Functional near-infrared spectroscopy: Difference between revisions
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===Continuous wave === |
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Continuous wave (CW) system uses light sources |
Continuous wave (CW) system uses light sources with constant frequency and amplitude. In fact, to measure absolute changes in HbO concentration with the mBLL, we need to know photon path-length. However, CW-fNIRS does not provide any knowledge of photon path-length, so changes in HbO concentration are relative to an unknown path-length. Many CW-fNIRS commercial systems use estimations of photon path-length derived from computerized [[Monte Carlo method|Monte-Carlo simulations]] and physical models, to approximate absolute quantification of hemoglobin concentrations. |
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<math>\text{OD} = \operatorname{log}_{10}(I_{0}/I)=\epsilon\cdot [X]\cdot l \cdot \text{DPF} + G</math> |
<math>\text{OD} = \operatorname{log}_{10}(I_{0}/I)=\epsilon\cdot [X]\cdot l \cdot \text{DPF} + G</math> |
Revision as of 01:12, 27 March 2020
Functional near-infrared spectroscopy (fNIRS), or Optical Topography as it is called in Japan exclusively, is the use of near-infrared spectroscopy (NIRS) for functional neuroimaging. Using fNIRS, cerebral hemodynamic responses are measured by near-infrared light, which go in line with cerebral activation or deactivation. In particular, this technology is capable of visualizing changes both in oxy- and deoxyhemoglobin concentration.
Description
fNIRS is based on the absorption of near infrared light by hemoglobin. The light moves, or propagates, through the head and lends information about blood volume, flow and oxygenation. This technique is safe, non-invasive, and can be used with other imaging modalities.
To specify, fNIRS is a non-invasive imaging method involving the quantification of chromophore concentration resolved from the measurement of near infrared (NIR) light attenuation or temporal or phasic changes. fNIRS spectrum light takes advantage of the optical window in which (a) skin, tissue, and bone are mostly transparent to NIR light (700–900 nm spectral interval) and (b) hemoglobin (Hb) and deoxygenated-hemoglobin (deoxy-Hb) are strong absorbers of light. These are the principals adapted from pulse oximeters.
There are four different ways for infrared light to interact with the brain tissue: transmission, reflection, scattering, and absorption. fNIRS focuses on absorption: differences in the absorption spectra of deoxy-Hb and oxy-Hb allow the measurement of relative changes in hemoglobin concentration through the use of light attenuation at multiple wavelengths. Two or more wavelengths are selected, with one wavelength above and one below the isosbestic point of 810 nm—at which deoxy-Hb and oxy-Hb have identical absorption coefficients. Using the modified Beer-Lambert law (mBLL), relative concentration can be calculated as a function of total photon path length.[1]
Typically, the light emitter and detector are placed ipsilaterally (each emitter/detector pair on the same side) on the subject's skull so recorded measurements are due to back-scattered (reflected) light following elliptical pathways. fNIRS is most sensitive to scalp and skull, so in order to have an increased sensitivity to the superficial cortex, there needs to be a larger source-detector ratio.
Modified Beer–Lambert law
Changes in light intensity can be related to changes in relative concentrations of hemoglobin through the modified Beer–Lambert law (mBLL). The Beer lambert-law has to deal with concentration of hemoglobin. This technique also measures relative changes in light attenuation as well as using mBLL to quantify hemoglobin concentration changes.[2]
Basic functional near infrared spectroscopy (fNIRS) abbreviations
CBF = cerebral blood flow CBV = cerebral blood volume CMRO2= metabolic rate of oxygen CW= continuous wave DCS = diffuse correlation spectroscopy FD = frequency-domain Hb, HbR= deoxygenated hemoglobin HbO, HbO2= oxygenated hemoglobin HbT= total hemoglobin concentration HGB = blood hemoglobin SaO2= arterial saturation SO2= hemoglobin saturation SvO2= venous saturation TD=time-domain |
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History
US & UK
In 1977, Jöbsis[3] reported that brain tissue transparency to NIR light allowed a non-invasive and continuous method of tissue oxygen saturation using transillumination in neonates. Transillumination (forward-scattering) was of limited utility in adults because of light attenuation and was quickly replaced by reflectance-mode based techniques - resulting in development of NIRS systems proceeding rapidly. Then, by 1985, the first studies on cerebral oxygenation were conducted by M. Ferrari. Later, in 1989, following work with David Delpy at University College London, Hamamatsu developed the first commercial NIRS system: NIR-1000 Cerebral Oxygenation Monitor. NIRS methods were initially used for cerebral oximetry in the 1990’s. In 1993, four publications by Chance et al PNAS, Hoshi & Tamura J Appl Physiol, Kato et al JCBFM, Villringer et al Neuros. Lett. demonstrated the feasibility of fNIRS in adult humans. NIRS techniques were further expanded on by the work of Randall Barbour, Britton Chance, Arno Villringer, M. Cope, D. T. Delpy, Enrico Gratton, and others. Currently, wearable fNIRS are being developed.
