Quantum networking links quantum processors through remote entanglement for distributed quantum information processing and secure long-range communication. Trapped ions are a leading quantum information processing platform, having demonstrated universal small-scale processors and roadmaps for large-scale implementation. Overall rates of ion–photon entanglement generation, essential for remote trapped ion entanglement, are limited by coupling efficiency into single mode fibers and scaling to many ions. Here, we show a microfabricated trap with integrated diffractive mirrors that couples 4.1(6)% of the fluorescence from a 174Yb+ ion into a single mode fiber, nearly triple the demonstrated bulk optics efficiency. The integrated optic collects 5.8(8)% of the π transition fluorescence, images the ion with sub-wavelength resolution, and couples 71(5)% of the collected light into the fiber. Our technology is suitable for entangling multiple ions in parallel and overcomes mode quality limitations of existing integrated optical interconnects.
A small chain of trapped ions, confined along the node of an oscillating electric field in a Paul trap, provides a well controlled quantum system that can be cooled to the quantum ground state and precisely manipulated with lasers and microwaves.1,2,3,4,5,6,7,8 The ions are simultaneously strongly coupled to each other through the Coulomb force, and decoupled from the surrounding environment. The strong mutual coupling is critical for implementing deterministic multi-qubit entangling gates,9, 10 while the external decoupling enables memory coherence times approaching 1 min2 and single qubit gate error rates11 below 10−4. Small-scale quantum processors can be linked together into quantum networks1 using remote entanglement4 to realise the proposed roadmap for large-scale quantum information processing3. Recent developments include implementation of the Shor factoring algorithm12 and a programmable quantum computer module based on five ions.13 In these experiments, the ions’ fluorescence was collected using complex multi-element bulk optics, which may be less suitable for scaling to massively parallel systems.
Ion fluorescence plays two complementary roles in quantum information processing: state readout through the collection of multiple photons, and the creation of remote entanglement through entanglement swapping of photons coupled into single optical modes. The fidelity and readout speed for qubit state detection in trapped ion QIP depends only on the fluorescence collection efficiency.14 While efficient coupling into single-mode structures, including optical fibers or arrays of waveguides for collection from multiple ions,15 requires a collection apparatus that is also capable of producing a high quality ion image. Collection efficiencies in free space of up to 54.8%16 have been realised in custom fabricated parabolic mirror with very large solid angle coverage. However these devices are highly labor intensive to construct and not scalable. A more scalable approach used reflected curved surface optics into microfabricated ion traps,8 but the ion image quality of such system remains insufficient for good single mode coupling. In fact for both local processing and remote networking, a scalable optical interface that can efficiently interface multiple ions with single mode guiding structures is necessary to achieve large, massively parallel implementations.
Diffractive optics offers a solution to this problem since they are scalable, can engineer out geometrical aberrations at the design phase for efficient coupling into single mode structures, and are compatible with several platform such as neutral atom chip traps17 or crystal color centers.18 Previous efforts using diffractive lenses with traditional macro traps have demonstrated a 4.2% collection efficiency19 in free space as well as near diffraction-limited imaging in both fluorescence20 and absorption21 modalities, the latter being important for implementing quantum photonic receivers without the need for ion–photon interaction enhancement by an optical cavity.22
Here, we exploit the potential of diffractive optics and demonstrate a scalable photon–ion interface realised on a multi-zone micro-fabricated surface trap with integrated diffractive mirrors. Our trap is based on a proven design23 and is shown in Fig. 1a. The substrate under the central grounding electrode was patterned and etched before coating with 100 nm of aluminum to also act as an array of diffractive mirrors (see Methods). We tested the properties of the integrated mirror by measuring its collection efficiency with a protocol for the creation of triggered single photons and acquiring a near diffraction-limited image of a single ion. With such image quality we were able to obtained an overall coupling efficiency from ion into single mode fiber which doubled what was previously achieved with micro-trap and multimode fibers by direct collection6 and with the use of diffractive lenses7 respectively.
The diffractive mirror has a focal length of 59.6 μm which correspond to the ion height necessary for high resolution imaging, when the collimated flourescence is refocused by an external lens at the desired magnification (Fig. 1c). The integrated optic has a design diffraction efficiency of 50%, which includes 92% aluminum reflectivity in the ultra-violet, and is 80 μm wide by 127 μm long. The width of the mirror is limited by the center ground electrode size and the length is set to match the industry standard 127 μm pitch of V-groove fiber arrays for simultaneous coupling of multiple ions. The diffractive mirror has a numerical aperture (NA) of 0.55 in the 80 μm direction and 0.73 in the 127 μm direction parallel to the radiofrequency (RF) rails, capturing 13.3% of the total solid angle. This is equivalent to a circular NA of 0.68, which maximizes the overall rate of entanglement generation per unit surface area of the trap.15
The trap is loaded with 174Yb+ ions by isotope selective photo-ionization from an effusive Yb beam passing through a slot in the chip surface (Fig. 1a farthest left ion image). Trapped ions are Doppler cooled and shuttled from the loading zone to the various diffractive optic focus sites by varying the potential in the segmented DC voltage electrode arrays. A conventional bulk optics imaging system (Fig. 1b) allows the ion to be observed at all points along the RF rail for diagnostic purposes. As an indication of the robustness of diffractive optics as an imaging solution, a test diffractive mirror patterned around the Yb oven loading slot was successfully used to image ions, despite the large central void which reduced its collection efficiency. A magnetic field coplanar with the chip, at 45° to the RF rails, sets the direction of the quantization axis. The laser’s direction is aligned with the magnetic field such that circularly polarized light excites either the σ + or σ − transitions.
