Near-infrared window in biological tissue

The near-infrared (NIR) window (also known as optical window or therapeutic window) defines the range of wavelengths from 650 to 1350 nanometre (nm) where light has its maximum depth of penetration in tissue.[1] Within the NIR window, scattering is the most dominant light-tissue interaction, and therefore the propagating light becomes diffused rapidly. Since scattering increases the distance travelled by photons within tissue, the probability of photon absorption also increases. Because scattering has weak dependence on wavelength, the NIR window is primarily limited by the light absorption of blood at short wavelengths and water at long wavelengths. The technique using this window is called NIRS. Medical imaging techniques such as fluorescence image-guided surgery often make use of the NIR window to detect deep structures.

Absorption properties of tissue components

The absorption coefficient (${\displaystyle \mu _{a}}$) is defined as the probability of photon absorption in tissue per unit path length.[2] Different tissue components have different ${\displaystyle \mu _{a}}$ values. Moreover, ${\displaystyle \mu _{a}}$ is a function of wavelength. Discussed below are the absorption properties of the most important chromophores in tissue. The molar extinction coefficient (${\displaystyle \varepsilon \,}$) is another parameter that is used to describe photon absorption in tissue. By multiplying ${\displaystyle \varepsilon \,}$ by the molar concentration and by ln(10), one can convert ${\displaystyle \varepsilon \,}$ to ${\displaystyle \mu _{a}\,}$.

Figure 1: The molar extinction coefficients of HbO2 and Hb.[3]

Blood

Blood consists of two different types of hemoglobin: oxyhemoglobin (${\displaystyle HbO_{2}}$) is bound to oxygen, while deoxyhemoglobin (${\displaystyle Hb}$) is unbound to oxygen. These two different types of hemoglobin exhibit different absorption spectra that are normally represented in terms of molar extinction coefficients, as shown in Figure 1. The molar extinction coefficient of Hb has its highest absorption peak at 420 nm and a second peak at 580 nm. Its spectrum then gradually decreases as light wavelength increases. On the other hand, ${\displaystyle HbO2}$ shows its highest absorption peak at 410 nm, and two secondary peaks at 550 nm and 600 nm. As light wavelengths passes 600 nm, ${\displaystyle HbO_{2}}$ absorption decays much faster than Hb absorption. The points where the molar extinction coefficient spectra of ${\displaystyle Hb}$ and ${\displaystyle HbO_{2}}$ intersect are called isosbestic points.

By using two different wavelengths, it is possible to calculate the concentrations of oxyhemoglobin (${\displaystyle C_{HbO2}}$) and deoxyhemoglobin (${\displaystyle C_{Hb}}$) as shown in the following equations:

${\displaystyle \mu _{a}(\lambda _{1})=\ln(10)\varepsilon _{HbO2}(\lambda _{1})C_{HbO2}+\ln(10)\varepsilon _{Hb}(\lambda _{1})C_{Hb}\,}$

${\displaystyle \mu _{a}(\lambda _{2})=\ln(10)\varepsilon _{HbO2}(\lambda _{2})C_{HbO2}+\ln(10)\varepsilon _{Hb}(\lambda _{2})C_{Hb}\,}$

Figure 2: The absorption spectrum of water.[4]

Here, ${\displaystyle \lambda _{1}}$ and ${\displaystyle \lambda _{2}}$ are the two wavelengths; ${\displaystyle \varepsilon _{HbO2}}$ and ${\displaystyle \varepsilon _{Hb}}$ are the molar extinction coefficients of ${\displaystyle HbO_{2}}$ and ${\displaystyle Hb}$, respectively; ${\displaystyle C_{HbO2}}$ and ${\displaystyle C_{Hb}}$ are the molar concentrations of ${\displaystyle HbO_{2}}$ and ${\displaystyle Hb}$ in tissue, respectively. Oxygen saturation (${\displaystyle SO_{2}}$) can then be computed as

${\displaystyle SO_{2}={\frac {C_{HbO2}}{C_{HbO2}+C_{Hb}}}}$

Water

Although water is nearly transparent in the range of visible light, it becomes absorbing over the near-infrared region. Water is a critical component since its concentration is high in human tissue. The absorption spectrum of water in the range from 250 to 1000 nm is shown in Figure 2. Although absorption is rather low in this spectral range, it still contributes to the overall attenuation of tissue.