Japan
Meanwhile, in the mid-80's, Japanese researchers at the central research laboratory of Hitachi Ltd set out to build a NIRS-based brain monitoring system using a pulse of 70-picosecond rays. This effort came into light when the team, along with their leading expert, Dr Hideaki Koizumi (小泉 英明), held an open symposium to announce the principle of "Optical Topography" in January 1995. In fact, the term "Optical Topography" derives from the concept of using light on "2-Dimensional mapping combined with 1-Dimensional information", or topography. The idea had been successfully implemented in launching their first fNIRS (or Optical Topography, as they call it) device based on Frequency Domain in 2001: Hitachi ETG-100. Later, Harumi Oishi (大石 晴美), a PhD-to-be at Nagoya University, published her doctoral dissertation in 2003 with the subject of "language learners' cortical activation patterns measured by ETG-100" under the supervision of Professor Toru Kinoshita (木下 微)—presenting a new prospect on the use of fNIRS. The company has been advancing the ETG series ever since.
Spectroscopic techniques
Currently, there are three modalities of fNIR Spectroscopy:
1. Continuous Wave
2. Frequency Domain
3. Time-Domain
Continuous wave
Continuous wave (CW) system uses light sources with constant frequency and amplitude. In fact, to measure absolute changes in HbO concentration with the mBLL, we need to know photon path-length. However, CW-fNIRS does not provide any knowledge of photon path-length, so changes in HbO concentration are relative to an unknown path-length. Many CW-fNIRS commercial systems use estimations of photon path-length derived from computerized Monte-Carlo simulations and physical models, to approximate absolute quantification of hemoglobin concentrations.
Where is the optical density or attenuation, is emitted light intensity, is measured light intensity, is the attenuation coefficient, is the chromophomore concentration, is the distance between source and detector and is the differential path length factor, and is a geometric factor associated with scattering.
When the attenuation coefficients are known, constant scattering loss is assumed, and the measurements are treated differentially in time, the equation reduces to:
Where is the total corrected photon path-length.
Using a dual wavelength system, measurements for HbO2 and Hb can be solved from the matrix equation:[4]
Due to their simplicity and cost-effectiveness, CW-fNIRS is by far the most common form of functional NIRS since it is the cheapest to make, applicable with more channels, and ensures a high temporal resolution. However, it does not distinguish between absorption and scattering changes, and cannot measure absolute absorption values: which means that it is only sensitive to relative change in HbO concentration.
Still, the simplicity and cost-effectiveness allow CW-based devices to be the most favorable for clinical applications such as neonatal care, patient monitoring systems, optical tomography systems, and so forth. Moreover, thanks to its portability, wireless CW systems have been developed—allowing individuals to be monitored in ambulatory, clinical and sports environments.[5][6][7]
Frequency Domain
Frequency domain (FD) system comprises NIR laser sources which provide an amplitude-modulated sinusoid at frequencies near 100 MHz. FD-fNIRS measures attenuation, phase shift and the average path length of light through the tissue. Multi Distance, which is a part of the FD-fNIRS, is insensitive to differences in skin color—giving constant results regardless of subject variation.
Changes in the back-scattered signal's amplitude and phase provide a direct measurement of absorption and scattering coefficients of the tissue, thus obviating the need for information about photon path-length; and from the coefficients we determine the changes in the concentration of hemodynamic parameters.
Because of the need for modulated lasers as well as phasic measurements, FD system-based devices are more technically complex (therefore more expensive and much less portable) than CW-based ones. However, the system is capable of providing absolute concentrations of HbO and HbR.
