A Laboratory Test of the Equivalence Principle as Prolog to a Spaceborne Experiment Robert D.
Download ReportTranscript A Laboratory Test of the Equivalence Principle as Prolog to a Spaceborne Experiment Robert D.
A Laboratory Test of the Equivalence Principle as Prolog to a Spaceborne Experiment Robert D. Reasenberg and James D. Phillips Smithsonian Astrophysical Observatory Harvard-Smithsonian Center for Astrophysics 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 1 of 26 Motivation for Testing the Equivalence Principle can be found at this conference. • Central to the present accepted theory of gravity. – Some theorists argue it is the place to look for a breakdown of general relativity. • The evidence that leads to dark energy may be telling us that we need a new gravity theory. • Attempts to create a quantum theory of gravity show a failure of the equivalence principle. • Gravity is the least well tested force. 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 2 of 26 POEM Gen-I: Chamber Optics and Slide Photodetector & Amplifier Vacuum Chamber A Beamsplitter (injectorextractor) Compensator Key Technologies: Cart Laser gauge; Capacitance gauge; Track Test Mass Assembly Motion system. B Gen-I, Gen-II, Gen-III, ?? 11/6/2015 Reasenberg & Phillips Quad Cell Modulated Light Entering Chamber (from beam launcher) Quantum to Cosmos 3 of 26 Gen-I TMA Φ = 44.5 mm h = 36.5 mm 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 4 of 26 A Vacuum Chamber in Free Fall? • Advantages – No mechanisms or motors in vacuum or power shafts passing through the wall to operate on each toss, at high speed and at sub-mm accuracy. • Laser gauge and capacitance gauge components must move with the TMA. – Chamber is relatively small. • Disadvantages – Massive object (ca. 50 kg) moves at up to 5 m/s, but must have low vibration level and rapid change of direction. – A vacuum pump must ride with chamber. 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 5 of 26 Second Pair of TMA, Gen-II • Cancellation of gravity gradient. • Δg / g = 1.6 10-7 (for Δh = 0.5 m) – Local sources vary. A B • Requires absolute distance. – dg/dz = 3 10-7 g / m. – TMA is 30% test mass. – Science goal (Gen-III): σ (Δg) / g = 5 × 10-14 – Measurement goal = 1.5 10-14 => Δh-error < 0.05 μm. 11/6/2015 Reasenberg & Phillips Quantum to Cosmos B A 6 of 26 Interchanges, Gen-III • Gen-III goal: σ (Δg) / g = 5 × 10-14 – Requires control of systematic error. • Gen-III introduces interchanges to cancel systematic errors. – Robotic left-right. • Perhaps every 10 minutes. – Manual top-bottom. • Requires braking vacuum => separate runs 1 or 2 days apart. – Manual interchange of test substance between TMA. • One interchange per experiment – if needed. 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 7 of 26 Principal Systematic Error Sources, I • Earth’s gravity gradient. – Absolute distance measurement. – Top-bottom interchange. – Second pair of TMA. • Coriolis force and transverse velocity. – Capacitance gauge measures velocity. – Air slide reduces vibration => reduced transverse velocity. • Gravity gradient due to local mass (parked cars). – Second pair of TMA. – Frequent left-right interchanges of TMA. 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 8 of 26 Principal Systematic Error Sources, II • Rotation of TMA around horizontal axis. – Measured with capacitance gauge and calibrated by inducing fast rotation with high voltage on capacitance gauge electrodes. • Misalignment of measurement beam WRT cavity. – Measure beam position. – Measured TMA position with capacitance gauge. – Measure effect by exaggerated beam tilt. 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 9 of 26 Why the Tracking Frequency Laser Gauge? No other laser gauge will do. • When we started working on POINTS, there was no adequate laser gauge. – We needed 2 pm in 1 minute to 1 hour. – We found only one serious contender, the standard heterodyne gauge. • For POEM, we need 1 pm in 1 s. – We would like 0.1 pm in 1 s! – We also need absolute distance to 0.01 μm (differential, averaged over an experiment) 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 10 of 26 TFG Block Diagram Classic Realization Stabilized Laser VFS Frequency Shifter (ADM) L VCO Frequency Counter Analog Output Phase Modulator fm ~ Interferometer (Hopping) Controller Tracking Frequency laser Gauge: loop closed by Pound-Drever-Hall locking. 