Time-resolved functional near-infrared spectroscopy
A.Torricelli, D.Contini, A.Pifferi, L.Spinelli and R.Cubeddu
ULTRAS-CNR-INFM and IFN-CNR, Politecnico di Milano, Dipartimento di Fisica
L.Craighero, L.Fadiga
Faculty of Medicine – DBSTA, Section of Human Physiology, Università di Ferrara
Trieste Workshop - “Tools to study language acquisition in early infancy”, May 5-8, 2006
Principles of functional NIRS (fNIRS)
1
10000
2
1 

  a1   HHb   HHb
 O2 Hb   O21Hb
  2 
 2 
 O2 Hb   O22Hb
 a  HHb   HHb
ASSORBIMENTO
(cm-1 M-1
)
(cm
-1
M-1)
9000
8000
HbO
7000
6000
Hb
HHb
5000
4000
3000
O2H
b
2000
1000
0
600
700
800
900
1000
LUNGHEZZA D'ONDA (nm)
wavelength
(nm)


 a1  O22Hb   a2  O21Hb
HHb   1  2 
2  1 
 HHb O2 Hb   HHb
 O2 Hb


2  1 
1  2 




 HHb
a
HHb
a
O Hb  
1  2 
2  1 
 2




 O2 Hb
HHb
O
Hb
HHb
2

tHb  HHb   O2 Hb 


O2 Hb 
 SO2 

HHb   O2 Hb 
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Lambert-Beer law
Light attenuation in a clear medium
L
I L   I 0 exp   a L 
I(0)
I(L)
a =  C
 I 0 
   a L   CL
A  ln 
 I L  
dz
z
I = light intensity [W cm-2]
a = absorption coefficient [cm-1]
L = source-detector distance = pathlength [cm]
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Light Propagation in Diffusive Media
clear medium
turbid medium
Light scattering is greater than absorption
 Photons pathlength is not the geometrical
source-detector distance
 Attenuation is dependent also on scattering
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Modified Lambert-Beer Law
A   CL B  G
B = Differential Pathlength Factor (DPF)
[-]
G = Signal loss due to scattering
[-]
L = source-detector distance
[cm]
L* = L B = effective pathlength
[cm]
Main problem: B (DPF) and G depend on wavelength, geometry,
subject, ...
Partial solution:
 Monitor changes, not absolute values
A   L B C
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Principles of Time-Resolved fNIRS
Intensity
r
’s , a
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time
Time-resolved fNIRS
Effect of scattering
log10I
Effect of absorption
log10I
Slope changes
’s
Slope do not change!
Time position
changes
time
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a
Time position
do not change!
time
Motor task on human subject:
- Time-gate analysis
Head is not homogeneous!
r
a2
Martelli et al. Perturbation model for light propagation
through diffusive layered media Phys. Med. Biol. 50
2159-2166 (2005)
’s0 , a0
S0
’s1 , a1
S1
’s2 , a2
S2
Semi-empirical approach: time-gate analysis
r
I
time
Steinbrink et al. Phys Med Biol 46:879-896 (2001)
Del Bianco et al. Phys Med Biol 47:4131-4144 (2002)
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scalp/skull
csf
brain
Motor task on human subject:
- Time-gate & microscopic Lambert-Beer law
0.10
690 nm
0.08
0.08
0.06
0.06
0.04
0.04
log(I/Io)
log(I/Io)
0.10
0.02
0.00
-0.02
-0.04
baseline
task
baseline
task
recovery
0.02
0.00
-0.02
-0.04
recovery
-0.06
-0.06
Early gate (0-750 ps)
Late (2000-2750 ps)
-0.08
-0.10
0
20
40
60
80
Early gate (0-750 ps)
Late (2000-2750 ps)
-0.08
-0.10
100
0
20
40
time (s)
0.10
0.06
0.04
0.02
690 nm
820 nm
0.00
-0.02
-0.08
-0.10
1000
1500
100
 a   a0   a
-0.06
500
80
 Rr , t; i  
   ai vt
ln 
 R0 r , t; i  
-0.04
0
60
time (s)
0.08
max contrast
820 nm
2000
2500
i
i
i
1 

  a1   HHb   HHb
 O2 Hb   O21Hb
  2 
 2 
 O2 Hb   O22Hb
 a  HHb   HHb
[ Nomura et al., Phys Med Biol 42:1009-1022 (1997) ]
time-gate delay (ps)
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PoliMi multi-channel time-resolved fNIRS system
- new set-up: S16-D64
S1
PicoQuant
PDL800
variable ND
delay
Piezojena
F-SM19
690 nm
Laser
driver
50%
variable ND
820 nm
2x2
fused splitter
50%
TCSPC-2
4 ch
router-2
TCSPC-3
4 ch
router-3
TCSPC-4
4 ch
router-4
R1
R2
R3
R4
clock
S16
Microchip Technology
dsPIC30F6014
4 ch
router-1
2x4 fused
splitter
S9
CHIP
TCSPC-1
1x9
fiber switch
OZOptics
VISNIR5050
sync
clock
1x9
fiber switch
S8
Hamamatsu
R5900-20-M4
8 ch
amp-1
8 ch
amp-2
F1
4 anodes
PMT-1
4 anodes
PMT-2
4 anodes
PMT-3
4 anodes
PMT-4
Becker & Hickl, SPC-134, HRT-41, HAFC-26
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F16
System characterization:
- detection section
4 anode PMT
+ high sensitivity: SS20 0.6%, SS25 6.0% @820 nm
18 mm
+ large area (9x9 mm2 each quadrant)
— temporal resolution (TTS 300 ps)
Fiber bundle
+ large NA (0.5)
3 mm
+ home-made, low cost
— seven 1-mm plastic fibers: not so flexible!
— modal dispersion limits length to 1.5 m
 4 fiber bundles in each quadrant
 total number of fiber bundles 64
… now limited to 16!!
 See poster ME21 Contini et al. for details
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System characterization:
- Instrument response function (IRF)
510 ps FWHM
520 ps FWHM
FWHM  500 ps
 5 ms minimum acquisition time per single channel
 max injected power < 0.5 mW
 8 MHz (2MHz/board)  106 ph/s per wavelength

