution in the trace space obtained from the slit scan. is the angle of the single electron trajectory with respect to the whole beam trajectory. is the rms beam size measured at the slit location. is applied to correct for possible sensitivity limitation of low intensity beamlets. 2 x y x p p x / x 2 / x x 2 x The Emittance Measurement System

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Page 1: Emittance Measurement Wizard at PITZ

A.Shapovalov ([email protected]) for the BIW2010, Santa Fee, New Mexico, USA

Emittance Measurement Wizard at PITZ.

Abstract

The Photo Injector Test Facility at DESY, Zeuthen site (PITZ) develops

electron sources of high brightness beams, required for linac based free

electron lasers (FELs) like FLASH or the European XFEL. One of the key

issues in electron beam optimization is the minimization of the transverse

emittance. The main method to measure emittance at PITZ is a single slit

scan technique, implying local beam divergence measurement by insertion

of the slit mask at a definite location within the beam and measurements of

the transmitted beamlet profile downstream of the slit station. “Emittance

Measurement Wizard” (EMWiz) is the program used by PITZ operators for

automated emittance measurements. EMWiz combines an acquisition

program for beam and beamlet image recording and a postprocessing tool

for the analysis of the measured transverse phase space of the electron

beam. It provides a way to execute the difficult emittance measurements in

an automatic mode and to get a calculated emittance result.

Photo Injector Test facility at DESY, Zeuthen site (PITZ)

Three EMSY stations are located in the current setup. The first EMSY station (EMSY1)

behind the exit of the booster cavity is used in the standard emittance measurement

procedure. It is at 5.74 m downstream the photocathode corresponding to the expected

minimum emittance location.

Emittance Measurement at PITZ

Transverse emittance measurement

using slit scan technique

For this technique, the local divergence is estimated

by transversely cutting the electron beam into thin slices.

Then, the size of the beamlets created by the slits is

measured at the YAG screen at some distance

downstream the EMSY station. The 10 m slit and a

distance between the slit mask and the beamlet

observation screen of 2.64 m are used in the standard

emittance measurement. In the emittance measurement

setup and procedure, intrinsic cuts have been minimized

by e.g. using highly sensitive screens, a 12 bit signal

resolution CCD-camera and a large area of interest to

cover the whole beam distribution. Therefore, emittance

value is called 100% rms emittance. The momenta of the

beam after the gun and the booster acceleration are

measured using spectrometers with screen stations in the

dispersive arm downstream the RF-gun and in the first

dispersive arm downstream the booster cavity.

The normalized rms emittance is calculated using the formula:

222

2xxxx

x

xn

EMSY1

(z = 5.74 mm)

beamlet

screen

2.64 m

Schematic representation of the single slit scan

technique.

Measurement results in summer 2009

0.3

0.5

0.7

0.9

1.1

1.3

377 379 381 383 385 387 389

main solenoid current, A

rms

be

am

siz

e,

mm

Xrms Yrms XYrms

a)

b) c)

Measured beam size (top) and normalized projected

emittance (bottom) vs. main solenoid current at EMSY1

station for a gun phase of +6 degree off-crest and booster

phase on-crest (opened symbols for fast scan and solid

symbols for detailed scan).

0.8

1.0

1.2

1.4

1.6

1.8

2.0

377 379 381 383 385 387 389

main solenoid current, A

emit

tan

ce, m

m m

rad

Ex Ey Exy

Ex Ey Exy

Transverse distribution (a), horizontal (b), and vertical (c)

phase space of the best emittance point at the solenoid

current ~383.5 A.

The Emittance Measurement SYstem (EMSY) consists of

horizontal and vertical actuators. Stepper motors are

provided to move separately each one of the four axes of

EMSY which give the precise spatial positioning and

orientation of the components. On each of the actuators,

either a YAG or OTR screen is mounted to observe the

beam distribution. A single and a multi slit masks are

mounted consecutive to take samples from the transverse

phase space of the electron beam. A CCD camera is used to

observe the screens.

