VECTOR MAGNETIC SENSOR BASED ON A STRETCHABLE WHISPERING GALLERY MODE MICRORESONATOR

Abstract

An apparatus includes a light source, an optical fiber, having a tapered region, coupled to the light source, a stretchable microresonator in contact with the tapered region of the fiber and in contact with a magnetostrictive material, and a polarization controller that controls polarization of light in the tapered region.

Claims

1. An apparatus comprising: a light source; an optical fiber, having a tapered region, coupled to said light source; a stretchable microresonator in contact with said tapered region of said fiber and in contact with a magnetostrictive material; and a polarization controller that controls polarization of light in said tapered region.

2. The apparatus according to claim 1, wherein said microresonator comprises a vector magnetometer based on a whispering gallery mode (WGM) double-tailed microsphere (DTM), configured to detect strain induced on said magnetostrictive material in response to a change in the ambient magnetic field.

3. The apparatus according to claim 1, further comprising an arm coupled between said stretchable resonator and said magnetostrictive material.

4. The apparatus according to claim 1, in which a permanent magnetic field is used to increase a sensitivity of said microresonator by increasing a magnetostriction coefficient of said magnetostrictive material.

5. A method in which a stretchable microresonator is connected to a tapered fiber and to a magnetostrictive material, comprising: connecting a magnetostrictive material to a static stage; connecting an arm to said static stage or to an edge of said magnetostrictive material, avoiding any contact between said arm and a central region of said magnetostrictive material; connecting one of the fiber tails of a stretchable microresonator to an edge of said arm; connecting one of the fiber tails of said microresonator to the edge of said magnetostrictive material; and bringing a tapered fiber in contact with said microresonator to achieve optical coupling.

6. The method according to claim 5, wherein said tapered fiber is transverse to the fiber tails of said stretchable microresonator.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0010] The present invention will be understood and appreciated more fully from the following detailed description taken in conjunction with the drawings in which:

[0011] FIG. 1 is a simplified schematic illustration of a laser system in accordance with a non-limiting embodiment of the invention, which includes a tunable laser diode 1, a polarization controller (PC) 2, a magnetic sensor 3 based on a double-tailed microsphere, a magnetic coil 4, a power supply 5, a photodetector 6, and an optical spectrum analyzer 7.

[0012] FIG. 2 is a simplified schematic illustration of a magnetic sensor in accordance with a non-limiting embodiment of the invention, based on a double-tailed microsphere (DTM) attached to a magnetostrictive rod. A DTM with a length L.sub.DTM is attached to a magnetostrictive rod with a length L using a high strength arm. A large elongation of a long TDR is converted to a very short DTM, and hence, achieve a large strain-to-magnetic field ratio. The inset is a picture of an actual device.

[0013] FIGS. 3A-3C are simplified graphs of magnetometer sensitivity for L/L.sub.DTM8.4 (FIG. 3A), for L/L.sub.DTM=5.2 (FIG. 3B), and for L/L.sub.DTM=1 (FIG. 3C).

DETAILED DESCRIPTION

[0014] An embodiment of the invention is presented in FIG. 1. A tunable single mode laser is used to measure the shapes and the spectral shifts of the WGMs of the DTMs. Light is coupled to the microspheres using a tapered fiber. A three-pedal polarization controller (PC) between the laser output and the microsphere is used to excite TE and/or TM WGMs.

[0015] A DTM with a length L.sub.DTM is connected to a magnetostrictive rod of length L. The magnetostrictive rod changes its shape in response to a variation in the magnetic field B and induces a strain according to its magnetostriction coefficient =.sub.B.Math.B where .sub.B is in units of /mT. By placing the magnetostrictive material in contact with the microresonator, the change in its shape applies a force on the microresonator which consequently alters its shape and radius as well. The elongation of the DTM, L.sub.DTM, is equal to that of the TDR, L. The magnetometer is sensitive only to magnetic fields aligned with the axis of the DTM.

[0016] The sensitivity of the magnetometer is improved by increasing the ratio between the length of the magnetostrictive rod, L, and that of the DTM, L.sub.DTM. The elongation of the magnetostrictive rod, L, increases linearly with its increase in length. This elongation is, in turn, converted to the DTM; the shorter the DTM, the larger the strain it sustains. L/L.sub.DTM is increased by adding a high strength arm as shown in FIG. 2.

Example

[0017] This demonstration uses a tunable single mode laser (velocity, model 6328) with a center wavelength of =1550 nm. This laser is used to measure the shapes and the spectral shifts of the WGMs of the DTMs. The Q-factor of the DTMs is on the order of 10.sup.8. Light is coupled to the microspheres using a tapered fiber (SMF28) with a waist diameter of 2 m. Terfenol-D rods are used as a magnetostrictive material (from TdVib LLC). (The invention is not limited to Terfenol-D, and can be carried out with other magnetostrictive materials, such as but not limited to, Galfenol.) A magnetic coil is used to apply a magnetic field along the axis of the TDR (7 mT max). The magnetic field was measured using a 3-axes magnetic sensor (AKM, Hall effect) with a resolution of 100 nT.

[0018] Three ratios of L/L.sub.DTM are used. A stiff silica slide (1 mm thickness) is connected as a high strength arm to one or both sides of the DTM (see FIG. 2). The laser is repeatedly swept across specific WGMs, detected by a photodetector and monitored with an oscilloscope. The magnetic coil was fed with a square wave of current at a rate of 1 Hz, far slower than the sweeping speed of the optical source.

[0019] The results shown in FIGS. 3A-3C demonstrate the strong dependence of the magnetometer sensitivity on the L/L.sub.DTM ratio. A maximal sensitivity of 3.35 pm/mT is obtained. The minimal detection limit of the sensor in this example can be evaluated via the minimal spectral shift that may be measured. A common metric used is the HWHM of the WGM, which is governed by its Q factor. In the mentioned microspheres the spectral width of the WGMs is on the order of 0.015 pm, resulting in a magnetic detection limit of 2 T. This is not a fundamental metric, and a spectral resolution of even a tenth of the WGM FWHM can be reached.

[0020] According to the measured sensitivities presented in FIGS. 3A-3C, the magnetostriction coefficient .sub.B of the TDRs for the magnetic fields used in the experiments is 1.4 /mT. It has been well established in the literature that the Terfenol-D magnetostriction coefficient is highly dependent on the magnetic field work point. For higher magnetic fields (20-40 mT), .sub.Band hence the sensitivity of the magnetic sensorcan be increased by a factor of 10. This can be achieved by applying a self DC magnetic field on the order of 20 mT using a permanent magnet.

TABLE-US-00001 TABLE 1 Relevant parameters in the example Parameter Symbol Value Laser central wavelength .sub.0 1550 nm Microresonator (sphere) diameter D 170-180 m Microresonator Q factor Q 10.sup.8 Length of the magnetostrictive rods L 20-30 mm Length of the DTM L.sub.DTM 2-5 mm