Title: Mirrors for Advanced Interferometer substrate and coating requirements
1Mirrors for Advanced Interferometer substrate
and coating requirements
- S.Rowan
- ESF workshop
- Perugia
- 20-23rd September 2005
2Reminder of motivation
- Analyse the recent developments in technologies
foreseen for Advanced detectors to explore the
path needed for a European 3rd generation
gravitational wave detector
- Consider here technology status of some aspects
of the detector mirrors and coatings - Thermal noise from mirrors and coatings forms an
important limit to design sensitivities at most
sensitive point in mid-frequency band
Coated fused silica mirror 18cm diameter
3Timescales
- VIRGO/GEO/LIGO all plan Advanced upgrades
- VIRGO (Benoit, yesterday)
- 2008/9 VIRGO
- 2011 (?) Advanced VIRGO
- LIGO
- 2008/9 (?) staged improvements
- 2010-13 Advanced LIGO
- GEO
- 2008 ? GEO-HF staged improvements
- 3rd European detector (20??)
- Common theme for Advanced detectors is higher
laser power (Benno) and new mirrors - What is the status of technologies related to
low-thermal-noise mirrors? (Gregg will talk re
thermal loading effects)
4Current mirrors
- All detectors currently use fused silica
substrates with coatings formed from SiO2/Ta2O5 - Optics in the detectors were installed several
years ago
- Design curves for GEO, LIGO, VIRGO which we use
were based on best models for thermal noise at
that time - The same optics are still installed but our
models for the thermal noise have changed a lot
LIGO fused silica mirror (10kg) in suspension
cradle
5Three significant changes
- Levin for mirrors with inhomogeneous loss we
should not simply add incoherently the noise
from the thermally excited modes of a mirror
loss from a volume close to the laser beam
dominates - Penn et al loss in silica may be modelled as sum
of surface, thermoelastic, and frequency
dependent bulk losses the latter improving
towards low frequency - Levin, (Nakagawa, Crooks, Harry et al)
- Dissipation from dielectric mirror coatings is
at a significant level
6Substrates - Fused silica
- Two big vendors used Corning (LIGO) ,
- Heraeus (LIGO, VIRGO, GEO)
- Each vendor makes a number of different optical
grades - Empirical measurements suggest
- Heraeus fused silica has lower mechanical loss
than Corning - The various Heraeus Suprasil grades have
different loss from one another
7Substrates fused silica
- Semi-empirical model developed by Penn et al
(Phys Rev Lett, Submitted) arXivegr-qc/0507097
Mechanical loss in fused silica
- C1, C2, C3, C4 are constants fitted to existing
loss measurements, and dependent of the exact
grade of silica used
8Substrates fused silica
- Penn et al point out
- The internal friction of very pure fused
silica is associated with strained Si-O-Si bonds,
where the energy of the bond has minima at two
different bond angles, forming an asymmetric
double-well potential. Redistribution of the bond
angles in response to an applied strain leads to
mechanical dissipation - Empirically we deduce that the manufacturing and
processing of the different grades of silica is
affecting the distribution of bond angles -
9Bulk loss
- Empirically it seems that Suprasil 311, 312 are
the grades of silica with the lowest loss (SV not
as low ??) - Good! -We tend to choose these for our optical
needs - However we dont yet understand in detail what
processing (annealing/cooling/ temps/rates
geometry etc) optimises the mechanical loss (eg
why is Corning silica not as good as Heraeus..?) - (Penn et al actively researching this area)
- Understanding this would perhaps allow us to
lower loss even further
10Surface loss
- Empirically, measurements are consistent with the
existence of a surface loss limit - Annealing samples allows them to approach this,
but dissipation then reaches a lower limit - The source(s) of dissipation for this surface
layer are not unambiguously determined
(microcracks, polishing damage what about flame
annealled samples??)
11Substrates fused silica
- Status of current models and experiments suggest
substrate thermal noise could be 10 times lower
(or more?) than old design sensitivities - good
news!! - Maybe we can lower it even further however.
