Open Access
1 July 2005 Intersubject variability of near-infrared spectroscopy signals during sensorimotor cortex activation
Hiroki Sato, Yutaka Fuchino, Masashi Kiguchi, Takusige Katura, Atsushi Maki, Takeshi Yoro, Hideaki Koizumi
Author Affiliations +
Abstract
We investigate the intersubject signal variability of near-infrared spectroscopy (NIRS), which is commonly used for noninvasive measurement of the product of the optical path length and the concentration change in oxygenated hemoglobin (ΔC′oxy) and deoxygenated hemoglobin (ΔC′deoxy) and their sum (ΔC′total) related to human cortical activation. We do this by measuring sensorimotor cortex activation in 31 healthy adults using 24-measurement-position near-infrared (NIR) topography. A finger-tapping task is used to activate the sensorimotor cortex, and significant changes in the hemisphere contralateral to the tapping hand are assessed as being due to the activation. Of the possible patterns of signal changes, 90% include a positive ΔC′oxy, 76% included a negative ΔC′deoxy, and 73% included a positive ΔC′total. The ΔC′deoxy and ΔC′total are less consistent because of a large intersubject variability in ΔC′deoxy; in some cases there is a positive ΔC′deoxy. In the cases with no positive ΔC′oxy in the contralateral hemisphere, there are cases of other possible changes for either or both hemispheres and no cases of no change in any hemoglobin species in either hemisphere. These results suggest that NIR topography is useful for observing brain activity in most cases, although intersubject signal variability still needs to be resolved.

1.

Introduction

Near-infrared spectroscopy (NIRS) was first developed for noninvasive monitoring of cerebral oxygenation.1, 2 Later, its ability to measure the secondary metabolic signals accompanying neural activities was demonstrated.3, 4, 5, 6, 7 Cortical activation can be assessed by calculating the product of the concentration change and the effective optical path length for oxygenated hemoglobin (ΔCoxy) and deoxygenated hemoglobin (ΔCdeoxy) and their sum (ΔCtotal) in the cerebral cortex. A near-infrared (NIR) topography with multiple measurement positions was developed from the NIRS technique as a noninvasive modality for functional mapping.8, 9, 10, 11 It has been gaining wide acceptance12, 13, 14, 15, 16, 17, 18, 19, 20, 21, 22 due to its noninvasiveness, handiness, and measurability without subject constraint. These advantages even make it possible to measure brain functions in healthy infants.12, 13, 20, 23

While methods to obtain absolute concentration changes multiplied by the mean optical path length (which can be estimated using time-resolved measurement) have been suggested,24, 25, 26 it is inappropriate to use the mean path length as an alternative to the effective path length in the activation region.27, 28 We therefore use the product of the effective optical path length and the concentration change in the hemoglobin species ( ΔCoxy , ΔCdeoxy , and ΔCtotal ) as the NIRS signals. The ability of NIRS to measure ΔCoxy and ΔCdeoxy individually is an important advantage compared with one representative imaging method—blood oxygenation level-dependent functional magnetic resonance imaging (BOLD fMRI), which measures the relative changes in only the paramagnetic deoxygenated hemoglobin that accompany oxygenation changes in the blood. NIRS is thus useful for examining the circulatory basis of brain activation.

The relationship between neural activity and hemodynamic changes, which cause changes in both the BOLD signal and NIRS signals, is an important issue in neuroscience. In general, the intensity of the BOLD signal increases with functional activation, which corresponds to a negative ΔCdeoxy ,29, 30 and NIRS techniques have usually detected a positive ΔCoxy and a negative ΔCdeoxy during a variety of stimulus paradigms.3, 5, 11, 21, 30, 31, 32 However, contrary to the general understanding, a drop in the BOLD signal in fMRI studies33, 34 and a negative ΔCoxy , together with a positive ΔCdeoxy in NIRS studies,5, 30, 35 have been reported. In addition, increases in all hemoglobin species have been observed in some NIRS studies.6, 22, 36, 37 Moreover, Seiyama et al. had conducted simultaneous fMRI and NIRS measurements and used NIRS function to explain the variability in the BOLD signal (increase, decrease, or no change) during cortical activation.35 Although there are various patterns in the physiological changes caused by brain activation, they have not been classified, and their occurrence probabilities are still unknown, as are the pattern mechanisms.

In the present study, we examined how activation patterns, measured using NIRS, in the same cortical area vary among healthy adults with the aim of validating NIR topography for functional mapping and for explaining the circulation mechanisms in brain activation. The NIRS signals ( ΔCoxy , ΔCdeoxy , and ΔCtotal ) may be affected by anatomical variability such as thicknesses of skull and cerebrospinal fluid (CSF) layers as suggested by previous studies,27, 28 and the wavelength dependence of sensitivity may cause a cross talk effect between ΔCoxy and ΔCdeoxy .38, 39, 40 However, the NIRS technique cannot provide anatomical information and there is no technique that specifies optical property for each layer of head in vivo, thus it is not possible to estimate the exact cross talk effect in practice. Therefore, to improve the existing method, we first need to assess the consistency of NIRS activation signals among a larger number of subjects.

We measured the activity in the sensorimotor cortex of 31 adults performing a simple sensorimotor task and evaluated the NIRS signals using a statistical analysis method. Sensorimotor cortex activation has already been investigated by a number of functional studies using positron emission tomography (PET),41, 42 fMRI,43, 44 and NIRS.11, 32 This study aims to provide a useful database that can be used for application of the NIR topography in both clinical and research fields. A portion of this study has been reported in abstract form.45

2.

Materials and Methods

2.1.

Subjects

31 healthy adults (21 men, 10 women; mean age 34±8.9 , range 23 to 56) gave written informed consent before the experiments. All the subjects showed right-handedness except one, and none reported a history of neurological disorders.

2.2.

NIRS Measurement

An NIR topography system with 24 measurement positions (ETG-100, Hitachi Medical Corporation, Japan) was used. The system irradiates light at 780- and 830-nm wavelength through an optical fiber to the same measurement point simultaneously. The reflected light was detected every 100ms using an avalanche photodiode (APD) located 30mm from the incident position.

We regarded the midpoint of the source-detector distance as the measurement position because the sensitivity of NIRS to chromophore-concentration changes is highest there.46, 47, 48 Optical fibers were used for both the irradiating and detecting the lights. The average power of each light source was 1.5mW , and each source was modulated at a distinctive frequency (1.0to10kHz) to enable separation using a lock-in amplifier after detection. Ten irradiated positions and eight detection positions were configured to measure the 24 positions (Fig. 1 ).

