Acoustic wave spectroskopy across the Brillouin zone
Transcript of Acoustic wave spectroskopy across the Brillouin zone
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Acoustic wave spectroscopy across Acoustic wave spectroscopy across the Brillouin zonethe Brillouin zone
Optical excitation of acoustic waves through wavevector and frequency specification
Keith A. Nelson Research GroupDepartment of Chemistry
MIT
Optical probe pulse
Signal
20 nm metal films
Sample
Optical pulse
sequenceAcoustic
waveSapphire substrate
Samplereference beam
excprobe
glass
probe beam to detector
samplemask
excitation beams
ND filter
Jeremy Johnson, Darius Torchinsky Christoph Klieber, Thomas Pezeril
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OutlineAcoustic wave generation & detection
MHz frequency range Impulsive stimulated Brillouin, thermal scatteringLongitudinal & shear waves
GHz frequency range Multiple-pulse picosecond ultrasonicsLongitudinal & shear waves
Supercooled liquids & glassesTests of mode-coupling theoryTests of “shoving” model & Poisson ratio predictionComparison between longitudinal & shear dynamics
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reference beamexc
probe
glass
probe beam to detector
samplemask
excitation beams
ND filter
λ= 1-200 µmν = 10-1000 MHz
Acoustic waves at all frequencies & wavelengths
Multiple pulses ⇒
time (ns)0 200 400 600 800
inte
nsity
glycerol 330 K
glycerol 275 K
glycerol 195 K
Goopωτ ≈ 1
Liquid
ωτ > 1
Solidωτ < 1
165 GHz36 nmqd < 1
Two approaches for MHz and GHz ranges
Glass multiple correlation lengths dglycerol multiple
correlation times τ
Optical probe pulse
Signal
20 nm metal films
Sample
Optical pulse
sequence
Acoustic wave
Sapphire substrate
Sample
Crossed beams ⇒ λ= 5-500 nmν = 10-1000 GHz
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Coherent control GHz-THz acoustic waves
Frequency range 20 MHz – 2 THzMacroscopic-mesoscopic wavelengths
Detailed study of thermal transport, phononics, nm correlation lengths
pulse shaper
delay line
partial reflector
lens f1 sample
probe
from laser
“Deathstar” multiple-pulse excitation of acoustic modes Frequency tunable throughout the Brillouin zone
165 GHz transmission through silica
sapphire silica
Al films
ExcitationProbe
Signal
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GHz longitudinal & shear wave generation
• elastically anisotropic material
shear wave generation:
Las
er I
llum
inat
ion
Las
er I
llum
inat
ion
crystallattice
canted crystallattice
MBE deposited iron thin film
• broken sample symmetry
metal film metal film metal film metal film thickness thickness thickness thickness ~~~~10 nm10 nm10 nm10 nm
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Selects acoustic polarization & frequency
Setup for depolarized Brillouin scattering
Detection: Depolarized Brillouin scattering
Shear wave data from silica glass
Signal from substrate reveals acoustic wave after propagation through sample
Silica glass or sapphire substrate used for different frequency ranges
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Depolarized Brillouin scattering detection
Enhancement of shear wave spectral brightness
Deathstar multiple-pulse excitationExcitation period matches Brillouin frequency
50 GHz shear waves measured in sapphire substrate
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Four-wave mixing and acoustic waves
Acoustic wavevector selected experimentallyAcoustic response driven “impulsively” by short laser pulses
Impulsive stimulated Brillouin & thermal scatteringReal-time observation through time-resolved four-wave mixing
probe
excitationpulses
signal
Crossed excitation pulses form interference “grating” patternSpatially periodic, temporally “impulsive” driving force exerted
Spatially periodic material response diffracts probe lightGrating wavevector is the phonon wavevectorq
r
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Heterodyne detection 4-wave mixing setup
Coherent scattering angle varied for wavevector selection
~ 30 MHz – 3 GHz frequency range now reached
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ISTS data from glycerolq = 0.086 µm-1 ↔ Λ = 73 µm
Acoustic & slower density dynamics
0.0 0.2 0.4 0.6 0.8 1000 2000 3000 4000 5000 6000 7000 8000
195 K
220 K
230 K
275 K
330 K
time (microseconds)
inte
nsi
ty
High T ωτ < 1 weak acoustic damping
Intermediate T ωτ ~ 1strong acoustic damping
Low T ωτ < 1 weaker acoustic damping
Lower T ωτ << 1 weak acoustic damping
Very low T ωτ <<< 1weak acoustic damping
slow structural relaxation
slower structural relaxation
thermal diffusion
thermal diffusion
thermal diffusion
thermal diffusion
thermal diffusion
acoustic wave
steady-statethermal expansion
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ISTS data from glycerolq=0.086 µm-1
~7 decades temporal range
0.01 0.1 1 10 100 1000 10000
195 K
220 K
230 K
275 K
330 K
inte
nsity
log time (microseconds)
High T –ωτ < 1, weak acoustic damping
Intermediate T –ωτ ~ 1, strong acoustic damping
