Low Mechanical Dissipation in Fused Silica S. D. Penn, G. M. Harry, A. M. Gretarsson, S. E. Kittleberger, P. R. Saulson, J. J. Schiller, J. R. Smith, S.

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Presentation transcript:

Low Mechanical Dissipation in Fused Silica S. D. Penn, G. M. Harry, A. M. Gretarsson, S. E. Kittleberger, P. R. Saulson, J. J. Schiller, J. R. Smith, S. O. Swords Syracuse University LSC Meeting August 2000 LIGO-G D

Experimental Apparatus

Initial Q measurements 1998 measurement Q = 21 ‰ 10 6 at f = 732 Hz Measured in smaller bell jar post storage measurement Q = 37 ‰ 10 6 at f = 2868 Hz Measured in larger bell jar, after storage and measurement with calipers knocked against copper tube Q = 18 ‰ 10 6 at f = 1579 Hz Measured in larger bell jar, surface hit against copper tube multiple times

Flame polishing Natural gas flame polished sample surface Surface brought to transition temperature Polished for 15 minutes Cooled for 15 minutes Quickly returned to lab, reattached to suspension, and pumped down to vacuum Q = 57 ‰ 10 6 at f = 726 Hz

Ringdow data

Additional bob in suspension Added additional bob to to check for excess suspension loses Replaced center bob with two smaller bobs Sample carefully handled so surface was never touched Q = 49 ‰ 10 6 at f = 726 Hz

Graph of Q for all modes

Dissipation vs diameter in fused silica fibers

Flame polish of rod stock sample Repeated experiment with 3 mm rod stock straight from Heraeus rather than drawn from larger bob Flame polished in same way, but only on surface Surface contained visible flaws even after flame polish Found Q = 20.4 ‰ 10 6 at 113 Hz

B. Lunin’s data on fused silica

Syracuse temperature data

Possible indication of cause of dissipation (Nowick and Berry, p. 59) f 1 = 8400 Hz T 1 = 105 C f 2 = 726 Hz T 1 = 25 C E a = 0.31 eV A plausible value for activation energy

Implications for LIGO II NS Binary Inspiral range Sapphire 202 Mpc 30 million silica 166 Mpc 57 million silica 193 Mpc

Implications for LIGO II Low dissipation may be unobtainable with polished mirrors Optical coatings may greatly increase thermal noise Even obtaining 30 million Q may be challenging Further experiments are needed and some underway at Syracuse

Suggestions for further research Thick flame polished drawn rods –6 mm in vacuum, 10 mm planned –can we flame polish mirror-like geometries? Get further Q vs T data – C oven built Explore alternatives/additions to physical polishing –chemical treatments –learn more about Russian experience (B Lunin) –other possibilities?

Coating experiment update Measured uncoated Q on 16.5 cm diameter, 2 cm thick disk –Q = 3.5 ‰ 10 6 Disk being coated at REO Using smaller, 7.5 cm diameter, 2.5 mm thick, polished but not flat, disks –1st welded directly to suspension –2nd connect by bonded ear

Violin mode sensor

Non vacuum mock up made with stainless steel fiber Feedback controls for all pendulum modes Laser noise eater working Seismic noise seen –may have to build isolation Preliminary results: thermal noise measured in one violin mode, in air, with steel wire

Anelastic aftereffect experiment

Future plans Ringdown experiment with silicate bonded fused silica rods (with J. Hough and S. Rowan) Ellipsometry experiment to measure coating  on excess 40 m mirror Anelastic aftereffect measurements on sapphire including thermoelastic damping Further  vs temperature work