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LISA Pathfindermeasuring pico-meters and femto-Newtons in space

M Hewitson for the LPF teamBarcelona, February 15th 2012

Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Observing from Space

2Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Observing from Space

2Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Observing from Space

• Push down to much lower frequencies: mHz

2Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Observing from Space

• Push down to much lower frequencies: mHz

• Stability of ground-based instruments is difficult to achieve at these frequencies• seismic wall ~10 Hz

2Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Observing from Space

• Push down to much lower frequencies: mHz

• Stability of ground-based instruments is difficult to achieve at these frequencies• seismic wall ~10 Hz

2Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Observing from Space

• Push down to much lower frequencies: mHz

• Stability of ground-based instruments is difficult to achieve at these frequencies• seismic wall ~10 Hz

• Going to space:• Increase arm-length (increase sensitivity, ∆L/L )

2Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Observing from Space

• Push down to much lower frequencies: mHz

• Stability of ground-based instruments is difficult to achieve at these frequencies• seismic wall ~10 Hz

• Going to space:• Increase arm-length (increase sensitivity, ∆L/L ) • Quite environment (reduce noise)

2Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

LISA concept

3Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

LISA concept

3

SC

Telescope

OB

OB

PM

PM

GRS

GRS

Thruster

Thruster

Thruster

Thruster

Thruster

Thruster Telescope

Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

LISA concept

3

SC

Telescope

OB

OB

PM

PM

GRS

GRS

Thruster

Thruster

Thruster

Thruster

Thruster

Thruster Telescope

GRAVITATIONAL REFERENCE SENSOR (GRS) Test Mass + Drag free

Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

LISA concept

3

SC

Telescope

OB

OB

PM

PM

GRS

GRS

Thruster

Thruster

Thruster

Thruster

Thruster

Thruster Telescope

GRAVITATIONAL REFERENCE SENSOR (GRS) Test Mass + Drag free

OPTICAL METROLOGY Optical Bench (OB) + Phasemeter (PM)

Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

LISA concept

3

SC

Telescope

OB

OB

PM

PM

GRS

GRS

Thruster

Thruster

Thruster

Thruster

Thruster

Thruster Telescope

GRAVITATIONAL REFERENCE SENSOR (GRS) Test Mass + Drag free

OPTICAL METROLOGY Optical Bench (OB) + Phasemeter (PM)

THRUSTER

Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

LISA Measurement -> LISA Pathfinder

4Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

LISA Measurement -> LISA Pathfinder

4

a longway

Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

LISA Measurement -> LISA Pathfinder

4

a longway

Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

The LISA Pathfinder Mission

• Technology demonstrator for a LISA-like mission:• Local interferometry• micro-Newton propulsion• Gravitational Reference Sensor• Drag-free control

• LPF will be placed in orbit around L1• Requirements relaxed

• 1 order of magnitude in differential acceleration• LPF req. 3x10-14 m/s2 @ 1mHz

• 1 order of magnitude higher frequency• LPF meas. bandwidth 1mHz < f < 30mHz

5Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

The LISA Pathfinder Mission

• Technology demonstrator for a LISA-like mission:• Local interferometry• micro-Newton propulsion• Gravitational Reference Sensor• Drag-free control

• LPF will be placed in orbit around L1• Requirements relaxed

• 1 order of magnitude in differential acceleration• LPF req. 3x10-14 m/s2 @ 1mHz

• 1 order of magnitude higher frequency• LPF meas. bandwidth 1mHz < f < 30mHz

5Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

The LISA Pathfinder Team

6

Netherlands: - ISS SCOE

Germany: - Co-Principle Investigator - LTP Architect (Astrium)- Laser

Switzerland:- ISS Front End Electronics

Italy: - Principle Investigator - Inertial Sensor- Caging Mechanism

United Kingdom: - Optical Bench- Phase-meter - Charge Management

France:- Laser modulator

Spain: - Data Diagnostics System- Data Management Unit

Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Payloads on board LISA Pathfinder

• The LISA Technology Package (LTP)• European payload• Full system

• thrusters, test-masses, inertial sensor, interferometers, etc

• The Disturbance Reduction System (DRS)• NASA payload• Alternative thrusters• Alternative drag-free control

7Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Payloads on board LISA Pathfinder

• The LISA Technology Package (LTP)• European payload• Full system

• thrusters, test-masses, inertial sensor, interferometers, etc

• The Disturbance Reduction System (DRS)• NASA payload• Alternative thrusters• Alternative drag-free control

7Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

The LISA Technology Package (LTP)

8Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

x-axis measurement

9Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

IFO X1: SC-TM1 measurement

10Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Drag-free on TM1

11Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

IFO X12: TM1-TM2 displacement

12Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Suspension control

13Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Spacecraft

14Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Spacecraft

14Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Spacecraft

14Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

.

15Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

The LTP

16Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

The LTP

16

Reference Laser Unit

Data Management Unit

Phasemeter

Optical Bench

Vacuum EnclosureInertial Sensor

Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012 17Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Current status (what’s missing?)

18Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Current status (what’s missing?)• Micro-propulsion system

• problems with Ca FEEPs in the past• may now be solved

• ESA have been looking at alternative systems• modified Ca FEEPs, Indium FEEPS, Cold gas,

mini-RIT, Colloid• further testing to be done before deciding on a

solution

18Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Current status (what’s missing?)• Micro-propulsion system

• problems with Ca FEEPs in the past• may now be solved

• ESA have been looking at alternative systems• modified Ca FEEPs, Indium FEEPS, Cold gas,

mini-RIT, Colloid• further testing to be done before deciding on a

solution

• Caging mechanism• Construction of original launch-lock proved

challenging• ESA investigating alternatives

• New cam-based system, single-shot mechanism• single-shot mechanism has been selected

18Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Testing: On-station Thermal Tests

• Uses a thermal-optical qualification model in place of the flight LTP• Consists of a flight optical bench, with flight mounting

struts, and thermal mass dummies of the inertial sensors

19Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Testing: On-station Thermal Tests

• Uses a thermal-optical qualification model in place of the flight LTP• Consists of a flight optical bench, with flight mounting

struts, and thermal mass dummies of the inertial sensors

19

Alberto Lobo’s talk

Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Science Goals

20Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Science Goals

• Obtain the best geodesic motion possible• quietest differential acceleration of the two TMs

• 3 x 10-14 m s-2 /√Hz at 1 mHz• pm accuracy position measurement of TM-SC, TM-TM

• commissioning by changing system parameters• determine best configuration by experiments

20Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Science Goals

• Obtain the best geodesic motion possible• quietest differential acceleration of the two TMs

• 3 x 10-14 m s-2 /√Hz at 1 mHz• pm accuracy position measurement of TM-SC, TM-TM

• commissioning by changing system parameters• determine best configuration by experiments

• Develop a noise model of the system• allows the projection of the performance of

technologies to LISA

20Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Science Goals

• Obtain the best geodesic motion possible• quietest differential acceleration of the two TMs

• 3 x 10-14 m s-2 /√Hz at 1 mHz• pm accuracy position measurement of TM-SC, TM-TM

• commissioning by changing system parameters• determine best configuration by experiments

• Develop a noise model of the system• allows the projection of the performance of

technologies to LISA

20Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Mission Operations

• We have 90 days to achieve the goals• characterise and optimise the system

• All days are filled with pre-planned experiments• some flexibility is built-in

• Data analysis of the experiments will be done in real-time

21Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Mission Operations

• We have 90 days to achieve the goals• characterise and optimise the system

• All days are filled with pre-planned experiments• some flexibility is built-in

• Data analysis of the experiments will be done in real-time

21Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Experiments

22

• Technical studies are broken down into investigations

• These investigations are then packed into the time-line

Measurement of Parasitic Voltages

Measurement of differential acceleration noise on LISA Pathfinder

Measurement of cross-talk between the y-axis and the x-axis on the LTP

Measurement of LTP dynamical coefficients by system identification

Analysis of Data from the Radiation Monitor on LISA Pathfinder

Thermal experiments on board the LTP

Magnetic experiments on board the LTP

OPD noise investigations for LTP

Laser frequency noise characterisation for LTP

Laser Amplitude Noise Characterisation for LTP

The Drift Mode for LISA Pathfinder

Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Estimating residual differential TM acceleration (1)

• The direct observables of the instrument are displacements

• We need to estimate residual forces acting on the TMs

• We can:• estimate acceleration of the SC

• derived from SC-TM1 displacement• estimate differential acceleration of two TMs

• derived from differential displacement of two TMs

23Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Estimating residual differential TM acceleration (2)

24

�DS�1 �C

⇥⇤o = ⇤A + DS�1⇤on

Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Estimating residual differential TM acceleration (2)

24

�DS�1 �C

⇥⇤o = ⇤A + DS�1⇤on

observationnoise

Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Estimating residual differential TM acceleration (2)

24

�DS�1 �C

⇥⇤o = ⇤A + DS�1⇤on

observationnoiseresidual

acceleration

Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Estimating residual differential TM acceleration (2)

24

�DS�1 �C

⇥⇤o = ⇤A + DS�1⇤on

observationnoiseresidual

acceleration

measurement

Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Estimating residual differential TM acceleration (2)

24

�DS�1 �C

⇥⇤o = ⇤A + DS�1⇤on

observationnoiseresidual

acceleration

measurement

system

Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Estimating residual differential TM acceleration (2)

24

�DS�1 �C

⇥⇤o = ⇤A + DS�1⇤on

⇥A

⇥on

⇥o

S

C

D�1

Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Estimating residual differential TM acceleration (2)

