CN201734698U - Minisize optical fiber probe of single-fiber dual-beam interference system - Google Patents

Abstract

The utility model relates to a minisize optical fiber probe of a single-fiber dual-beam interference system, wherein the probe comprises a single-mode optical fiber (1) and a wedged optical fiber (2) which are connected into a whole; and alternatively the tail end of the single-mode optical fiber is cut into wedge-shaped. The wedge end of the wedged optical fiber (2) is provided with an optical fiber end surface (3) which can adjust the optical divide ratio of reflected light and transmitted light; and the optical fiber end surface (3) and the vertical direction form an angle Theta. The probe can condense the laser in the optical fiber by the wedged optical fiber so as to reduce the speckle of the laser, thus improving the signal-to-noise ratio of the system; and the reflecting and exiting ratio of the laser on the wedged optical fiber end surface can be changed by adjusting the angle of the wedged optical fiber end surface, thus improving the interference effects of the signal light and the reference light. The probe is compact in structure, simple in manufacturing process, and convenient in use.

Description

Single fiber two-beam interference system mini optical fibre probe

Technical field

The utility model relates to optical-coherence tomography (OCT) systems technology, mainly is the fibre-optical probe about common-path optical-coherence tomography system.

Background technology

Optical-coherence tomography (Optical Coherence Tomography, be called for short OCT) is a kind of high-resolution, contactless biological tissue's imaging technique.Have atraumatic, untouchable, simple to operate as a kind of imaging examination method, the imaging of high-resolution cross section, image is directly perceived, clear.Feasible research of the unique function of this technology and clinical practice are very extensive, especially the optical-coherence tomography technology combine with the based endoscopic imaging technology form in peep the optical-coherence tomography technology, can carry out imaging to the histoorgan of organism inside, greatly expand its range of application.

Optical-coherence tomography is a kind of novel optical imagery mode, is can realize imaging to the transverse section of the microstructure of material internal and biosystem by measuring rear orientation light and back reflected laser.Its employed light source is visible light or near infrared light, and imaging also is only to be applicable to visible light or the transparent medium of near infrared light.The optical-coherence tomography technical development so far, from the structure of light path, mainly contain two classes: a class is a bifocal path structure, reference arm and feeler arm are independently; Another kind of is the monochromatic light line structure, and promptly reference arm and feeler arm lump together.In being total to path OCT system, the shared optical path of reference arm and sample arm.The light that light source sends enters reference arm (sample arm) through fiber coupler, and a part of light is in the reflection of plane of reference place, as reference light; Another part light transmission pickup probe shines sample interior and obtains very weak rear orientation light, and coupled back into optical fibers as sample light, with the reference light coherent superposition, produces interference signal once more.Interference signal is got back to fiber coupler by reference arm (sample arm), enters detector.Because organism inner-cavity structure irregular, advance its interior optical fiber or optical fiber image transmission beam of people and exist buckling phenomenon inevitably, cause polarization state to change by its transmitting beam, and use and reference arm is dissimilar or the chromatic dispersion mismatch that causes during different length optical fiber, image drift that temperature fluctuation causes, the periodically vibration that causes of life regular movements etc., all can cause image quality significantly to descend.And, require to use the probe of different length during at different tissues or regional imaging, each replacing of probe, all need carry out the operations such as light path coupling, dispersion compensation and polarization state adjusting of big stroke range, these factors sometimes even can exceed system and can and can not get satisfactory result for the scope of regulating.Therefore, the sensor probe of system adopts path structure altogether, can effectively reduce interferential influences such as fiber-optic vibration, bending, is fit to very much based endoscopic imaging, so just can obtain the high-resolution imaging of inside of human body histoorgan.External a lot of scientific research institutions have all carried out the research of this respect, the probe system of 360 degree circular scannings of the rotary optical component construction that adopts as the G.J.Tearney group of the Harvard Medical School of the U.S.; The OCT miniature probe that Y.T.Pan and J.M.Zara propose based on rotation photo-coupler and MEMS (MEMS); The Xingde Li group of University of Washington proposes the scanheads based on piezoelectric ceramics.Above-mentioned method all has pluses and minuses separately, and as the scanheads based on rotary optical assembly and optical coupler, the coupling efficiency of its light is lower, and the size of probe is bigger; Miniature probe based on the MEMS technology is made suitable complexity, and manufacturing cost and specification requirement are all than higher; Scanheads based on piezoelectric ceramics needs very high driving voltage, needs higher energy consumption, and this is unfavorable for the low-carbon economy of advocating at present and produces certain potential safety hazard in human body.Therefore, how under the condition of fairly simple manufacturing process and lower manufacturing cost, design simple and compact for structure, energy consumption is low and common path OCT scanheads with higher efficiency of light energy utilization, just becomes a general objective of OCT probe designs.

