Transport processes in nano-structured materials by non-linear time-resolved spectroscopy
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Transcript of Transport processes in nano-structured materials by non-linear time-resolved spectroscopy
Transport processes in nano-structured materials Transport processes in nano-structured materials by non-linear time-resolved spectroscopy by non-linear time-resolved spectroscopy
R. Torre
LENS e Dip. di Fisica , Università di Firenze INFM CRS Soft, c/o Universita’ La Sapienza
Dip. di Fisica, Univ. di Firenze
Transport Processes
These transport phenomena are relevant both for
fundamental physics and for technological applications.
Among them, the design of innovative materials for sound
and heat control.
• Acoustic waves propagation in nano-structured matter
• Flow of liquids in micro/nano pores
• Heat diffusion in heterogeneous media
Nano-structured materials
Nano-porous glasses filled with liquids
Colloidal suspensions
Gel-forming Mixtures
Random Structures
Ordered Structures
2D Fononic Crystals
Nano-porous glasses
Porous silica produced by sol-gel techniques.
These materials can be “easily” filled by liquids.
The physic models for these phenomena are still an open question .
The sound propagation in this materials shows extraordinary phenomena, as the
existence of a second slow longitudinal acoustic wave.
The flow processes are strongly modified by the porous dimension and surfaces.
Spectroscopic Techniques and Facilities
at the European Lab. for Non-Linear Spectroscopy (LENS)
Transient Grating Spectroscopy
Ultrafast Optical Kerr Effect Spectroscopy
Continuous Tech.
Time-Resolved Tech.
Light Scattering, Raman-Brilluoin Spectroscopy
Microscope for single-particle fluorescence
Time-Domain Tera Hertz Spectroscopy
Transient Grating Spectroscopy
DOE:Phase Grating LA2
APD
DigitalOscilloscope
Sample
CW Probe
Pulsed Excitation
InterferenzialFilter
LA1
El
Eso
Phase Control Neutral Filter
Chopper
SD
Eec
Eec
Eso
=532 nm
=1064 nm, t=20 ps
El+ES
LC
Nd-Yag mode-locked Laser
CW single-mode Laser
100 101 102 103 104
Data Fit
HD
-TG
sig
nal
(arb
.un.)
Time (ns)
T = 20 °C, q = 1.00 m-1
Damped acoustic oscillations, Cs and s
Thermal diffusion, tViscous flow, v
tvS tttS
TGHD CeBeetqCAS // sin
Transient Grating Exp. on Vycor glass with WaterR. Cucini, A.Taschin, P.Bartolini e R.Torre
Vycor 7930 (Corning), porous diameter 4 nmFilled with bi-distilled water
Eur. Phys. J. ST, 141, 133–136 (2007) ; Philos. Mag., 87, 715-722 (2007)Phys. Rev. Lett., submitted
100 101 102 103 104
T = 90 °C T = 80 °C T = 70 °C T = 60 °C T = 50 °C T = 40 °C T = 30 °C T = 20 °C T = 10 °C T = 4 °C T = 0 °C T = -5 °C T = -10 °C
HD
-TG
sig
nal
(ar
b.u
n.)
Time (ns)
-10 0 10 20 30 40 50 60 70 80 90
3.96
3.98
4.00
4.02
4.04
4.06
4.08
4.10
4.12
4.14
Cs
(Km
/sec
)
Temperature (°C)
Biot prediction
data q=1.00 m-1
-10 0 10 20 30 40 50 60 70 80 90
30
40
50
60
2000
4000
6000
8000
10000
Aco
usti
c re
laxa
tion
tim
e (n
s)
Temperature (°C)
data q = 1 m-1
Biot prediction
Transport Processes vs Biot model M. A. Biot, J. Acoust. Soc. Am., 28, 168 (1956).M. A. Biot, J. Acoust. Soc. Am., 28, 179 (1956).
• Very Good agreement on Cs A relatively simple theory based on continuum model
predicts correctly the high frequency (1.3 GHz) sound velocities in nano-structured materials.
• Very Poor predictions on s The model fails completely the sound damping.
