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Photothermal SpectroscopyLecture 1 - Principles
Aristides Marcano Olaizola (PhD)Research ProfessorDepartment of Physics and EngineeringDelaware State University, US
Outlook
1. Photothermal effects: thermal lens and thermal mirror.
2. Sensitivity of the photothermal methods.
3. Photothermal characterization of materials.
4. Photothermal spectroscopy – a new kind of spectroscopy
Photothermal are those effects that occur in matter due to the generation of heat that follows the absorption of energy from electromagnetic waves.
Photoelastic – changes in density due to temperature
Photorefractive – change of the refraction index due to temperature
TVV T
TTnn
There are two major characteristics of the photothermal effects:
• Universality• Sensitivity
In any interaction of light and matter there is always a release of heat
Consider one absorbing atom contained in 1 L of water
h
Consider also that a beam of light illuminates the sample continuously. The atom will absorb one photon and will release the energy of this photon toward the surrounding water molecules (heating) in 10-10- 10-13 s.
Thermal diffusion will remove the generated heat. However, this effect is slow. It will take between tens of ms to seconds to equilibrate the temperatures. During this time the atom will accumulate the energy of 108-1013 photons. This can raise the temperature an average of 10-3 oC.
Photothermal method has a phase character. The signal is in most of the cases proportional to the change of phase
TTnL
2
S. E. Bialkowski. “Photothermal Spectroscopy Methods forChemical Analysis”. New York: Wiley, 1996.
Photothermal Effects
Thermal lens
Focused beam
Photothermal Mirror Effect
Thermal lens act like a phase plate
E
)r(ieE r
z
)r(nL2)r(
L
)()( rTTnrn
The change in temperature T is proportional to absorption
To calculate the induced phase we calculate first the distribution of temperature generated thanks to the absorption of a Gaussian beam in the sample.
Excitation Gaussian Beam Intensity
Gaussian Beam Amplitude
oo
o
zzartgi
zRrki
zar
azatEtrzE
)(2)(exp
/)()(),,(
2
2
2
22 /1)( oo zzaza
zzzzR o /)( 22
beam spot radius
curvature radius
2/2oo az Rayleigh range
z sample’s position
For a given sample’s position z and for continuous excitation (CW) the intensity of the excitation beam is
2
2
2
2exp2),(ar
aPtrW o
This function has axial symmetry. It is convenient to solve the Laplace equation in cylindrical coordinates.
where Po is the total light power
Thermal diffusivity equation –Laplace Equation
We write the Laplace equation considering axial symmetry
D thermal diffusivity coefficient absorption coefficient
pC heat capacity density
pCtrWTD
tT ),(2
In cylindrical coordinates with axial symmetry
2
22 1
zrr
rr
We will also neglect the dependence on z (thin lens approximation)
The solution of this equation was first obtained by Whinnery in 1973 (add ref here)
ddtrGtWC
trTt
p
0 0
),,,(),(),(
)(4
exp)(2
)(2/),,(22
tDr
tDtDrItrG o
Io is the modified Bessel function of zeroth order
Using the table integral
2
22
0
22
24/expexp)(
ppbdpbIo
We obtain
4/oo PT
and is the thermal conductivity coefficient
where
darTtrTctt
o )/21/(1
1
22 /2exp)/1(),(
Datc 4/2
-20 -10 0 10 200.000
0.001
0.002
0.003
0.004
t=0.1 s
t=1 s
t=10 s
t=100 sTe
mpe
ratu
re c
hang
e (o K
)
r/re
For water using a 30 mW of 532 nm light
Field of Temperatures generated by the absorption of a beam of light
Refraction index depends on temperature
22
2
o TTnT
Tnn)T(n
For most of the solvents first order is enough. For example for ethanol
TC1043.1)T(n 1o4
Thermal lens works as a phase plate(thin lens approximation)
E
))r(iexp(E
)r(
r
)(2)( rTTnLr
p
The solid samples the thermoelastic effects add an additional term
)(2)( rTnTnLr T
p
Where T is the linear thermo-elastic coefficient
CW excitaion
1
))(/21/(1
))(2exp(1),,(ztt
o
c
dgzmtzg
The phase difference with respect to the center of the beam is
)(/)()( 22 zazazm p
peo dTdnLP 2
where
)t,z,0(n)t,z,r(n2)t,z,r( p
Using the results obtained for the temperature
Mode matching coefficient
D
ApertureSample
Focusing lens
Single beam photothermal lens (PTL) experiment
Pump-probe experiment (m>1)
Probe focusing lens
Beamsplitter
sample
Aperture
Detector
Pump filter
Pump focusing lens
ap z, ab d
zop
zob
Advantages of the pump-probe experiment
1.Higher sensitivity2.Time dependence experiments possible3.Spectroscopy possible by using tunable pump sources.4.Detection technology in the visible. No need of UV or IR detectors.5.Different experimental configurations possible.
