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# Fiber cavities with integrated mode matching optics

## Abstract

In fiber based Fabry-Pérot Cavities (FFPCs), limited spatial mode matching between the cavity mode and input/output modes has been the main hindrance for many applications. We have demonstrated a versatile mode matching method for FFPCs. Our novel design employs an assembly of a graded-index and large core multimode fiber directly spliced to a single mode fiber. This all-fiber assembly transforms the propagating mode of the single mode fiber to match with the mode of a FFPC. As a result, we have measured a mode matching of 90% for a cavity length of ~400 μm. This is a significant improvement compared to conventional FFPCs coupled with just a single mode fiber, especially at long cavity lengths. Adjusting the parameters of the assembly, the fundamental cavity mode can be matched with the mode of almost any single mode fiber, making this approach highly versatile and integrable.

## Introduction

Optical Fabry-Pérot cavities are essential tools for a wide range of applications in science and technology. In recent years, newly developed laser ablation techniques made it possible to fabricate high-quality mirrors directly on the facets of optical fibers, leading to the advent of miniaturized fiber-based Fabry-Pérot cavities (FFPCs)1. FFPCs support significantly smaller mode volumes compared to the conventional Fabry-Pérot cavities based on bulk optical mirrors. The resulting quantum mechanical effects have been exploited in atomic2, 3, molecular4, solid state5,6,7, and optomechanical systems8 and are crucial for applications in quantum science and technology. Furthermore, due to their compactness and integration with fiber optics, FFPCs have many potential technological applications beyond fundamental scientific research, e.g., tunable frequency filters9, scanning microscopy10, gas sensing11 and micro-fluidics12. Recently several novel laser machining methods have been developed13, 14, and detailed characterizations of FFPCs have been carried out15,16,17,18. Despite these latest developments, the limited spatial mode matching of FFPCs to their inputs and outputs is still a substantial hindrance for many applications. In contrast to conventional Fabry-Pérot cavities, where mode matching can be achieved with free space optics, this is not possible with FFPCs. Usually, FFPCs are directly coupled to a single mode (SM) fiber where the mode matching is simply the overlap between the cavity mode and the output mode emanating from the SM fiber. There are no controllable elements once the cavity geometry and the type of the SM fiber are fixed. In particular, the mode matching efficiencies will be severely limited when the cavity length becomes much longer than the Rayleigh range of the output mode of the SM fiber. Using large mode field diameter fibers such as photonic crystal fibers14 or tapered fibers, which adiabatically transform the fiber mode diameter to that of the cavity, the mode matching can be improved. However, the mismatch of the wavefront curvatures ultimately limits the mode matching efficiency.

In this letter we demonstrate a novel design of FFPCs which enables optimized mode matching between the cavity and fiber output mode, and which is also free from the constraints of the cavity and fiber geometries. Using a concatenation of graded-index (GRIN) and multimode (MM)/core-less fibers with their proper lengths spliced together, a versatile all-fiber mode-matching assembly can be built. With this assembly directly attached to a FFPC, not only the field diameter of the fiber mode but also its wavefront curvature can be precisely engineered to match the mode of the FFPC. As a result, this technique enables the use of almost any optical SM fibers as an input/output for FFPCs in a fully integrated manner. We have designed, built and characterized a FFPC with integrated mode matching assembly and have measured a mode matching efficiency of up to 90% where the conventional design only achieves ~30%.

## Results

### Concept

In order to achieve an optimal mode overlap between an optical cavity and a laser beam in free space, a single lens with an appropriate focal length (f) has to be located at the right distance (L) from the position of the cavity (see Fig. 1(a)). Our design follows the same concept but in an all-fiber implementation (Fig. 1(b)). As the focusing element we employ a large core GRIN fiber (OFS, BF04432-1) to avoid distortion of the transmitted mode by the core-cladding interface. The gradient constant (g) of the GRIN fiber is the parameter that determines its length and hence, the effective focal length. Firstly, the GRIN fiber is spliced (Fujikura FSM1000 ARC Master) to a cleaved single mode fiber (IVG, Cu800). Then the GRIN fiber is precisely cleaved (Fujikura CT100) under a microscope19 to a predefined length to within ±15 μm. Even though the splice losses between the SM and GRIN fibers are low (≈0.01 dB as specified by the splicer analysis), they result in a modification of the effective mode field diameter at the SM-GRIN interface, which needs to be taken into account when cleaving the GRIN fiber. The actual mode waist is confirmed by measuring the mode profile at the output of the SM-GRIN assembly along the axial direction. To this end, a laser beam is coupled into the other end of the SM fiber and the output beam from the GRIN fiber is measured using a knife edge translating across the beam. Fitting the measurement with the propagation of a Gaussian beam, the waist size (ω 0) and its position with respect to the end facet of the GRIN fiber (z 0) is found. To evaluate g, the measurements are repeated for different GRIN fiber lengths. Figure 1(c) and (d) illustrates measurements of ω0 and z 0 as a function of GRIN fiber length. The length of GRIN fiber is chosen from these measurements, such that the resulting mode waist matches that of the FFPC. To position the cavity mirrors at the optimal distance from the GRIN fiber a piece of a MM fiber is spliced to it. This fiber serves as a spacer as well as a carrier for the cavity mirror. Due to the large core size of the MM fiber, it does not disturb the free propagation of the mode shaped by the GRIN fiber. Based on the waist position measurement (Fig. 1(d)), the MM fiber is cleaved at the optimal position for the desired cavity geometry. Finally, the end facet of the MM fiber is laser ablated13. The resulting mode matching fiber assembly (FA), shown in Fig. 1(e), is a concatenation of a SM, GRIN and MM fiber which are directly spliced together, producing a co-axial all-fiber structure. The final mode profile is measured again at the output of FA using knife edge method, (see Fig. 1(f)), which clearly depicts that the output beam is converging to a waist outside the assembly. After characterizing the mode, the end facet of the MM fiber is coated with a highly reflective dielectric coating (20 ± 5 ppm transmission at 866 nm from Laseroptik GmbH).

