28/Jul/2011 SRF’11 @Chicago 1 Test Results of the International S1-Global Cryomodule Kirk

28Jul2011 SRFrsquo11 Chicago

1

Test Results of the International S1-Global Cryomodule

Kirk

superconducting rf test facility

C Pagani P Pierini A Bosotti R Paparella INFN (Italy)

K Jensch D Kostin L Lilje A Matheisen W-D Moeller M Schmoekel P Schilling H Weise N Walker DESY (Germany)

T Arkan S Barbanotti M Battistoni H Carter

M Champion A Hocker R Kephart J Kerby D Mitchell Y Pischalnikov TJ Peterson M Ross W Schappert B Smith FNAL (USA)

C Adolphsen C Nantista SLAC (USA)

M Akemoto S Fukuda K Hara H Hayano N Higashi E Kako H Katagiri Y Kojima Y Kondo T Matsumoto H Matsushita

S Michizono T Miura H Nakai H Nakajima K Nakanishi S Noguchi N Ohuchi T Saeki M Satoh T Shidara T Shishido T Takenaka A Terashima N Toge K Tsuchiya K Watanabe S Yamaguchi

A Yamamoto Y Yamamoto(Kirk) K Yokoya M Yoshida KEK (Japan)

2

International Team for ldquoS1-Globalrdquo


61 persons from 5 Labs


28Jul2011 3

Overview Motivation amp History of S1-Global Cavity Coupler and Tuner in S1-Global Cavity performance at VT Assembly and Cryomodule test Status Coupler conditioning at RT Tuner test with low power 2K LFD measurement LFD compensation by piezo 7 cavities operation Dynamic loss measurement (including Static loss) RF response at Quench for MHI-06 Summary

SRFrsquo11 Chicago


28Jul2011 4

Motivation amp History of S1-Global Motivation

Comparison of hardware performance concerning SRF technology for ILCCavityPower couplerTunerCryomodule

Mutual understanding among SRF researchers engineers and technicians

HistoryThis project was launched in a discussion of ILC-GDE in 2008The preparation including VT was in progress in 2009The assembly work started at the beginning of 2010The cryomodule test finished on Feb2011

SRFrsquo11 Chicago



Blade Tuner (FNALINFN) Saclay Tuner (DESY)

Slide-Jack Tuner (KEK)

TTF-III Coupler (DESYFNAL) STF-II Coupler (KEK)

TESLA Cavity (DESYFNAL)Tesla-like (KEK)

Comparisonof

Performance

Main components in S1-G cryomodule

E Kako

The coupling is variable for both couplers


28Jul2011 6

S1-Global Cryomodule

SRFrsquo11 Chicago

Cryomodule-C(4 TESLA cavities 4 TTF-III couplers)

Cryomodule-A(4 TESLA-like cavities 4 STF-II couplers)

2 Blade tuners 2 Saclay tuners4 Slide-jack tuners (center or end)


28Jul2011 SRFrsquo11 Chicago 7

Cavity Performance VT

2 cavities from FNAL 2 cavities from DESY

8 Cavities for S1-Global (ave 30 MVm)4 cavities from KEK

E Kako



Collaboration for Cryomodule Assembly

Cavity string assembly (2010 Jan)

Tuner assembly (2010 Feb)

Coupler assembly (2010 Mar)

KEK Cavity string assembly (2010 Mar)

E Kako



Installation into tunnel



Collaboration for Cryomodule Tests

Tuner performance tests (2010 July)

Cavity processing (2010 Sept)

Dynamic loss meas (2010 Nov)Lorentz detuning tests (2010 Oct)E Kako


Cryomodule-C KLY1 (2MW)Cryomodule-A KLY2 (5MW)

05 ms 5 Hz 500 kW15 ms 5 Hz 200 kW


RF processing of input couplers

Aug 25 ~ Sept 07 (10 days) E Kako



RF processing time of input couplers

Cryomodule-C(TTF-III couplers)ave processing time~ 21 hours

Cryomodule-A(STF-II couplers)ave processing time~ 13 hours

20 hr

20 hr

Vacuum IL 2x10-4 Pa

at room temperature

E KakoThe difference of the conditioning time between them is probably due to the structure of RF window