Low T – ωτ < 1, weak acoustic damping
even slower structural relaxation
slower structural relaxation
structural relaxation slower than thermal diffusion at this q
thermal diffusion
Acoustic signal on ns time scales
Slower structural relaxation on ns-µs
time scales
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Shear wave generation VH excitation pulse polarizations
λ/2
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Shear acoustic wavesDepolarized impulsive stimulated Brillouin scattering (ISBS)
Recent results show different longitudinal & shear relaxation dynamics
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MHz-GHz acoustic capabilitiesMultiple-pulse GHz frequency selection
~ 10-400 GHz longitudinal frequency range Can be extended to > 1 THz
~ 5-50 GHz shear frequency range Can be extended to ~ 100 GHzChristoph Klieber
Crossed-pulse GHz wavevector selection~ 30-3000 MHz longitudinal frequency range
Can be extended to > 10 GHz
~ 100-1000 MHz shear frequency range Can be extended to ~ 50-5000 MHzJeremy Johnson
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Picosecond Shear Acoustic Waves
in Liquid Glycerol
Christoph Klieber, Thomas Pezeril, Kara Manke, Keith A. Nelson Department of Chemistry, Massachusetts Institute of Technology
Stephan Andrieu Laboratoire de Physique des Matériaux UMR7556, Université H. Poincaré / Nancy I
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Motivation
Probing high-frequency acoustic responses of liquids
Mapping the frequency dependence of the mechanical response of liquids over as many orders of magnitude as possible
Test first-principles theory and model predictions for supercooled liquids
Our Approach
Generation of coherent shear acoustic wave packets
“Death Star” pulse shaper for frequency selectivity and enhancement
Picosecond Brillouin spectroscopy (PBS) analysis
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Newton’s rings
● Study of thin liquid films of variable thicknesses
● Brillouin frequency tunable between 20/40 GHz and 50/95 GHz with prism
● Either glass or sapphire as a gauge Brillouin medium
Shear Acoustic Waves in Liquid Glycerol
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Brillouin phase
frequency thickness speed
The Brillouin phase is proportional to the time of flight through the liquid film
Brillouin amplitude
thicknessacousticattenuation
The Brillouin amplitude carry out information on the acoustic damping at the Brillouin frequency
Picosecond Brillouin spectroscopy (PBS)
Shear Acoustic Waves in Liquid Glycerol
0
PUMP
PROBE
X
liquid
iron
substrate
substrate
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Glycerol at Room Temperature
� Longitudinal speed of sound has reached its infinite-frequency value
� Shear frequency range overlaps with the high-frequency edge of alpha relaxation
� Close to linear frequency dependence of attenuation
� This indicates a frequency dependent shear viscosity
3
2
32
s ss
α ρνηω
=
Speed of Sound
Attenuation
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Temperature Dependent Acoustic Moduli of Glycerol
22( ) ( ) ˆˆ ˆ( ) ( ) ( ) ( )
ˆ( )i M
qα ω ν ωων ω ν ω ω ρ ν ω
ω ω′⋅′= ≈ − = ⋅
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Instant. Shear Modulus and Static Shear Viscosity
� Measurement of the high frequency limits of the elastic moduli K∞ / G∞, even far above the glass transition temperature
� Instantaneous shear modulus G∞
can be used to estimate the shear viscosity through the well-known Maxwell relation:
S ( )TA
Gη τ α∞= ⋅
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Conclusion
� Robust measurement applicable to many liquid and soft matter samples
� Measurement of longitudinal and shear acoustic properties of liquid Glycerol at GHz frequencies
Measurements at higher frequencies
Measurements over larger temperature interval
Other liquids, tests of first-principles theory and model predictions for supercooled liquids
More shear measurements of water
Outlook
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Coherent MHz Longitudinal and Shear Acoustic Phonons in Glass
Forming Liquids
Jeremy A. Johnson, Darius H. Torchinsky, Keith A. Nelson
Fragility of Viscous Liquids: Cause(s) and Consequences8 Oct 2008
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Outline
• Experimental– ISTS (longitudinal)
– ISBS (shear and longitudinal)
• Results and Tests of Theory– Shoving Model (shear)– Poisson Ratio (shear and longitudinal)
– TPP (shear vs. longitudinal)– DC704 (longitudinal)
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Impulsive Stimulated Scattering
• Crossed laser pulsesgenerate counter-propagating acoustic waves with wavelength Λ
• Probe beam diffracts off of relaxing region and time dependent relaxation is observed
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ISTS Signal
0 50 100 150 200 250 300
t (ns)
Schmidt, Chiesa, Torchinsky, Johnson, Nelson, Chen. Journal of Applied Physics 103, 083529 (2008).