Acoustic Propagation Temperature Dependence
Viscous Flow of the water inside the nano-porous
Thermal Diffusion in the nano-structured material
Temperature Dependence
-10 0 10 20 30 40 50 60 70 80 90
0
1
2
3
4
5
6
v & t (
s)
Temperature (°C)
fit
v
t
Biot model
Transport Processes vs Biot model
• Very Good agreement on v The water flow can be correctly described as the
diffusive wave predicted by Biot Model.
• No predictions on t ?
Wave-Vector Dependence
0.5 1.0 1.5 2.0 2.5
3.6
3.8
4.0
4.2
4.4
CS (
km/s
)
q (m-1)
T = 40 °C T = -10 °C
Sound Velocities
Transport Processes vs Biot model
0.0 0.5 1.0 1.5 2.0 2.5 3.0
0.00
0.03
0.06
0.09
0.12
0.15
0.18
S (
ns-1
)
q1.2
T = -10 °C T = 40 °C
Damping of Sound
0 1 2 3 4 5 6 7
0.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
T = 40 °C T= -10 °C
v (s
-1)
q2 (m-2)
Diffusion Rate of the Liquid
• Cs does not depend on q Very weak acoustic dispersion effect
s=1/s qx , with x ≈ 1.2 Anomalous sound damping
v=1/v q2 Simple diffusion process
2D Fononic Crystals
preliminary test
Ordered micro-Structures in Polymeric Films by Holographic Patterning.
100 m
2 m
1 m
Image from Optical Microscope
I. Malfanti, A.Taschin, P.Bartolini and R.Torre,
F.Simoni and F.Vita, Univ. Polit. Marche.
Epi-fluorescence image from a dye filled sample
Intensity profile in a selected direction
40 50 60 70 80 90 100
-0.5
0
0.5
1
1.5 Transient Grating preliminary results
Longitudinal Acoustic Phonon propagating in the 2D Lattice
Time nsec
Final Remarks
Non-linear time-resolved spectroscopy enables accurate and
precise investigations of the transport phenomena, covering a
particularly wide dynamic range.
Physics of transport phenomena in micro/nano-structured media
is a fundamental topic of material science.
Transient grating studies of filled nano-porous glasses show that
the Biot elastic model is able to predict correctly several transport
processes in a nano-structured medium. Nevertheless, some clear
limitations of the model are present.
Structured Glasses and Fluids
Group@LENS
• Permanent staff
R. Eramo
P. Bartolini
R. Torre
• Postdocs
A. Taschin
M. Plazanet
• PhD students
R. Cucini
I. Malfanti
LENS is an European FacilityEuropean Researchers can use the labs submitting a proposal.
www.lens.unifi.it
R
>> R,
Onde acustiche vs mezzi eterogenei
Le onde propagano in un mezzo efficace
R
Le onde vengono diffuse
Effetti di multiple scatteringTeorie mezzo-effettivo
risonante
Teorie di omogenizzazioneMezzo-effettivo non risonanteModello di Biot
~ R,
Mezzi eterogenei solido-liquido
Topologia• Sfere di vetro/silice in liquidi• Colloidi
• Sfere consolidate con liquidi• Vetri porosi Percolativa
Mezzo effettivo
Modello di Biot
Non-Percolativa
Sistemi non percolativi, mezzo-efficace
1 sola onda longitudinale che propaga con velocità efficace
Onde acustiche in sistemi solido-liquido
),,,(1 2
1
ls
ls
fKK
c
, porosità, , tortuosità
Ks, Kl , moduli elastici
s, l, densità
Sistemi percolativi, modello Biot
2 onde longitudinali che propagano con velocità diverse
),,,,,,(
),,,,,,(
22
11
fslsm
fslsm
KKKfc
KKKfc
Km , modulo elastico del solido percolante senza liquido
Teoria di Biot sulla propagazione acustica nei mezzi porosi (1956) (1)
c
2
2
aρl
lc
(1) M.A.Biot, J.Acoust. Soc. Am., 28, 168, (1956)
La teoria di Biot prevede l’esistenza di due onde acustiche longitudinali di prima e
seconda specie, corrispondenti al moto del liquido e della matrice rispettivamente in fase ed in controfase.