Summary of the invention

Technical problem: the purpose of this utility model is at the deficiencies in the prior art, and a kind of single fiber two-beam interference system mini optical fibre probe that common-path optical is learned the imaging of coherent tomographic technology that is used for is provided.The fine probe of this common-path optical is based on cuneiform optical fiber and angled fiber end face, cuneiform optical fiber is used to dwindle the spot size of flashlight, angled fiber end face provides reference signal and the size of reference signal has been regulated, to reach best interference effect, obtain the interference signal of best signal to noise ratio.

Technical scheme: single fiber two-beam interference of the present utility model system mini optical fibre probe, this probe comprises single-mode fiber and cuneiform optical fiber, single-mode fiber is connected into as a whole with cuneiform optical fiber, or directly cuts into wedge shape at the tail end of single-mode fiber.The wedge end of described cuneiform optical fiber is provided with a fiber end face of regulating laser reflected light and transillumination splitting ratio on cuneiform optical fiber, and fiber end face and vertical direction have a angle θ.Described angle is that the concrete size of θ is to be determined by the splitting ratio of reflected light R and transillumination T, calculates according to fresnel's law:

$R=\frac{{\tan }^2(\mathrm{\&theta;}-{\mathrm{\&theta;}}_1)}{{\tan }^2(\mathrm{\&theta;}+{\mathrm{\&theta;}}_1)}{\mathrm{<figure-callout\; id="2"\; label="cos"\; filenames="HSA00000206106000012.png,HSA00000206106000013.png"\; state="\{\{state\}\}">cos</figure-callout>}}^2\mathrm{\&alpha;}+\frac{{\sin }^2(\mathrm{\&theta;}-{\mathrm{\&theta;}}_1)}{{\sin }^2(\mathrm{\&theta;}+{\mathrm{\&theta;}}_1)}{\sin }^2\mathrm{\&alpha;}$

$T=\frac{\sin 2\mathrm{\&theta;}\sin 2{\mathrm{\&theta;}}_1}{{\sin }^2(\mathrm{\&theta;}+{\mathrm{\&theta;}}_1){\cos }^2(\mathrm{\&theta;}-{\mathrm{\&theta;}}_1)}{\mathrm{<figure-callout\; id="2"\; label="cos"\; filenames="HSA00000206106000012.png,HSA00000206106000013.png"\; state="\{\{state\}\}">cos</figure-callout>}}^2\mathrm{\&alpha;}+\frac{\sin 2\mathrm{\&theta;}\sin 2{\mathrm{\&theta;}}_1\mathrm{}}{{\sin }^2(\mathrm{\&theta;}+{\mathrm{\&theta;}}_1)}{\sin }^2\mathrm{\&alpha;}$

nsinθ＝n ₁sinθ ₁

Wherein: θ is the angle of end face and vertical direction, θ ₁Be the angle of transillumination and normal line of butt end, α is the angle of the vibrations face and the plane of incidence.N is the refractive index of fiber core, n ₁Refractive index for air.