### Mode matching between fiber and cavity mode

To evaluate the mode matching between the fiber and cavity modes, we set up a FFPC. One of the fibers is clamped on a custom-made fiber mount, including a sheer piezo actuator which can translate the fiber along its axis for fine tuning and scanning of the cavity length. This mount is in turn attached to a kinematic prism stage to allow angular adjustment. The second fiber is mounted on a motorized translation stage facilitating 3-dimensional adjustment of the fiber position. In particular, the fiber can be translated to adjust the cavity length. To facilitate the fiber cavity alignment and the measurement of the distance between the fiber tips, two perpendicularly arranged microscopes are used to radially observe the fiber cavity. Hence, the cavity length can be measured to within ±5 μm. After adjusting the fiber alignment with the microscopes, laser light at 854 nm is coupled into one of the fibers while the light transmitted through the cavity and entering into the second fiber is detected using a photo diode at the uncoated fiber end. The fibers are then further aligned by observing the cavity transmission, to maximize the transmission of the TEM00 mode, while scanning the length of the cavity with the piezo actuator.

In order to determine the mode matching between the fiber and the cavity modes, we use an FA as the input of the cavity and a MM fiber, with a laser machined and high reflectivity coated end facet, as the output. The FA has a designed waist size of 8.1 μm at a distance of 230 μm from the end facet of the assembly and a radius of curvature (ROC) of 700 μm. The MM fiber for the cavity output has a ROC of 540 μm. Using these parameters, the expected mode matching from the numerical simulation is better than 90% for cavity lengths between 180 μm and 520 μm, with a maximum of 99.9% at 460 μm.

Employing a MM fiber at the output of the cavity is beneficial as the entire cavity transmission spectrum can be observed without spatially filtering high order transverse modes of the cavity. As described in ref. 15, the mode matching of a FFPC can not be determined by simultaneously observing the cavity’s reflection and transmission since the reflected light at the cavity input is mode-filtered by the SM input fiber. Thus, utilizing the resonant dips in the reflection would greatly overestimate the cavity coupling. Therefore in this work, only the transmission spectra are used to determine the mode matching.

The ratio of the cavity transmission intensities of the fundamental TEM00 mode (T 00) and of the modes of order n, m (T nm ) defined by

$$\beta =\frac{{T}_{00}}{\sum _{n,m}{T}_{nm}},$$
(1)

can be used to estimate the real mode matching efficiency η 00 of the fiber mode to the cavity’s fundamental mode. This approximation for the mode matching (β = η 00) is valid as long as the damping for all the cavity modes is the same. The transmission intensity T nm is not only a function of the mode-matching efficiency η nm but also of the cavity finesse $${ {\mathcal F} }_{nm}$$ for the corresponding mode:

$${T}_{nm}=\tilde{\eta }{\eta }_{nm}{ {\mathcal F} }_{nm}^{2}{I}_{in},$$
(2)

where $$\tilde{\eta }$$ includes the efficiencies independent of the mode orders, as well as the detection and propagation efficiencies, and I in is the intensity of the input beam. When the values of $${ {\mathcal F} }_{nm}$$ are the same irrespective of the mode order, β = η 00 is satisfied in Eq. (1) from the normalization condition $${\sum }_{n,m}{\eta }_{nm}=1$$. Otherwise the contribution of the higher order modes may be underestimated, leading to an overestimation of the mode matching. In particular, clipping losses20 can lead to an increased damping for the high order modes due to their larger spatial extension on the cavity mirrors.

To eliminate this effect on our measurements, we measure the finesses of all the modes visible in the transmission spectrum to confirm uniform damping of the modes. To this end, the cavity length, L c , is measured using a calibrated microscope and the free spectral range (FSR) is calculated as FSR = c/2L c . An electro-optic modulator is used to generate sidebands on the laser to act as a frequency calibration of the transmission spectrum to evaluate the cavity linewidth δν 13. The finesse is then calculated by $${\mathcal F} ={\rm{F}}{\rm{S}}{\rm{R}}/\delta \nu$$.