ID: TUPSM057

is the Lorentz factor corresponding to the beam energy.

and are the second central moments of the electron beam distribution in the trace space obtained from

the slit scan.

is the angle of the single electron trajectory with respect to the whole beam trajectory.

is the rms beam size measured at the slit location.

is applied to correct for possible sensitivity limitation of low intensity beamlets.

2x

yx ppx /

x2/ xx

2x

The Emittance Measurement System

Page 2: Emittance Measurement Wizard at PITZ

It is possible to observe video stream in

a separate window.

EMWiz has own plot system. It is much

faster than ROOT, but the development is

still ongoing.

The spectrum tool shows the number of pixels in the image

with a given intensity. Major part of image pixels should have

intensity between 50% and 70% of maximum intensity. Control of

saturation is one important criteria for obtaining good data quality

The most complex tool is “PreScan”. It is a

hands-off procedure for signal quality testing and

finding the scan limits of emittance

measurements.

The Scan&Grab control panel collects

features for measurement procedures

and actuator control.

The scan info panel gives possibility to set

EMSY device, change scan limits, observe

the actuator position, control the laser

shutter.

The video system at PITZ has 24 digital cameras with 8 and 12 effective bits per pixel and 7 video servers.

The video part of EMWiz manages the cameras by reading properties, changing settings and connecting to a

video server. The client makes it possible to get the video image, to apply filters, to grab and to save video

images. Calculation of important values is going simultaneously with the drawing process.

The process of data collection in EMWiz stores all machine

parameters continuously and informs an operator about critical

fluctuations of controlled parameters, which can influence the

measurement reliability. The list of the parameters can be

changed via an XML-config file. This GUI is based on a config

file and can be easily transformed with new demands.

At first, the equipment should be adjusted before

the measurements. Some necessary actions are

executed by others programs and there

measurement results such as the Lorentz factor are

put in corresponding fields of this option panel.

EMWiz has a black box feature. All

actions of the operator to the program and

machine, system status, error events and

alarms with time-stamp are stored to a log-

file. With help of an expert, one can open a

hidden window, to support the shift crew

remotely for fixing of a problem.

The shared memory watcher is an expert program. At present, the wizard consists of

separated programs, each of them for one logical task. Communication between

program parts is realized by a shared memory. This approach gives the possibility to use

EMWiz components on different user stations with starting on one host. This increases

graphics productivity and decreases the CPU loading. In the future it is planned to add

network communication, which will give possibility to use parts of the wizard on different

machines.

Rescan window. An operator can

scan some beamlets again.

EMWiz is a multithread, multiprocessor,

multiwindow application with user-friendly

interface, flexible design which based on XML-

config-file. An operator can save and load GUI

setting, e.g. window positions and sizes, values

in fields.

The main panel of EMWiz informs an operator

about system status, program flows, errors,

recommendations. EMWiz is done for 64 bits

Scientific Linux CERN version 5.0.

The Fast Scan panel receives settings from the

basic part of EMWiz. An operator can make “Fast

Scan” procedure with the measurement time of about

20 seconds for one solenoid setting compared to

about 30 minutes with old “Step Scan” procedure.

This panel allows to set scan parameters

manually or automatically, which receives the

settings from the basic part of EMWiz through

shared memory.

Last step in the measurement is to calculate

the emittance. The tool “calculator” exists for this

purpose. The operator sets a folder with saved

data, the tool checks this folder and shows only

good sets (MOI image, EMSY image, slit scan

image file, background file, data file with

parameters of system). A lot of processing of the

data is ongoing during calculation. Different

filters, formulas and etc. is applied to the video

data. A user can select to plot all intermediate

results after each complex calculation. At the

end of the calculation the emittance plot is

shown by default .

Panel “Results” shows information about the

selected path, folders, files for data recording.

For plotting, ROOT is integrated to EMWiz. It gives possibility

to use all features of mathematical apparatus and graphic

potential of CERN’s ROOT.

Main Panel & Video System Alarm & Measurement System

Fast Scan & Emittance CalculatorCommunicator & Plot System

A.Shapovalov ([email protected]) for the BIW2010, Santa Fee, New Mexico, USA

Emittance Measurement Wizard at PITZ.

ID: TUPSM057