Fig. 1

Arrangement of measurement positions in probe patterns over left and right sensorimotor areas centered on locations C3 and C4, respectively.

044001_1_005504jbo1.jpg

The measurement area was determined for each subject based on the international 10–20 system.49 We measured an area of 6×6cm in the left and right parietal areas centered on C3 and C4 , respectively (Fig. 1). The 6×6-cm square was defined as the measurement area for each hemisphere based on the arrangement of optical fibers (irradiation and detection positions). The probe patterns were positioned parallel to the line connecting Cz to T3 (left hemisphere) or T4 (right hemisphere). The centers of the bilateral measurement areas were considered to correspond to each primary sensorimotor area based on previous studies examining the relationship between the international 10–20 locations and cortical area.50, 51, 52 In particular, Okamoto et al. recently reported that the C3 and C4 locations correspond to the central fissure with a standard deviation of less than 10mm among 17 Mongoloids,50 the same race as our subjects.

2.3.

Task Paradigm

The sensorimotor cortices were activated using a finger-tapping task. The fingers of one hand were placed on the tip of the thumb in serial order (forefinger, second finger, third finger, little finger, third finger, second finger, forefinger). The subjects were asked to repeat the tapping sequence at 3Hz timed to the rate of the term “finger tapping” blinking on a CRT monitor for 30s (activation) followed by 30s of rest (baseline). There were a total of five activation/baseline cycles per session. Two sessions of finger tapping (one left-hand tapping and one right-hand tapping) were conducted per subject in a counterbalanced order among subjects. During the measurements, the subject sat on a chair and was instructed to fix his or her gaze on the fixation point at the center of the screen and to concentrate on the task.

2.4.

Data Analysis

We defined a period of 55s , consisting of a 5-s prestimulation resting period, a 30-s stimulation period in the finger-tapping state, and a 20-s poststimulation resting period as one (task) block. The detected temporal data for the attenuation change at each wavelength were separated into five blocks. Each block was baseline corrected using the data for the pre- and poststimulation periods; the products of the effective optical path length and the concentration changes of the independent hemoglobin species ( ΔCoxy and ΔCdeoxy ) were calculated by applying the modified Beer-Lambert Law11 as follows:

Eq. 1

ΔCoxy=LΔCoxy=εdeoxy(λ2)ΔA(λ1)+εdeoxy(λ1)ΔA(λ2)E,

Eq. 2

ΔCdeoxy=LΔCdeoxy=εoxy(λ2)ΔA(λ1)εoxy(λ1)ΔA(λ2)E,
where

Eq. 3

E=εdeoxy(λ1)εoxy(λ2)εdeoxy(λ2)εoxy(λ1).
ΔCoxy and ΔCdeoxy are expressed as the indefinite effective optical path length in the activation region (L) multiplied by the concentration change ( ΔCoxy and ΔCdeoxy ). The ΔA , εoxy , and εdeoxy indicate the logarithm of the intensity change in the detected light, the absorption coefficient of the oxygenated hemoglobin, and that of the deoxygenated hemoglobin, respectively, for two wavelengths (λ1,λ2) . Note that we assume that the path length is equal for every wavelength because accurate estimation of L is almost impossible with the current technique.

The activation signals were statistically assessed. Assuming that the hemodynamic time courses induced by the task varied among the subjects, we defined a 25-s activation period for each subject. We used a within-subject averaged time course over the five blocks to select the one 25-s activation period with maximum absolute value of the mean change for each hemoglobin species. The 25-s activation period was allowed to shift from the initial 5s after task onset to starting 15s after task onset; the earliest period was from 5s after task onset to task completion, and the latest period was from 15s after task onset to 10s after task completion (Fig. 2 ).

Fig. 2

Schematic diagram of analysis parameters for a task block. Mean value of 5s for prestimulation (R) and mean value of 25s for activation (A) were used for statistical analysis. Note that A could shift from 5s after task onset to 10s after task completion, depending on the maximum absolute value for each case.

044001_1_005504jbo2.jpg

The mean changes in hemoglobin during the prestimulation period and those during the activation period were calculated for each block. We calculated the t value (paired t test) between the mean hemoglobin changes in the prestimulation periods of five blocks and those in the activation periods of the same five blocks, and identified measurement positions with significant t values (two-tailed t test, p<0.1 ) as activation points.14, 36 We determined the threshold for each NIRS signal ( ΔCoxy , ΔCdeoxy , and ΔCtotal ). This statistical analysis was designed to determine the consistency (reproducibility) of changes for the five activation periods. With this analysis, causeless changes are not detected as activation because the statistical value does not reach the threshold unless similar changes arise in every (or almost every) activation period. In addition, using activation periods 25s long reduces the possibility of misidentifying an increase or decrease due to spontaneous oscillations during a cycle of around 10 as activation.53 Moreover, a t test using the variance of the mean value in the resting period and that in the activation period across task blocks reduces the effect of high-frequency system noise. Note that although the determination of the activation period based on the peak timing differs from the analytical method we used in our previous report,45 these differences in the results were negligible.

3.

Results

3.1.

Occurrence Probability of Typical Activation Pattern

We assessed the occurrence probability of the typical activation pattern (positive ΔCoxy , negative ΔCdeoxy , and positive ΔCtotal ) for each measurement-position (Fig. 3 ). Positive ΔCoxy and ΔCtotal in the hemisphere contralateral to the tapping hand were observed with high probability. In addition, the measurement positions with high probabilities were around the center of the measurement area (left hemisphere: positions 6 and 9; right hemisphere: position 16). Contrary to that, negative ΔCdeoxy as a whole showed less probability, although the activation centers were almost the same as those for ΔCoxy and ΔCtotal (left hemisphere: position 9; right hemisphere: position 16). The mean signal amplitudes for subjects who showed the typical activation pattern are given in Table 1 . The mean amplitudes for ΔCoxy and ΔCtotal were 0.109 and 0.104mMmm , respectively, while that for ΔCdeoxy was about half (0.048mMmm) . The amplitudes sometimes varied widely among subjects, from small [Fig. 4(a) ] to large [Fig. 4(b)].

