Terahertz paintmeter for noncontact monitoring ofthickness and drying progress in paint film
Takeshi Yasui, Takashi Yasuda, Ken-ichi Sawanaka, and Tsutomu Araki

We propose a paintmeter for noncontact and remote monitoring of the thickness and drying progress ofa paint film based on the time-of-flight measurement of the echo signal of a terahertz (THz) electromagnetic pulse. The proposed method is effectively applied to two-dimensional mapping of the painting
thickness distribution for single-layer and multilayer paint films. Furthermore, adequate parameters forthe drying progress are extracted from the THz pulse-echo signal and effectively applied to monitor the
wet-to-dry transformation. The THz paintmeter can be a powerful tool for quality control of the paint filmon the in-process monitoring of car body painting. © 2005 Optical Society of America
OCIS codes: 110.6960, 120.4290, 300.6270, 310.1620.

1. Introduction

The painting of industrial products such as car bodies
is important for rust prevention, waterproofing, andcolor effect. Hence, strict quality control of the paintfilm by use of a paintmeter (a piece of test equipmentused to measure painting thickness) is required tomaintain these functions. An in-process paintmetershould meet the following requirements: (a) noncontact and remote measurement, (b) suitability for avariety of paint films and substrates, (c) high precision for thickness determination, (d) individual thickness determination for multilayered paint, (e)detailed mapping of thickness distribution, (f) detection of painting defect, and (g) monitoring of wet-todrytransformation.
However,commerciallyavailable thickness meters, including ultrasonic testing,1 eddy-current testing,2 and electromagnetic testing,3 are based on contact measurement. Althoughsuch contact-type thickness meters with hand-heldscanners are powerful tools for portable applications,they are not necessarily suited for in-process paintmonitoring because they do not adequately meet theabove requirements. The applicability of conventional thickness meters to the above requirements is

The authors are with the Graduate School of Engineering Science, Osaka University, 1-3 Machikaneyama, Toyonaka, Osaka
560-8531, Japan. T. Yasui’s e-mail address is t-yasui@me.es.osakau.ac.jp.
Received 22 March 2005; revised manuscript received 21 July
2005; accepted 25 July 2005.
0003-6935/05/326849-08$15.00/0© 2005 Optical Society of America

summarized in Table 1. One possible method for noncontact and remote measurement is optical probing.
However, colored paint film is usually opaque andcauses strong scattering of visible and infrared light,
resulting in decreased reliability of the measurement. Therefore, to our knowledge, few studies on
optical thickness meters have reported successful results.4 Furthermore, it is difficult to monitor the wetto-dry transformation of the paint film in all themethods mentioned above.
In contrast, the ultrashort pulse of electromagnetic
radiation in the teraherz (THz) pulse5 frequency
range, namely, a THz electromagnetic pulse, adds
such features as deep penetration and low scattering.
THz tomography is based on the time-of-flight measurement of the THz pulse echo. Because it serves asa remote, noninvasive probe, THz tomography has
been attracting attention as a possible substitute forthe invasive x rays and contact ultrasonic waves in
the fields of nondestructive testing and biomedical
measurements.6,7 Since THz tomography can reveal
internal structures, depending on the distribution of
the group refractive index in a given sample, it also
provides a high potential for use in the multifunctional paintmeter described above. Furthermore, if
there is a distinct spectroscopic difference in the THz
region between the wet and dry condition of a paintfilm, it will cause a temporal change of the THz pulseecho signal depending on the degree of drying. In thispaper we propose a new testing technique, called theTHz paintmeter, that uses a THz pulse to measure
the thickness and dryness of a paint film. After describing the basic performance of the THz paintmeter, we demonstrate two-dimensional (2D) mapping
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Table 1. Applicability of Conventional Thickness Meters

Requirements for In-Process Paintmeter

Ultrasonic
Testing

Eddy-Current
Testing

Electromagnetic
Testing

Noncontact and remote measurement
Suitability for various paint films and substrates
High precision for thickness determination
Individual thickness determination for multilayered paintDetailed mapping of thickness distribution
Detection of painting defectMonitoring of wet-to-dry transformation

No
Yes
Yes
Partially
No
No
No

No
Partially
Yes
No
No
No
No

No
Partially
Yes
No
No
No
No

of the painting thickness distribution in single-layer
and multilayer paint films, and we also perform monitoring of the wet-to-dry transformation of a paintfilm.