Adjustment of frequency (f0 )

Cryomodule - C Cryomodule - A

1300000MHz130000MHz

129992MHz

(A4MHI-09 129991 MHz limit)C2ACC011 Tuner did not work

f0 = 129991 MHz (operation)

E KakoThe cause of these tuner troubles are probably due to the mechanical stress



QL of Variable Input Coupler

24 X 106

Cryomodule ndash C(TTF-III couplers)

Cryomodule ndash A(STF-II couplers)

E Kako The both couplers have a good performance for the adjustment of QL

QL = 24 x 106 Δfbw = 542Hz



Cavity performance between VT and CT

Ave 30MVm VTAve 28MVm CT (single cavity)Ave 26MVm CT (7 cavities)

Unfortunately the gradient did not achieve the ILC specification



severe drop




Status of high power operation

Real time detuning monitor

S Michizono



Frequency shift due to Lorentz detuningC4Z109 (29MVm) A2MHI-06 (38MVm)

FBon Piezooff FBon Piezooff

Pre-detuningby motor tuneramp piezo tunerwith DC voltage

Compensationby piezo tuner inpulsed operation

Flat TopFlat Top

Rise Time Rise Time

200~500 Hz 2~3 kHz

E Kako


Pulse-shortening amp Data Analysis method


50μsec step shortening

100 pulses average


Result of LFD measurement


Cryomodule-A Cryomodule-C

We can estimate the detuning frequency for the period of rise-up flat-top and full-pulse

f = K Eacc2

rise-upflat-topfull-pulse


K [Hz(MVm)2] stiffness parameter



Comparison of Detuning Frequency by LFD

TESLA-like cavity package has a stiffer structure than others



Parameters of Piezo drive pulse

delay time

dc V

drive V

drive frequency (Hz)

Single pulse of inverse cosine waveform

Eacc

Pinput

D ft

Pre-detuning by motor tuner

control panel

Piezo drive pulse

RF Feedback ON E Kako



Result of Piezo Compensation for LFD

Δfpeak-to-peak



QL ΔfAES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9

1708 1853

6305 pulses

7 Cavities OperationACC11 detuned


25SRFrsquo11 Chicago 28Jul2011

7 Cavities Operation

Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9


AES4 ZANON108ZANON109

MHI5 MHI6 MHI7 MHI9ACC11

Required rf power for 8-cav operation

ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06

More RF power is necessary for MHI6 and 7This means the inner conductor of the input coupler may be expanded due to the heatingThe couplers lead to more over-coupled situation

E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm



RF response of Quench for MHI6 40MVm



Dynamic Loss measurement

STF-II coupler has more heat loss than TTF-IIIThis point should be improved in the near future



TroublesThe performance of the two cavities dropped

between VT and CT

The tuners of the two cavities did not work at 2K

These problems are investigated in the near future



Summarybull Assembly work by the S1-Global team was successful

bull 6 of 8 cavities reached the almost same gradient at the cryomodule test as the vertical test

bull Mechanical vibration modes were found to vary from cavity to cavity

bull LFD measurement was successful MHI cavity turned out to be stiffer

bull Compensation by piezo was successful All types of the tuners tested have demonstrated good effectiveness

bull Simultaneous operation of seven cavities was comparatively stable The QL decreased gradually during the operation for every power coupler

bull From the results of the dynamic loss measurement it was observed the STF-II coupler has a larger heat loss

bull Communication among the international members of the S1-Global team worked well



Thank you for your attention


C Pagani P Pierini A Bosotti R Paparella INFN (Italy)

K Jensch D Kostin L Lilje A Matheisen W-D Moeller M Schmoekel P Schilling H Weise N Walker DESY (Germany)

T Arkan S Barbanotti M Battistoni H Carter

M Champion A Hocker R Kephart J Kerby D Mitchell Y Pischalnikov TJ Peterson M Ross W Schappert B Smith FNAL (USA)

C Adolphsen C Nantista SLAC (USA)

M Akemoto S Fukuda K Hara H Hayano N Higashi E Kako H Katagiri Y Kojima Y Kondo T Matsumoto H Matsushita