We measured the collection efficiency of the integrated optics using a single photon generation protocol based on optical-pumping (see Fig. 2 and Methods). The protocol relies on selective illumination with σ + and σ − polarized lasers followed by emission of a π photon which pumps the atom into a dark ground state (Fig. 2a, b). Differences in the radiation distribution patterns results in our optic collecting 17.4% of the fluorescence from π polarized and 11.3% from σ polarized transitions. In the direction perpendicular to the quantization axis and parallel to the collection optic axis, π and σ photons are orthogonally polarized. With this geometry, single π photons were selectively detected placing a linear polariser before a photomultiplier tube (PMT). To verify the integrity of our single photon generation protocol, we measured the second order correlation g (2)(τ) of the fluorescence collected through the integrated mirror with a 50/50 non-polarizing beam splitter and two detectors (Fig. 2c). Our large NA results in polarization blurring24 of the σ photons far from the collection optic axis. To reduce the transmission of σ photons through the polariser, we used an iris to temporarily decrease the NA from 0.68 to 0.48 and measured a g (2)(0) of 0.12(2) (Fig. 3d). This value is well below threshold of 0.5 for a single photon emitter,25 but larger than our expected residual value for g (2)(0) of 0.069. The difference is likely due to residual polarization blurring, imperfections of the polarization purity of the excitation laser and background scattering of the incident laser light off the chip’s surface. Residual polarization blurring is an intrinsic aspect of the dipole radiation patterns26 and protocols, which leverage time-bin or frequency encoding may be necessary to realize the full advantage of large NA optics for efficient generation of remote entanglement. The 308 kHz repetition rate of this protocol is comparable with the present state of the art for remote entanglement ion trapping experiments.5
In order to measure the collection efficiency of the diffractive mirror, we ran the triggered single photon protocol 184,000 times and counted 770 photons. Adjusting for known loss processes (i.e. 19% detector quantum efficiency, 50(5)% transmission through the iris, and 24% losses through other optical elements including the polariser) we measured a 5.8(8)% collection efficiency for our diffractive mirror on the π transition. In comparison, our theoretical efficiency of 8.7% is the product of the 17.4% solid angle coverage for the π transition and the 50% expected diffraction efficiency. This value indicates that our diffraction efficiency is 33(7)% and not the expected 50%, most likely due to fabrication imperfections in the optics.
Figure 3 shows a near diffraction-limited image of an ion with a sub-wavelength spot size of 338(0.7) nm horizontal (H) and 268(0.6) nm vertical (V) FWHM diameter. This is only slightly larger (0.6% for horizontal and 4% for vertical) than the diffraction limited size of 336 nm (H) and 257 nm (V), and approaching the state of the art 280 nm circular spot size reported for a speciality 81% solid angle coverage parabolic reflector optic.16 The M 2 mode quality of the spot was 1.36 (H) and 1.54 (V), compared to an ideal Gaussian (M 2 = 1). This non-ideal behavior is driven by increased divergence in the beam due to astigmatism from the aperture and the fundamentally non-Gaussian distribution of the ion’s emission.
We benchmarked the collection and imaging capabilities of the integrated mirror by coupling the ion’s fluorescence into a single mode fiber. We remove the iris and polariser from the set-up and used a mode matching telescope for adjusting the average radius of the ion fluorescence image to that of a single fiber mode with an estimated spatial mode overlap of 98%. The ion image’s average M 2 of 1.45 reduces the predicted coupling efficiency to 68%. We measured a transmission from the ion through a single mode fiber of 57(4)%, which combined with a 80% fiber transmission due to propagation and Fresnel losses correspond to a single mode coupling efficiency of 71(5)%. This value is in good agreement with the estimated 68% coupling efficiency and combined with the 5.8(8)% π transition collection efficiency from the diffractive optics and 8.3% losses through other optical elements, gives us a total measured coupling efficiency from ion to fiber of 4.1(6)%. This ion-fiber coupling efficiency is nearly triple the previous best of 1.4% using a conventional lens,5 corresponding to a 8.6 times gain in entanglement generation rate. This efficiency could be substantially improved with larger NA optics or modifying the optic’s design to mode-match a specific transition’s intensity distribution to a single mode fiber. More sophisticated multi-level diffraction gratings27 could improve the diffraction efficiency towards 99%.