The time delay 共⌬t兲 between two pulse echoes is givenby⌬t ⫽ 共2ngd兲兾c,(1)2. Principle

The principle of the THz paintmeter is shown in Fig.
1. Let us consider a single layer of paint on a substrate. The thickness and the group refractive index
of the paint film are d and ng, respectively [Fig. 1(a)].
When the THz pulse is incident to the painting surface, the pulses are reflected at the air–paint boundary [boundary (1)] and the paint–substrate boundary[boundary (2)] because of the discontinuity of thegroup refractive index. This discontinuity results inthe development of successive echo pulses [Fig. 1(b)].

where c is the velocity of light in a vacuum. Hence,
assuming that the ng value is a known constant in thefrequency range of the spectrum of the THz pulse
used in the measurements, we can determine thegeometric thickness (d) through the measurement of⌬t of the THz pulse echo. Such a principle can easily
be extended to many types of paint films and substrates, multilayer paint films, wet paint films, or the
2D distribution of the painting thickness.
3. Experimental Setup

We used a THz tomography setup based on the reflection configuration shown in Fig. 2. The setup consists of a mode-locked Ti:sapphire (ML Ti:S) laser
oscillator, photoconductive antenna (PCA) for THz
generation, and free-space electro-optic sampling(FSEOS) for THz detection. Our laser is an 80 MHz
ML Ti:S laser (Spectra-Physics, MaiTai). The laser
pulse has a duration of 100 fs and an average power

Fig. 1. Principle of the THz paintmeter. (a) Single-layer paintfilm and (b) temporal waveform of THz pulse echo.
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Fig. 2. Experimental setup. ML Ti:S laser, mode-locked Ti:sapphire laser; BS, beam splitter; L, lens; PCA, photoconductive antenna; SiL, hemispherical silicon lens; OAP1, OAP2, and OAP3,
off-axis parabolic mirrors; ZnTe, zinc telluride crystal; FODL, fast
optical delay line; CR, corner reflector; P, polarizer; ␭兾4, quarterwave plate; RP, Rochon prism; AB-PD, autobalanced photoreceiver; LIA, lock-in amplifier; OSC, oscillator; AMP, amplifier.

Table 2. Basic Performance of the Present System

Pulse Width(ps)Spectrum Bandwidth(THz)

Measurement Time
(temporal waveform/s)

Signal-to-Noise
Ratio

Spatial Resolution
(mm)

0.4

0–2

1

100

1.7

of 1 W at 800 nm. The laser pulse is split into a pumpbeam and a probe beam with a beam splitter. The
pump beam is focused onto a PCA with a lens (L),which was fabricated on low-temperature-grown
GaAs with a bowtie length of 1 mm and a gap of
5 ␮m. To improve the signal-to-noise ratio in the
FSEOS, we applied fast chopping of the THz pulse byelectric bias modulation of the PCA.8 The electric biasof the PCA is modulated in a unipolar sinusoidal
wave with an appropriate offset (amplitude of 20 Vp-p,
offset of 10 V, frequency of 100 kHz) by the combination of an oscillator and an amplifier. The resulting
THz beam is focused on a sample via a hemisphericalsilicon lens, two off-axis parabolic mirrors (OAP1 andOAP2), and a plane mirror. For measurement of thepainting thickness distribution, a 2D moving stage
that scans the sample position laterally (XY stage)
was adopted. The THz echo beam reflected on thesample is recollimated and focused onto a 1 mm thick(110) zinc telluride (ZnTe) crystal for the FSEOS sensor with two off-axis parabolic mirrors (OAP2 andOAP3). The effective focal lengths of OAP1, OAP2,and OAP3 are 76.2 mm. On the other hand, the probe
beam via a fast optical delay line (FODL, APE, Scan
Delay, stroke length of ⫾11.5 mm, scan rate of 1 Hz,
resolution ⬍0.5% of actual scan range) and a polarizer (P) is incident to the ZnTe crystal collinear to theTHz pulse by another beam splitter. When the THz
pulse and the probe pulse are incident to the ZnTe
crystal simultaneously, the electric field of the THz
pulse causes transient birefringence in the probe
light as an electro-optical Pockels effect. After passing through the ZnTe crystal, the birefringencechange is converted into an amplitude change bybalance-detection optics composed of a quarter-wave
plate (␭兾4) and a Rochon prism, and then the amplitude change is detected with an autobalanced photoreceiver (New Focus Inc., 2007-M, bandwidth of
125 kHz) and a lock-in amplifier (NF Corporation,
5610B, bandwidth of 200 kHz, time constant of
1 ms). The temporal waveform of the THz electricfield is obtained by a sampling measurement using
the FODL. Finally, analog output from the lock-in
amplifier is measured by a digital oscilloscope triggered by the position signal of the FODL. The basic
performance of the present system is summarized inTable 2.