- Coatings now are a dominant source of thermal
noise
12Consider an Advanced LIGO-Like design
Penn et al
- Coating thermal noise is expected to be the
dominant noise source at mid frequencies for
advanced interferometer designs
13Coating studies
- Thermal noise from the dielectric mirror coatings
applied to test masses is -essentially
acceptable- for Adv. LIGO, (Adv. VIRGO ?) - However, reduction in coating noise translates
directly to interferometer sensitivity - Unacceptable for any future detectors beyond Adv.
LIGO - Studies carried out with coatings from number of
vendors - (MLD, Waveprecision, REO, LMA Lyon)
- to study the mechanical dissipation of
ion-beam-sputtered dielectric - coatings via loss measurements
- Focussed initially on SiO2/Ta2O5 coatings
14Mechanical loss of multi-layer SiO2/Ta2O5
coatings with varying proportions of SiO2 and
Ta2O5
15Silica and tantala mechanical loss results
5.E-04
y 1.78E-09x 3.17E-04
5.E-04
Assume for each material fresidual f0 fff
4.E-04
4.E-04
3.E-04
Loss
3.E-04
2.E-04
Silica residual loss
2.E-04
Tantala residual loss
y 1.32E-09x 1.16E-04
1.E-04
5.E-05
0.E00
0
10
20
30
40
50
60
70
80
Frequency kHz
For tantala fresidual (3.2 0.1) x
10-4 f(1.8 0.4) x 10-9
For silica fresidual (1.2 0.2) x
10-4 f(1.3 0.5) x 10-9
16Status
- Measured losses are dominated by intrinsic loss
of the materials involved - Ta2O5 is mechanically lossier than SiO2
- Studies carried out of loss of Ta2O5 doped with
TiO2 - suggestion by LMA
17Doping of Ta2O5 with TiO2
Loss Angle of SiO2 /TiO2 doped Ta2O5 at 100 Hz
- Clear improvement with addition of titania
- Appears no strong correlation with amount of TiO2
- However exact concentrations of TiO2 not known
- Results from Ian MacLaren in Glasgow now
available
-4
x 10
3
Small Coater
Large Coater
2.5
Loss Angle
2
1.5
0
10
20
30
40
50
60
Relative Concentration
18Doping of Ta2O5 with TiO2
- Mechanism by which TiO2 reduces dissipation not
yet known - (Helping prevent movement of oxygen
vacancies..??) - Recent measurements by Black et al (Caltech)
confirm reduction in thermal noise from doped
coatings
Loss Angle of SiO2 /TiO2 doped Ta2O5 at 100 Hz
-4
x 10
3
Small Coater
Large Coater
2.5
Loss Angle
2
1.5
0
10
20
30
40
50
60
Relative Concentration
19Importance of material properties
- NB to get previous loss results needed to know
the Youngs modulus of the individual coating
materials - Previous results use best estimates of
properties ( these are typically not well known
for ion-beam-sputtered coatings) - I. Wygant et al (Stanford) measured the acoustic
impedance of witness multi-layer samples using an
ultrasonic reflection technique - If coating density is known then this allows
Youngs modulus to be found - However it has proved difficult to extract
precise properties of the individual materials
from measurements of multi-layers
20Material properties next steps
- Studies of some single layers of materials would
be very valuable - Study loss, Youngs modulus and density (may have
to study as a function of thickness) - These would then help inform our analysis of
multi-layer coatings - Necessary both to quantify our loss measurements
and thermal noise calculations
21Other approaches
- Pinto et al studying algorithms to vary
thickness and periodicity of coating layers - Optimise for desired reflectivity whilst
minimising amount of Ta2O5 present - Use flat-topped laser beams to more efficiently
average coating and substrate thermal noise?
