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Suspension Subsystem
Overview
The test-mass suspension subsystem must preserve the low intrinsic
mechanical losses (and thus the low thermal noise) in the fused silica
suspension fibers and sapphire test mass material. It must provide
actuators for length and angular alignment, and attenuate seismic noise.
The Advanced LIGO reference design suspension is similar in design to
the GEO 600 multiple pendulum suspensions, with requirements to achieve
a seismic wall of ~10 Hz. A variety of suspension designs are needed for
the main interferometer and input conditioning optics.
The suspension forms the interface between the seismic isolation and the
suspended optics. It provides seismic isolation and the means to control
the orientation and position of the optic. These functions are served
while minimally compromising the thermal noise contribution from the test
mass mirrors and only introducing a negligible amount of thermal noise
from the suspension elements.
The optic (which in the case of the main arm cavity mirror serves also as
the test mass) is attached to the suspension fiber during the suspension
assembly process and becomes part of the suspension assembly. Features on
the test mass will be required for attachment and potentially for actuation.
The test mass suspension system is mounted (via bolts and/or clamps) to the
seismic isolation system by attachment to the SEI optics table.
Local signals are generated and fed to actuators to damp solid body motions
of the suspension components; in addition, control signals generated by the
interferometer sensing/control (ISC) are received and turned into forces on
the test mass to obtain and maintain the operational lengths and angular
orientation. There are two variants of the test mass suspension: one for
the End Test Mass (ETM) which carries potentially non-transmissive actuators
behind the optic, and one for the Input Test Mass (ITM) which must leave the
input beam free to couple into the Fabry-Perot arm cavity. There are also
variants for the beamsplitter, folding mirror, and recycling mirrors; and for
the mode cleaner, input matching telescope, and suspended steering mirrors.
A multiple-pendulum is the basis. This has two benefits:
- it provides a mechanical filter to reduce noise injected by the
controllers and the thermal noise of the lower Q isolation stages above,
- it enables a considerable reduction of control forces exerted on the
test mass itself.
The latter feature will allow the elimination of the magnets attached to the
test mass in initial LIGO (which are the largest source of excess dissipation
on the test mass), and should allow the test mass to reach a mechanical loss
(and thus thermal noise) limited principally by the substrate material. Furthermore,
eliminating the magnets reduces a potential source of correlation between the
interferometers due to correlated environmental magnetic fields. Thus both technical
noise and fundamental thermal noise should be substantially reduced in such a suspension.
Multiple simple pendulum stages also improve the seismic isolation of the test mass
for horizontal excitation of the pendulum support point; this is a valuable feature,
but requires augmentation with vertical isolation to be effective. Vertical seismic
noise can enter into the noise budget through a variety of cross-coupling mechanisms,
most directly due to the curvature of the earth over the baseline of the interferometer.
Simple pendulums have high natural frequencies for vertical motion. Thus, another key
feature of the suspension is the presence of additional vertical compliance in the
upper stages of the suspension to provide lower natural frequencies and consequently
better isolation.
Further detail can be found in the Design Requirements Document.
Key parameters of the test-mass suspension design are listed in Table 1;
other suspensions have requirements relaxed from these values.
Table 1 Test mass suspension parameters
| Suspension parameters |
Value |
| Test mass |
40 kg, sapphire |
| Penultimate masses |
Fused silica, high-density glass, or low-grade saphhire |
| Upper masses |
36 kg, stainless steel |
| Test mass suspension fibre |
Fused silica ribbon or tapered fibre |
| Upper mass suspension fibres |
Steel |
| Approximate suspension lengths |
0.5 m test mass, 0.3, 0.3 m intermediate, 0.6 m top |
| Vertical compliance |
Trapezoidal cantilever springs |
| Optic-axis transmission at 10 Hz |
10-6 |
| Test mass actuation |
Electrostatic (acquisition), photon pressure (operation) |
| Upper stage actuation, sensing |
Magnets/coils, incoherent occultation sensors |
Concept/Options
The testmass mirror is suspended as the lowest mass of a quadruple pendulum
as shown in Figure 1; the four stages are in series. Sapphire is the
reference design mirror substrate material. However, the basic suspension design
is compatible with fused silica masses and a "fall-back" to this alternate may
be made shortly before final design. Both materials are amenable to low-loss
bonding of the fiber to the test mass. The mass above the mirror- the intermediate
mass- is made of a moderately low-mechanical-loss glassy or crystalline material
such as fused silica, high-density glass, or low-grade sapphire.
The masses at the top are suspended from two cantilever-mounted, approximately
trapezoidal, pre-curved, blade springs (inspired by and similar to the VIRGO blade
springs), and two steel wires. The blade springs are stressed to about half of the
elastic limit.
The penultimate mass is suspended from 4 cantilever springs and 2 steel wire loops.
Fused silica pieces form the break-off points at the intermediate mass. These are
attached to the penultimate and final mass using hydroxy catalysis bonding, which
is demonstrated to contribute negligible mechanical loss to the system. The upper
support stages suspension wires are not vertical and this gives some control over
mode frequencies and coupling factors.
Tolerable noise levels at the intermediate mass are within the range of experience
on prototype interferometers (10-17m/Hz1/2) and many aspects of the
technology have been tested. There are, however, no meaningful test results at
less than ~150 Hz. At the top-mass, the main concern is to avoid acoustic emission
or creep (vibration due to slipping or deforming parts).