general use. We determined the delay time 共⌬t兲 between the first and the second echoes [see Fig. 1(b)] at
each painting thickness for the BA and WE paints
using the proposed system. The ⌬t value was calculated from the stage displacement of the FODL. The
stage displacement is equivalent to the optical thickness of the paint film 共ngd兲. The painting thickness(geometric thickness d) was measured beforehandwith a contact-type thickness meter (eddy-current
type, precision of ⫾3% of the actual thickness). The
behavior of the THz pulse in the paint film is shownin Fig. 1. Since the ng value gives the spectroscopic
characteristics of the paint, it is inherent in eachpaint. Hence, the difference of the ng value between
different paints changes the optical thickness at thesame d value, resulting in the sample-dependent
time delay. Figure 3 shows the relationship between
the painting thickness d and the delay time ⌬t (oroptical thickness ngd). Since a linear relationship between the painting thickness and the optical thickness was confirmed for each sample, we performed
the linear approximation of the data as y ⫽ ␣x, where
y is the optical thickness, ␣ is the slope constant, andx is the painting thickness (geometric thickness). The
calculated linear approximations are y ⫽ 1.81x for BA
paint (fitting error of R ⫽ 0.996) and y ⫽ 2.61x for WE
paint (fitting error of R ⫽ 0.968). Since the slope
constant of the approximate curve indicates thegroup refractive index of the paint film, the ng value
was 1.81 for the BA paint and 2.61 for the WE paint.
Conversely, if the group refractive index is known,

4. Results
A.

Thickness Measurement of a Single-Layer Paint Film

Two dry single-layer paint films on an aluminum (Al)plate were prepared as samples: quick-drying black
acryl (BA) paint and white enamel (WE) paint for

Fig. 3. Relationship between painting thickness and delay time ofTHz pulse echoes (or optical thickness). The solid lines were obtained from the linear approximation of the data as y ⫽ ␣x, where
y is the optical thickness, ␣ is the slope constant (group refractive
index), and x is the painting thickness (geometric thickness).
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the painting thickness is determined by the precise
measurement of the time delay. We here define theprecision as the standard deviation of the differencesof each measurement value from the value on theapproximated curve. The resultant precision was 4
␮m for BA, due to the nonlinearity of the FODL, theprecision of the contact-type thickness meter, and兾or
the inconsistency of the measurement spot between
the THz paintmeter and the contact-type thickness
meter. Although the minimum painting thickness in
Fig. 3 is 40 ␮m for BA and 48 ␮m for WE because of
the limitations of sample preparation, the thickness
resolution 共dmin兲 is determined from Eq. (1) as follows:
dmin ⫽ 共c⌬T兲兾共2ng兲,(2)where ⌬T is the temporal width of the THz pulse(0.4 ps, see Table 2). The thickness resolution in thepresent system is estimated to be 30 ␮m for BA and44 ␮m for WE. Work is in progress to improve thisresolution by the application of a separation algorithm of superposed pulse echoes based on a linear
optimization technique.
We next applied the THz paintmeter to several
kinds of paint films actually used for car bodies. Table
3 summarizes the components of the resin and pigment used in these samples. The substrates of thesesamples are plates of galvanized sheet iron. To compare the performance of the paintmeter for noncontact measurement of painting thickness, we applied
optical coherence tomography (OCT)9 to all the samples. Another ML Ti:S laser (Femtolasers Produktions GmbH, FemtoSource sPRO, pulse duration of
9.5 fs, central wavelength of 780 nm, spectral widthof 100 nm) was used as the laser source for the OCT.
Figure 4 shows a comparison of the pulse-echo signal
in the THz paintmeter and OCT for a metallic paintsample (sample C, thickness of 436 ␮m for the THz
paintmeter and 103 ␮m for OCT). Two pulse-echo
signals from the paint surface (air–paint boundaryand paint–substrate boundary) were clearly observedin the THz paintmeter, whereas OCT detected only
one pulse echo from the sample surface. In general,such a metallic paint film, with a pigment containing
a lot of fine Al flakes (grain diameter of 10–25 ␮m,
thickness of 0.3–0.4 ␮m), behaves as a multiplescattering medium in the visible and infrared regions; however, in the THz region, the Al flakes
hardly cause multiple scattering because of the rela-Fig. 4. Pulse-echo signal of a single-layer metallic paint film. (a)THz paintmeter and (b) OCT. The thickness of the paint film
samples is 436 ␮m for the THz paintmeter and 103 ␮m for the
OCT.