Time-Domain
Time-domain (TD) system introduces a short NIR pulse with a pulse length usually in the order of picoseconds—around 70 ps. Through time-of-flight measurements, photon path-length may be directly observed by dividing resolved time by the speed of light. Information about hemodynamic changes can be found in the attenuation, decay, and time profile of the back-scattered signal. For this photon-counting technology is introduced, which counts 1 photon for every 100 pulses to maintain linearity. TD-fNIRS does have a slow sampling rate as well as a limited number of wavelengths. Because of the need for a photon-counting device, high-speed detection, and high-speed emitters, time-resolved methods are the most expensive and technically complicated.
TD-based devices are totally immobile, space-consuming, the most difficult to make, costliest, hugest, and heaviest. Even so, they have the highest depth sensitivity and are capable of presenting most accurate values of baseline hemoglobin concentration and oxygenation.
Diffuse Correlation Spectroscopy
Diffuse correlation spectroscopy (DCS) systems use localized gradients in light attenuation to determine absolute ratios of oxy-Hb and deoxy-Hb. Using a spatial measurement, DCS systems do not require knowledge of photon path-length to make this calculation, however measured concentrations of oxy-Hb and deoxy-Hb are relative to the unknown coefficient of scattering in the media. This technique is most commonly used in cerebral oxymetry systems that report a Tissue Oxygenation Index (TOI) or Tissue Saturation Index (TSI).[8]
System Design
A few open-source fNIRS models are available online:
Data Analysis Software
HOMER3
HOMER3 allows users to obtain estimates and maps of brain activation. It is a set of matlab scripts used for analyzing fNIRS data. This set of scripts has evolved since the early 1990s first as the Photon Migration Imaging toolbox, then HOMER1 and HOMER2, and now HOMER3.[9]
NIRS Toolbox
It is the most recent one. This toolbox is a set of Matlab based tools for the analysis of functional near-infrared spectroscopy (fNIRS). This toolbox defines the +nirs namespace and includes a series of tools for signal processing, display, and statistics of fNIRS data. This toolbox is built around an object-oriented framework of Matlab classes and namespaces. .[10]
AtlasViewer
AtlasViewer allows fNIRS data to be visualized on a model of the brain. In addition, it also allows the user to design probes which can eventually be placed onto a subject.
Application
fNIRS has been successfully implemented as a control signal for Brain-Computer Interface systems.[12][13][14][15][16]
Brain Mapping
Cerebral Oximetry
NIRS monitoring is helpful in a number of ways. Preterm infants can be monitored reducing cerebral hypoxia and hyperoxia with different patterns of activities.[17] It is an effective aid in Cardiopulmonary bypass, is strongly considered to improve patient outcomes and reduce costs and extended stays.
There are inconclusive results for use of NIRS with patients with traumatic brain injury, so it has been concluded that it should remain a research tool.
fNIRS Cap
fNIRS electrode locations and names are specified by the International 10–20 system. In addition to the standard positions of electrodes, short separation channels can be added. Short separation channels allow the measurement of scalp signals. Since the short separation channels measure the signal coming from the scalp, they allow the removal of the signal of superficial layers. This leaves behind the actual brain response. Short separation channel detectors are usually placed 8mm away from a source. They do not need to be in a specific direction or in the same direction as a detector.[18]
Functional Neuroimaging
The use of fNIRS as a functional neuroimaging method relies on the principle of neuro-vascular coupling also known as the haemodynamic response or blood-oxygen-level dependent (BOLD) response. This principle also forms the core of fMRI techniques. Through neuro-vascular coupling, neuronal activity is linked to related changes in localized cerebral blood flow. fNIRS and fMRI are sensitive to similar physiologic changes and are often comparative methods. Studies relating fMRI and fNIRS show highly correlated results in cognitive tasks. fNIRS has several advantages in cost and portability over fMRI, but cannot be used to measure cortical activity more than 4 cm deep due to limitations in light emitter power and has more limited spatial resolution. fNIRS includes the use of diffuse optical tomography (DOT/NIRDOT) for functional purposes. Multiplexing fNIRS channels can allow 2D topographic functional maps of brain activity (e.g. with Hitachi ETG-4000, Artinis Oxymon, NIRx NIRScout, etc.) while using multiple emitter spacings may be used to build 3D tomographic maps.