Fig. 4

Representative time courses of ΔCoxy , ΔCdeoxy , and ΔCtotal . Typical pattern (positive ΔCoxy , negative ΔCdeoxy , and positive ΔCtotal ) is shown in (a) and (b); changes in (b) are larger than those in (a). An all-positive pattern (positive ΔCoxy , ΔCdeoxy , and ΔCtotal ) is shown in (c) and (d). Pattern in (d) was a rare case— ΔCdeoxy was positive similar to ΔCoxy . Two exceptional patterns are shown in (e) and (f). The pattern with only a negative ΔCdeoxy , (e), was observed in only two subjects. The pattern with a negative ΔCoxy and a positive ΔCdeoxy , (f), was observed in only one subject.

044001_1_005504jbo4.jpg

Fig. 3

Color maps of occurrence probabilities of typical activation pattern (positive ΔCoxy , negative ΔCdeoxy , and positive ΔCtotal ) for each measurement position.

044001_1_005504jbo3.jpg

Table 1

Mean signal amplitude of each hemoglobin species among subjects who showed typical activation pattern (positive ΔCoxy′ , negative ΔCdeoxy′ , positive ΔCtotal′ ). An activation position with the highest signal amplitude within the contralateral hemisphere to the tapping hand for each subject was used.

ΔCoxy′ ΔCdeoxy′ ΔCtotal′
Mean signal amplitude ±SD (mMmm) 0.109±0.063 0.047±0.026 0.104±0.056

The numbers of subjects who showed a significant ΔCoxy , ΔCdeoxy , or ΔCtotal (either positive or negative) for the hemisphere contralateral to the tapping hand are shown in Table 2 . The most common change was a positive ΔCoxy (90%; left hemisphere 2831 , right hemisphere 2831 ). Moreover, in 91% of the subjects showing this change, at least one of the four measurement positions in the central area (left hemisphere: positions 4, 6, 7, and 9; right hemisphere: positions 16, 18, 19, and 21) was included. A negative ΔCdeoxy and a positive ΔCtotal were less frequently observed ( ΔCdeoxy : 76%, left hemisphere 2431 , right hemisphere 2331 ; ΔCtotal : 73%, left hemisphere 2331 , right hemisphere 2231 ). In 91% of the subjects showing a negative ΔCdeoxy and in 89% of the ones showing a positive ΔCtotal , at least one of the four measurement positions in the central area was included. Although ΔCdeoxy was generally negative, 16% of the subjects showed a positive ΔCdeoxy . A negative ΔCoxy was observed for only one subject for the hemisphere contralateral to the tapping hand.

Table 2

Number of subjects (out of 31) who showed a significant ΔCoxy′ , ΔCdeoxy′ , or ΔCtotal′ (two-tailed t test, p<0.1 ). Numbers in () show the number of subjects having a significant change at measurement positions in the central area (left hemisphere: positions 4, 6, 7, 9; right hemisphere: positions 16, 18, 19, 21).

Left hemisphere(right-hand tapping)Right hemisphere(left-hand tapping)
ΔCoxy Positive28 (25)28 (26)
Negative1(1)1(0)
Insignificant22
ΔCdeoxy Positive3 (3)7 (1)
Negative24 (21)23 (22)
Insignificant41
ΔCtotal Positive23 (22)22 (18)
Negative4 (3)3 (1)
Insignificant46

3.2.

Variability of Activation Pattern

To determine the relationships among ΔCoxy , ΔCdeoxy , and ΔCtotal in detail, we classified the various patterns of combination. The patterns and appearance frequencies are shown in Table 3 . Note that a significance threshold was set for each NIRS signal, so a significant change in one signal ( ΔCoxy or ΔCdeoxy ) will not result in a significant change in ΔCtotal (sum of ΔCoxy and ΔCdeoxy ) due to a subthreshold change (noise) in the other signal.

Table 3

Patterns of hemoglobin changes and their occurrence rate among 31 subjects.  *1 ↑ increase, ↓ decrease, -subthreshold change. The changes were assessed using a two-tailed t test (p<0.1) . When both changes appeared for one condition, the change for more measurement positions was used; when both changes appeared for the same number of measurement positions, the change with the maximum t value (absolute value) was used.  *2 A subject’s change characterized by positive ΔCdeoxy′ and negative ΔCoxy′ in the right hemisphere during both-hand tapping [Fig. 4(f)]. The subject showed only a negative ΔCoxy′ in the left hemisphere during right-hand taping (↓--), but a similar pattern of a negative ΔCoxy′ and a positive ΔCdeoxy′ was observed in the right (ipsilateral) hemisphere.  *3 Three cases including both hemispheres of one subject. ΔCdeoxy′ was consistently negative, though ΔCoxy′ tended to be noisy.  *4 The pattern with a positive ΔCdeoxy′ only in the right hemisphere (-↑-), while the subject showed all-positive pattern (↑ ↑ ↑) in the left (ipsilateral) hemisphere.

Change pattern*1 Left Hemisphere(Right-hand tapping)Right Hemisphere(Left-hand tapping)
ΔCoxy′ ΔCdeoxy′ ΔCtotal′
1817
23
-22
35
00
-00
-20
-00
--11
00
00
-00
00
00
-0 1*2
-00
-00
-- 1*2 0
-00
-00
-- 2*3 1*3
-00
-00
--0 1*4
--00
--00
---00
Total3131

The most common pattern (positive ΔCoxy , negative ΔCdeoxy , positive ΔCtotal ; ↑↓↑ in Table 3) was shown in 18 and 17 subjects (total 56%) for the left and right hemispheres, respectively. Similar to the most common pattern, the patterns in which ΔCoxy was positive and ΔCdeoxy was negative without a positive ΔCtotal (↑↓↓ and ↑↓-) were seen in four and five subjects (total 15%) for the left and right hemispheres, respectively. In addition, positive ΔCoxy and ΔCtotal with subthreshold ΔCdeoxy (↑-↑) and a positive ΔCoxy with subthreshold ΔCdeoxy and ΔCtotal (↑--) were observed in four and one subjects (total 6%) for the left and right hemispheres, respectively.

Another frequent pattern was the all-positive pattern (↑↑↑ in Table 3), which was observed in three and five subjects (total 13%) for the left and right hemispheres, respectively. There were mainly two types of changes in this pattern; a general type showed a strong positive ΔCoxy and ΔCtotal with a positive ΔCdeoxy [Fig. 4(c)], and a singular type that showed a strong positive ΔCoxy and ΔCdeoxy , resulting in a stronger positive ΔCtotal [Fig. 4(d)].

A significant characteristic of all these patterns was a positive ΔCoxy , which was observed in 90% of the cases.