Cuneiform optical fiber can be assembled the laser of single-mode fiber output, is radiated on the sample, and the end face of cuneiform optical fiber is cut and has a certain degree, and is used to regulate the splitting ratio of laser output.

Beneficial effect: compare with background technology, the utlity model has following technique effect:

What 1, this fibre-optical probe used is single-mode fiber and cuneiform optical fiber, has that volume is little, a compact conformation, the simple advantage of manufacturing process.

2, this fibre-optical probe only is to use single-mode fiber and cuneiform optical fiber, and optical fiber is processed, and does not add any driving device, has reduced the consumption of energy, and low-carbon environment-friendly has also improved safety.

3, by using cuneiform optical fiber, can improve the efficiency of light energy utilization of off-axis point imaging to convergences that collimate of the laser in the imaging fibre, and then the signal to noise ratio of raising overall system.

Description of drawings

Below in conjunction with drawings and Examples this utility model is further specified.

Fig. 1 is the structural representation of common-path optical-coherence tomography system.

Fig. 2 A is a fibre-optical probe of the present utility model.Fig. 2 B is the vertical view of Fig. 2 A.Fig. 2 C is the side view of Fig. 2 A.

Fig. 3 A is the light path sketch map of single-mode fiber and cuneiform optical fiber combination.Fig. 3 B is the light path sketch map of the angled single-mode fiber of end face.

Fig. 4 A is the mould speckle figure of single-mode fiber, and Fig. 4 B is the mould speckle figure of cuneiform optical fiber.

Fig. 5 is the interference curve of common-path optical-coherence tomography probe experiment.

Have among the figure: single-mode fiber 1, cuneiform optical fiber 2, fiber end face 3, sample 4 to be tested.

The specific embodiment

Below in conjunction with drawings and Examples this utility model is further described, it is more obvious that the purpose of this utility model and effect will become.

Shown in Figure 1 is the schematic diagram of common-path optical-coherence tomography system.As shown in the figure, the light that light source sends is transferred to 2 * 2 bonders through single-mode fiber, behind 2 * 2 bonders, light is divided into two-way, wherein one tunnel single-mode fiber is tied a knot, thereby the reflected light that has suppressed this road, another road is connected to fibre-optical probe with single-mode fiber, in this road both as with reference to arm also as feeler arm.Light through 2 * 2 bonders enters reference arm (sample arm), and a part of light is in the reflection of plane of reference place, as reference light; Another part light transmission pickup probe shines sample interior and obtains very weak rear orientation light, and coupled back into optical fibers as sample light, with the reference light coherent superposition, produces interference signal once more.Interference signal is got back to fiber coupler by reference arm (sample arm), enters detector.

Shown in Fig. 2 A, the fibre-optical probe that this utility model is used for common-path optical-coherence tomography system comprises single-mode fiber 1 and cuneiform optical fiber 2, and single-mode fiber 1 and cuneiform optical fiber 2 link together, and the tail end of cuneiform optical fiber 2 is cut the θ that has a certain degree.Shown in Fig. 2 B is the vertical view of Fig. 2 A.Fig. 2 C is the side view of Fig. 2 A, and the fiber end face 3 shown in Fig. 2 C is θ with the angle of vertical direction.The effect at θ angle is that laser reflects on fiber end face 3 and the splitting ratio of transmission in order to regulate, thereby improves interference effect, improves the signal to noise ratio of system.

