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词条 Biophotonics
释义

  1. Applications

  2. FRET

  3. Biofluorescence

  4. Bioluminescence

  5. Biophosphorescence

  6. Biolasing

  7. Light sources

     Lasers  Gas lasers  Diode lasers  Solid state lasers  Fiber lasers  ps lasers  Ultrafast lasers  Ultrachrome lasers  OPOs  Swept sources  THz sources  LEDs  SLEDs  Lamps  Single photon sources 

  8. References

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The term biophotonics denotes a combination of biology and photonics, with photonics being the science and technology of generation, manipulation, and detection of photons, quantum units of light. Photonics is related to electronics and photons. Photons play a central role in information technologies, such as fiber optics, the way electrons do in electronics.

Biophotonics can also be described as the "development and application of optical techniques, particularly imaging, to the study of biological molecules, cells and tissue". One of the main benefits of using the optical techniques which make up biophotonics is that they preserve the integrity of the biological cells being examined.[1][2]

Biophotonics has therefore become the established general term for all techniques that deal with the interaction between biological items and photons. This refers to emission, detection, absorption, reflection, modification, and creation of radiation from biomolecular, cells, tissues, organisms, and biomaterials. Areas of application are life science, medicine, agriculture, and environmental science.

Similar to the differentiation between "electric" and "electronics," a difference can be made between applications such as Therapy and surgery, which use light mainly to transfer energy, and applications such as diagnostics, which use light to excite matter and to transfer information back to the operator. In most cases, the term biophotonics refers to the latter type of application.

Applications

Applications

Biophotonics is an interdisciplinary field involving the interaction between electromagnetic radiation and biological materials including: tissues, cells, sub-cellular structures, and molecules in living organisms.[3]

Recent biophotonics research has created new applications for clinical diagnostics and therapies involving fluids, cells, and tissues. These advances are allowing scientists and physicians opportunities for superior, non-invasive diagnostics for vascular and blood flow, as well as tools for better examination of skin lesions. In addition to new diagnostic tools, the advancements in biophotonics research have provided new photothermal, photodynamic, and tissue therapies.[4]

Dermatology By observing the numerous and complex interactions between light and biological materials, the field of biophotonics presents a unique set of diagnostic techniques that medical practitioners can utilize. Biophotonic imaging provides the field of dermatology with the only non-invasive technique available for diagnosing skin cancers. Traditional diagnostic procedures for skin cancers involve visual assessment and biopsy, but a new Laser Induced Fluorescence spectroscopy technique allow dermatologists to compare spectrographs of a patient's skin with spectrographs known to correspond with malignant tissue. This provides doctors with earlier diagnosis and treatment options.[3]

“Among optical techniques, an emerging imaging technology based on laser scanning, the optical coherence tomography or OCT imaging is considered to be a useful tool to differentiate healthy from malignant skin tissue.” The information is immediately accessible and eliminates the need for skin excision.[3] This also eliminates the need for the skin samples to be processed in a lab which reduces labor costs and processing time.

Furthermore, these optical imaging technologies can be used during traditional surgical procedures to determine the boundaries of lesions to ensure that the entirety of the diseased tissue is removed. This is accomplished by exposing nanoparticles that have been dyed with a fluorescing substance to the acceptable light photons.[4] Nanoparticles that are functionalized with fluorescent dyes and marker proteins will congregate in a chosen tissue type. When the particles are exposed to wavelengths of light that correspond to the fluorescent dye, the unhealthy tissue glows. This allows for the attending surgeon to quickly visually identify boundaries between healthy and unhealthy tissue, resulting in less time on the operating table and higher patient recovery. “Using dielectrophoretic microarray devices, nanoparticles and DNA biomarkers were rapidly isolated and concentrated onto specific microscopic locations where they were easily detected by epifluorescent microscopy”[3]