The 10% that did not show a positive ΔCoxy were grouped into three patterns; the first is the pattern with a negative ΔCoxy and a positive ΔCdeoxy in the right hemisphere during left tapping [Fig. 4(f); ↓↑- in Table 3]. In addition, the same subject showed only a negative ΔCoxy in the left hemisphere during right-hand tapping (↓--), but a similar pattern of a negative ΔCoxy and a positive ΔCdeoxy was observed in the right (ipsilateral) hemisphere. We therefore classified the changes for this subject as the same pattern. Another is the pattern with a negative ΔCdeoxy only [Fig. 4(e); -↓-]. This pattern was observed in two subjects (both hemispheres in one; one hemisphere in the other). The last is the pattern with a positive ΔCdeoxy only in the right hemisphere (-↑-) while the subject showed all-positive pattern (↑↑↑) in the left (ipsilateral) hemisphere [Fig. 4(d)]. Note that in every case of these three patterns there was a hemoglobin change in at least one of the hemispheres.

4.

Discussion

4.1.

Occurrence Probability of Typical Activation Pattern

First, we examined the occurrence probability of the typical activation pattern (positive ΔCoxy , negative ΔCdeoxy , and positive ΔCtotal ) in the hemisphere contralateral to the tapping hand. These physiological changes were consistent with the accepted theory29, 30 and previous NIRS studies.11, 32 The occurrence probabilities in a previous study32 were nearly consistent with our results for both ΔCoxy (about 89% in the previous study and 90% in ours) and ΔCdeoxy (about 84% in the previous study and 76% in ours). Moreover, the combination of a positive ΔCoxy and a negative ΔCdeoxy was observed in 73 and 71% of the cases for the previous and present study, respectively.

Our results showed that a negative ΔCdeoxy was observed less frequently in the activation center than positive ΔCoxy and ΔCtotal (Fig. 3; left hemisphere: position 9; right hemisphere: position 16). This could be due to the smaller total number of ΔCdeoxy activation positions compared to the other hemoglobin species for each subject, which is supported by our finding that the number of subjects with positive ΔCdeoxy did not differ much from those with positive ΔCtotal (Table 2).

One possible reason for this is the effect of systemic changes on the responses of ΔCoxy and ΔCtotal . It has been suggested that a finger-tapping task can lead to systemic changes in blood pressure and heart rate that affect measurements of ΔCoxy in particular.54, 55 Both ΔCoxy and ΔCtotal had a larger activation area, i.e., they were measured at more positions, while the activation area for ΔCdeoxy was more focused. While monitoring the systemic effects and using an analytical method that subtracts the effects from the signals would be ideal,54 a more practical approach may be to design a task paradigm that does not induce systemic variance between the rest period and task period.

Although it was difficult to distinguish the systemic effects from the cortical response in this study, the activation area for ΔCdeoxy may actually have been smaller than those for ΔCoxy and ΔCtotal for most subjects. A previous study of simultaneous recordings of fMRI and NIRS signals suggests that ΔCdeoxy provides more specific information for focal cerebral responses than ΔCoxy .56 Moreover, another study of simultaneous recordings showed that an activation map using ΔCoxy did not overlap maps using ΔCdeoxy and BOLD signals.35 Further study of the spatial and temporal diversities between the two signals ( ΔCoxy and ΔCdeoxy ) is thus important. Higher spatial resolution, however, will be needed before NIR topography can be used to analyze the activation centers accurately.

We also observed that the probable positions of highest activation differed between the left (position 9) and right hemisphere (position 16). Possible reasons for this longitudinal asymmetry of the highest activation positions are a methodological problem and an anatomical characteristic of the cerebral cortex. The methodological problem is possible inaccurate placement of the measurement probes, since we placed them by hand though we did determine the positions according to the international 10–20 system. We need to develop a better method for accurate positioning. The anatomical characteristic is possible asymmetry due to the anatomical asymmetry of the cerebral cortex. According to a previous study,57 the parietal and temporal cortices of the left hemisphere are larger than those of the right hemisphere in most subjects. As a result, even though the probes are placed symmetrically on the head surface, they may actually be shifted upward in relation to the cerebral cortex. A placement error of only a few millimeters can mislead the peak activation position to the next measurement position when the investigated area is placed at the center of the measurement area surrounded by four measurement positions.46

Even with this possible low spatial resolution, our finding that measurement positions with high activation probabilities were around the center of the measurement area (left hemisphere: positions 4, 6, 7, and 9; right hemisphere: positions 16, 18, 19, and 21) suggests that the 10–20 international system is useful in determining the measurement area for NIR topography.

Examination of the activation probabilities in detail (Table 2) shows that a negative ΔCdeoxy , which can cause the typical BOLD signal pattern, was not as consistently observed (negative 76%, positive 16%) as a positive ΔCoxy (positive 90%, negative 3%). This peculiar feature of ΔCdeoxy —the possibility of it being positive or negative—might be another reason for the less-focused activation in ΔCdeoxy . Our results suggest that the ΔCdeoxy signal can occasionally vary not only in amplitude but also in direction, which conflicts with the common idea of BOLD fMRI.

The variable behavior of ΔCdeoxy may be due to the variability of the cross talk effect39, 40 among subjects; however, it is not possible to estimate the actual cross talk effect for an individual. Although we used a wavelength pair of 780 and 830nm , which is not an optimal wavelength pair (e.g., 690 and 830nm ) for reducing the cross talk effect, as suggested by some simulation studies,38, 58 we did previously determine that the primary shape of the activation signal (positive change or negative change) does not depend on the wavelength pair (either 692 and 830nm or 782 and 830nm ).45 We therefore think the variability of ΔCdeoxy was not due solely to the wavelengths used.

Another possibility is that the variability in ΔCdeoxy reflects some physiological phenomena relating to brain activation, since unusual behavior in the ΔCdeoxy or the BOLD signal has been previously reported.30, 33 The variability of hemodynamic responses is normally considered to be dependent on several factors such as cerebral blood flow (CBF), cerebral blood volume (CBV), and oxygen consumption rate (CMRO2) .35 One previous study showed positive, negative, and silent BOLD signals with a negative, positive, and subthreshold ΔCdeoxy , respectively, while ΔCoxy showed various behaviors by simultaneous measurement of fMRI and NIRS.35 Another study demonstrated positive ΔCoxy and ΔCdeoxy in the capillary area along with a negative ΔCdeoxy and positive ΔCoxy in the large vein area.37

4.2.