0 5 10 15 20 25 30 35 40
t (µµµµs)
acoustic signal
3.7 µm 397 MHz
thermal signal
• Short times gives measurement of acoustic frequency and damping rate
• Longer times gives measurement of thermal decay rate
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ISTS Signal• With acoustic frequency and
damping rate, we can determine the frequency dependent complex modulus
• Slow rise allows direct time domain measurement of structural relaxation (α-relaxation)
( )2
22
qM AA
A
Γ−=′ ωρω
( )2
2
qM AA
A
Γ=′′ ωρω
( ) ( ) ( )ωωω MiMM ′′+′=*
( ) KWWKWWte
βτ−
liquid
viscous
glass
structural relaxation
Longitudinal acoustic signal from the glass former DC704 with an acoustic wavelength of 38.1µm as the sample is cooled.
moreviscous
D.H. Torchinsky, K.A. Nelson. In Preparation.
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Depolarized ISBS
• Crossed laser pulses with perpendicular polarizations generate counter-propagating shear acoustic waves
• Probe beam is depolarized as it diffracts off of the shear acoustic waves
regions of linear polarization create
shearing force on an element of the
material
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Shear ISBS• With shear acoustic frequency
and damping rate, we can determine the frequency dependent complex shear modulus
• Because there is no absorption, there are no direct structural relaxation or thermal features in the data
( )2
22
qG ss
s
Γ−=′ ωρω
( )2
2
qG ss
s
Γ=′ ωρω
( ) ( ) ( )ωωω GiGG ′′+′=*
Shear waves in 2-benzylphenol(87%)/o-terphenyl(13%), 5-phenyl 4-ether, and diethylphthalate at their respectice Tg. Insets show the Fourier spectrum on the GHz scale
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Shear Wave GalleryS
igna
l (ar
b)
Freq (GHz)
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Shear Wave GalleryS
igna
l (ar
b)
Freq (GHz)
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Outline
• Experimental– ISTS (longitudinal)
– ISBS (shear and longitudinal)
• Results and Tests of Theory– Shoving Model (shear)– Poisson Ratio (shear and longitudinal)
– TPP (shear vs. longitudinal)– DC704 (longitudinal)
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Shoving Model
• relaxation depends on rearranging region and surrounding liquid
– strong short range repulsion– elastic response in surroundings
• shoving work depends on infinite frequency elastic moduli: bulk (K∞) and shear (G∞)
• G∞ controls relaxation
( ) ( ) ( ) ( )
∆=
∆=Tk
TET
Tk
TET
BB
expor exp 00 ηηττ
Dyre et al. Phys. Rev. B53, 2171-2174 (1996).
Angell, C. A. Science, 267, 5206 (1995).
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Direct Test of Shoving Model
V
VVc
2)(
3
2 ∆=( )
= ∞
Tk
VTGT
B
c)(exp0ττ
TTG
TTGX
g
g
)(
)(
∞
∞=
Mechanical Dielectric
These results support to the notion that the dynamics of the glass transition are governed by the evolution of the shear modulus.
