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Dmitry Gudkov Phase correction of the CLIC TBM in CLEX Dmitry Gudkov Wilfrid Farabolini.

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Presentation on theme: "Dmitry Gudkov Phase correction of the CLIC TBM in CLEX Dmitry Gudkov Wilfrid Farabolini."— Presentation transcript:

1 Dmitry Gudkov Phase correction of the CLIC TBM in CLEX Dmitry Gudkov Wilfrid Farabolini

2 Dmitry Gudkov Contents Problem description Confirmation of the problem existence Possible solutions Ongoing and future actions

3 Dmitry Gudkov Problem description The problem was presented by Wilfrid during the CLIC meeting on 16-Dec-2014 Slides by W. Farabolini: https://indico.cern.ch/event/356495/contribution/4/material/slides/2.pptx

4 Dmitry Gudkov Confirmation of the problem existence The feasibility of a phase ~ 180 o shift have been investigated using the existing waveguide network (not installed on the TBM): -2 ports network analyser (Agilent) is used -Sij parameters at the 11.994 GHz frequency are measured Output 1Output 2 S12 phase [ o ]+25-66.8 S12 amplitude [dB]-3.28-3.25 S11 [dB]-35.8 S22 [dB]-43.5-45.5 The phase difference between the hybrid output 1 and output 2 is 91.8 o

5 Dmitry Gudkov Confirmation of the problem existence 243.7 Distance between the input of the first AS and second AS in the SAS is 243.7 which corresponds to 9 and ¾ (9.75) times the bunch spacing at 11.994 GHz free space wavelength (25 mm); The RF phase at the second structure input must be -270 deg. or + 90 o from the RF phase at the first structure input; To obtain this phase the output #1 of the hybrid coupler must feed the 2 nd structure; However in the current installation the hybrid is turned and the output #1 feeds the 1 st structure.

6 Dmitry Gudkov Possible solutions Solution 1: Squeezing waveguide dimensions Attempt to obtain a phase shift of 180 o by squeezing existing piece of the waveguide network; The test was performed on the H-bent waveguide Result: The expected phase shift is accompanied by a large increase of the S11 and S22 reflections (- 17 dB for a phase shift of 56 o ): Evolution of phase shift (blue) and reflection (red) during waveguide squeezing It is not likely to fulfil the required 180 o phase shift; Method can be used for final phase adjustment on a range of 15 o approximately.

7 Dmitry Gudkov Possible solutions Solution 2: Additional waveguide segment for phase compensation Bending of distribution waveguides to allow spacer insertion; Spacer manufacturing and installation. Result: Sij parameters remain very acceptable: Preliminary bending was performed: deformedOutput 1Output 2 S12 phase [deg]-80.6-81.2 S21 [dB]-3.15-2.99 S11 [dB]-32-32.1 S22 [dB]-5.8-6.1 non-deformedOutput 1Output 2 S12 phase [deg]-96.1-79.1 S21 [dB]-3.15-2.99 S11 [dB]-29.8-29.4 S22 [dB]-5.76-6.06 The phase shift due to the deformation is minor (about 1 deg). 2 outputs of this non-deformed waveguide have a difference of phase of 17 deg. Such a difference of phase can be fixed by squeezing the waveguide.

8 Dmitry Gudkov Ongoing and future actions 1. Spacers design and manufacturing: Spacer Type 1: Copper part, works as big gasket Spacer Type 2: 2-sided CLIC RF vacuum flange 2. Accurate phase control will require many RF network measures during the installation and can be achieved by a limited squeeze of the waveguide and/or by flange torque control.


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