S Michizono T Miura H Nakai H Nakajima K Nakanishi S Noguchi N Ohuchi T Saeki M Satoh T Shidara T Shishido T Takenaka A Terashima N Toge K Tsuchiya K Watanabe S Yamaguchi

A Yamamoto Y Yamamoto(Kirk) K Yokoya M Yoshida KEK (Japan)

2

International Team for ldquoS1-Globalrdquo


61 persons from 5 Labs


28Jul2011 3


SRFrsquo11 Chicago


28Jul2011 4





SRFrsquo11 Chicago







Comparisonof

Performance


E Kako



28Jul2011 6


SRFrsquo11 Chicago









E Kako








E Kako












05 ms 5 Hz 500 kW15 ms 5 Hz 200 kW









20 hr

20 hr

Vacuum IL 2x10-4 Pa

at room temperature






1300000MHz130000MHz

129992MHz







24 X 106




QL = 24 x 106 Δfbw = 542Hz








severe drop






S Michizono







Flat TopFlat Top

Rise Time Rise Time

200~500 Hz 2~3 kHz

E Kako





100 pulses average






f = K Eacc2











delay time

dc V

drive V



Eacc

Pinput

D ft


control panel

Piezo drive pulse





Δfpeak-to-peak



QL ΔfAES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9

1708 1853

6305 pulses





Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT

















28Jul2011 3


SRFrsquo11 Chicago


28Jul2011 4





SRFrsquo11 Chicago







Comparisonof

Performance


E Kako



28Jul2011 6


SRFrsquo11 Chicago









E Kako








E Kako












05 ms 5 Hz 500 kW15 ms 5 Hz 200 kW









20 hr

20 hr

Vacuum IL 2x10-4 Pa

at room temperature






1300000MHz130000MHz

129992MHz







24 X 106




QL = 24 x 106 Δfbw = 542Hz








severe drop






S Michizono







Flat TopFlat Top

Rise Time Rise Time

200~500 Hz 2~3 kHz

E Kako





100 pulses average






f = K Eacc2











delay time

dc V

drive V



Eacc

Pinput

D ft


control panel

Piezo drive pulse





Δfpeak-to-peak



QL ΔfAES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9

1708 1853

6305 pulses





Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT

















28Jul2011 4





SRFrsquo11 Chicago







Comparisonof

Performance


E Kako



28Jul2011 6


SRFrsquo11 Chicago









E Kako








E Kako












05 ms 5 Hz 500 kW15 ms 5 Hz 200 kW









20 hr

20 hr

Vacuum IL 2x10-4 Pa

at room temperature






1300000MHz130000MHz

129992MHz







24 X 106




QL = 24 x 106 Δfbw = 542Hz








severe drop






S Michizono







Flat TopFlat Top

Rise Time Rise Time

200~500 Hz 2~3 kHz

E Kako





100 pulses average






f = K Eacc2











delay time

dc V

drive V



Eacc

Pinput

D ft


control panel

Piezo drive pulse





Δfpeak-to-peak



QL ΔfAES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9

1708 1853

6305 pulses





Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT






















Comparisonof

Performance


E Kako



28Jul2011 6


SRFrsquo11 Chicago









E Kako








E Kako












05 ms 5 Hz 500 kW15 ms 5 Hz 200 kW









20 hr

20 hr

Vacuum IL 2x10-4 Pa

at room temperature






1300000MHz130000MHz

129992MHz







24 X 106




QL = 24 x 106 Δfbw = 542Hz








severe drop






S Michizono







Flat TopFlat Top

Rise Time Rise Time

200~500 Hz 2~3 kHz

E Kako





100 pulses average






f = K Eacc2











delay time

dc V

drive V



Eacc

Pinput

D ft


control panel

Piezo drive pulse





Δfpeak-to-peak



QL ΔfAES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9

1708 1853

6305 pulses





Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT

















28Jul2011 6


SRFrsquo11 Chicago









E Kako








E Kako












05 ms 5 Hz 500 kW15 ms 5 Hz 200 kW









20 hr

20 hr

Vacuum IL 2x10-4 Pa

at room temperature






1300000MHz130000MHz

129992MHz







24 X 106




QL = 24 x 106 Δfbw = 542Hz








severe drop






S Michizono







Flat TopFlat Top

Rise Time Rise Time

200~500 Hz 2~3 kHz

E Kako





100 pulses average






f = K Eacc2











delay time

dc V

drive V



Eacc

Pinput

D ft


control panel

Piezo drive pulse





Δfpeak-to-peak



QL ΔfAES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9

1708 1853

6305 pulses





Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT





















E Kako








E Kako












05 ms 5 Hz 500 kW15 ms 5 Hz 200 kW









20 hr

20 hr

Vacuum IL 2x10-4 Pa

at room temperature