Figure 3: The molar extinction coefficients of eumelanin and pheomelanin.[5]

Other tissue components with less significant contributions to the total absorption spectrum of tissue are melanin and fat.

Figure 4: The absorption coefficient spectrum of fat.[6]

Melanin

Melanin is a chromophore that exists in the human epidermal layer of skin responsible for protection from harmful UV radiation. When melanocytes are stimulated by solar radiation, melanin is produced.[7] Melanin is one of the major absorbers of light in some biological tissue (although its contribution is smaller than other components). There are two types of melanin: eumelanin which is black-brown and pheomelanin which is red-yellow.[8] The molar extinction coefficient spectra corresponding to both types are shown in Figure 3.

Fat

Fat is one of the major components in tissue that can comprise 10-40% of tissue. Although not many mammalian fat spectra are available, Figure 4 shows an example extracted from pig fat.[9]

Figure 5: The scattering coefficient spectrum of biological tissue.[10]

Scattering properties of tissue components

Optical scattering occurs due to mismatches in refractive index of the different tissue components, ranging from cell membranes to whole cells. Cell nuclei and mitochondria are the most important scatterers.[11] Their dimensions range from 100 nm to 6 μm, and thus fall within the NIR window. Most of these organelles fall in the Mie regime, and exhibit highly anisotropic forward-directed scattering.[12]

Light scattering in biological tissue is denoted by the scattering coefficient (${\displaystyle \mu _{s}}$), which is defined as the probability of photon scattering in tissue per unit path length.[13] Figure 5 shows a plot of the scattering spectrum.[14]

Effective attenuation coefficient

Attenuation of light in deep biological tissue depends on the effective attenuation coefficient (${\displaystyle \mu _{eff}}$), which is defined as

${\displaystyle \mu _{\text{eff}}={\sqrt {3\mu _{a}(\mu _{a}+\mu '_{s})}}}$

where ${\displaystyle \mu '_{s}}$ is the transport scattering coefficient defined as

${\displaystyle \mu '_{\text{s}}=\mu _{s}(1-g)\,}$

where ${\displaystyle g}$ is the anisotropy of biological tissue, which has a representative value of 0.9. Figure 5 shows a plot of transport scattering coefficient spectrum in breast tissue, which has a wavelength dependence of ${\displaystyle \lambda \,^{-0.7}}$.[15] The effective attenuation coefficient is the dominant factor for determining light attenuation at depth ${\displaystyle d}$ ≫ 1/ ${\displaystyle \mu _{\text{eff}}}$.

Estimation of the NIR window in tissue

The NIR window can be computed based on the absorption coefficient spectrum or the effective attenuation coefficient spectrum. A possible criterion for selecting the NIR window is given by the FWHM of the inverse of these spectra as shown in Figure 7.

In addition to the total concentration of hemoglobin, the oxygen saturation will define the concentration of oxy and deoxyhemoglobin in tissue and so the total absorption spectrum. Depending on the type of tissue, we can consider different situations. Below, the total concentration of hemoglobin is assumed to be 2.3 mM.

Figure 6 (a): Spectra for arteries (SaO₂ ≈ 98%).

Absorption coefficient: λ_min = 686 nm; NIR window = (634 - 756) nm.

Effective attenuation coefficient: λ_min = 690 nm; NIR window = (618 - 926) nm.

Figure 6 (b): Spectra for veins (SvO₂ ≈ 60%).

Absorption coefficient: λ_min = 730 nm; NIR window = (664 - 932) nm.

Effective attenuation coefficient: λ_min = 730 nm; NIR window = (630 - 1328) nm.

Figure 6 (c): Spectra for breast tissue (StO₂ ≈ 70%).

Absorption coefficient: λ_min = 730 nm; NIR window = (656 - 916) nm.