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 11 of 26 4 TFG Advantages • Intrinsically free of the cyclic bias characteristic of heterodyne laser gauges. • Able to operate in a cavity for increased sensitivity. • Absolute distance available at little additional cost. • Able to suppress polarization errors (nm scale or much smaller with a cat’s eye) and, when used in a cavity, to suppress alignment errors. 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 12 of 26 TFG Precision • Shot noise limit, HeNe power of 1 μW, 1 s. – Michelson intrinsic precision: 0.06 pm. – Similar for heterodyne gauge. • Current TFG limitation is “technical noise.” – σ < 10 pm on 0.1 s samples. (12/02) . 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 13 of 26 TFG Absolute Distance • Fringe spacing in optical frequency, Φ = c/(2L). • Measure Φ, get L with no ambiguity length. – Measure optical frequency before and after a hop of K fringes to get ΔF. K>1 increases precision. – L = K c / (2 ΔF) • Precision degraded by η = ΔF / F. • Either use two lasers to read simultaneously or hop fast to avoid errors due to fluctuating path. – TFG does hop fast (50 kHz demonstrated), unlike most narrow-linewidth laser systems. 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 14 of 26 How Large Can η Be? • Using HeNe & an ADM, 500 MHz / 470 THz = 10-6. • Using a semiconductor laser, the frequency counter limit yields 2 GHz / 200 THz = 10-5. – This yields wave count => connect to phase measurement. • Using a series of markers. – Assume the DFB laser we are using. – 60 GHz / 200 THz = 3 10-4. 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 15 of 26 Coriolis • Coriolis acceleration. – Vertical Coriolis acceleration: ac = 2 ve-w |ω| cos(latitude). – Earth rotation: |ω| = 7.292 10-5 /s. – Require ve-w be measured to 33 nm/s [bias < 0.25 nm/s]. • Add capacitance gauge. – Collaboration with W. Hill (Rowland Institute at Harvard). – 5 degrees of freedom for each of 4 TMA. – TMA free floating and minimal drive signal. 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 16 of 26 POEM Capacitance Gauges Collaboration with Winfield Hill, Rowland Institute at Harvard Vacuum TMA + - Cal. 11/6/2015 ADC Correlator 24 bit 100 kHz s/w in PC f1, f2, …, f5 Estimates of 5 positions (x, y: top and bottom & z) per TMA, at 1 kHz + - ~ f 1 Out Moving Reasenberg & Phillips Quantum to Cosmos Static 17 of 26 TMA, exclusive of feet. Drive: 0.1 V rms, 10 – 20 kHz Drive plates, 3 of 5 sets. Sensitivity: < 8 nm @ 1 s. Pick-up ring. Electrode gaps: 1 mm (nominal) 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 18 of 26 Motion System • Slide (commercial now). – Follow nominal trajectory. – Low vibration motion. • Torsion bar bouncer. – Store and return energy. – Do no harm. (Cause no shock.) • Horizontal cable hit by moving system. – Soft onset of force on moving system, from geometry. – Effective mass of cable, 0.05 kg (chamber, 40 kg). 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 19 of 26 Torsion Bar Bouncer • Torsion bar with lever holds each end of cable. – Bar working size, 74 x 1 inch. – 4340 steel, heat treated. (Racing car industry) – Made possible by moving-chamber approach • Internal modes of torsion bar (cf. coil springs). – F > 1 kHz. – Small moment of inertia (vs Mchamber Rlever2). • Status: working well – alone and with motor. – Replaces system with ¼ inch cable running over pulleys. This had too much friction. 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 20 of 26 Present Slide • Anorad slide including linear motor, Renishaw gauge, and track rollers running on small rails. • TMA must be launched vertically. • Vibration at micron level (mostly 100 – 200 Hz). – Transverse velocity 3 mm / s • Long-standing plan: Use air-bearing slide. 