Optical Tweezers

Optical tweezers (or traps) are scientific tools employed to maneuver microscopic particles such as atoms, DNA, bacteria, viruses, and other types of nanoparticles. It uses the lights momentum to exert small forces on a sample. This technique allows for the organizing and sorting of cells, the tracking of the movement of bacteria, and the changing of cell structure[5]

Laser Micro-scalpels are a combination of fluorescence microscopy and a femtosecond laser “can penetrate up to 250 micrometers into tissue and target single cells in 3-D space.”[6] The technology, which was patented by researchers at the University of Texas at Austin, means that surgeons can excise diseased or damaged cells without disturbing or damaging healthy surrounding cells in delicate surgeries involving areas such as the eyes and vocal chords.[6]Photoacoustic microscopy (PAM) is an imaging technology that utilizes both laser technology and ultrasound technology. This dual imaging modality is far superior at imaging deep tissue and vascular tissues than previous imaging technologies. The improvement in resolution provides higher quality images of deep tissues and vascular systems, allowing non-invasive differentiation of cancerous tissues vs healthy tissue by observing such things as “water content, oxygen saturation level, and hemoglobin concentration.”[7] Researchers have also been able to use PAM to diagnose endometriosis in rats.[4]Low Level Laser Therapy (LLLT), although somewhat controversial as to it efficacy, can be used to treat wounds by repairing tissue and preventing tissue death. However, more recent studies indicate that LLLT is more useful for reducing inflammation and assuaging chronic joint pain. In addition, it is believed that LLLT could possibly prove to be useful in the treatment of severe brain injury or trauma, stroke, and degenerative neurological diseases.[8]Photodynamic Therapy (PT) uses photosynthesizing chemicals and oxygen to induce a cellular reaction to light. It can be used to kill cancer cells, treat acne, and reduce scarring. PT can also kill bacteria, viruses, and fungi. The technology provides treatment with little to no long-term side effects, is less invasive than surgery and can be repeated more often than radiation. Treatment is limited, however, to surfaces and organs that can be exposed to light, which eliminates deep tissue cancer treatments.[9]Photothermal therapy most commonly uses nanoparticles made of a noble metal to convert light into heat. The nanoparticles are engineered to absorb light in the 700-1000 nm range, where the human body is optically transparent. When the particles are hit by light they heat up, disrupting or destroying the surrounding cells via hyperthermia. Because the light used does not interact with tissue directly, photothermal therapy has few long term side effects and it can be used to treat cancers deep within the body.[10]

FRET

Fluorescence Resonance Energy Transfer, also known as Foerster Resonance Energy Transfer (FRET in both cases) is the term given to the process where two excited "fluorophores" pass energy one to the other non-radiatively (i.e., without exchanging a photon). By carefully selecting the excitation of these flurophores and detecting the emission, FRET has become one of the most widely used techniques in the field of Biophotonics, giving scientists the chance to investigate sub-cellular environments. See the full article on FRET

Biofluorescence

Biofluorescence describes the absorption of ultraviolet or visible light and the sub sequential emission of photons at a lower energy level (S_1 excited state relaxes to S_0 ground state) by intrinsically fluorescent proteins or by synthetic fluorescent molecules covalently attached to a biomarker of interest. Biomarkers are molecules indicative or disease or distress and are a typically monitored systemically in a living organism, or by using an ex vivo tissue sample for microscopy, or in vitro: in the blood, urine, sweat, saliva, interstitial fluid, aqueous humor, or sputum. Stimulating light excites an electron, raising energy to an unstable level. This instability is unfavorable, so the energized electron is returned to a stable state almost as immediately as it becomes unstable.The time delay between excitation and re-emission that occurs when returning to the stable ground state causes the photon that is re-emitted to be a different color (i.e. it relaxes to a lower energy and thus the photon emitted is at a shorter wavelength, as governed by the Plank-Einstein relation) than the excitation light that was absorbed. This return to stability corresponds with the release of excess energy in the form of fluorescent light. This emission of light is only observable whilst the exciation light is still providing photons to the fluorescent molecule and is typically excited by blue or green light and emits purple, yellow, orange, green, cyan, or red. Biofluorescence is often confused with the following forms of biotic light: bioluminescence and biophosphorescence.

