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Mirrors for Advanced Interferometer substrate and coating requirements

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Thermal noise from mirrors and coatings forms an important limit to design ... Deformation of mirror surface is proportional to a/kth [Winkler et al., 1991] ... – PowerPoint PPT presentation

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Title: Mirrors for Advanced Interferometer substrate and coating requirements


1
Mirrors for Advanced Interferometer substrate
and coating requirements
  • S.Rowan
  • ESF workshop
  • Perugia
  • 20-23rd September 2005

2
Reminder 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
3
Timescales
  • 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)

4
Current 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
5
Three 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

6
Substrates - 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

7
Substrates 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

8
Substrates 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

9
Bulk 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

10
Surface 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??)

11
Substrates 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

12
Consider 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

13
Coating 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

14
Mechanical loss of multi-layer SiO2/Ta2O5
coatings with varying proportions of SiO2 and
Ta2O5
15
Silica 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
16
Status
  • 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

17
Doping 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
18
Doping 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
19
Importance 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

20
Material 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

21
Other 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?

22
Conclusions
  • 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

23
Where 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??

24
Challenges 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

25
Mechanical 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
26
Mechanical 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).
27
Mechanical 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

28
Mechanical 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

29
3rd 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
30
Conclusions 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
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