tionship between the wavelength 共⬇300 ␮m兲 and thegrain size. The applicability of the THz paintmeterand OCT for all samples is summarized in Table 3.
From these results, one can confirm the advantage of
the THz paintmeter for opaque paint films. We determined the group refractive index of each sample in
the THz region in the same manner as for Fig. 3. The
resulting ng values are also shown in Table 3. Here,let us consider the difference in ng values among
these samples. There are differences in the ng values
among the four paint films (samples A, B, C, and D)
comprised of a common resin (acryl–melamine) andTable 3. Components of Resin and Pigment, Applicability of THz Paintmeter and OCT, and Group Refractive Indices in the THz Region with Respect
to Five Kinds of Car Body Paints

THz Paintmeter

6852

SampleResin

Pigment

Applicabilityng

OCT
Applicability

A
B
C
D
E

Acryl–melamine
Acryl–melamine
Acryl–melamine
Acryl–melamine
Polyester–melamine

None
Mica
Al flake
Titanium oxide
Titanium oxide

Yes
Yes
Yes
Yes
Yes

1.50
1.66
3.61
2.01
2.02

Yes
Yes
No
No
No

APPLIED OPTICS 兾 Vol. 44, No. 32 兾 10 November 2005

ing thickness was calculated from the time-delay values at each point and the group refractive index of
2.61. The resultant painting thickness for each step isconsistent with the values determined by the contacttype thickness meter 共95, 145, and 200 ␮m兲. We canclearly perceive a detailed distribution of the painting
thickness for each step as well as a blunt edge between adjacent steps.
B.

Fig. 5. Shown is the 2D distribution of the painting thickness fora single-layer WE paint film. PX and PY indicate the X and Y coordinates of the sample position, respectively.

different pigments (none, mica, Al flake, and titanium oxide). On the other hand, no recognizable difference in ng values was observed between the twopaint films (samples D and E) comprised of different
resins (acryl–melamine and polyester–melamine)
and a common pigment (titanium oxide). Therefore
we can conclude that the difference in the ng values ismainly due to the pigment components. Also, such a
difference in the ng values implies a propagation
mechanism of the THz pulse in the paint film. In
samples B, D, and E, which contained the nonmetal
pigment (mica or titanium oxide), the THz pulse
could be transmitted through the paint film directly
because of the excellent transmittance power to nonmetal pigments. As a result of the poor transmittanceto metal pigments, the THz pulse in sample C, whichcontained the metal pigment (Al flake), was diffracted by the fine grains of the Al flake and thenpropagated through the paint film. Because of theresulting enlargement of the optical path length, theng value of sample C was larger than those of samples
B, D, and E. From all these results, we conclude thevalidity of the THz paintmeter for actual car body
paint.
It is of practical importance to extend the THz
paintmeter to the distribution measurement of thepainting thickness. Therefore we applied the proposed method to a single-layered WE paint film witha three-step surface on an aluminum substrate. The
sample position was laterally scanned by the 2D moving stage at 1 mm兾step within an area 9 mm
⫻ 20 mm. Figure 5 shows the 2D distribution of thepainting thickness for the stepped sample, in which
PX and PY indicate the X and Y coordinates of thesample position, respectively (see Fig. 2). The paint-

