PETS components and waveguide PETS components and waveguide - - PowerPoint PPT Presentation

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PETS components and waveguide PETS components and waveguide - - PowerPoint PPT Presentation

PETS components and waveguide PETS components and waveguide connections CLIC W CLIC Workshop 2007 k h 2007 David Carrillo Index A design to connect PETS with accelerating structures will be discussed choke flange And also we will deal


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SLIDE 1

PETS components and waveguide PETS components and waveguide connections

CLIC W k h 2007 CLIC Workshop 2007

David Carrillo

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SLIDE 2

Index

A design to connect PETS with accelerating structures will be discussed

choke flange

And also we will deal with two components for testing the PETS

Input coupler

p p

Single test bar device

David Carrillo CIEMAT

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SLIDE 3

Choke flange X-band

  • This device allows power transmission without electrical contact

between waveguides M ti ti D i th CLIC ti th t li (d i d i )

  • Motivation: During the CLIC operation the two linacs (drive and main)

will have independent alignment. That is why the development of the special device which transfer power without mechanical contact from PETS to accelerating structures is important PETS to accelerating structures is important

David Carrillo CIEMAT

Schematic layout of independent alignment of the two linacs with the fixed RF phase

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SLIDE 4

Choke flange

  • It consists of a transition from rectangular to circular waveguide
  • In between there is a choke that stop electromagnetic energy to flow

t d d id f ll t i i f t th th t

  • utwards and provide full transmission of energy to the other port
  • This device is flexible and provides a place to produce vacuum inside

the waveguide

  • Being equipped with outside bellow it will provide the range of the

possible transverse orientations of the two waveguides

David Carrillo CIEMAT 3D solid view of quarter of choke flange

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SLIDE 5

Choke flange

es (dB) ation mode

Electric field complex

e) and radia

p magnitude

S11(blue Frequency (GHz)

It i t i i i fl ti d It is necessary to minimize reflection and radiation through the choke. Also there is a compromise between length and E field on the

  • surface. Device has been designed as short as

E magnitude It will be tested at SLAC at nominal power of 135/2 MW (E

David Carrillo CIEMAT

  • surface. Device has been designed as short as

possible p ( field on surface < 30 MV/m

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SLIDE 6

Choke flange. Shifts & twist

X-shift

Shifts in different directions and twists are simulated in order to

study the device performance

20

z x

40

S11 (dB)

0.5 mm 0.3 mm

y

60

S

0.2 0.0

Frequency (GHz)

11.6 11.8 12 12.2 12.4 80

Coordinate axis x-shift appears to be the

David Carrillo CIEMAT

x shift appears to be the most critical displacement issue

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SLIDE 7

Choke flange. Shifts & twist

Z-shift

20 12

0 5 mm

Dynamic range for the accepted f (S11< 45 dB)

40 40 −

0.5 mm

  • 0.5 mm

S11 (dB) performance (S11< -45 dB) X – shift: ± 0.25 mm Y – shift: ± 0.5 mm

20 12

Twist

11.6 11.8 12 12.2 12.4 80 60

Y-shift

Z – shift: ± 0.5 mm Twist: < 50

40 40 −

30

20 12

(dB)

11.6 11.8 12 12.2 12.4 80 60

50

Frequency (GHz)

60 40 40 −

0.5 mm

S11

x, y shifts do not change the transmitted RF phase

q y ( )

David Carrillo CIEMAT

Frequency (GHz)

11.6 11.8 12 12.2 12.4 80

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SLIDE 8

Mode launcher

Inside the PETS, electrons are decelerated and they produce

mode TM01. In order to measure PETS RF quality this mode must be put into the PETS by the mode launcher (coupler)

The input signal is the fundamental one (TE10 mode) in the

rectangular waveguide which is transformed into the TM01 (not f d t l) i th i l id fundamental) in the circular waveguide

David Carrillo CIEMAT

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SLIDE 9

Mode launcher

S11 S12 (TE11) S12 (TE11) It is designed for low t t Not only reflection must be minimized but also Electric field complex

Frequency (GHz)

David Carrillo CIEMAT

power tests be minimized but also transmission to TE11 magnitude

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SLIDE 10

Mode launcher

Two

couplers will be built to provide low power RF measurements

The number of measures will be done:

Test the couplers themselves

Measure S parameters with extractor/or both couplers

Measure S parameters with extractor/or both couplers

Measure phase-advance between PETS cells PETS Power Mode

David Carrillo CIEMAT

PETS Extractor launcher

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SLIDE 11

Testing single PETS bar

  • A device has been designed to do RF tests of the single PETS bar
  • It consists of two side blocks that will be put together with a single PETS

b i d t t i id d (TE ) ith h d bar in order to create inside a mode (TE10) with same phase advance, vg, etc as the decelerating mode (TM01)

PETS Single bar PETS Single bar Phase/period=90 Frequency =11.994 GHz V / 0 466 David Carrillo CIEMAT Vg/c=0.466

Mode TE10

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SLIDE 12

Testing single PETS bar

Full assembly y simulation PETS bar + 2 side David Carrillo CIEMAT wr90 taper PETS bar + 2 side blocks

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SLIDE 13

Testing single PETS bar

  • Without this device, all single bars must be put together (8 bars), and it

can only be measured performance of the whole PETS as can be seen y p in the following picture

  • With the single test bar device, a defective bar could be found (if we

ever get one ☺) It would be possible as well to know specifically which

David Carrillo CIEMAT

ever get one ☺) It would be possible as well to know specifically which is wrong with the bar (matching cells, shape profile, etc)

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SLIDE 14

Conclusions

A Choke flange design has been done, which will allow a

flexible connection between PETS and accelerating structures and also will provide a vacuum port

Single bar test device will allow us to measure RF quality of

single bars before putting all together

Mode launcher designed will be used to introduce and extract

power in order to test phase-shift and S parameters for PETS power in order to test phase shift and S parameters for PETS

David Carrillo CIEMAT