Bioluminescence

Bioluminescence differs from biofluorescence in that it is the natural production of light by chemical reactions within an organism, whereas biofluorescence and biophosphorescence are the absorption and reemission of light from the natural environment.

Biophosphorescence

Biophosphorescence is similar to biofluorescence in its requirement of light at specified wavelengths as a provider of excitation energy. The difference here lies in the relative stability of the energized electron. Unlike with biofluorescence, here the electron retains stability in the forbidden triplet state (unpaired spins), with a longer delay in emitting light resulting in the effect that it continues to “glow-in-the-dark” even long after the stimulating light source has been removed.

Biolasing

A biolaser is when laser light is generated by or from within a living cell. Imaging in biophotonics often relies on laser light, and integration with biological systems is seen as a promising route to enhancing sensing and imaging techniques. Biolasers, like any laser system, requires three components gain medium, optical feedback structure and pump source. For the gain medium, a variety of naturally produced fluorescent proteins can be used in different laser structure[11]. Enclosing an optical feedback structure in a cell has been demonstrated using cell vacuoles[12], as well as using fully enclosed laser systems such as dye doped polymer microspheres[13], or semiconductor nanodisks lasers. [14]

Light sources

{{unreferenced section|date=July 2011}}

The predominantly used light sources are beam lights. LEDs and superluminescent diodes also play an important role. Typical wavelengths used in biophotonics are between 600 nm (Visible) and 3000 nm (near IR).

Lasers

Lasers play an increasingly important role in biophotonics. Their unique intrinsic properties like precise wavelength selection, widest wavelength coverage, highest focusability and thus best spectral resolution, strong power densities and broad spectrum of excitation periods make them the most universal light tool for a wide spectrum of applications. As a consequence a variety of different laser technologies from a broad number of suppliers can be found in the market today.

Gas lasers

Major gas lasers used for biophotonics applications, and their most important wavelengths, are:

- Argon Ion laser: 457.8 nm, 476.5 nm, 488.0 nm, 496.5 nm, 501.7 nm, 514.5 nm (multi-line operation possible)- Krypton Ion laser: 350.7 nm, 356.4 nm, 476.2 nm, 482.5 nm, 520.6 nm, 530.9 nm, 568.2 nm, 647.1 nm, 676.4 nm, 752.5 nm, 799.3 nm- Helium–neon laser: 632.8 nm (543.5 nm, 594.1 nm, 611.9 nm)- HeCd lasers: 325 nm, 442 nm

Other commercial gas lasers like carbon dioxide (CO2), carbon monoxide, nitrogen, oxygen, xenon-ion, excimer or metal vapor lasers have no or only very minor importance in biophotonics.

Major advantage of gas lasers in biophotonics is their fixed wavelength, their perfect beam quality and their low linewidth/high coherence. Argon ion lasers can also operate in multi-line mode. Major disadvantage are high power consumption, generation of mechanical noise due to fan cooling and limited laser powers. Key suppliers are Coherent, CVI/Melles Griot, JDSU, Lasos, LTB and Newport/Spectra Physics.

Diode lasers

The most commonly integrated laser diodes, which are used for diode lasers in biophotonics are based either on GaN or GaAs semiconductor material. GaN covers a wavelength spectrum from 375 to 488 nm (commercial products at 515 have been announced recently) whereas GaAs covers a wavelength spectrum starting from 635 nm.

Most commonly used wavelengths from diode lasers in biophotonics are: 375, 405, 445, 473, 488, 515, 640, 643, 660, 675, 785 nm.