Probebeam
L2B
S A
DF
L1
ae
Pumpbeam
z d
Pump-probe optimized mode-mismatched experiment (m>>1)
We define the PTL signal as
)0,,()0,,(),,(
),(tzW
tzWztWtzS
p
pp
b
pp rdrrtzEtzW0
22,,,(),,(
where z is the sample position, b is the aperture radius.
For the sake of simplicity we can consider the radius of the aperture small (b→0). Then the signal can be calculated as
2
22
)0,0,,(
)0,0,,(),0,,(),(
tzE
tzEtzEtzS
p
pp
Plane of the sample Detection plane
We suppose r, r’ << (d-z)
R
r
'r
d-z=d’
x
y y’
x’
’
We calculate the probe amplitude at the far field using the Fresnel approximation
Using a Fresnel diffraction approximation we obtain*
0
)),()1(exp(),0,,( dgtgigiVtzEp
1
))(/21/(1
))(2exp(1),,(ztt
o
c
dgzmtzg
dzzzzzV oppopopp /]1)/[(/ 2
zop is the Rayleigh range of the probe field, zp is the probe beam waist position, d is the detector position
* Shen J, LoweRD, Snook RD (1992) Chem Phys165: 385-396. DOI:10.1016/0301-0104(92)87053-C.
For small phases we can also obtain*
c
co ttVmmV
tmVttzS/22121
/4tan),(222
1
)(/)()( 22 zazazm p
peo dTdnlP
Dzaztc 4/)()( 2
* Marcano A, Loper C, Melikechi N (2002) Pump probe mode mismatched Z-scan, J OptSoc Am B 19: 119-124.
-2 -1 0 1 2
-0,004
0,000
0,004T
L si
gnal
1 s
0.01 s0.001 s
Sample position (cm)The TL signals were calculated using the following parameters: o=0.01, p=632 nm, e=532 nm, zop=0.1 cm, ze=0.1 cm, d=200 cm, D=0.891 10-3 cm2/s and different time values as indicated.
m=1
-20 -10 0 10 20
0,0000
0,0015
0,0030
0.01 s
0.1 s
1 sT
L si
gnal
Sample position (cm)The TL signals were calculated using the following parameters: o=0.01, p=632 nm, e=532 nm, zp=100 cm, ze=0.1 cm, L=200 cm, ae=0 and D=0.891 10-3 cm2/s and different time values as indicated
Optimized mode mis-match experiment
Mode-mismatched scheme
Probe transmission through the aperture
0 5 100
20
40
T(z,t)To
Phot
ocur
rent
(nA
)
Time (s)
Transmitted through the aperture probe light (632 nm) using 250 mW of 532 nm excitation beam of light . The sample is a 2-mm column of water
Experimental PTL signal
PTL signal calculated using the data of previous slide. The solid line is the theoretical fitting of the data.
o
o
TTtTtzS
)(),(
(a)
(b)
Time (sec)
TL
sign
al (a
rb. u
nits
)
0 . 0 0 . 5 1 . 0- 5 0 0 0
0
5 0 0 0
0 . 0 0 . 5 1 . 0
- 0 . 5
0 . 0
0 . 5
PTL signal as a function of time from the distilled water sample (a) and BK7optical glass slab (b). The doted line is the pump field time dependence. Thesignal-to-noise ratio for the PTL is 10 and 75000 for BK7 glass and water,respectively.