Thickness Measurement of a Multilayer Paint Film

We extended the THz paintmeter to a multilayer
paint film. It is difficult to determine the individual
painting thickness for each layer with a conventional
thickness meter. The prepared sample was a twolayer paint film. To evaluate the applicability to paintfilms on a nonmetal substrate, the same paints usedin the previous experiment (BA and WE in Fig. 3)
were layered on a polyethylene substrate 共ng ⫽1.80兲, as depicted in Fig. 6(a). The difference of the ng
values at the air–BA, BA–WE, and WE–substrateboundaries is approximately 0.8, resulting in the appearance of a THz pulse echo at each boundary. Figure 6(b) shows the impulse response signal of the THz
echo-pulse train for the two-layer paint film based on
numerical Fourier deconvolution.7 Here the polarity
and intensity of the impulse response signal dependon the difference of the ng values across each boundary. The first positive echo pulse [(1)] and the second
one [(2)] were generated from the air–BA and
BA–WE boundaries, respectively. The third was anegative echo [(3)] generated from the WE–substrateboundary. In this way, pulse echoes from each boundary developed successively in the picosecond range,
thus confirming that the time sequence profile of thepulse echoes depends on the internal structure of the
two-layer paint film. In addition, we determined eachthickness distribution for the two-layer paint film byscanning the sample laterally. Figure 6(c) shows theresult of individual thickness distributions of the twolayer painted film calculated from the time delay andthe ng value. The observed uniformity of the thickness distribution was 239 ⫾ 33 ␮m [(mean) ⫾ (standard deviation)] and 158 ⫾ 11 ␮m for the BA and WE
layers, respectively. The lack of uniformity for the BA
layer is obvious. From this result, we confirm that the
proposed THz paintmeter is applicable to a multilayer paint film.
C.

Detection of Paint-Off Area

One of the significant defects of paint film quality is
the paint-off, which is the separation of the paint film
from the substrate, because the substrate is highly
subject to the corrosion resulting from moisture or
salt penetration through the paint-off area of thecoating. Such paint-off is caused by poor painting
quality, unsuitable time for painting, contaminationon the painting substrate, an undesirable surrounding for painting, and兾or deterioration by aging. Thereis considerable need for nondestructive inspection of
the paint-off area because it is difficult to detect itwith the conventional thickness meter. In our next
experiment, we tried to detect a paint-off area on a
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Fig. 7. Detection of the partial paint-off area. (a) Sample and (b)2D distribution of the paint-off area. The paint-off area with the
maximum air gap of 555 ␮m is observed within the area PX⫽ 2.5–10 mm.

third positive echo at the WE–air-gap and air-gap–
substrate boundaries, respectively. Figure 7(b) shows
the 2D distribution of the partial paint-off area calculated from the time delay and the group refractive
indices of WE and air. We confirmed the paint-off
area with the maximum air gap of 555 ␮m within thearea PX ⫽ 2.5–10 mm.
D.

Fig. 6. Shown is the 2D distribution of painting thickness for a
two-layer paint film on a nonmetal substrate. (a) Sample, (b) impulse response of the THz echo-pulse train, (c) 2D distribution of
the individual painting thickness. The difference of the ng values at
the air–BA, BA–WE, and WE–substrate boundaries are approximately 0.8.

paint film. A single-layer WE painting on an aluminum substrate was prepared so that part of the painting separated from the aluminum substrate, as
shown in Fig. 7(a). Two positive pulse echoes from theair–WE and WE–substrate boundaries were observed in the intact area. In contrast, the paint-off
area appeared as a second negative pulse echo and a
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APPLIED OPTICS 兾 Vol. 44, No. 32 兾 10 November 2005

Monitoring of the Drying Process

Another advantage of our THz paintmeter is the noncontact and remote monitoring of a wet paint film. As
an actual in-process control of the painting quality,
monitoring of the paint drying condition is often required in addition to the thickness measurement. If
there is a distinctive difference of the spectroscopic
characteristics (index of refraction and兾or absorption) in the THz range between the wet condition andthe dry condition of the paint film, the wet-to-dry
transformation will cause a temporal change of theTHz pulse-echo train. In general, the drying processof acryl paint is temporally advanced by the volatilization of an organic solvent (e.g., paint thinner)added to the paint. The volatilization helps the transformation to the dry condition. In our previous paper,
we confirmed the obvious difference of spectroscopic
characteristics between the dry paint film and thewet one by THz time-domain spectroscopy.10 The
spectral change accompanying the wet-to-dry transformation results in attenuation, delay, and兾or distortion of the THz pulse echoes. Therefore, in thisFig. 8. Temporal evolution of a THz pulse-echo signal before andafter painting. The drying process is almost completed after
10 min.

paper, we tried to monitor the wet-to-dry transformation of BA paint on an aluminum plate using a temporal profile of the THz pulse-echo signal. Figure 8
shows the temporal evolution of the THz pulse-echo
signal before and after painting. Only one pulse echo
from the air–substrate boundary was observed before
painting, while two pulse echoes appeared after
painting: The first echo came from the air–BA boundary and the second one from the BA–substrate boundary. The two echo pulses did not separate completely
because the paint film was very thin with respect tothe corresponding pulse width. These two pulse echoes temporally evolved in time delay and pulse
height. For example, the time delay between the twopulse echoes decreased over time, whereas the heightof each negative echo pulse increased over time. After
10 min, the temporal change was almost finishedbecause of the quick-drying paint, implying completion of the drying process. To evaluate dryness, it isnecessary to investigate whether any drying degree