24

�DS�1 �C

⇥⇤o = ⇤A + DS�1⇤on

⇥A

⇥on

⇥o

S

C

D�1

Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Estimating residual differential TM acceleration (2)

24

�DS�1 �C

⇥⇤o = ⇤A + DS�1⇤on

⇥A

⇥on

⇥o

S

C

D�1

Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Parameter estimation

• Employ different estimation methods to work with multiple inputs, multiple outputs

• All methods require a parametric model of the system

25Wednesday, February 15, 12

0 0.5 1 1.5 2 2.5 3x 104

−6

−5

−4

−3

−2

−1

0

1

2

3

4 x 10−9 Time origin: 2010−04−23 07:36:36.000 UTC

Am

plitu

de [

m]

Time [s]

LinearNonlinearMCMC

M Hewitson, LPF, Barcelona, 15th Feb 2012

Parameter estimation

26

0 0.5 1 1.5 2 2.5 3x 104

−5

−4

−3

−2

−1

0

1

2

3 x 10−8 Time origin: 2010−04−23 07:36:36.000 UTC

Am

plitu

de [

m]

Time [s]

LinearNonlinearMCMCData

Wednesday, February 15, 12

0 0.5 1 1.5 2 2.5 3x 104

−6

−5

−4

−3

−2

−1

0

1

2

3

4 x 10−9 Time origin: 2010−04−23 07:36:36.000 UTC

Am

plitu

de [

m]

Time [s]

LinearNonlinearMCMC

M Hewitson, LPF, Barcelona, 15th Feb 2012

Parameter estimation

26

0 0.5 1 1.5 2 2.5 3x 104

−5

−4

−3

−2

−1

0

1

2

3 x 10−8 Time origin: 2010−04−23 07:36:36.000 UTC

Am

plitu

de [

m]

Time [s]

LinearNonlinearMCMCData

10−4 10−3 10−2 10−1 10010−12

10−11

10−10

10−9

10−8

10−7

Spec

tral

den

sity

[m

Hz−

1/2 ]

Frequency [Hz]

LinearNonlinearMCMCNoise o_12

Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Results using mission simulator

• We can simulate experiments using the mission simulator• 3D, non-linear, time-domain simulation

• We can recover the parameters with high precision• very dependent on having a good model

27Wednesday, February 15, 12

M Hewitson, LPF, Sheffield, 13th September 2011 28

Data Analysis

Wednesday, February 15, 12

M Hewitson, LPF, Sheffield, 13th September 2011 28

Data Analysis

•DA Software• Toolbox of algorithms to act on the data• Repository for storing data products• Client for submitting and retrieving to/from repository• Documentation and testing

Wednesday, February 15, 12

M Hewitson, LPF, Sheffield, 13th September 2011 28

Data Analysis

•DA Software• Toolbox of algorithms to act on the data• Repository for storing data products• Client for submitting and retrieving to/from repository• Documentation and testing

•DA Activities• Simulate experiments• Design, build and test analyses and associated tools• Train scientists

Wednesday, February 15, 12

M Hewitson, LPF, Sheffield, 13th September 2011 28

Data Analysis

•DA Software• Toolbox of algorithms to act on the data• Repository for storing data products• Client for submitting and retrieving to/from repository• Documentation and testing

•DA Activities• Simulate experiments• Design, build and test analyses and associated tools• Train scientists

LTPDAhttp://www.lisa.aei-hannover.de/ltpda/

Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Noise budget

• Various noise contributions can be directly measured

• Some noise couplings must be modelled• using estimates of physical parameters together with

a system model• Some noise contributions must be estimated/

modelled from design

29Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Requirements Differential Force Noise Budget

30Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Free-flight experiment

31Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Free-flight experiment

• Capacitive actuation will be close to limiting around 1mHz

31Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Free-flight experiment

• Capacitive actuation will be close to limiting around 1mHz

• Do an experiment with the actuation off• must be short otherwise the TM will drift too far• repeat many times

31Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Free-flight experiment

• Capacitive actuation will be close to limiting around 1mHz

• Do an experiment with the actuation off• must be short otherwise the TM will drift too far• repeat many times

• Experiment:• kick test-mass away• turn off actuation• let the test-mass drift (in parabola)• repeat

31Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Simulation

32Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

PSD Estimate

33

Simulation with requirement-level noises but x3 reduced direct TM

force noise

Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Towards s/LISA/%s

34Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012

Conclusion• LPF is well on its way!

• Most of the hardware is there• awaiting thrusters and

launch lock• Most of the

experiments are already defined• many are even tested

with DA in place• We have a clear path

to launch• Launch in 2014

35Wednesday, February 15, 12

M Hewitson, LPF, Barcelona, 15th Feb 2012 36

Thank you

Wednesday, February 15, 12

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