Fast calculation of FP cavity for modal model

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Fast calculation of FP cavity for modal model Keiko Kokeyama Ochanomizu University And National

Fast calculation of FP cavity for modal model Keiko Kokeyama Ochanomizu University And National Astronomical Observatory of Japan

Contents • • • Introduction Basic formulae Approximations Simulation result Summary 1

Contents • • • Introduction Basic formulae Approximations Simulation result Summary 1

Introduction • • Time domain fast module Modal model version (TEM 00, TEM 01

Introduction • • Time domain fast module Modal model version (TEM 00, TEM 01 …) Calculate the light field of Fabry-Perot cavity] Total simulation time ∝ 1 / time step τ ∝ calculation points Laser field etc. Calculate once per 2 Nτ[s] * * * Calculate once per τ[s] * * * 1 step : τ=L 0/c time • To reduce the calculation points, appropriate approximations were used 2

Basic formulae Ein m 1 E 1 r 1 Eout P E 2 r

Basic formulae Ein m 1 E 1 r 1 Eout P E 2 r 2 P E 4 m 2 E 3 L 0 z 1 τ=L 0/c z 2 Matrix dimensions depend on the order of mode Ein ~ Eout light fields P Propagators (matrix) r 1(t), r 2(t) Reflectivities, tilt effects (including θ) z 1, z 2 Length changes L 0 Cavity length (constant) P is like : r 1(t) is like : 3

Basic formulae Ein (1) r 1 Eout E 1(t) can be solved : E

Basic formulae Ein (1) r 1 Eout E 1(t) can be solved : E 2 E 1 E 4 z 1 P L 0 r 2 E 3 z 2 (2) Recursively apply this stepwise formulae : (3) 1 st term: input field at time t (current) 2 nd term: N terms (steps) summation 3 rd term: field at (t-2 Nτ) It takes long time to calculate N terms (steps) summation 4

Approximation By using linear approximation, that is, by assuming that all physics quantities change

Approximation By using linear approximation, that is, by assuming that all physics quantities change linear in time, one step calculation gives the current field with the field 2 N τ [s] before N times summation without any approximations (3) Linear approximation for mirror positions and tilt angles r 1(t), r 2(t) depend on tilts θ Some further approximation are used to express the final result in an explicit analytic from. (4) No summation with approximations 5

Simulation Results All parameters =0 6

Simulation Results All parameters =0 6

Simulation Results L 0=resonant point +2*10^(-6) One mirror starts from a position slightly off

Simulation Results L 0=resonant point +2*10^(-6) One mirror starts from a position slightly off from the resonance point and moves toward the resonant point and passes it 7

Simulation Results N=20 N=50 N=200 8

Simulation Results N=20 N=50 N=200 8

Summary • Approximation formulae were developed • Calculations became faster when N is big

Summary • Approximation formulae were developed • Calculations became faster when N is big (100~) To do • Accuracy validation is undergoing (How big N is available? Any reference? ) • Compare with E 2 E calculation using primitive mirrors 9