Hyperscanning
Hyperscanning involves two or more brains monitored simultaneously to investigate interpersonal (across-brains) neural correlates in various social situations, which proves fNIRS to be a suitable modality for investigating live brain-to-brain social interactions.[19]
Music and the Brain
fNIRS can be used to monitor muscians' brain activity while playing musical instruments.[20][21][22][23]
Pros and Cons
The advantages of fNIRS are, among other things: noninvasiveness, low-cost modalities, perfect safety, high temporal resolution, full compatibility with other imaging modalities, and multiple hemodynamic biomarkers.
However, any system can't be without its limitations. For fNIRS those include: low brain sensitivity, low spatial resolution, and shallow penetration depth.
Future Direction
Despite a few limitations, fNIRS devices are relatively small, lightweight, portable and wearable. Thanks to these features, applications for the devices are astounding—which makes them easily accessible in many different scenarios. For example, they have the potential to be used in clinics, a global health situation, a natural environment, and it could be used as a health tracker.
Ultimately, future at-risk individuals in hospitals could benefit from neuromonitoring and neurorehabilitation that fNIRS can offer.
fNIRS Compared with other neuroimaging techniques
Comparing and contrasting other neuroimaging devices is an important thing to take into consideration. When comparing and contrasting these devices it is important to look at the temporal resolution, spatial resolution, and the degree of immobility. EEG (electroencephalograph) and MEG (magnetoencephalography) have high temporal resolution, but a low spatial resolution. EEG also has a higher degree of mobility than MEG has. When looking at fNIRS, they are similar to an EEG. They have a high degree of mobility as well as temporal resolution, and they have low spatial resolution. PET scans and fMRIs are grouped together, however they are distinctly different from the other neuroimaging scans. They have a high degree of immobility, medium/high spatial resolution, and a low temporal resolution. All of these neuroimaging scans have important characteristics and are valuable, however they have distinct characteristics.
Among all other facts, what gives fNIRS a special point of interest is that it is compatible with some of these modalities, including: MRI, EEG, and MEG.
See also
- Near-infrared spectroscopy
- Diffuse optical tomography[24]
- Functional neuroimaging
- Cognitive neuroscience[25]
- The Society for Functional Near Infrared Society (external link)
References
- ^ Villringer, A.; Chance, B. (1997). "Non-invasive optical spectroscopy and imaging of human brain function". Trends in Neurosciences. 20 (10): 435–442. doi:10.1016/S0166-2236(97)01132-6. PMID 9347608.
- ^ Modified Beer Lambert Law, retrieved 2020-03-26
- ^ "Functional near-infrared spectroscopy", Wikipedia, 2019-11-26, retrieved 2019-11-26
- ^ Ayaz, H.; Shewokis, P. A.; Curtin, A.; Izzetoglu, M.; Izzetoglu, K.; Onaral, B. (2011). "Using MazeSuite and Functional Near Infrared Spectroscopy to Study Learning in Spatial Navigation". Journal of Visualized Experiments (56): 3443. doi:10.3791/3443. PMC 3227178. PMID 22005455.
- ^ "Functional near-infrared spectroscopy", Wikipedia, 2019-11-26, retrieved 2019-11-26
- ^ "Functional near-infrared spectroscopy", Wikipedia, 2019-11-26, retrieved 2019-11-26
- ^ "Functional near-infrared spectroscopy", Wikipedia, 2019-11-26, retrieved 2019-11-26
- ^ "Functional near-infrared spectroscopy", Wikipedia, 2019-11-26, retrieved 2019-11-26
- ^ "HOMER2". HOMER2. Retrieved 2019-11-26.
- ^ Template:Santosa, H., Zhai, X., Fishburn, F., & Huppert, T. (2018). The NIRS Brain AnalyzIR Toolbox. Algorithms, 11(5), 73.
- ^ Aasted, Christopher M.; Yücel, Meryem A.; Cooper, Robert J.; Dubb, Jay; Tsuzuki, Daisuke; Becerra, Lino; Petkov, Mike P.; Borsook, David; Dan, Ippeita; Boas, David A. (April 2015). "Anatomical guidance for functional near-infrared spectroscopy: AtlasViewer tutorial". Neurophotonics. 2 (2): 020801. doi:10.1117/1.NPh.2.2.020801. ISSN 2329-423X. PMC 4478785. PMID 26157991.
