peter : a hardware simulator for lisa pf tm-grs system
DESCRIPTION
PeTeR : a hardware simulator for LISA PF TM-GRS system. L. Marconi and R. Stanga Università degli Studi di Firenze & INFN Firenze M. Bassan , F. De Marchi, G. Pucacco and M. Visco Università di Roma “ Tor Vergata” & INFN Roma 2. Motivations. - PowerPoint PPT PresentationTRANSCRIPT
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PeTeR: a hardware simulator for LISA PF TM-GRS system
23/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
L. Marconi and R. StangaUniversità degli Studi di Firenze & INFN Firenze
M. Bassan, F. De Marchi, G. Pucacco and M. ViscoUniversità di Roma “Tor Vergata” & INFN Roma 2
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223/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
Motivations We intend to investigate the spurious forces that may act on the LISA PF TM, with a TM in quasi free-fall along 2 DoF.
With a TM in free fall conditions on 2 DoFs we can: analyze cross talks between two soft DoFs, evaluate the effects on one DoF, when we apply feedback to the second DoF.
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23/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
The experimental scheme
1 DoF rotational. 1 DoF translational.
1 DoF rotational +
1 DoF translational.
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423/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
The experimental setup in Firenze
The double pendulum is enclosed in a vacuum tank (residual pressure lower than 10-4 Pa).
We are using, from Trento University, a 4mm gap sensor in Mo and SHAPAL and a hollow 46mm TM in Al, that matches the flight model geometry.
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523/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
It works!
Control of the 2 DoFs.
Free oscillations of the 2 DoFs.
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623/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
Sensitivity: thermal noise of the W fibers
Using the fluctuation-dissipation theorem:
Dynamical equations for a 2 DoFs system:
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723/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
Sensitivity:capacitive read-out noise
ETH Zurich made for us a replica of the flight model capacitive read out electronics, each channel is read with a capacitive-inductive resonant bridge at 100kHz, the electronics generates also the waveform for the actuation.
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823/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
Noise spectrum - DoF ϕ
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923/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
Noise spectrum - DoF x
The capacitive x signal is coupling directly to the seismic noise of the laboratory .
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1023/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
Residual acceleration noise DoF ϕ
Using the two time series, with the dynamical equations of the system, we compute the total torque noise on ϕ.
Considering a: - mTM= 2kg, - l=0.02m,we obtain the residual acceleration.
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1123/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
Residual acceleration noise DoF x
Using the two time series, with the dynamical equations of the system, we compute the total torque noise on x.
Considering a : - mTM= 2kg, - l=0.15m,we obtain the residual acceleration.
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1223/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
The optical read-out (ORO)
For more details see the Luciano Di Fiore’s talk:“Development of an Optical Read/Out system for the LISA/NGO GRS: a status report” (INFN Napoli)
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1323/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
…using the ORO
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1423/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
8 DoFs model We developed also a more realistic 8 DoFs model which reproduces the frequency observed:
For more details see tomorrow ’s talk:“Analytic Model for the Rototranslational Torsion Pendulum”,by Fabrizio De Marchi (Università di Roma “Tor Vergata”).
DoF central fiber (Hz) lateral fiber (Hz)rotational 1.343·10-3 2.171·10-3
simple pendulum 0.435 0.614
boucing 10.393 7.926
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1523/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
8 DoFs model
measured simulated
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1623/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
1 DoF free, 1 DoF controlled
With our apparatus we can, for the first time, simulate the influence of the drag-free system of LISA PF on the sensitivity axis.
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1723/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
x free, ϕ controlled
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1823/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
ϕ free, x controlled
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1923/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
DC bias measurement
Stray DC bias related to spatially varying DC surface potentials couplings with the residual TM charge (q) are expected to be a significant noise source (Antonucci et al, 2012):
Any spurious DC bias distribution generates a Δx (Δϕ) that couples to the charged test mass producing a force (torque).
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2023/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
DC bias measurement:simplified model
The DC bias effect can be measured by simulating a modulated test mass charge applying a sinusoidal signal to z electrodes, assuming for all the x-electrods a uniform potential, the force and the torque produced at the first harmonic of the voltage modulation frequency ωz, for a TM centered, can be written as:
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2123/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
DC bias measurement:preliminary results
Modulation parameters: Vz = 6V fz = 3mHz
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2223/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
DC bias measurement:compensation
The residual stray DC bias Δϕ, Δx must be less than 100mV (LISA PF requirement).
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2323/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
q measurement Applying to x-electrods the VCOMP + VMODsin(ωMODt), with VMOD=5V and fMOD=3mHz, following the table:
we can demodulate the force and the torque:
obtaining:
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2423/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
Next steps Direct measurement of the rotation of the central fiber, to have an independent evaluation of x, Installation of a tip-tilt stage, to better align TM with GRS and with the optical readout.
Analyze the cross-talk between 2 soft DoFs.
Measurement of the residual magnetic moment of the TM and the cross-bar, realization of a controlled thermal box surrounding the vacuum chamber to operate at constant temperature, investigate the correlation with the seismic noise.
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2523/05/2012 9th LISA Symposium 21-25 May 2012, BnF Paris
Thank you!