Vycor+CCl4
L’onda di seconda specie non si propaga
Frequenza caratteristica c: funzione della viscosità l, della densità del liquido l e del diametro medio dei pori a.
c Propagazione dell’onda di seconda specie
c 75 GHz
Mp200nm+CCl4 c 30 MHz 3 GHz
l
l2
a
aδc Rc
Il fluido è viscosamente agganciato alla matrice solida e si muove in fase con esso: propagazione di una sola onda acustica.
Solamente uno strato di liquido è viscosamente agganciato alla matrice. Il resto del liquido si disaccoppia: propagazione di una seconda onda con velocità prossima a quella del liquido di bulk.
Matrice
Porzione di liquido agganciata
Parte del liquido disaccoppiata
100 101 102 103 104-1.0
-0.5
0.0
0.5
1.0
-0.5
0.0
0.5
1.0
-1.0
-0.5
0.0
0.5
1.0
1.5
100 101 102
-0.1
0.0
0.1
PM-CCl4, q = 0.997 m-1, T = 293 K
HD
-TG
sig
nal [
Arb
.Un.
]
Vycor-CCl4, q = 0.997 m-1, T = 293 K
PM-CCl4, q = 0.997 m-1, T = 293 K
HD
-TG
sig
nal [
Arb
.Un.
]
data fit
Time [s]
residues
Time [ns]
Vycor + CCl4
PM200 + CCl4
3.68
3.70
3.72
3.74
3.76
240 260 280 300 320 340
0.8
1.2
1.6
2.0
2.4
3.98
4.00
4.02
4.04
q = 2.09 m-1 Biot, f >> fc
q = 1.39 m-1
q = 1.00 m-1
CS [
Km
/s]
PM
Temperature [K]
effective medium Vyvor-CCl4
effective medium PM-CCl4
CCl4, q = 1 m-1
Biot, f << fc
Vycor
20
40
60
80
100
120
140
60
80
100
120
30006000
240 260 280 300 320 34040
50
60
70
80
90
q = 2.09 m-1
q = 1.39 m-1
q = 1.00 m-1
Biot theory predictions
Sq1.5
S [ns
] Sq2
Temperature [K]
Vycor + CCl4
369
12151821
260 270 280 290 300 310 320 330 340
11
12
13
14
15
16
48
1216
40
60
80
q = 2.09 m-1, q = 1.39 m-1, q = 1.00 m-1
Sq1.
5 S
[ns
]
Temperature [K]
Sq0.
5
Biot theory predictions
PM200 + CCl4
Modello Biot vs mezzo-efficace
s
mm NK
)1(34
Veloc. long. solido percolante
l
lK
Velocità long.
liquido percolante
Onda veloce
Onda lenta
c
mm NK3
4
Parametro di rigidità della matrice solida0
Non
per
cola
tivo
per
cola
tivo
Sfere di silicein acqua
Sfere di silice consolidate in acqua
Fluidi elettroreologici
+
-
+
-
Sospensioni colloidali di particelle polarizzabili in solventi non-polarizzabili
Sfere di silice, con o senza coatings, in liquidi molecolari
Fluidi elettroreologici rappresentano mezzi eterogenei con caratteristiche strutturali e dinamiche controllabili
Aumento della shear viscosity
Ordine colonnare indotto
Sistema non-percolativo
percolativo
c
Parametro di rigidità del sistema
Non percolativo
Percolativo
Campo elettrico
Come varia la propagazione acustica in funzione del campo elettrico ?
mutiple scattering e localizzazione ?
effetti di bandgap fononiche ?
• Anistropia di percolazione• Fase solida con ordine cristallino delle nanosfere
Onda veloce ?
Onda lenta ?
R << RR
Misure di equilibrio in funzione della geometria e di E
Prop. planareom
eotropica
Misure di non-equilibrio in funzione del tempo
( misure strutturali e dinamiche dopo rapida accensione di E)
E
tempo