Laser Diodes are available in 4 classes:

- Single edge emitter/broad stripe/broad area- Surface emitter/VCSEL- Edge emitter/Ridge waveguide- Grating stabilized (FDB, DBR, ECDL)

For biophotonic applications, the most commonly used laser diodes are edge emitting/ridge waveguide diodes, which are single transverse mode and can be optimized to an almost perfect TEM00 beam quality. Due to the small size of the resonator, digital modulation can be very fast (up to 500 MHz). Coherence length is low (typically < 1 mm) and the typical linewidth is in the nm-range. Typical power levels are around 100 mW (depending on wavelength and supplier).

Key suppliers are: Coherent, Melles Griot, Omicron, Toptica, JDSU, Newport, Oxxius, Power Technology.

Grating stabilized diode lasers either have an lithographical incorporated grating (DFB, DBR) or an external grating (ECDL). As a result, the coherence length will raise into the range of several meters, whereas the linewidth will drop well below picometers (pm). Biophotonic applications, which make use of this characteristics are Raman spectroscopy (requires linewidth below cm-1) and spectroscopic gas sensing.

Solid state lasers

Solid-state lasers are lasers based on solid-state gain media such as crystals or glasses doped with rare earth or transition metal ions, or semiconductor lasers. (Although semiconductor lasers are of course also solid-state devices, they are often not included in the term solid-state lasers.) Ion-doped solid-state lasers (also sometimes called doped insulator lasers) can be made in the form of bulk lasers, fiber lasers, or other types of waveguide lasers. Solid-state lasers may generate output powers between a few milliwatts and (in high-power versions) many kilowatts.

Fiber lasers

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ps lasers

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Ultrafast lasers

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Ultrachrome lasers

Many advanced applications in biophotonics require individually selectable light at multiple wavelengths. As a consequence a series of new laser technologies has been introduced, which currently looks for precise wording.

The most commonly used terminology are supercontinuum lasers, which emit visible light over a wide spectrum simultaneously. This light is then filtered e.g. via acousto-optic modulators (AOM, AOTF) into 1 or up to 8 different wavelengths. Typical suppliers for this technology was NKT Photonics or Fianium. Recently NKT Photonics bought Fianium,[15] remaining the major supplier of the supercontinuum technology on the market.

In another approach (Toptica/iChrome) the supercontinuum is generated in the infra-red and then converted at a single selectable wavelength into the visible regime. This approach does not require AOTF's and has a background-free spectral purity.

Since both concepts have major importance for biophotonics the umbrella term "ultrachrome lasers" is often used.

OPOs

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Swept sources

Swept sources are designed to continuously change ('sweep') emitted light frequency in time. They typically continuously circle through a pre-defined range of frequencies (e.g., 800 +/- 50 nm). Swept sources in the terahertz regime have been demonstrated. A typical application of swept sources in biophotonics is Optical Coherence Tomography (OCT) Imaging.

THz sources

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LEDs

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SLEDs

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Lamps

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Single photon sources

See single photon sources

Single photon sources are novel types of light sources distinct from coherent light sources (lasers) and thermal light sources (such as incandescent light bulbs and mercury-vapor lamps) that emit light as single particles or photons.