1300000MHz130000MHz

129992MHz







24 X 106




QL = 24 x 106 Δfbw = 542Hz








severe drop






S Michizono







Flat TopFlat Top

Rise Time Rise Time

200~500 Hz 2~3 kHz

E Kako





100 pulses average






f = K Eacc2











delay time

dc V

drive V



Eacc

Pinput

D ft


control panel

Piezo drive pulse





Δfpeak-to-peak



QL ΔfAES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9

1708 1853

6305 pulses





Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT























E Kako












05 ms 5 Hz 500 kW15 ms 5 Hz 200 kW









20 hr

20 hr

Vacuum IL 2x10-4 Pa

at room temperature






1300000MHz130000MHz

129992MHz







24 X 106




QL = 24 x 106 Δfbw = 542Hz








severe drop






S Michizono







Flat TopFlat Top

Rise Time Rise Time

200~500 Hz 2~3 kHz

E Kako





100 pulses average






f = K Eacc2











delay time

dc V

drive V



Eacc

Pinput

D ft


control panel

Piezo drive pulse





Δfpeak-to-peak



QL ΔfAES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9

1708 1853

6305 pulses





Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT



























05 ms 5 Hz 500 kW15 ms 5 Hz 200 kW









20 hr

20 hr

Vacuum IL 2x10-4 Pa

at room temperature






1300000MHz130000MHz

129992MHz







24 X 106




QL = 24 x 106 Δfbw = 542Hz








severe drop






S Michizono







Flat TopFlat Top

Rise Time Rise Time

200~500 Hz 2~3 kHz

E Kako





100 pulses average






f = K Eacc2











delay time

dc V

drive V



Eacc

Pinput

D ft


control panel

Piezo drive pulse





Δfpeak-to-peak



QL ΔfAES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9

1708 1853

6305 pulses





Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT
























05 ms 5 Hz 500 kW15 ms 5 Hz 200 kW









20 hr

20 hr

Vacuum IL 2x10-4 Pa

at room temperature






1300000MHz130000MHz

129992MHz







24 X 106




QL = 24 x 106 Δfbw = 542Hz








severe drop






S Michizono







Flat TopFlat Top

Rise Time Rise Time

200~500 Hz 2~3 kHz

E Kako





100 pulses average






f = K Eacc2











delay time

dc V

drive V



Eacc

Pinput

D ft


control panel

Piezo drive pulse





Δfpeak-to-peak



QL ΔfAES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9

1708 1853

6305 pulses





Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT


















05 ms 5 Hz 500 kW15 ms 5 Hz 200 kW









20 hr

20 hr

Vacuum IL 2x10-4 Pa

at room temperature






1300000MHz130000MHz

129992MHz







24 X 106




QL = 24 x 106 Δfbw = 542Hz








severe drop






S Michizono







Flat TopFlat Top

Rise Time Rise Time

200~500 Hz 2~3 kHz

E Kako





100 pulses average






f = K Eacc2











delay time

dc V

drive V



Eacc

Pinput

D ft


control panel

Piezo drive pulse





Δfpeak-to-peak



QL ΔfAES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9

1708 1853

6305 pulses





Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT





















20 hr

20 hr

Vacuum IL 2x10-4 Pa

at room temperature






1300000MHz130000MHz

129992MHz







24 X 106




QL = 24 x 106 Δfbw = 542Hz








severe drop






S Michizono







Flat TopFlat Top

Rise Time Rise Time

200~500 Hz 2~3 kHz

E Kako





100 pulses average






f = K Eacc2











delay time

dc V

drive V



Eacc

Pinput

D ft


control panel

Piezo drive pulse





Δfpeak-to-peak



QL ΔfAES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9

1708 1853

6305 pulses





Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT




















1300000MHz130000MHz

129992MHz







24 X 106




QL = 24 x 106 Δfbw = 542Hz








severe drop






S Michizono







Flat TopFlat Top

Rise Time Rise Time

200~500 Hz 2~3 kHz

E Kako





100 pulses average






f = K Eacc2











delay time

dc V

drive V



Eacc

Pinput

D ft


control panel

Piezo drive pulse





Δfpeak-to-peak



QL ΔfAES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9

1708 1853

6305 pulses





Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT



















24 X 106




QL = 24 x 106 Δfbw = 542Hz








severe drop






S Michizono







Flat TopFlat Top

Rise Time Rise Time

200~500 Hz 2~3 kHz

E Kako





