Transcript Slide 1
Mechanical amplifiers for the DUAL detector: lumped and distributed element design Paolo Falferi for DUAL collaboration - IFN - Trento 3rd ILIAS-GW Meeting, October 26th – 27th 2006, London Goal a wideband acoustic detector complementary to the advanced interferometric detectors in the high frequency range (1-10 kHz), compact, reliable, (relatively) cheap Exploit recent progress • Improvement of readout sensitivity (SQUID based and optomechanical devices) • New materials for the test masses. • New techniques (FEM) for design optimization of the test masses and Give up the classical scheme of the resonant readout developed to enhance the bar displacement light transducer mass narrow bandwidth No Small Masses: DUAL Design Evolution dual sphere dual cylinder single-mass dual Pros and Cons Pros and Cons Pros and Cons •omnidirectional •arrival direction ID •not selective •complicated (construction and suspension Pbm) •not omnidirectional •no arrival direction ID •selective •less complicated (suspension Pbm) •not omnidirectional •no arrival direction ID •selective •simple Sensitivity of a Single-mass DUAL Detector Molybdenum Rext = 0.5m Rint = 0.15m L = 3m M = 22 ton T/Q = 10-8 ε0 K ε0=kbTn/hw Bonaldi et al. Phys. Rev. D 74 22003 2006 Optimal Transducer Characteristics e0=1 Sxx= 6x10-46 m2/Hz Sff= 1.8x10-23 N2/Hz Noise stiffness (Sff/Sxx)1/2 = 1.7x1011 N/m Optomechanical and Capacitive Transducers (wide area and selective) C C=30 nF Ebias 2x108 V/m QL SQUID amplifier F106 PinW Sxx=6x10-44 m2/Hz Sxx=6x10-44 m2/Hz Noise Matching K n S FF S XX K mec K n Readout Noise Stiffness K mec Test Mass Mechanical Stiffness Mechanical Amplifier: Lumped Element Design REQUIREMENTS • Broadband amplification up to 5.0 kHz • Displacement gain factor about 10 • Negligible intrinsic thermal noise • Lower mechanical stiffness Y Leverage type amplifier X H.J. Paik, proceedings First AMALDI Conference (1995) Displacement Gain = Y/X=1/a»1 Limitations for the lumped element mechanical amplifier: bandwidth-gain limit Bandwidth-gain limit Kr w f G0 Mb Kr Kr Ka Kr Mb wf = cut-off frequency G0 = effective gain in practice for a Mo single-mass DUAL with amplifier G0=10 and nf=5000 Hz are achievable but... Kr Ka Limitations for the lumped element mechanical amplifier: back action noise problem 11 Single-mass DUAL k = 1.7x10 (N/m) 8 Single-mass DUAL with lumped mech. amplifier k = 5x10 (N/m) -19 10 The amplifier that permits the requested gain and bandwidth is "too soft": the readout back action noise spoils the detector performance -20 10 1/2 -1/2 Shh (Hz ) -21 10 -22 10 -23 10 The lumped element design must be abandoned -24 10 0 2000 4000 Frequency (Hz) 6000 8000 mechanical amplifier: distributed element design The longitudinal slots make the tangential displacements of the external surface larger than the internal diameter changes The thickness of the slot is the length to be measured for the detection Selection of the quadrupolar modes is still possible mechanical amplifier: distributed element design Whip (transverse wave concentrator) (D Blair et al, J Phys D: Appl Phys 20, 162 (1987) ) Gain 6 L1 x Minimum Gain y (out of resonance) x y Min L2 L 1 L2 3/ 4 L1 30 L2 Single-mass DUAL detector, Mo, T=0, M=22 t, R=0.5 m, L=3 m -19 -19 10 10-19 11 11 8 11 (N/m) Single-massDUAL DUALkkwith k= 1.7x10 Single-mass lumped (N/m) mech. amplifier k = 5x10 (N/m) Single-mass DUAL ==1.7x10 1.7x10 (N/m) 10 Single-mass k =mech. 1x10 amplifier (N/m) k = 5x108 (N/m) Single-mass DUAL DUAL with with slots lumped 11 8 Single-mass DUAL kwith = 1.7x10 slots and(N/m) whips k = 6x10 (N/m) 8 Single-mass DUAL with lumped mech. amplifier k = 5x10 (N/m) -20 -20 10 10-20 -21 -21 1/2 1/2 -1/2 -1/2 1/2 (Hz -1/2)) SS (Hz Shhhh ) (Hz hh 10 10-21 -22 -22 10 10-22 -23 -23 10 10-23 -24 -24 10 10-24 00 2000 2000 4000 4000 Frequency Frequency(Hz) (Hz) Frequency (Hz) 6000 6000 8000 8000 Single-mass DUAL detector with slots and whips Mo, M=22 t, R=0.5 m, L=3 m, Quantum Limited Readout, Q=107 10 -20 10 -21 10 -22 10 -23 10 -24 Shh 1/2 -1/2 (Hz ) 8 Single-mass DUAL with slots and whips k = 6x10 (N/m) T=0K T = 0.05 K T = 4.2 K 0 2000 4000 Frequency (Hz) 6000