Variability of Activation Pattern

Next, we examined the various patterns in more detail using classification analysis for the various combinations of hemoglobin changes (Table 3). We considered the patterns with a positive ΔCoxy and without a positive ΔCdeoxy (↑ ↓ ↓, ↑ ↓-, and ↑-↑ in Table 3) to be the same as the most common pattern (↑ ↓ ↑) seen in this study. These patterns were observed in 25 and 23 subjects (77%) for the left and right hemispheres, respectively. As mentioned before, the variety of patterns for ΔCdeoxy and ΔCtotal could depend on CBF, CBV, and CMRO2 29, 30, 33 and on the proportions of the capillary and large vein areas in the measurement region.37 Simulation studies in which the proportions of these factors were changed might be useful in determining the physiological mechanism leading to each pattern. In addition, the cross talk effect due to anatomical characteristics or different SNRs in the ΔCdeoxy signal may have resulted in the pattern with subthreshold ΔCdeoxy (↑-↑).

The all-positive pattern (↑↑↑ in Table 3), which was occasionally observed (13%), was also reported in a number of previous NIRS studies.6, 22, 37 In one of the previous studies, this pattern occurred in capillary areas such as the inferior frontal gyrus (Broca’s area), while the common pattern with a negative ΔCdeoxy occurred in large vein areas such as the superior temporal area.37 If the variability of the hemodynamics depends on the distribution of the vascular system, there could be a large variability in the distributive condition of vessels among subjects, even for the same cortical area.

Our observation on both the common pattern and the all-positive pattern in the same cortical area during the same activation paradigm suggests that the variation in hemoglobin changes depends on the subject’s anatomical characteristics and condition rather than the characteristics of the measurement area or the paradigm.

The patterns described earlier showing a positive ΔCoxy were observed in 90% of the subjects. This suggests high reliability of ΔCoxy as an activation signal, whereas some previous studies used only ΔCtotal to identify cognitive-related activation.13, 16, 17

The other 10% are interpreted as follows: an atypical pattern with a positive ΔCdeoxy [Fig. 4(f); ↓↑ - and - ↑ - in Table 3] was observed in one subject. The combination pattern, which is similar to the deactivation in fMRI30, 33, 34, 35 and PET,59, 60 possibly appears when CMRO2 significantly increases during activation.35 Another possibility for this pattern is that the signal pattern showed blood stealing or neural suppression due to neighboring activation, but the reason only deactivation could be observed remains unexplained. Another is the pattern with a negative ΔCdeoxy only [Fig. 4(e); - ↓ - in Table 3], which was observed in two subjects (both hemispheres in one; one hemisphere in the other). This pattern might result from less sensitivity for ΔCoxy . While the ΔCoxy signal tended to increase more, the level did not reach the statistical threshold for these subjects. This is possibly due to greater noise in the ΔCoxy signal than in the ΔCdeoxy one. Physiological noise, such as low frequency oscillations53 or systemic changes,54, 55 can have more effect on ΔCoxy than on ΔCdeoxy . Although it may be possible to subtract the systemic changes from NIRS signals by using simultaneously recorded data for the arterial saturation and heart rate,54 simultaneous measurements of these physiological signals with NIRS is difficult.

Another pattern was a positive ΔCdeoxy only in the right hemisphere (-↑-in Table 3) during left-hand tapping, while this subject showed an all-positive pattern (↑ ↑ ↑) in the ipsilateral (left) hemisphere as well as during contralateral right-hand tapping [Fig. 4(d)]. While activation in both hemispheres during unilateral finger movement has been reported,61, 62 predominant activation in the ipsilateral one rarely occurs in normal adults. Further examination with anatomical imaging will be necessary to explain this unusual lateralization.

5.

Conclusion

We study the variability of NIRS signals induced by sensorimotor activation in 31 healthy subjects using NIR topography. Activation patterns with a positive ΔCoxy for the hemisphere contralateral to the tapping hand were observed with high probability (90%). Moreover, every other case showed other significant changes for either or both hemispheres, suggesting that NIR topography is useful for observing brain activity in most cases. In addition, our finding that activation positions tended to be around the center of the measurement area demonstrated the effectiveness of the 10–20 international system for determining the measurement positions.

Although this study evaluated NIRS signals that may have been affected by cross talk, intersubject anatomical variation, and systemic changes accompanying the task, we believe that it is important to evaluate the variability of NIRS signals in spite of these effects, because the NIRS technique has been widely used in its present state and improvements in the technique will come with its usage.

Relating the activation patterns to the anatomical characteristics of the subjects requires further examination of the anatomical variability among subjects and its effects on NIRS signals as well as the development of better techniques. In addition, further experiments under a wider variety of conditions for the measurement area, task paradigm, and subject group will be helpful for understanding the activation patterns. Moreover, invasive animal studies may be needed to generate a more sophisticated theory explaining the physiological mechanism of these various activation patterns.

Acknowledgments

We thank Eiju Watanabe, Naoki Tanaka, Tsuyoshi Yamamoto, Fumio Kawaguchi, and Michiyuki Fujiwara for their helpful suggestions; Yukari Yamamoto, Akiko Obata, Hirokazu Atsumori, and Peck Hui Koh for their technical assistance; and Hideo Kawaguchi, Noriyuki Ichikawa, and Nobuyuki Osakabe for their general support.

References

1. 

S. Wray, M. Cope, D. T. Delpy, J. S. Wyatt, and E. O. Reynolds, “Characterization of the near infrared absorption spectra of cytochrome aa3 and haemoglobin for the non-invasive monitoring of cerebral oxygenation,” Biochim. Biophys. Acta, 933 (1), 184 –192 (1988). https://doi.org/10.1016/0005-2728(88)90069-2 0006-3002 Google Scholar

2. 

F. F. Jobsis-VanderVliet, C. A. Piantadosi, A. L. Sylvia, S. K. Lucas, and H. H. Keizer, “Near-infrared monitoring of cerebral oxygen sufficiency. 1. Spectra of cytochrome c oxidase,” Neurol. Res., 10 (1), 7 –17 (1988). 0160-6412 Google Scholar

3. 

A. Villringer, J. Planck, C. Hock, L. Schleinkofer, and U. Dirnagl, “Near infrared spectroscopy (NIRS): a new tool to study hemodynamic changes during activation of brain function in human adults,” Neurosci. Lett., 154 (1–2), 101 –104 (1993). https://doi.org/10.1016/0304-3940(93)90181-J 0304-3940 Google Scholar

4. 

T. Kato, A. Kamei, S. Takashima, and T. Ozaki, “Human visual cortical function during photic stimulation monitoring by means of near-infrared spectroscopy,” J. Cereb. Blood Flow Metab., 13 (3), 516 –520 (1993). 0271-678X Google Scholar

5. 

