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T18 structure tested at ASTA resonant ring at DIAGNOSTICS OF RF BREAKDOWNS IN HIGH-GRADIENT ACCELERATING STRUCTURES field and current measurements before (left) and during (right) a breakdown power level measurements A. Palaia, Uppsala University, Sweden V. Dolgashev, J. Lewandowski, S. Weathersby, SLAC National Accelerator Laboratory, CA, USA Supported by the Royal Swedish Academy of Science and the Knut and Alice Wallenberg foundation. Andrea Palaia, [email protected] The resonant ring at ASTA allows high power structure testing in a two-arm wave guide loop meant to recirculate the field such that it constructively interferes with itself increasing the power level in the structure at every turn. Estimation of the breakdown locations in the structure using phase and time information from RF measurements phase difference between forward and reflected RF phase and time information for each breakdown event compared with the position of each cell (red crosses) breakdowns distribution along the structure Can we say something about the properties of the object reflecting RF during a breakdown? The RF reflection measured during a breakdown can be thought as the reflection due to a mismatched load of normalized impedance z L in a microwave circuit. Assuming that the object responsible for the reflection is characterized by the complex permittivity ε and by a unitary magnetic permeability, z L = √ε = (1-Γ) / (1+Γ) where Γ is the reflection coefficient. Exploring the possibility that the RF reflection is caused by a plasma (non-collisional and quasi-neutral) with permittivity ε grown in the structure during the breakdown, suggests that its density would be about 5 10 15 electrons per cubic centimetre. The T18_vg2.6_disk is a 2π/3 travelling wave X-band structure based on CLIC requirements (100 MV/m). It is the result of the CERN-SLAC-KEK collaboration. RF signal processing (IQ demodulation and envelope detection) is numerically realized off-line. The diagnostics built for the resonant ring allows power level and field measurements as well as the measurement of currents emitted during and after a breakdown. DIPAC 2011 The phase difference between forward and reflected field tells us the breakdown location in the structure short of an integer number of wavelengths. Time information given by the instant at which the reflected field appears and the instant at which the forward field measurement shows missing power together with phase information uniquely determines the breakdown location in the structure.

DIAGNOSTICS OF RF BREAKDOWNS - accelconf.web.cern.ch · T18 structure tested at ASTA resonant ring at DIAGNOSTICS OF RF BREAKDOWNS IN HIGH-GRADIENT ACCELERATING STRUCTURES power level

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Page 1: DIAGNOSTICS OF RF BREAKDOWNS - accelconf.web.cern.ch · T18 structure tested at ASTA resonant ring at DIAGNOSTICS OF RF BREAKDOWNS IN HIGH-GRADIENT ACCELERATING STRUCTURES power level

T18 structure tested at ASTAresonant ring at

DIAGNOSTICS OF RF BREAKDOWNSIN HIGH-GRADIENT ACCELERATING STRUCTURES

field and current measurements before (left) and during (right) a breakdownpower level measurements

A. Palaia, Uppsala University, SwedenV. Dolgashev, J. Lewandowski, S. Weathersby, SLAC National Accelerator Laboratory, CA, USA

Supported by the Royal Swedish Academy of Scienceand the Knut and Alice Wallenberg foundation. Andrea Palaia,[email protected]

The resonant ring at ASTA allows high power structure testing in a two-arm wave guide loop meant torecirculate the field such that it constructively interferes with itself increasing the power level in the structureat every turn.

Estimation of the breakdown locations in the structure using phase and time information from RF measurements

phase difference between forwardand reflected RF phase and time information for each breakdown eventcompared with the position of each cell (red crosses)breakdowns distribution along the structure

Can we say something about the properties of the object reflecting RF during a breakdown?The RF reflection measured during a breakdown can be thought as the reflection due to a mismatched load ofnormalized impedance zL in a microwave circuit.Assuming that the object responsible for the reflection is characterized by the complex permittivity ε and by aunitary magnetic permeability,zL = √ε = (1-Γ) / (1+Γ)where Γ is the reflection coefficient.Exploring the possibility that the RF reflection is caused by a plasma (non-collisional and quasi-neutral) withpermittivity ε grown in the structure during the breakdown, suggests that its density would be about 5 1015electrons per cubic centimetre.

The T18_vg2.6_disk is a 2π/3travelling wave X-band structurebased on CLIC requirements (100MV/m). It is the result of theCERN-SLAC-KEK collaboration.

RF signal processing (IQdemodulation and envelopedetection) is numerically realizedoff-line.

The diagnostics built for theresonant ring allows power leveland field measurements as wellas the measurement of currentsemitted during and after abreakdown.

DIPAC 2011

The phase difference between forward and reflected field tells us the breakdown location in the structure short of an integer number of wavelengths.Time information given by the instant at which the reflected field appears and the instant at which the forward field measurement shows missing power together with phaseinformation uniquely determines the breakdown location in the structure.