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The epithelium of the cornea and conjunctiva needs continuous moistening. With closed eyelids, the tear fluid fills the entire space, and when open, it spreads over the anterior surface of the eye forming a thin film. Tear film has a thickness of 4 7 μm and performs protective, metabolic and optical functions. The direct involvement of the corneal and conjunctival epithelium into formation of tear film was demonstrated in [1]. The tear film covers the whole corneal and conjunctival surface, from the area of transition from the keratinous multilayered epithelium of the eyelid skin edges to the non-corroborating multilayer epithelium of the conjunctiva and up to the corneal center. Thus it allows considering the tear film as one of the corneal layers. Numerous causes leading to the loss of normal properties and structure of the tear film, lead to changes in the water-electrolyte balance. They also cause a decrease in the volume of tear fluid, a decrease in sensitivity and a development of corneal epitheliopathy. A complex of signs of the corneal and conjunctival epithelium lesion due to a decrease in the quality and/or amount of tear fluid defines a concept of ‘dry eye syndrome’ [2]. The assessment of pre-corneal tear film is a leading direction in the diagnosis of dry eye syndrome. In clinical practice the most common method for determining the stability of the tear film is Norn test. Non-invasive methods for studying the stability of a tear film include thioscopy. Confocal microscopy expands the possibilities of studying the anatomy of the cornea at the level of its microstructure. It has been shown recently [3,4] for in vivo measurements of corneal tissue hydration and tear film dynamic control the terahertz (THz) reflectometry might be efficiently used. In the present study we apply frequencydomain THz reflectometry technique for sensing of the ocular surface system. Our study allows the dynamic control of pre-corneal tear film thinning and sensing of corneal tissue hydration level in clinical applications. The concept of the proposed technique was based on THz photomixing approach. Typical photomixer consists of two independent tunable laser sources yielding the difference frequency in a desired THz region by heterodyning. Two laser beams with different frequencies light a photoconductive antenna (PCA), where running fringes with the THz difference frequency excite carries in the semiconductor material. The solid-state lasers are used as elements of a laser heterodyne. The single-mode selection of the laser is done using distributed feedback (DFB) the diffraction grating technologically etched close to the p-n junction of the diode structure. PCA consists of an electrical dipole and semiconductor quick enough to produce carriers in time with the beat frequency. When the heterodyned laser beams light the surface of the semiconductor, than carriers appear in the material. If the metal antenna is polarized with some voltage then carriers give a periodical short circuit for the antenna and PCA converts the photocurrent into a THz wave. The proposed apparatus was based on two DFB diode lasers with precise resonator temperature control. The lasers generated narrow 10 kHz line in the range of 1530 – 1608 nm with average power of 22 mW each. X-type fiber optical beam splitter with the splitting ratio 50/50 combined both lasers output. The outputs of the splitter were connected to the THz emitter and receiver low-temperature InGaAs bowtie PCA (BATOP GmbH). The bias voltage for the THz emitter (0/6 V, 40 kHz) was provided by the function generator. The difference frequency range of DFB lasers allowed tuning of the output THz radiation within a range of 0.04-0.1 THz. High-density polyethylene lens (HDPE) with focal distance of 30 mm focused THz signal to the ocular surface system. The specularly reflected THz signal was guided through second similar HDPE-lens into the receiver PCA module. The digital lock-in amplifier SR 810 (Stanford Research Systems) was used to measure the resulting photocurrent. Both THz emitter and receiver were were embeded into the clinical ophthalmic apparatus (Fig.1) allowed measuring the eye reflection in THz range simultaneously with using of the other standard ophthalmological methodic. For the in vivo study the special experimental protocol was developed. For each human eye cornea the reflected signal versus time was measured and reflection coefficient was calculated. Each measurement started at the time of eye opening. During the measurement series the testee human was requested to keep the eye open as long as possible. The same time he was able to close the eye as soon as he willing doing that. The measurements continued until the next eye closing.

Application of THz radiation for in situ control of eye cornea hydration level