-1 0 -5 0 5 1 00 .0
1 .0 x 1 0 -7
(a)
(b)
Sample position (cm)
-10 0 10-0 .0010
-0 .0005
0.0000
Z-scan signal for the distilled water sample(a) and the BK7 optical glass slab (b).
Marcano A. , C. Loper and N. Melikechi, Appl. Phys. Lett., 78, 3415-3417 (2001).
-10 0 10
-0.0006
-0.0004
-0.0002
0.0000PT
L si
gnal
4 Hz
7 Hz
Sample position (cm)
PTL signal from water for two different chopping frequencies : 4 y 7 Hz.
0 2 40.0
0.2
0.4
0.6
T=0
T=15 cm-1
PTL
Sig
nal
Time (s)
T=8.6 cm-1
a b
0 2 4
0.0
0.4
0.8
1.2
T=15 cm-1
Nor
mal
ized
PT
L S
igna
l
Time (s)
T=0
PTL signal is nearly scattering free
a- PTL signal as a function of time for samples (water with latex microspheres) with turbidities of 0, 8.6 and 15 cm-1 obtained using 80 mW of 532 nm CW light from the DPSS Nd-YAG laser,b- Normalized PTL signal for T=0 (black) and T=15 cm-1 (light grey) over the stationary values showing the different signal-to-noise ratios.
2 4 6 8 101E-4
1E-3
0.01
0.1
1
Turbidity (cm-1)
PTL signal
Transmittance
PTL signal as a function of turbidity The solid line is the model prediction.The dependence of transmittance is also plotted for comparison
0.0 0.5 1.0-0.6
-0.3
0.0
0.3
0.6
Time (s)
Pump
PTL signalMeat 2 mm
PTL
Sig
nal
1 10
0.01
0.1
PTL
Sig
nal
Turbidity (cm-1)
Whole milk in water
The signal can be detected in highly turbid samples
Marcano A., Isaac Basaldua, Aaron Villette, Raymond Edziah, Jinjie Liu, OmarZiane, and Noureddine Melikechi, “Photothermal lens spectrometrymeasurements in highly turbid media”, Appl. Spectros. 67 (9), 1013-1018, 2013(DOI: 10.1366/12-06970).
Photothermal Mirror MethodThis method involves the detection of the distortion of a probe beam whose reflection profile is affected by the photo-elastic deformation of a polished material surface induced by the absorption of a focused pump field
Pump beam
ReflectedDistorted Beam
Photothermal Micromirror
The theoretical model used to explain the PTM method is based on the simultaneous resolution of the thermo-elastic equation for the surface deformations and the heat conduction equation.
pCtrITDT
t),(2
Tuu T )1(2)21( 2
where is the Poisson ratio, T is the thermo-elastic
0),,( tzT
Boundary conditions
000
zzzzrz Normal stress components
),0,0(),0,(2 tutru zzp
Initial condition 0)0,,( zrT
The phase difference will be
u(z,r,t)
z
r
Sample
Pumpbeam
Scheme of the PTM experiment
•L. Malacarne, F. Sato, P. R. B. Pedreira, A. C. Bello, R. S. Mendes, M. L.Baesso, N. G. C. Astrath and J. Shen, “Nanoscale surface displacementdetection in high absorbing solids by time-resolved thermal mirror”, Appl.Phys. Lett.92(13), 131903/3 (2008). DOI: 10.1063/1.2905261.•F. Sato, L. C. Malacarne, P. R. B. Pedreira, M. P. Belancon, R. S. Mendes, M.L. Baesso, N. G. Astrath and J. Shen, “Time-resolved thermal mirror method:A theoretical study”, J. Appl. Phys.104(5), 053520/9 (2008). DOI:10.1063/1.2975997.•L. C. Malacarne, N. G. C. Astrath, G. V.B.Lukasievicz, E. K. Lenzi, M. S.Baesso and S. Bialkowski, “Time-resolved thermal lens and thermal mirrorspectroscopy with sample-fluid heat coupling: A complete model for materialcharacterization’, Appl. Spectros.65(1), 99-104 (2011). DOI: 10.1366/10-06096.•V. S. Zanuto, L. S. Herculano, M. S. Baesso, G.V.B. Lukazievicz, C. Jacinto,L. C. Malacarne and N.G.C. Astrath, “Thermal mirror spectrometry: anexperimental investigation of optical glasses”, Opt. Mat.35(5), 1129–1133(2013).DOI: 10.1016/j.optmat.2013.01.003.•N. G. C. Astrath, L. C. Malacarne, V. S. Zanuto, M. P. Belancon, R. S.Mendes, M. L. Baesso and C. Jacinto, “Finite size effect on the surfacedeformation thermal mirror method”, J. Opt. Soc. Am. B28(7), 1735-1739(2011). DOI:10.1364/JOSAB.28.001735.