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Direct Test of Shoving Model
V
VVc
2)(
3
2 ∆=( )
= ∞
Tk
VTGT
B
c)(exp0ττ
TTG
TTGX
g
g
)(
)(
∞
∞=
Mechanical Dielectric
These results support to the notion that the dynamics of the glass transition are governed by the evolution of the shear modulus.
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Direct Test of Shoving Model
The root mean square deviation quantifies the amount of departure from the shoving model predicted behavior.
Deviation from the dielectric relaxation data suggests a trend of increasing deviation with increasing fragility.
A similar trend in the mechanical relaxation data is not as clear.
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Outline
• Experimental– ISTS (longitudinal)
– ISBS (shear and longitudinal)
• Results and Tests of Theory– Shoving Model (shear)– Poisson Ratio (shear and longitudinal)
– TPP (shear vs. longitudinal) – DC704 (longitudinal)
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Poisson Ratio Prediction
( )gTTdT
dm
=
= ηln
∆=Tk
ET
B
lexp)( 0ηη
mT
E
g
l 10ln2.19 2
=∆
∞∞ +∝ xGKTg
A proposed linear correlation between the fragility and instantaneous Poisson ratio
Angell, C. A. Science, 267, 5206 (1995).
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Poisson Ratio Prediction
−=
∞
∞ 41.029 GKm
( )gTTdT
dm
=
= ηln
∆=Tk
ET
B
lexp)( 0ηη
mT
E
g
l 10ln2.19 2
=∆
∞∞ +∝ xGKTg
Novikov; Sokolov. Nature431, 961-963 (2004).
A proposed linear correlation between the fragility and instantaneous Poisson ratio
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Poisson Ratio Prediction
1. 2BP87/oTP13
2. 5-phenyl 4-ether3. Ca(NO3)2 4H2O4. DC7045. diethyl phthalate6. m-fluoroaniline 7. propylene carbonate8. salol9. m-toluidine10. triphenyl phosphite
m-toluidine
salol
Our results introduce more disagreement with the proposed correlation between fragility and the Poission ratio.
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0.0E+00
5.0E+04
1.0E+05
1.5E+05
2.0E+05
2.5E+05
3.0E+05
3.5E+05
4.0E+05
4.5E+05
0 200 400 600 800 1000 1200 1400 1600
Tg (K)
M V
/ k
b
0.0E+00
2.0E+04
4.0E+04
6.0E+04
8.0E+04
1.0E+05
1.2E+05
G V
/ k b
N&S Long
Our Long
N&S Shear
Our Shear
Poisson Ratio Prediction
∞∞ +∝ xGKTgK∞
G∞
One proposed assertion is the linear relationship between the bulk and shear moduli and Tg.
This assertion is not supported by our data
Egami et al. propose that the relationship should be
And they show this correlation for metallic glasses.
( )∞∞ +⋅∝ xGKVTg
Egami et al. Phys Rev B76, 024203 (2007).
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Outline
• Experimental– ISTS (longitudinal)
– ISBS (shear and longitudinal)
• Results and Tests of Theory– Shoving Model (shear)– Poisson Ratio (shear and longitudinal)
– TPP (shear vs. longitudinal)– DC704 (longitudinal)
In preparation
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Summary
• ISS allows generation and probing of coherent longitudinal and shear acoustic phonons in the MHz frequency regime
• This has allowed direct tests of the shoving model, the proposed correlation between Poisson ratio and fragility, and some aspects of MCT
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Outlook
• Extend accessible acoustic frequency range of ISS to provide overlap between our two techniques and provide a large range of longitudinal (9-10 decades) and shear (4-5 decades) acoustic waves
• Allow test of MCT predicted relationship between ‘a’ and ‘b’ exponents
Comparison of MCT solution for χ"(ω) with the two power laws. a is the exponent for the β–relaxation regime and b is the exponent for the α–relaxation regime.
log(ω)
log
(χ")
ωωωω-b ωωωωa
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Acknowledgements
� Prof. Keith Nelson
� Dr. Thomas Pezeril
� Christoph Klieber
� Dr. Darius Torchinsky
� Jeremy Johnson
� Kara Manke
� Stephan Andrieu, Univ. Poincaré
Thank you for your attention!
This work was supported in part by
• DOE Grant No DE-FG02-00ER15087
• NSF grants CHE-0616939
• DMR-0414895