Fig. 9. Monitoring of the drying process. (a) Parameter of THz
pulse-echo signal; (b) temporal change of t1, t2, and 共t2 ⫺ t1兲 values; (c) temporal change of pulse-echo contrast (PEC). The
t1, and 共t2 ⫺ t1兲 values relate to the geometric thickness and optical
thickness of the paint film, respectively. The PEC value is definedas PEC ⫽ 共E2 ⫺ Ebottom兲兾共E2 ⫹ Ebottom兲.

parameters can be extracted from the observed waveform of the THz echo pulse in Fig. 8. The possible
parameters extracted from the THz echo signal are
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6855

illustrated in Fig. 9(a). The first and second echocome from the paint surface and the paint–substrateboundary, and their times are t1 and t2, respectively.
Hence, the t1 value relates to the geometric thickness(d) of the paint film, whereas the 共t2 ⫺ t1兲 value relates
to the optical thickness 共ngd兲 of the paint film. Figure9(b) shows the temporal change of t1, t2, and共t2 ⫺ t1兲 obtained from the pulse profiles shown in Fig.
8. The increase of the t1 value indicates the physicalshrinking of the wet paint film by the drying process.
In contrast, the t2 value remains almost constant,even when the t1 value increases, resulting in a similar change of the 共t2 ⫺ t1兲 value to the t1 value. This
result implies that the decrease of the optical thickness is mainly due to the decrease of the geometricthickness caused by physical shrinking. Such asmooth decay curve with respect to the drying process
reflects the wet-to-dry transformation in the paintfilm. Another dryness parameter is the height of theTHz echo pulses. The characteristic changes of thetemporal evolution in Fig. 8 include the height increase in the two negative pulse echoes [E1 and E2 in
Fig. 9(a)] and the disappearance of the depression
between them [Ebottom in Fig. 9(a)]. E1 depends on thegroup refractive index of the painting surface, andhence reflects the degree of drying only near thepainting surface. On the other hand, the E2 value
reflects the drying process of the whole paint film,
and it is a result of the THz absorption in the whole
paint film and the reflection at the air–BA and BA–
substrate boundaries. We empirically defined thepulse-echo contrast, called PEC, as PEC ⫽ 共E2⫺ Ebottom兲兾共E2 ⫹ Ebottom兲. Figure 9(c) shows the temporal change of the PEC value with respect to thedrying process. As one can see, the PEC value showsa smooth decay curve with respect to the drying process, and so this feature is suitable for monitoring thedegree of drying in the painting.
5. Conclusion

We have proposed a THz paintmeter to monitor the
thickness and degree of drying in a paint film basedon THz tomography. The precision and resolution of
the thickness determination of a single-layer paintfilm were 4 and 30 ␮m for BA paint, respectively.
The proposed method is useful to determine thethickness of each layer in multilayer painting andcan be extended to 2D mapping of the painting thickness distribution. The temporal change of the THz
pulse echoes is effective to monitor the drying processof a paint film. For practicality, we proposed the PEC
value, which is extracted from the temporal waveform of the THz echo pulse. This value is an indicatorof the degree of drying in a thin paint film. From all
the experiments, we conclude that the proposed THz
paintmeter is a powerful tool for the measurement of
the painting thickness and the drying progress inpaint films. Furthermore, a rapid THz paintmeter
combining real-time 2D THz tomography11,12 or asyn-

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APPLIED OPTICS 兾 Vol. 44, No. 32 兾 10 November 2005

chronous optical sampling THz time-domain measurement13 will open the door for in-processmonitoring of the painting quality of car bodies andother painted products.
This work was supported by the Industrial Technology Research Grant Program in 2004 from the
New Energy and Industrial Technology Development
Organization of Japan, the Strategic Information andCommunications R&D Promotion Programme from
the Ministry of Internal Affairs and Communicationsof Japan, the Mazda Foundation, and the Suzuki
Foundation. We are grateful to Takakazu Yamane at
Mazda Motor Corporation and Mamoru Hashimotoat Osaka University for their productive discussions.
We also thank Toshiyasu Mitsunari for his technicalsupport in our experiments.
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