22Conclusions
- 2nd generation of detectors will use fused silica
optics - Coatings will be the limiting source of thermal
noise in these advanced detector test masses - To go to 3rd generation detectors we need better
coatings or maybe to cool?? - Results from Yamamoto et al suggest coating loss
angle does not decrease significantly with
lowering T but still gain in reducing thermal
noise -
23Where does this leave us for 3rd generation
detectors?
- Limited by coating thermal noise/optical noise
- Possibly considering cooling to reduce the
coating noise - Thermal noise is not the only issue for substrate
and coating developments - Other substrate and coating issues
- Thermal loading effects can be significant see
talk by Gregg - The low thermal conductivity of silica may prove
to make it unattractive for higher power
operation - Necessitate switch to sapphire/silicon some other
material??
24Challenges for future detectors
- Future detectors may require higher levels of
laser power - In addition, further reductions in test mass and
suspension thermal noise are required - Possible materials meeting these requirements are
sapphire or silicon are there others???
- Mirror substrates must sustain high thermal loads
and maintain optical figure - Deformation of mirror surface is proportional to
a/kth Winkler et al., 1991. - a substrate expansion coefficient
- kth substrate thermal conductivity
- Would like a substrate material for which a/kth
is minimised
25Mechanical dissipation - silicon
- Silicon
- Both thermoelastic and intrinsic thermal noise
may be reduced by cooling
- Thermoelastic noise is proportional to a and
should vanish at T 120 K and 18 K where a tends
to zero - Intrinsic thermal noise exhibits two peaks at
similar temperatures - Silicon may allow significant thermal noise
improvements at low temperatures but material
properties need further study
Calculated intrinsic thermal and thermoelastic
noise _at_ 10 Hz in a single silicon test mass,
sensed with a laser beam of radius 6 cm
26Mechanical dissipation - sapphire
- Sapphire
- studied in the US as part of Ad LIGO substrate
downselect - studied by colleagues in Japan for LCGT
- Likely to have levels of intrinsic and
thermoelastic dissipation similar to silicon
(slightly lower) but without the nulls in
expansion coefficient - Could be interesting, particularly at higher
frequencies
Sapphire piece used in spot polishing
compensation demonstration 25cm diameter sample
(photo courtesy Goodrich).
27Mechanical dissipation from coatings
- Potential sources of loss
- Dissipation intrinsic to the coating materials
(defects, vacancies etc?) - Thermoelastic damping (see Fejer et al, Phys Rev
D, Braginsky,PLA) resulting from the different
thermal and elastic properties of the coating and
substrate
- In both cases resulting thermal noise level
depends on relative thermal and elastic
properties of coating and substrate - It follows that the optimum coating for a fused
silica or sapphire mass may not be the ideal
choice for a silicon mass
28Mechanical dissipation in coatings (contd)
- Diffractive coatings
- To use silicon as a diffractive optic, either
- a diffraction grating can be etched on to the
surface of the test mass onto which a coating is
applied - (Institute for Applied Optics, University of
Jena) - or
- the test mass can be coated, and a diffraction
grating etched into the coating surface - (Lawrence Livermore National Laboratories).
- The mechanical dissipation associated with such
coatings (room and cryo) needs investigated
293rd generation detectors - a problem of size
- Test masses of gt50 kg are desirable
- Silicon ingots of 450kg have been manufactured,
but aspect ratio is not optimal - Sapphire is available up to only 40kg
- Use composite test masses??,
Silicon ingot in growth furnace
Cradle ? Segmented design?
Bonded interfaces
Pic. from D. Coyne
Separate mass segments
30Conclusions cont
- Analyse the recent developments in technologies
foreseen for Advanced detectors to explore the
path needed for a European 3rd generation
gravitational wave detector - Status of substrate/coating technology for
Advanced Detectors is in pretty good shape
(silica doped coatings) - Limited by coating thermal noise but various
approaches discussed here may help us - For 3rd generation detectors cooling and/or a
change of substrate material is likely to be
needed really need to work hard on how to beat
coating thermal noise