Y. Hoshi and M. Tamura, “Detection of dynamic changes in cerebral oxygenation coupled to neuronal function during mental work in man,” Neurosci. Lett., 150 (1), 5 –8 (1993). https://doi.org/10.1016/0304-3940(93)90094-2 0304-3940 Google Scholar

6. 

Y. Hoshi and M. Tamura, “Dynamic multichannel near-infrared optical imaging of human brain activity,” J. Appl. Physiol., 75 (4), 1842 –1846 (1993). 8750-7587 Google Scholar

7. 

B. Chance, Z. Zhuang, C. UnAh, C. Alter, and L. Lipton, “Cognition-activated low-frequency modulation of light absorption in human brain,” Proc. Natl. Acad. Sci. U.S.A., 90 (8), 3770 –3774 (1993). 0027-8424 Google Scholar

8. 

H. Koizumi, Y. Yamashita, A. Maki, T. Yamamoto, Y. Ito, H. Itagaki, and R. P. Kennan, “Higher-order brain function analysis by trans-cranial dynamic near-infrared spectroscopy imaging,” J. Biomed. Opt., 4 (4), 403 –413 (1999). https://doi.org/10.1117/1.429959 1083-3668 Google Scholar

9. 

Y. Yamashita, A. Maki, Y. Ito, E. Watanabe, H. Mayanagi, and H. Koizumi, “Noninvasive near-infrared topography of human brain activity using intensity modulation spectroscopy,” Opt. Eng., 35 (4), 1046 –1099 (1996). 0091-3286 Google Scholar

10. 

A. Maki, Y. Yamashita, E. Watanabe, and H. Koizumi, “Visualizing human motor activity by using non-invasive optical topography,” Front Med. Biol. Eng., 7 (4), 285 –297 (1996). 0921-3775 Google Scholar

11. 

A. Maki, Y. Yamashita, Y. Ito, E. Watanabe, Y. Mayanagi, and H. Koizumi, “Spatial and temporal analysis of human motor activity using noninvasive NIR topography,” Med. Phys., 22 (12), 1997 –2005 (1995). https://doi.org/10.1118/1.597496 0094-2405 Google Scholar

12. 

G. Taga, K. Asakawa, A. Maki, Y. Konishi, and H. Koizumi, “Brain imaging in awake infants by near-infrared optical topography,” Proc. Natl. Acad. Sci. U.S.A., 100 (19), 10722 –10727 (2003). https://doi.org/10.1073/pnas.1932552100 0027-8424 Google Scholar

13. 

M. Pena, A. Maki, D. Kovacic, G. Dehaene-Lambertz, H. Koizumi, F. Bouquet, and J. Mehler, “Sounds and silence: an optical topography study of language recognition at birth,” Proc. Natl. Acad. Sci. U.S.A., 100 (20), 11702 –11705 (2003). https://doi.org/10.1073/pnas.1934290100 0027-8424 Google Scholar

14. 

A. Obata, K. Morimoto, H. Sato, A. Maki, and H. Koizumi, “Acute effects of alcohol on hemodynamic changes during visual stimulation assessed using 24-channel near-infrared spectroscopy,” Psychiatry Res., 123 (2), 145 –152 (2003). 0165-1781 Google Scholar

15. 

Y. Noguchi, T. Takeuchi, and K. L. Sakai, “Lateralized activation in the inferior frontal cortex during syntactic processing: event-related optical topography study,” Hum. Brain Mapp, 17 (2), 89 –99 (2002). https://doi.org/10.1016/S0263-7863(98)00016-7 1065-9471 Google Scholar

16. 

Y. Minagawa-Kawai, K. Mori, I. Furuya, R. Hayashi, and Y. Sato, “Assessing cerebral representations of short and long vowel categories by NIRS,” NeuroReport, 13 (5), 581 –584 (2002). 0959-4965 Google Scholar

17. 

R. P. Kennan, D. Kim, A. Maki, H. Koizumi, and R. T. Constable, “Non-invasive assessment of language lateralization by transcranial near infrared optical topography and functional MRI,” Hum. Brain Mapp, 16 (3), 183 –189 (2002). 1065-9471 Google Scholar

18. 

R. P. Kennan, S. G. Horovitz, A. Maki, Y. Yamashita, H. Koizumi, and J. C. Gore, “Simultaneous recording of event-related auditory oddball response using transcranial near infrared optical topography and surface EEG,” Neuroimage, 16 (3 Pt 1), 587 –592 (2002). 1053-8119 Google Scholar

19. 

E. Watanabe, A. Maki, F. Kawaguchi, Y. Yamashita, H. Koizumi, and Y. Mayanagi, “Noninvasive cerebral blood volume measurement during seizures using multichannel near infrared spectroscopic topography,” J. Biomed. Opt., 5 (3), 287 –290 (2000). https://doi.org/10.1117/1.429998 1083-3668 Google Scholar

20. 

G. Taga, Y. Konishi, A. Maki, T. Tachibana, M. Fujiwara, and H. Koizumi, “Spontaneous oscillation of oxy- and deoxy- hemoglobin changes with a phase difference throughout the occipital cortex of newborn infants observed using non-invasive optical topography,” Neurosci. Lett., 282 (1–2), 101 –104 (2000). https://doi.org/10.1016/S0304-3940(00)00874-0 0304-3940 Google Scholar

21. 

H. Sato, T. Takeuchi, and K. L. Sakai, “Temporal cortex activation during speech recognition: an optical topography study,” Cognition, 73 (3), B55 –66 (1999). 0010-0277 Google Scholar

22. 

E. Watanabe, A. Maki, F. Kawaguchi, K. Takashiro, Y. Yamashita, H. Koizumi, and Y. Mayanagi, “Non-invasive assessment of language dominance with near-infrared spectroscopic mapping,” Neurosci. Lett., 256 (1), 49 –52 (1998). https://doi.org/10.1016/S0304-3940(98)00754-X 0304-3940 Google Scholar

23. 

J. C. Hebden, “Advances in optical imaging of the newborn infant brain,” Psychophysiology, 40 (4), 501 –510 (2003). https://doi.org/10.1111/1469-8986.00052 0048-5772 Google Scholar

24. 

J. S. Wyatt, M. Cope, D. T. Delpy, C. E. Richardson, A. D. Edwards, S. Wray, and E. O. Reynolds, “Quantitation of cerebral blood volume in human infants by near-infrared spectroscopy,” J. Appl. Physiol., 68 (3), 1086 –1091 (1990). 8750-7587 Google Scholar

25. 