References for PTM theory
dgmJtftg oo ),(8/exp),( 2
0
22
4exp2
2),(
2
ErfErfcf
wherectt / arg /;
Erf(x) is the error function and Erfc(x) is the complementary error function.
For opaque materials
A. Marcano, G. Gwanmesia, M. King and D. Caballero, Opt. Eng., 53(12), 127101 (2014). DOI:10.1117/1.OE.53.12.127101.
1pTo ))(1(P
is thermal quantum yield is the thermal conductivityP is the pump power
Datc 4
2
PTM time build-up
0
)),()1(exp(),( dgtgigiVtEp
Diffraction theory provides the value of the field amplitude of the center of the probe beam at the detection plane in a similar way it does for the PTL case
2
22
)0,(
)0,(),()(
tE
tEtEtS
p
ppPTM
0 2000 40000.0
0.5
1.0
Nor
mal
ized
PT
M S
igna
l
Time (t/tc)
=-0.1, zp=100
=-0.1, zp=2000
0 2000 40000.0
0.1
0.2
0.3
=-0.1, zp=100
PTM
Sig
nal
Time (t/tc)
=-0.1, zp=2000
PTM signal for different probe beam Rayleigh ranges
0.0 0.5 1.00.0
0.5
1.0PT
M st
atio
nary
val
ue
PTM signal as a function of PTM phase amplitude
Ref
Pump laser
Probe laser
S
Ampl.
Osc.
SG
DL
FL
B1
B2
M1
M2
M3
D
A
PTM mode-mismatch set-up
0 500 1000 15000.0
0.5
1.0
Nor
mal
ized
PT
M S
igna
l
Time (in tc units)
Glass filter532 nm, 15 mW
tc=1.6 10-3 s.Smax=0.56
0 1000 2000 30000.0
0.2
0.4
0.6
0.8
1.0
1.2
Nor
mal
ized
PT
Mt/tc
Glassy carbon445 nm, 146 mW, 3 Hz tc=60 10-6 sSstationary=0.235
0 500 1000 1500 20000.0
0.5
1.0Ni, 532 nm, 50 mW
tc=1.2 10-5 sSstationary=0.091
Nor
mal
ized
PT
M S
igna
l
Time (in tc units)
PTM signal from Ni and glassy carbon samples using 532 nm and 445 nm diode lasers
0.1 1 10 1001
10
100
1000
Sn
Pt
Ti
Cu
Ni
Quartz
t c (s)
D (10-6 m2s-1)
Equation y = a + b*x
Weight No Weighting
Residual Sum of Squares
0.02141
Pearson's r -0.99712Adj. R-Square 0.99282
Value Standard Error10-6 s Intercept 2.76241 0.0527210-6 s Slope -0.98565 0.03746
Dy2TiO5
Glass
Values of tc versus D
0.01 0.1 1 10 1000.01
0.1
1
10
Dy2Ti
2O
7
Dy2TiO5
SnNi
Cu
QuartzTi
Glassy Carbon
S e/P (W
-1)
o/P (W-1)
Glass
Stationary value versus PTM phase
Conclusions
PTL and PTM are versatile and sensitive technique to determine the absorption and photothermal properties of matters.
The use of pump-probe configuration allows the implementation of PTL an PTM spectroscopy as new method of analysis.