Sensing (for damping) of the solid-body modes of the suspension requires an improved
local sensor (required performance ~10-12 m/Hz1/2
at 10 Hz) or an alternative servo
configuration to meet the subsystem noise performance requirements.
Actuation is applied to all masses in a hierarchy of lower force and higher frequency
as the test mass is approached. Coils and magnets are used on upper stages, with
electrostatics (for locking) and photon pressure (for operation) used on the test
mass itself.
Other suspended optics will have noise requirements that are less demanding than
those for the test masses, but still stricter than the initial LIGO requirements,
especially in the 10-50 Hz range. Their suspensions will employ simpler suspensions
than those for the test masses, such as the triple suspension design for the mode
cleaner mirrors shown in Figure 1.
More design detail can be found in additional subsystem documentation.

Figure 1 Test mass suspension design elevation view sketches

Figure 2 Test mass suspension rendering
R&D Status/Development Issues
The primary role of the suspension is to realize the potential for low thermal
noise, and much of the research into suspension development explores the
understanding of the materials and defines processes to realize this mission.
In addition, design efforts ensure that the seismic attenuation and the control
properties of the suspension are optimized, and prototyping efforts ensure that
the real performance is understood.
The GEO-600 suspensions utilizing the basic multiple-pendulum construction,
fused-silica fibers, and hydroxy-catalysis attachments, have been in service
since 2001. The systems have been reliable and the controls function as modeled.
The noise performance will be demonstrated in 2003.
Significant design and modeling of the mode-cleaner triple suspensions has taken
place, and successful careful comparison of the quadruple test-mass model with
the MIT/GEO prototype has been made.
Test mass thermal noise is one of the basic noise limits to performance of the
Advanced LIGO design. To realize the reference design performance, the following
lines of research are being pursued:
- Measurement of the dissipation levels (that determine the levels of
thermal noise, according to the Fluctuation-Dissipation Theorem) of
the various fused silica and sapphire components and assembled systems,
to guarantee that we can reach the levels limited by the best material
properties.
- Qualification of production techniques to ensure that assembled suspensions
meet all of the specifications, including those related to thermal noise.
A separate measurement of the Q of components does not guarantee that the
complete system will realize its potential.
- Verification that we do indeed achieve the expected thermal noise levels,
without significant amounts of excess noise; both stationary (best
characterized in the frequency domain) and non-stationary (studied in
the time domain) performance are issues.
Development of the Advanced LIGO version of the suspension starts with the multiple
pendulum scheme based on the GEO 600 suspension, and GEO is leading the trade
studies. Within that framework, there are a number of specific questions to address,
including:
- choice of masses and dimensions for the masses for each stage,
- choice of wires or ribbons, dimensions, means of fabrication, and attachment,
- necessity of reaction masses, and designs of this system where required,
- sensing and actuation systems for the damping control,
- establishment of the actuator hierarchy, including whether we can construct
a system without any direct actuation on the test mass, and development of
electrostatic actuators
Tests for attenuation, parasitic resonances, and other defects in isolation properties
(along with consequent modifications of these pendulums) are a focus of the development
effort. GEO will characterize their system with Advanced LIGO requirements in mind.
Full-scale controls and noise test prototypes are in development and will be used to
test performance against requirements in laboratory-scale experiments.
Work Plan
The R&D program will include work on this subsystem through full-scale tests of all
principal variants of the suspensions in the MIT LASTI testbed. By the completion of
that test, the design will have been carried through the design requirements, preliminary
design, and substantially through the final design review. A final LASTI test will serve
to verify form, fit and conformance to functional requirements. Advanced LIGO construction
will commence with the final design review and with placement of production subcontracts
for all suspension subsystem components. Fabricated components must begin arriving at
the optics/vacuum preparation facilities at the two sites in early 2007.
A consortium of the University of Glasgow, University of Birmingham, and Rutherford
Appleton Laboratory has proposed to UK funding sources (PPARC) to supply the test-mass
suspensions for Advanced LIGO. The GEO group at the University of Glasgow is the originator
of the design, and is very well positioned to carry through with this effort.
Assembly of complete suspension subsystem units in the site facilities will start in 2006.
Suspension of the optics in the completed suspension units will be done at the time of final
installation. This will require readiness of optics processing and suspension fiber
processing systems at each site. Sufficient systems must be completed at both sites to
support installation in the interferometer vacuum chambers early in 2007.
WBS Definition
This element includes all R&D, design, prototype testing, and hardware for the
suspension subsystem upgrade, including suspension fibers and attachment to the
core optics. It includes the intermediate masses. This element provides small
suspensions mechanical hardware for other subsystems. It includes all physical
hardware for sensing and control (including the electrostatic actuator, but not
the photon actuator) of suspended masses. It includes all components of active
elements including programmable controls items, and software specific to local
control of this subsystem. It does not include general controls for the interferometer,
nor shared controls infrastructure. It does not include controls hardware and
software specific to other subsystems for which the mechanical suspensions are
supplied by this element.
Design Requirements
Conceptual Design
Quadruple Suspension Design for Advanced LIGO
R&D Activities
Design Estimate Sheets
Baseline Plan
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