D. T. Delpy, S. R. Arridge, M. Cope, D. Edwards, E. O. Reynolds, C. E. Richardson, S. Wray, J. Wyatt, and P. van der Zee, “Quantitation of pathlength in optical spectroscopy,” Adv. Exp. Med. Biol., 248 41 –46 (1989). 0065-2598 Google Scholar

26. 

D. T. Delpy, M. Cope, P. van der Zee, S. Arridge, S. Wray, and J. Wyatt, “Estimation of optical pathlength through tissue from direct time of flight measurement,” Phys. Med. Biol., 33 (12), 1433 –1442 (1988). https://doi.org/10.1088/0031-9155/33/12/008 0031-9155 Google Scholar

27. 

E. Okada and D. T. Delpy, “Near-infrared light propagation in an adult head model. 1. Modeling of low-level scattering in the cerebrospinal fluid layer,” Appl. Opt., 42 (16), 2906 –2914 (2003). 0003-6935 Google Scholar

28. 

E. Okada and D. T. Delpy, “Near-infrared light propagation in an adult head model. 2. Effect of superficial tissue thickness on the sensitivity of the near-infrared spectroscopy signal,” Appl. Opt., 42 (16), 2915 –2922 (2003). 0003-6935 Google Scholar

29. 

U. Dirnagl, L. Edvinsson, and A. Villringer, “Measuring cerebral blood flow and metabolism,” Cerebral Blood Flow and Metabolism, 371 –383 Lippincott Williams & Wilkins, Philadelphia, PA (2002). Google Scholar

30. 

A. Villringer, “Physiological changes during brain activation,” Functional MRI, 3 –13 Springer, Berlin (1999). Google Scholar

31. 

H. Obrig, R. Wenzel, M. Kohl, S. Horst, P. Wobst, J. Steinbrink, F. Thomas, and A. Villringer, “Near-infrared spectroscopy: does it function in functional activation studies of the adult brain?,” Int. J. Psychophysiol, 35 (2–3), 125 –142 (2000). 0167-8760 Google Scholar

32. 

H. Obrig, C. Hirth, J. G. Junge-Hulsing, C. Doge, T. Wolf, U. Dirnagl, and A. Villringer, “Cerebral oxygenation changes in response to motor stimulation,” J. Appl. Physiol., 81 (3), 1174 –1183 (1996). 8750-7587 Google Scholar

33. 

A. Shmuel, E. Yacoub, J. Pfeuffer, P. F. Van de Moortele, G. Adriany, X. Hu, and K. Ugurbil, “Sustained negative BOLD, blood flow and oxygen consumption response and its coupling to the positive response in the human brain,” Neuron, 36 (6), 1195 –1210 (2002). 0896-6273 Google Scholar

34. 

C. E. Stark and L. R. Squire, “When zero is not zero: the problem of ambiguous baseline conditions in fMRI,” Proc. Natl. Acad. Sci. U.S.A., 98 (22), 12760 –12766 (2001). 0027-8424 Google Scholar

35. 

A. Seiyama, J. Seki, H. C. Tanabe, I. Sase, A. Takatsuki, S. Miyauchi, H. Eda, S. Hayashi, T. Imaruoka, T. Iwakura, and T. Yanagida, “Circulatory basis of fMRI signals: relationship between changes in the hemodynamic parameters and BOLD signal intensity,” Neuroimage, 21 (4), 1204 –1214 (2004). 1053-8119 Google Scholar

36. 

H. Sato, M. Kiguchi, F. Kawaguchi, and A. Maki, “Practicality of wavelength selection to improve signal-to-noise ratio in near-infrared spectroscopy,” Neuroimage, 21 (4), 1554 –1562 (2004). 1053-8119 Google Scholar

37. 

T. Yamamoto and T. Kato, “Paradoxical correlation between signal in functional magnetic resonance imaging and deoxygenated hemoglobin content in capillaries: a new theoretical explanation,” Phys. Med. Biol., 47 (7), 1121 –1141 (2002). https://doi.org/10.1088/0031-9155/47/7/309 0031-9155 Google Scholar

38. 

K. Uludag, J. Steinbrink, A. Villringer, and H. Obrig, “Separability and cross talk: optimizing dual wavelength combinations for near-infrared spectroscopy of the adult head,” Neuroimage, 22 (2), 583 –589 (2004). 1053-8119 Google Scholar

39. 

K. Uludag, M. Kohl, J. Steinbrink, H. Obrig, and A. Villringer, “Cross talk in the Lambert-Beer calculation for near-infrared wavelengths estimated by Monte Carlo simulations,” J. Biomed. Opt., 7 (1), 51 –59 (2002). https://doi.org/10.1117/1.1427048 1083-3668 Google Scholar

40. 

D. A. Boas, T. Gaudette, G. Strangman, X. Cheng, J. J. Marota, and J. B. Mandeville, “The accuracy of near infrared spectroscopy and imaging during focal changes in cerebral hemodynamics,” Neuroimage, 13 (1), 76 –90 (2001). https://doi.org/10.1006/nimg.2000.0674 1053-8119 Google Scholar

41. 

S. T. Grafton, R. P. Woods, J. C. Mazziotta, and M. E. Phelps, “Somatotopic mapping of the primary motor cortex in humans: activation studies with cerebral blood flow and positron emission tomography,” J. Neurophysiol., 66 (3), 735 –743 (1991). 0022-3077 Google Scholar

42. 

P. E. Roland, B. Larsen, N. A. Lassen, and E. Skinhoj, “Supplementary motor area and other cortical areas in organization of voluntary movements in man,” J. Neurophysiol., 43 (1), 118 –136 (1980). 0022-3077 Google Scholar

43. 

S. M. Rao, J. R. Binder, P. A. Bandettini, T. A. Hammeke, F. Z. Yetkin, A. Jesmanowicz, L. M. Lisk, G. L. Morris, W. M. Mueller, and L. D. Estkowski, “Functional magnetic resonance imaging of complex human movements,” Neurology, 43 (11), 2311 –2318 (1993). 0028-3878 Google Scholar

44. 

S. G. Kim, J. Ashe, A. P. Georgopoulos, H. Merkle, J. M. Ellermann, R. S. Menon, S. Ogawa, and K. Ugurbil, “Functional imaging of human motor cortex at high magnetic field,” J. Neurophysiol., 69 (1), 297 –302 (1993). 0022-3077 Google Scholar

45. 