Effective attenuation coefficient: λ_min = 730 nm; NIR window = (626 - 1316) nm.

Absorption spectrum for arteries

In this case ${\displaystyle SaO_{2}\,}$ ≈ 98% (arterial oxygen saturation). Then oxyhemoglobin will be dominant in the total absorption (black) and the effective attenuation (magenta) coefficient spectra, as shown in Figure 6 (a).

Absorption spectrum for veins

In this case ${\displaystyle SvO_{2}\,}$ ≈ 60% (venous oxygen saturation). Then oxyhemoglobin and deoxyhemoglobin will have similar contributions to the total absorption (black) and the effective attenuation (magenta) coefficient spectra, as shown in Figure 6 (b).

Figure 7: : Effective penetration depth in breast tissue (StO2 ≈ 70%). Effective attenuation coefficient: λ_min = 730 nm; NIR window = (626 - 1316) nm.

Absorption spectrum for breast tissue

To define ${\displaystyle StO_{2}\,}$ (tissue oxygen saturation) (or ${\displaystyle TSI\,}$ (tissue saturation index)), it is necessary to define a distribution of arteries and veins in tissue. an arterial-venous blood volume ratio of 20%/80% can be adopted.[16] Thus tissue oxygen saturation can be defined as ${\displaystyle StO_{2}\,}$ = 0.2 x ${\displaystyle SaO_{2}\,}$ + 0.8 x ${\displaystyle SvO_{2}\,}$ ≈ 70%.

The total absorption (black) and the effective attenuation (magenta) coefficient spectra for breast tissue is shown in Figure 6 (c). In addition, the effective penetration depth is plotted in Figure 7.

See also

• Optical window
• Near-infrared spectroscopy

References

1. Smith, Andrew M.; Mancini, Michael C.; Nie, Shuming (2009). "Bioimaging: Second window for in vivo imaging". Nature Nanotechnology. 4 (11): 710–711. doi:10.1038/nnano.2009.326. ISSN 1748-3387. PMC 2862008. PMID 19898521.
2. LV. Wang and HI. Wu, Biomedical Optics. Wiley. ISBN 978-0-471-74304-0, 2007.
3. Molar extinction coefficients of oxy and deoxyhemoglobin compiled by Scott Prahl. URL: http://omlc.ogi.edu/spectra/hemoglobin.
4. G. M. Hale, and M. R. Querry, Optical constants of water in the 200 nm to 200 µm wavelength region, Appl. Opt., 12, 555-563, 1973.
5. Extinction coefficient of melanin by Steven Jacques. URL: http://omlc.ogi.edu/spectra/melanin/extcoeff.html.
6. R.L.P. van Veen, H.J.C.M. Sterenborg, A. Pifferi, A. Torricelli, and R. Cubeddu, OSA Annual BIOMED Topical Meeting, 2004.
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9. R.L.P. van Veen, H.J.C.M. Sterenborg, A. Pifferi, A. Torricelli, and R. Cubeddu, OSA Annual BIOMED Topical Meeting, 2004.
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11. LV. Wang and HI. Wu, Biomedical Optics. Wiley. ISBN 978-0-471-74304-0, 2007.
12. T. Vo-Dinh, Biomedical Photonics Handbook. Taylor & Francis, Inc. ISBN 0-8493-1116-0, 2002.
13. LV. Wang and HI. Wu, Biomedical Optics. Wiley. ISBN 978-0-471-74304-0, 2007.
14. S. Jacques, C. Newman, D. Levy, and A. von Eschenbach. Univ. of Texas M. D. Anderson Cancer Center, 1987.
15. S. Srinivasan, B. Pogue, S. Jiang, H. Dehghani, C. Kogel, S. Soho, J. Gibson, T. Tosteson, S. Poplack, and K. Paulsen, K D 2003, Proc Natl Acad. Sci. USA 100 12349 54.
16. S. Nioka, S. Wen, J. Zhang, J. Du, X. Intes, Z. Zhao, and B. Chance, Simulation study of breast tissue hemodynamics during pressure perturbation. Oxygen Transport to Tissue XXVI 566, 17-22, 2006.