References

1. ^King's College London Centre for Biophotonics
2. ^{{cite journal|last1=SPIE|title=Gabriel Popescu plenary talk: Bridging Molecular and Cellular Biology with Optics|journal=SPIE Newsroom|date=2015|doi=10.1117/2.3201503.18}}
3. ^1 2 3 {{Cite journal|last=Serafetinides|first=Alexandros A.|last2=Makropoulou|first2=Mirsini|last3=Kotsifaki|first3=Domna G.|last4=Tsigaridas|first4=Giorgos|date=2017-01-05|title=Biophotonics for imaging and cell manipulation: quo vadis?|publisher=International Society for Optics and Photonics|volume=10226|pages=1022613|doi=10.1117/12.2263036|series=19th International Conference and School on Quantum Electronics: Laser Physics and Applications}}
4. ^1 2 {{Cite journal|last=Krafft|first=Christoph|date=2016|title=Modern trends in biophotonics for clinical diagnosis and therapy to solve unmet clinical needs|url=|journal=Journal of Biophotonics 9|volume=11-12|pages=1362–1375}}
5. ^{{Cite web|url=https://blocklab.stanford.edu/optical_tweezers.html|title=Block lab - Optical tweezers|website=blocklab.stanford.edu|access-date=2017-12-05}}
6. ^1 {{Cite web|url=https://www.biotechniques.com/news/NEWS-New-laser-microscalpel-to-target-diseased-cells/biotechniques-116068.html|title=BioTechniques - NEWS: New laser microscalpel to target diseased cells|website=www.biotechniques.com|access-date=2017-12-05}}
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8. ^{{Cite journal|last=Chung|first=Hoon|last2=Dai|first2=Tianhong|last3=Sharma|first3=Sulbha K.|last4=Huang|first4=Ying-Ying|last5=Carroll|first5=James D.|last6=Hamblin|first6=Michael R.|date=February 2012|title=The Nuts and Bolts of Low-level Laser (Light) Therapy|journal=Annals of Biomedical Engineering|volume=40|issue=2|pages=516–533|doi=10.1007/s10439-011-0454-7|issn=0090-6964|pmc=3288797|pmid=22045511}}
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10. ^{{Cite journal|last=Li|first=Jing-Liang|date=July–August 2010|title=Gold-Nanoparticle-Enhanced Cancer Photothermal Therapy|url=|journal=IEEE Journal of Selected Topics in Quantum Electronics |volume=16| issue=4 |pages=989–996 |doi=10.1109/JSTQE.2009.2030340 |via=|hdl=1959.3/74995}}
11. ^{{cite journal |last1=Gather |first1=Malte C. |last2=Yun |first2=Seok Hyun |title=Single-cell biological lasers |journal=Nature Photonics |date=12 June 2011 |volume=5 |issue=7 |pages=406–410 |doi=10.1038/NPHOTON.2011.99}}
12. ^{{cite journal |last1=Humar |first1=Matjaž |last2=Hyun Yun |first2=Seok |title=Intracellular microlasers |journal=Nature Photonics |date=27 July 2015 |volume=9 |issue=9 |pages=572–576 |doi=10.1038/NPHOTON.2015.129|pmid=26417383 |pmc=4583142 }}
13. ^{{cite journal |last1=Schubert |first1=Marcel |last2=Steude |first2=Anja |last3=Liehm |first3=Philipp |last4=Kronenberg |first4=Nils M. |last5=Karl |first5=Markus |last6=Campbell |first6=Elaine C. |last7=Powis |first7=Simon J. |last8=Gather |first8=Malte C. |title=Lasing within Live Cells Containing Intracellular Optical Microresonators for Barcode-Type Cell Tagging and Tracking |journal=Nano Letters |date=21 July 2015 |volume=15 |issue=8 |pages=5647–5652 |doi=10.1021/acs.nanolett.5b02491|pmid=26186167 }}
14. ^{{cite journal |last1=Fikouras |first1=Alasdair H. |last2=Schubert |first2=Marcel |last3=Karl |first3=Markus |last4=Kumar |first4=Jothi D. |last5=Powis |first5=Simon J. |last6=Di Falco |first6=Andrea |last7=Gather |first7=Malte C. |title=Non-obstructive intracellular nanolasers |journal=Nature Communications |date=16 November 2018 |volume=9 |issue=1 |pages=4817 |doi=10.1038/s41467-018-07248-0|pmid=30446665 |pmc=6240115 }}
15. ^{{Cite web |url=http://www.nktphotonics.com/nkt-photonics-acquires-fianium/ |title=NKT Photonics acquires Fianium |date=31 March 2016 |website=NKT Photonics |access-date=2016-07-04 |archive-url=https://web.archive.org/web/20160707170034/http://www.nktphotonics.com/nkt-photonics-acquires-fianium/ |archive-date=2016-07-07 |dead-url=yes |df= }}
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