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 21 of 26 Laser Gauge : Progress & Status • HeNe TFG works in moving system. • Two-channel frequency counter built. – Contiguous measurements – no dead time. – Precise synchronization. (Jim MacArthur, Harvard-Physics Electronics Shop) • Developing TFG using semiconductor lasers. – – – – 11/6/2015 DFB lasers at 1550 nm communications band. Lasers locked to reference cavity. Improved electronics being developed by contractor. On path to space-based application. Reasenberg & Phillips Quantum to Cosmos 22 of 26 Capacitance Gauge: Progress & Status • Architecture long established. • Electrode assemblies in hand – preliminary version. • All electronic components designed and in various stages of fabrication at Rowland Institute. – Packaging to be finalized soon. 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 23 of 26 Motion System: Progress & Status • Torsion-bar bouncer has high mechanical efficiency. – Motor servo can be (and has been) tuned less aggressively =>lower noise yet still follows trajectory to 10s of μm. • Vibration measured in present slide – too high. • Next step, air-bearing slide to replace wheels and track (as long planned). – – – – 11/6/2015 Use granite beam and porous graphite bearings. Preliminary designs completed – no serious problems. Found vendors: meet requirements at reasonable price. Have hardware to make clean dry compressed air. Reasenberg & Phillips Quantum to Cosmos 24 of 26 POEM Summary • The SAO Principle of Equivalence Measurement is a Galilean test of the WEP. • The goal for the Gen-III version of the experiment is σ (Δg) / g = 5 × 10-14 for several pairs of substances. • All Gen-I components are working and being tuned or modified for better performance; some components, originally described as part of Gen-II, are started. – Capacitance gauge (nearly finished). – Air slide (preliminary design). • The measurement system is being designed both for the control of systematic error and, where applicable, to be easily translated to be space-based. 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 25 of 26 More Information • www.cfa.harvard.edu/poem • [email protected] • 617-495-7108 • [email protected] • 617-495-7360 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 26 of 26 Principal Approaches Today • Torsion balance tests. – Sensitive to sun's gravity or horizontal component of earth's gravity. Also, other distant matter. – Best results: σ (Δg) / g = 4 × 10-13. • Adelberger et al. 2001. (confusion about factor of 3) • Galilean tests (dropping). – Sensitive to full vertical gravity of earth. – Niebauer et al. (Faller) 1987, σ (Δg) / g = 5 × 10-10. – Best results: σ (Δg) / g = 10-10 (Dittus 2001, 109 m tower, σ (Δg) / g = 10-12, projected). – Works (better) in space: our long-term goal. – POEM (σ (Δg) / g = 5 × 10-14, projected) 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 27 of 26 Heterodyne Gauge • Cyclic bias due to polarization leakage. – Multiple averaging reduces bias to 0.15 pm in few min. [Gursel, SPIE 2200, pp. 27-34, 1994]. – Abandoned by SIM in favor of concentric beams. – Variant without polarization: 3 pm in 1 sec. [Gursel, priv. comm. 2002]. • Absolute distance possible. – Requires either a second laser or a tunable laser. • Complexity. • Not able to operate in a cavity. 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 28 of 26 Classic TFG Performance 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 29 of 26 POEM Smooth Motion Problem • Coriolis acceleration. – Require ve-w be measured to 33 nm/s [bias < 0.25 nm/s]. • Capacitance gauge. – Dynamic range limit: 4 104. (engineering judgment) • Maximum transverse velocity for TMA. – (0.25 nm/s) (4 104) = 0.01 mm/s • Transverse velocity limit. – Vvertical = 5 m/s => slope error < 2 10-6. hard but possible 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 30 of 26 Straight Rails for Air Slide • Keeping the slope error < 2 10-6 is well within the capability of today’s optical fabrication techniques. – Could do better, even if we needed general non-flat shape. $(0.3 – 3) 105 • It is just within the capability of the precision granite industry. – $(4 - 7) 103 • Active system could compensate for irregular surface of rails, if needed. – E.g., PZT at each bearing and (averaged) inertial sensors. 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 31 of 26 Motion System, Cont. • Identified replacement motor controller that will permit still lower noise level. – Eliminates 5 μm encoder discretization. – More flexible and transparent control model. – Not known to be needed. 11/6/2015 Reasenberg & Phillips Quantum to Cosmos 32 of 26