TRANSVERSE RESISTIVEWALL IMPEDANCE FROM ZOTTER 2005S THEORY Elias

TRANSVERSE RESISTIVE-WALL IMPEDANCE FROM ZOTTER 2005’S THEORY Elias Métral (25 + 5 min, 25 slides) u u Introduction and motivation “Low-frequency” regime High-frequency regime Numerical applications for a § LHC collimator (vs. Burov-Lebedev 2002 and Bane 1991) § SPS MKE kicker (vs. Burov-Lebedev and 2 -wire measurements) u Review of Zotter’s theory ( For a circular beam pipe) § Any number of layers § Any beam velocity § Any frequency Unification of 3 regimes (BL, “thick-wall” and Bane) § Any σ (conductivity), ε (permittivity) and μ (permeability) u Conclusion and work in progress Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 1

INTRODUCTION AND MOTIVATION (1/2) THE MOTIVATION: THE LHC GRAPHITE COLLIMATORS u First unstable betatron line u Skin depth for graphite (ρ = 10 μΩm) u Collimator thickness One could think that the classical “thickwall” formula would be about right Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 2

INTRODUCTION AND MOTIVATION (2/2) u In fact it is not The resistive impedance is ~ 2 orders of magnitude lower at ~ 8 k. Hz ! A new physical regime was revealed by the LHC collimators Usual regime : New regime : Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 3

N. A. FOR A LHC COLLIMATOR (1/4) COMPARISON ZOTTER 2005 -BUROV&LEBEDEV 2002 Classical thick-wall BL’s results (real and imag. parts) in black: dots without and lines with copper coating Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 4

N. A. FOR A LHC COLLIMATOR (2/4) GLOBAL PLOT FROM ZOTTER 2005 Low beam velocity case (e. g. PSB : , ) Same as Bane 1991 Negative AC conductivity Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 5

N. A. FOR A LHC COLLIMATOR (4/4) Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 6

N. A. FOR A SPS MKE KICKER Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 7

REVIEW OF ZOTTER’S THEORY (1/17) u 1) Maxwell equations § In the frequency domain, all the field quantities are taken to be proportional to § Combining the conduction and displacement current terms yields with Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 8

REVIEW OF ZOTTER’S THEORY (2/17) u 2) Scalar Helmholtz equations for the longitudinal field components Using , one obtains (using the circular cylindrical coordinates r, θ, z) § The homogeneous equation can be solved by separation of variables Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 9

REVIEW OF ZOTTER’S THEORY (3/17) m is called the azimuthal mode number (m=1 for pure dipole oscillations) and k is called the wave number Reinserting the time dependence ( be a wave proportional to ), the axial motion is seen to , with phase velocity which may in general differ from the beam velocity R (r) is given by with Radial propagation constant The solutions of this differential equation are the modified Bessel functions and Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 10

§ REVIEW OF ZOTTER’S THEORY (4/17) Conclusion for the homogeneous scalar Helmholtz equations • For pure dipole oscillations excited by a horizontal cosine modulation propagating along the particle beam, one can write the solutions for Hz and Ez as C 1, 2 and D 1, 2 are constants to be determined • Sine and cosine are interchanged for a purely vertical excitation (see source fields) • Only the solutions of the homogeneous Helmholtz equations are needed since all the regions considered are source free except the one containing the beam where the source terms have been determined separately by Gluckstern (CERN yellow report 2000 -011) See slide 14 Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 11

REVIEW OF ZOTTER’S THEORY (5/17) u 3) Transverse field components deduced from the longitudinal ones using Maxwell equations (in a source-free region) Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 12

REVIEW OF ZOTTER’S THEORY (6/17) u 4) Source of the fields: Ring-beam distribution Infinitesimally short, annular beam of charge and radius traveling with velocity along the axis § Charge density in the frequency domain where is the horizontal dipole moment Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 13

REVIEW OF ZOTTER’S THEORY (7/17) § Longitudinal source terms (from Gluckstern) Valid for , i. e. in the vacuum between the beam and the pipe = region (1) with and will be determined by the boundary conditions at b and d Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 14

REVIEW OF ZOTTER’S THEORY (8/17) u 5) The total (i. e. resistive-wall + space charge) horizontal impedance with L the length of the resistive pipe and Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 15

REVIEW OF ZOTTER’S THEORY (9/17) § The space-charge impedance is obtained with a perfect conductor at r = b, i. e. when and , with • If and Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 16

REVIEW OF ZOTTER’S THEORY (10/17) § The resistive-wall impedance is obtained by subtracting the spacecharge impedance from the total impedance Only remains to be determined (by field matching) Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 17

REVIEW OF ZOTTER’S THEORY (11/17) u 6) Field matching § At the interfaces of 2 layers (r = constant) all field strength components have to be matched, i. e. in the absence of surface charges and currents the tangential field strengths and have to be continuous § Then the radial components of the displacement and of the induction are also continuous, i. e. matching of the radial components is redundant § At a Perfect Conductor (PC) : § At a Perfect Magnet (PM) : § At r Infinity Only is permitted as diverges Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 18

REVIEW OF ZOTTER’S THEORY (12/17) § General form of the field strengths in region (p) (Ep, Gp, αp and ηp) are constants to be determined … Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 19

u REVIEW OF ZOTTER’S THEORY (13/17) 7) General 1 -layer formula α 2 and η 2 are determined by the boundary conditions at the outer chamber wall r = d Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 20

REVIEW OF ZOTTER’S THEORY (14/17) d , or PC or PM (2) Layer 1 § d § Perfect Conductor (PC) (1) Vacuum Beam a b § Perfect Magnet (PM) d Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 21

u REVIEW OF ZOTTER’S THEORY (15/17) 8) General 2 -layer formula where the parameters (E 2, α 2) are 2 parameters out of 4 (α 2, η 2, E 2 and G 2) which have to be found by solving the matching equations at each layer boundary. The 4 unknowns are given by the following system of 4 linear equations Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 22

REVIEW OF ZOTTER’S THEORY (16/17) 1, 2, 3 refer to the vacuum (between the beam and the first layer), the first and second layer respectively Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 23

REVIEW OF ZOTTER’S THEORY (17/17) (3) Layer 2 e , or PC or PM (2) Layer 1 (1) Vacuum § e Beam a b d e Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 24

CONCLUSION AND WORK IN PROGRESS u Zotter 2005’s formula has been compared to other approaches from Burov-Lebedev 2002, Tsutsui 2003 (theory and HFSS simulations) and Vos 2003 (see Ref. 6 below) Similar results obtained in the new (Burov-Lebedev 2002) low-frequency regime u Work in Progress § Multi-bunch or “long” bunch Wave velocity Beam velocity § Finite length of the resistive beam pipe REFERENCES [1] [2] [3] [4] [5] [6] [7] [8] B. Zotter, CERN-AB-2005 -043 (2005) R. L. Gluckstern, CERN yellow report 2000 -011 (2000) E. Métral, CERN-AB-2005 -084 (2005) A. Burov and V. Lebedev, EPAC’ 02 (2002) K. L. F. Bane, SLAC/AP-87 (1991) F. Caspers et al. , EPAC’ 04 (2004) H. Tsutsui, LHC-PROJECT-NOTE-318 (2003) L. Vos, CERN-AB-2003 -005 -ABP (2003) and CERN-AB-2003 -093 -ABP (2003) Elias Métral, CERN-GSI bi-lateral working meeting on Collective Effects – Coordination of Theory and Experiments, GSI, 30 -31/03/06 25