- ^ Ayaz, H.; Shewokis, P. A.; Bunce, S.; Onaral, B. (2011). "An optical brain computer interface for environmental control". 2011 Annual International Conference of the IEEE Engineering in Medicine and Biology Society. Vol. 2011. pp. 6327–30. doi:10.1109/IEMBS.2011.6091561. ISBN 978-1-4577-1589-1. PMID 22255785.
{{cite book}}
:|journal=
ignored (help) - ^ Coyle, S. M.; Ward, T. S. E.; Markham, C. M. (2007). "Brain–computer interface using a simplified functional near-infrared spectroscopy system" (PDF). Journal of Neural Engineering. 4 (3): 219–226. Bibcode:2007JNEng...4..219C. doi:10.1088/1741-2560/4/3/007. PMID 17873424.
- ^ Sitaram, R.; Zhang, H.; Guan, C.; Thulasidas, M.; Hoshi, Y.; Ishikawa, A.; Shimizu, K.; Birbaumer, N. (2007). "Temporal classification of multichannel near-infrared spectroscopy signals of motor imagery for developing a brain–computer interface". NeuroImage. 34 (4): 1416–1427. doi:10.1016/j.neuroimage.2006.11.005. PMID 17196832.
- ^ Naseer N.; Hong M.J.; Hong K.-S. (2014). "Online binary decision decoding using functional near-infrared spectroscopy for the development of brain-computer interface". Experimental Brain Research. 232 (2): 555–564. doi:10.1007/s00221-013-3764-1. PMID 24258529.
- ^ Naseer N.; Hong K.-S. (2013). "Classification of functional near-infrared spectroscopy signals corresponding to the right- and left-wrist motor imagery for development of a brain-computer interfaces". Neuroscience Letters. 553: 84–89. doi:10.1016/j.neulet.2013.08.021. PMID 23973334.
- ^ {{Rahimpour, A., Noubari, H. A., & Kazemian, M. (2018). A case-study of NIRS application for infant cerebral hemodynamic monitoring: A report of data analysis for feature extraction and infant classification into healthy and unhealthy. Informatics in Medicine Unlocked, 11, 44-50.}}
- ^ Yücel, Meryem A.; Selb, Juliette; Aasted, Christopher M.; Petkov, Mike P.; Becerra, Lino; Borsook, David; Boas, David A. (July 2015). "Short separation regression improves statistical significance and better localizes the hemodynamic response obtained by near-infrared spectroscopy for tasks with differing autonomic responses". Neurophotonics. 2 (3): 035005. doi:10.1117/1.NPh.2.3.035005. ISSN 2329-423X. PMC 4717232. PMID 26835480.
- ^ mari (2018-02-04). "fNIRS Hyperscanning: A door to real-world social neuroscience research". The Society for functional Near Infrared Spectroscopy. Retrieved 2020-03-26.
- ^ "YouTube". www.youtube.com. Retrieved 2020-03-26.
- ^ fNIRS of playing piano, retrieved 2020-03-26
- ^ fNIRS of Observation, retrieved 2020-03-26
- ^ fNIRS of Imagery, retrieved 2020-03-26
- ^ "NIRx | fNIRS Systems | NIRS Devices". NIRx Medical Technologies. Retrieved 2019-11-26.
- ^ Yücel, Meryem A.; Selb, Juliette; Aasted, Christopher M.; Petkov, Mike P.; Becerra, Lino; Borsook, David; Boas, David A. (July 2015). "Short separation regression improves statistical significance and better localizes the hemodynamic response obtained by near-infrared spectroscopy for tasks with differing autonomic responses". Neurophotonics. 2 (3): 035005. doi:10.1117/1.NPh.2.3.035005. ISSN 2329-423X. PMC 4717232. PMID 26835480.
- ^ "NIRS / fNIRS". Cortech Solutions, Inc. Retrieved 2019-11-26.
- ^ "HOMER2". HOMER2. Retrieved 2019-11-26.
- ^ Aasted, Christopher M.; Yücel, Meryem A.; Cooper, Robert J.; Dubb, Jay; Tsuzuki, Daisuke; Becerra, Lino; Petkov, Mike P.; Borsook, David; Dan, Ippeita; Boas, David A. (April 2015). "Anatomical guidance for functional near-infrared spectroscopy: AtlasViewer tutorial". Neurophotonics. 2 (2): 020801. doi:10.1117/1.NPh.2.2.020801. ISSN 2329-423X. PMC 4478785. PMID 26157991.