H. Sato, Y. Fuchino, M. Kiguchi, T. Katsura, A. Maki, T. Yoro, and H. Koizumi, “Validation of NIR topography with sensorimotor cortex measurements in 31 healthy subjects,” (2004) Google Scholar

46. 

T. Yamamoto, A. Maki, T. Kadoya, Y. Tanikawa, Y. Yamad, E. Okada, and H. Koizumi, “Arranging optical fibres for the spatial resolution improvement of topographical images,” Phys. Med. Biol., 47 (18), 3429 –3440 (2002). https://doi.org/10.1088/0031-9155/47/18/311 0031-9155 Google Scholar

47. 

T. Yamamoto, A. Maki, Y. Yamashita, Y. Tanikawa, Y. Yamada, and H. Koizumi, “Noninvasive brain function measurement system: optical topography,” Proc. SPIE, 4250 339 –350 (2001). 0277-786X Google Scholar

48. 

N. C. Bruce, “Experimental study of the effect of absorbing and transmitting inclusions in highly scattering media,” Appl. Opt., 33 (28), 6692 –6698 (1994). 0003-6935 Google Scholar

49. 

G. H. Klem, H. O. Luders, H. H. Jasper, and C. Elger, “The ten-twenty electrode system of the International Federation. The International Federation of Clinical Neurophysiology,” Electroencephalogr Clin. Neurophysiol. Suppl., 52 3 –6 (1999). 0424-8155 Google Scholar

50. 

M. Okamoto, H. Dan, K. Sakamoto, K. Takeo, K. Shimizu, S. Kohno, I. Oda, S. Isobe, T. Suzuki, K. Kohyama, and I. Dan, “Three-dimensional probabilistic anatomical cranio-cerebral correlation via the international 10-20 system oriented for transcranial functional brain mapping,” Neuroimage, 21 (1), 99 –111 (2004). 1053-8119 Google Scholar

51. 

V. L. Towle, J. Bolanos, D. Suarez, K. Tan, R. Grzeszczuk, D. N. Levin, R. Cakmur, S. A. Frank, and J. P. Spire, “The spatial location of EEG electrodes: locating the best-fitting sphere relative to cortical anatomy,” Electroencephalogr. Clin. Neurophysiol., 86 (1), 1 –6 (1993). 0013-4649 Google Scholar

52. 

H. Steinmetz, G. Furst, and B. U. Meyer, “Craniocerebral topography within the international 10-20 system,” Electroencephalogr. Clin. Neurophysiol., 72 (6), 499 –506 (1989). 0013-4649 Google Scholar

53. 

H. Obrig, M. Neufang, R. Wenzel, M. Kohl, J. Steinbrink, K. Einhaupl, and A. Villringer, “Spontaneous low frequency oscillations of cerebral hemodynamics and metabolism in human adults,” Neuroimage, 12 (6), 623 –639 (2000). https://doi.org/10.1006/nimg.2000.0657 1053-8119 Google Scholar

54. 

M. A. Franceschini, S. Fantini, J. H. Thompson, J. P. Culver, and D. A. Boas, “Hemodynamic evoked response of the sensorimotor cortex measured noninvasively with near-infrared optical imaging,” Psychophysiology, 40 (4), 548 –560 (2003). https://doi.org/10.1111/1469-8986.00057 0048-5772 Google Scholar

55. 

V. Toronov, M. A. Franceschini, M. Filiaci, S. Fantini, M. Wolf, A. Michalos, and E. Gratton, “Near-infrared study of fluctuations in cerebral hemodynamics during rest and motor stimulation: temporal analysis and spatial mapping,” Med. Phys., 27 (4), 801 –815 (2000). https://doi.org/10.1118/1.598943 0094-2405 Google Scholar

56. 

A. Kleinschmidt, H. Obrig, M. Requardt, K. D. Merboldt, U. Dirnagl, A. Villringer, and J. Frahm, “Simultaneous recording of cerebral blood oxygenation changes during human brain activation by magnetic resonance imaging and near-infrared spectroscopy,” J. Cereb. Blood Flow Metab., 16 (5), 817 –826 (1996). 0271-678X Google Scholar

57. 

J. Pujol, A. Lopez-Sala, J. Deus, N. Cardoner, N. Sebastian-Galles, G. Conesa, and A. Capdevila, “The lateral asymmetry of the human brain studied by volumetric magnetic resonance imaging,” Neuroimage, 17 (2), 670 –679 (2002). 1053-8119 Google Scholar

58. 

G. Strangman, M. A. Franceschini, and D. A. Boas, “Factors affecting the accuracy of near-infrared spectroscopy concentration calculations for focal changes in oxygenation parameters,” Neuroimage, 18 (4), 865 –879 (2003). 1053-8119 Google Scholar

59. 

M. E. Raichle, A. M. MacLeod, A. Z. Snyder, W. J. Powers, D. A. Gusnard, and G. L. Shulman, “A default mode of brain function,” Proc. Natl. Acad. Sci. U.S.A., 98 (2), 676 –682 (2001). 0027-8424 Google Scholar

60. 

T. Paus, S. Marrett, K. J. Worsley, and A. C. Evans, “Extraretinal modulation of cerebral blood flow in the human visual cortex: implications for saccadic suppression,” J. Neurophysiol., 74 (5), 2179 –2183 (1995). 0022-3077 Google Scholar

61. 

S. C. Cramer, S. P. Finklestein, J. D. Schaechter, G. Bush, and B. R. Rosen, “Activation of distinct motor cortex regions during ipsilateral and contralateral finger movements,” J. Neurophysiol., 81 (1), 383 –387 (1999). 0022-3077 Google Scholar

62. 

R. Kawashima, P. E. Roland, and B. T. O’Sullivan, “Fields in human motor areas involved in preparation for reaching, actual reaching, and visuomotor learning: a positron emission tomography study,” J. Neurosci., 14 (6), 3462 –3474 (1994). 0270-6474 Google Scholar
©(2005) Society of Photo-Optical Instrumentation Engineers (SPIE)
Hiroki Sato, Yutaka Fuchino, Masashi Kiguchi, Takusige Katura, Atsushi Maki, Takeshi Yoro, and Hideaki Koizumi "Intersubject variability of near-infrared spectroscopy signals during sensorimotor cortex activation," Journal of Biomedical Optics 10(4), 044001 (1 July 2005). https://doi.org/10.1117/1.1960907
Published: 1 July 2005
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KEYWORDS
Near infrared spectroscopy

Sensorimotor cortex

Functional magnetic resonance imaging

Sensors

Statistical analysis

Analytical research

Blood

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