 See poster ME21 Contini et al. for details
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System characterization:
- Linearity for absorption
• Results for 690 nm, no major differences at 820 nm
0.6
A
0.5
B
C
D
-1
Meas. absorption (cm )
-1
Meas. absorption (cm )
0.6
0.4
0.3
0.2
0.1
8
0.5
7
0.4
6
5
0.3
4
0.2
3
2
0.1
1
0.0
0.0
0
0.1
0.2
0.3
0.4
0.5
True absorption (cm-1)
0
5
10
15
20
25
True scattering (cm-1)
• Negligible coupling between a and s’
• Inter-channel dispersion (CV) < 9%
• Integral non-linearity < 3%
 See poster ME21 Contini et al. for details
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System characterization:
- Noise
2004 - abs
2006 - abs
2006 - late gate
100.00%
@ 200K counts
CV (%)
10.00%
CV2004 - abs:  2%
1.00%
CV2006 - abs:  0.4%
0.10%
CV2006 - late gate:  0.1%
0.01%
1.E+03
1.E+04
1.E+05
1.E+06
1.E+07
counts (ph)
• Pifferi et al., “ ...The Medphot Protocol”, Applied Optics 44:2104-2114 (2005)
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Motor task on human subject:
- protocol
Motor area for right hand identified by Transcranial Magnetic Stimulation (TMS)
2 cm
S2
D2
2 cm
S1
D1
volounteer
solid phantom
Protocol: 20 s baseline, 20 s task (finger tapping with right hand at 2Hz), 40 s recovery
9 repetitions, acquisition time 1s
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Motor task on human subject:
- HHb and O2Hb
baseline
2.0
task
recovery
HHb
O2Hb
1.5
1.0
contrast ( M)
1.5
contrast ( M)
HHb
O2Hb
2.0
chan 1
0.5
0.0
solid phantom
0.0
-1.0
-1.0
20
30
40
50
60
70
80
0
10
time (s)
20
30
40
50
60
70
time (s)
HHb
O2Hb
3.0
2.5
9 repetitions
2.0
contrast ( M)
recovery
0.5
-0.5
10
task
1.0
-0.5
0
baseline
1.5
1.0
0.5
0.0
-0.5
-1.0
-1.5
0
80
160
240
320
400
480
time (s)
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560
640
720
80
Motor task on human subject:
- HHb and O2Hb (single trials)
15s task: 1 repetition
1.0
HHb
O2Hb
0.8
0.4
0.2
0.0
10s task : 1 repetition
-0.2
-0.4
1.0
-0.6
HHb
O2Hb
0.8
-0.8
0.6
0
20
40
time (s)
60
80
0.4
0.2
0.0
-0.2
5s task : 1 repetition
-0.4
-0.6
1.0
-0.8
HHb
O2Hb
0.8
-1.0
0
20
40
time (s)
60
80
0.6
contrast ( M)
-1.0
contrast ( M)
contrast ( M)
0.6
0.4
0.2
0.0
-0.2
-0.4
-0.6
-0.8
-1.0
0
20
40
time (s)
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60
80
Motor task on human subject:
- mapping HHb and O2Hb
D1
S1
D3
D4
S2
D2
D7
D6
S3
D5
D9
S4
D8
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2 cm
D11
Protocol: 20 s baseline, 20 s
task (finger tapping with right
hand at 2Hz), 40 s recovery
4 repetitions, acquisition time
250 ms
Time-resolved fNIRS of primate brain:
- first results
HHb
O2Hb
2.5
2.0
contrast ( M)
1.5
1.0
0.5
0.0
-0.5
-1.0
-1.5
task
-2.0
rest
-2.5
0
30
60
90
time (s)
S1
D1
1 cm
1 mm fiber
Optodes in direct contact with the dura
Task: grasp food
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120
150
Future Perspectives
Source: whitelight fiber laser
Optics: photonic crystal devices
www.fianium.com
Detection & Acquisition: IC SPAD
Zappa
et
al.,
“Complete
single-photon
counting and timing module in a microchip”
Optics Letters 30:1327-1329 (2005)
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Leon-Saval et al., “Multimode fiber devices
with
single-mode
performance”,
Optics
Letters 30:2545-2527 (2005)
Time-Resolved fNIRS at Null Source-Detector Separation
Improved contrast and
resolution
Torricelli et al. Phys Rev Lett 95, 078101 (2005)
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“Future” Perspectives?
"Pre-Crime" Image Thoughts of PreCogs
(2054)
Philip K. Dick, ”The Minority Report”
(1956)
Steven Spielberg, "Minority Report”
(2002)
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Thanks to Turgut Durduran, Upenn
Scarica

Time-resolved fNIRS