What Fig. 3 A showed is the light path sketch map of single-mode fiber 1 and cuneiform optical fiber 2 combinations.As shown in the figure, the light that light source sends enters in the single-mode fiber 1, be transferred in the cuneiform optical fiber 2 through single-mode fiber 1, because the converging action of 2 pairs of laser of cuneiform optical fiber, the mould speckle of transmission light in the single-mode fiber 1 is reduced, the energy of light is more concentrated, through over-angle is the fiber end face 3 of θ, part light is by fiber end face 3 reflected back cuneiform optical fibers 2, the light of another part is by fiber end face 3 outgoing, be radiated on the sample 4 to be tested, via sample 4 reflection and scattering effects to be tested, reflection and scattered light are coupled in the cuneiform optical fiber 2 more again, interfere effect with light by fiber end face 3 reflected back cuneiform optical fibers 2, interference signal passes to single-mode fiber 1 through cuneiform optical fiber 2, is passed in the detector by single-mode fiber 1, thereby forms a common-path optical-coherence tomography system.What Fig. 3 B showed is the common-path optical-coherence tomography probe of simplifying, and it is that the size at θ angle is between 3.35 ° to 43.23 ° with the single-mode fiber 1 tail end cutting θ that has a certain degree.The effect of θ angle also is in order to regulate the reflection of laser on fiber end face 3 and the splitting ratio of transmission, thereby improves interference effect.

The difference of Fig. 3 A and Fig. 3 B is to be added with cuneiform optical fiber 2 among Fig. 3 A, and cuneiform optical fiber 2 is in order to reduce mould speckle size, to compare with Fig. 3 B, and probe has better Effect on Detecting shown in Fig. 3 A, and better signal to noise ratio is arranged.

Shown in Fig. 4 A is the mould speckle figure of single-mode fiber, and shown in Fig. 4 B is the mould speckle figure of cuneiform optical fiber, learns that by the contrast of two figure the mould speckle of cuneiform optical fiber is significantly less than the mould speckle size of single-mode fiber, and this helps to improve the sensitivity and the resolution of system.

The interference curve figure that the experiment test of shown in Figure 5 is band angle probe arrives.Learn that by interference curve fiber end face 3 to the interference effect of distance within 10um between the sample 4 to be tested clearly.

Claims (3)

1. a single fiber two-beam interference system mini optical fibre is popped one's head in, it is characterized in that this probe comprises single-mode fiber (1) and cuneiform optical fiber (2), single-mode fiber (1) is connected into as a whole with cuneiform optical fiber (2), or directly cuts into wedge shape at the tail end of single-mode fiber.

2. single fiber two-beam interference according to claim 1 system mini optical fibre probe, the wedge end that it is characterized in that described cuneiform optical fiber (2) is provided with a fiber end face (3) of regulating laser at last reflected light of cuneiform optical fiber (2) and transillumination splitting ratio, and fiber end face (3) has a angle θ with vertical direction.

3. single fiber two-beam interference according to claim 1 system mini optical fibre probe is characterized in that described angle is that the concrete size of θ is to be determined by the splitting ratio of reflected light R and transillumination T, calculates according to fresnel's law:

$R=\frac{{\tan }^2(\mathrm{\&theta;}-{\mathrm{\&theta;}}_1)}{{\tan }^2(\mathrm{\&theta;}+{\mathrm{\&theta;}}_1)}{\cos }^2\mathrm{\&alpha;}+\frac{{\sin }^2(\mathrm{\&theta;}-{\mathrm{\&theta;}}_1)}{{\sin }^2(\mathrm{\&theta;}+{\mathrm{\&theta;}}_1)}{\sin }^2\mathrm{\&alpha;}$

$T=\frac{\sin 2\mathrm{\&theta;}\sin 2{\mathrm{\&theta;}}_1}{{\sin }^2(\mathrm{\&theta;}+{\mathrm{\&theta;}}_1){\cos }^2(\mathrm{\&theta;}-{\mathrm{\&theta;}}_1)}{\cos }^2\mathrm{\&alpha;}+\frac{\sin 2\mathrm{\&theta;}\sin 2{\mathrm{\&theta;}}_1\mathrm{}}{{\sin }^2(\mathrm{\&theta;}+{\mathrm{\&theta;}}_1)}{\sin }^2\mathrm{\&alpha;}$

nsinθ＝n ₁sinθ ₁

Wherein: θ is the angle of end face and vertical direction, θ ₁Be the angle of transillumination and normal line of butt end, α is the angle of the vibrations face and the plane of incidence, and n is the refractive index of fiber core, n ₁Refractive index for air.

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