In Fig. 2 the transmission spectra at three different cavity lengths are displayed with the insets showing details of the higher order mode peaks. In addition, Fig. 3 shows the finesse as well as the transmission intensity, T 00 of the fundamental mode as a function of the cavity length. The finesse exhibits the typical behavior of a fiber cavity with MM fiber mirrors13, 17, 21, with a plateau across most of the length range and a sharp drop at the edge of the stability limit. Similarly, T 00 is stable across most of the stability region of the cavity. However, the transmission spectra show a very different behavior with β = 74% at a cavity length of 132 μm, 69% at 536 μm and a 90% at the cavity length of 426 μm. At these three cavity lengths, we confirmed that the cavity finesse is identical within the measurement errors for all the modes visible in the spectrum, and hence, β is a good measure for mode matching.

We have also investigated the repeatability of the measurements using five different fiber assemblies and three of them have produced comparable values of β. The under-performing assemblies show a clear angle between the segment of the assemblies and radial offset respectively. The mode matching at a cavity length L c is related to the one at $${L}_{c}^{\mathrm{(0)}}$$ through

$${\eta }_{00}({L}_{c})=\frac{{T}_{00}({L}_{c})}{{T}_{00}({L}_{c}^{\mathrm{(0)}})}{(\frac{{ {\mathcal F} }_{00}({L}_{c}^{\mathrm{(0)}})}{{ {\mathcal F} }_{00}({L}_{c})})}^{2}{\eta }_{00}({L}_{c}^{\mathrm{(0)}}\mathrm{).}$$
(3)

Hence, from a single measurement of η 00 at a cavity length $${L}_{c}^{\mathrm{(0)}}$$, the mode matching efficiency at an arbitrary cavity length can be calculated by using only the transmission and finesse of the fundamental mode. Here we use the measurement at a cavity length of 132 μm (=$${L}_{c}^{\mathrm{(0)}}$$) as reference where β ≈ η 00 holds, and calculate the estimated mode matching efficiencies over the entire range of the cavity length by using Eq. (3) and the data set in Fig. 3. As shown in Fig. 4, the mode matching efficiencies calculated in this way fit well with the numerical prediction, constituting another strong evidence that our mode-matching assembly is working as expected. Figure 4 also shows a numerical simulation where the same cavity geometry is used but the FA is replaced with a SM fiber. One can see the substantial advantage of our FA for cavity lengths >150 μm.

Another interesting system is one where both sides of the cavity are constituted by the mode matching fiber assemblies (FA-FA system). This configuration implements a bi-directional input-output system (see Fig. 5a). Figure 5b shows a transmission spectrum for such a system with the input side of the cavity being the FA described above. The output side of the cavity is formed by another FA with ROC of 630 μm and designed for a waist size of 8.4 μm at a distance of 230 μm from the end facet of assembly. The length of the cavity is adjusted for the optimal mode matching between the fiber and the cavity modes. Here we see, the intensity ratio β of 98.6% at a cavity length of 420 μm, which is a result of the mode filtering happening on both sides of the cavity. In other words, in this scenario, the transmission T nm is proportional to $${\eta }_{nm}^{2}$$ instead of η nm , resulting in enhanced suppression of the higher order peaks. This value of β in turn corresponds to η 00 = 89% on average for a single FA, which is consistent with the results in Fig. 2 at the same cavity length.

## Discussion

In this paper, we have demonstrated a versatile method to optimize the mode matching between input/output optical fibers and FFPCs. Using appropriate lengths of GRIN and MM fibers, the modes of almost any SM fiber can be matched to the mode of a FFPC. This enables the use of standard polarization maintaining fibers as well as specialty fibers such as spun fibers or photonic crystal fibers in conjunction with FFPCs. With mode matching efficiencies of about 90%, FFPCs can now be utilized for a wide range of applications where good coupling between the cavity an optical SM fibers is crucial.

### Data availability

The data used in this publication can be accessed at DOI:http://sro.sussex.ac.uk/68269.

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## Acknowledgements

We gratefully acknowledge support from EPSRC through the UK Quantum Technology Hub: NQIT - Networked Quantum Information Technologies (EP/M013243/1) and EP/J003670/1. G.K.G., H.T. and M.K. thank Qiming Wu for his help in the preparation of the fibers.

## Author information

### Affiliations

1. #### Department of Physics and Astronomy, University of Sussex, Falmer, BN1 9QH, UK

• Gurpreet Kaur Gulati
• , Hiroki Takahashi
•  & Matthias Keller
2. #### Optoelectronics Research Centre, University of Southampton, Southampton, SO17 1BJ, UK

• Nina Podoliak
•  & Peter Horak

### Contributions

G.K.G. conceived the experiment(s), G.K.G., H.T. and M.K. conducted the experiment(s), N.P. and P.H. performed theoretical simulations. All authors reviewed the manuscript.

### Competing Interests

The authors declare that they have no competing interests.

### Corresponding author

Correspondence to Gurpreet Kaur Gulati.