100 pulses average






f = K Eacc2











delay time

dc V

drive V



Eacc

Pinput

D ft


control panel

Piezo drive pulse





Δfpeak-to-peak



QL ΔfAES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9

1708 1853

6305 pulses





Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT























severe drop






S Michizono







Flat TopFlat Top

Rise Time Rise Time

200~500 Hz 2~3 kHz

E Kako





100 pulses average






f = K Eacc2











delay time

dc V

drive V



Eacc

Pinput

D ft


control panel

Piezo drive pulse





Δfpeak-to-peak



QL ΔfAES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9

1708 1853

6305 pulses





Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT


















severe drop






S Michizono







Flat TopFlat Top

Rise Time Rise Time

200~500 Hz 2~3 kHz

E Kako





100 pulses average






f = K Eacc2











delay time

dc V

drive V



Eacc

Pinput

D ft


control panel

Piezo drive pulse





Δfpeak-to-peak



QL ΔfAES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9

1708 1853

6305 pulses





Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT




















S Michizono







Flat TopFlat Top

Rise Time Rise Time

200~500 Hz 2~3 kHz

E Kako





100 pulses average






f = K Eacc2











delay time

dc V

drive V



Eacc

Pinput

D ft


control panel

Piezo drive pulse





Δfpeak-to-peak



QL ΔfAES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9

1708 1853

6305 pulses





Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT






















Flat TopFlat Top

Rise Time Rise Time

200~500 Hz 2~3 kHz

E Kako





100 pulses average






f = K Eacc2











delay time

dc V

drive V



Eacc

Pinput

D ft


control panel

Piezo drive pulse





Δfpeak-to-peak



QL ΔfAES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9

1708 1853

6305 pulses





Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT




















100 pulses average






f = K Eacc2











delay time

dc V

drive V



Eacc

Pinput

D ft


control panel

Piezo drive pulse





Δfpeak-to-peak



QL ΔfAES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9

1708 1853

6305 pulses





Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT





















f = K Eacc2











delay time

dc V

drive V



Eacc

Pinput

D ft


control panel

Piezo drive pulse





Δfpeak-to-peak



QL ΔfAES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9

1708 1853

6305 pulses





Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT























delay time

dc V

drive V



Eacc

Pinput

D ft


control panel

Piezo drive pulse





Δfpeak-to-peak



QL ΔfAES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9

1708 1853

6305 pulses





Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT



















delay time

dc V

drive V



Eacc

Pinput

D ft


control panel

Piezo drive pulse





Δfpeak-to-peak



QL ΔfAES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9

1708 1853

6305 pulses





Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT



















Δfpeak-to-peak



QL ΔfAES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9

1708 1853

6305 pulses





Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT


















QL ΔfAES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9

1708 1853

6305 pulses





Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT



















Δf1708 1853

He pressure

He flow



QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT


















QL

AES4

ZANON108 ZANON109

MHI5 MHI6

MHI7 MHI9





ndash39

ndash35

ndash07

ndash11

ndash16

+05

ndash06


E Kako




Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT



















Eacc Eacc Eacc

φ φ φ

AES4

10MVm 10MVm

10MVm




Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT



















Eacc Eacc Eacc

φ φ φ

MHI6

10MVm10MVm 10MVm











between VT and CT


























between VT and CT























between VT and CT



















between VT and CT
































Documents

28/Jul/2011 SRF’11 @Chicago 1 Test Results of the International S1-Global Cryomodule Kirk