We have realised a microfabricated architecture for interfacing a single ion with single mode optical fiber and free space based on integrated diffractive mirrors, which is in-principle scalable to a large number of sites. Using a triggered single photon generation protocol, we measured a collection efficiency for the integrated optics of 5.8(8)% a coupling efficiency into a single mode optical fiber of 71(5)%. These mirrors are monolithic with the metallic trap electrode, cover a large solid angle, and can be within a few tens of microns from the ion without distorting the RF trapping potential. They are therefore an ideal platform for the implementation of quantum networks and remote entanglement sharing with trapped ions but also with other quantum light sources such as neutral atom chip traps17 or fixed emitters such as crystal color centers like NV−in diamond.18
The micro-fabrication procedure23 for the surface trap includes depositing multiple layers of aluminum (R = 92%, λ = 370 nm) separated by silicon dioxide insulating layers of various thicknesses. In order to incorporate the diffractive optical elements into this procedure, the oxide surface separating the control electrodes from the ground layer was patterned using e-beam lithography and reactive ion etching of the oxide. The patterned area was subsequently metallized with a 100 nm thick layer of aluminum and the chip was inspected to ensure that the contours of the diffractive optic had not compromised the electrical integrity of the ground electrode. The groove step design is a hybrid of a four level grating near the center with low spatial period and a two level grating near the edges where there is a high spatial period. Grating height step size is 45 nm for 4 level area and 90 nm for 2 level area. Approximating small chunks of the grating as 1D structures, the blazing profile was optimized in GSolver to account for the finite height of the grating and vector diffraction effects.
Fabrication imperfections can cause a mismatch between the optic focal point and the expected RF node altitude of 58.6 μm above the surface of the trap. This is a critical matching problem due to the small depth of focus in low aberration, large aperture ion imaging.20 To guard against this possibility our five collimating optics were fabricated with focal lengths ranging from f = 58.6 to 62.6 μm in 1 μm steps. Stray electrical fields from the neighboring oven loading zone precluded the use of the nominal f 0 = 58.6 μm mirror site and instead experiments were performed on the f +1μm = 59.6 μm focal length collimator. A DC potential was applied to shift the ion off the RF node and position it at the focal point. We observed it was more reliable to pull the ion towards the surface of the trap using a DC potential, rather than pushing it away the trap. While we did not observe a mismatch, for higher NA this parameter will become even more stringent. In future iterations this could be corrected dynamically with additional RF lines or statically by laser trimming the RF electrodes.
Triggered single photon generation protocol
To measure the collection efficiency of the integrated mirror we implemented an optical pumping based single photon generation protocol (Fig. 2). The protocol relies on decay into a dark optically pumped state requiring the emission of a terminal π polarized photon rather than a σ polarized photon (Fig. 2b). The ion was first Doppler cooled for 500 ns with two laser beams of σ + and σ − polarizations with 7 μW and 100 μm diameter at 370 nm, detuned −10 MHz from resonance. Each scattered photon has a 2/3 chance of returning to its original ground state via a σ decay, or a 1/3 chance of being optically pumped into the other ground state via a π transition. The ion was then optically pumped in the 2 S 1/2 m F = +1/2 state by 500 ns illumination with just the σ − light. 750 ns of wait time was introduced for acousto-optic modulator switching time to ensure all laser beams were off. The detection window was then activated for 1000 ns with a 250 ns pulse of σ + occurring 250 ns into the detection window. On average this process takes three scattering events (2σ and 1π) and the whole duration of one cycle is 3.25 μs. Since the collection optic was oriented perpendicular to the quantization axis, the σ and π photons had perpendicular linear polarizations allowing us to filter out the single π photon with a linear polariser and detect it on the PMT. Occasional decays (0.5%) into the 2 D [3/2] dark state were repumped out with 650 μW of 935 nm light and did not have a meaningful impact on the experiment.
The phase Fresnel mirrors were fabricated by M. Ferstl at the Heinrich-Hertz-Institut of the Fraunhofer-Institut für Nachrichtentechnik in Germany. This material is based upon work supported by the Office of the Director of National Intelligence (ODNI), Intelligence Advanced Research Projects Activity (IARPA) under U.S. Army Research Office (ARO) contract number W911NF1210600. All statements of fact, opinion, or conclusions contained herein are those of the authors and should not be construed as representing the official views or policies of IARPA, the ODNI, or the U.S. Government. This work was supported by the Australian Research Council (ARC) under DP130101613. D.K. was supported by ARC Future Fellowship FT110100513. E.W.S was supported by ARC Future Fellowship FT130100472. M.L. was supported by ARC-DECRA DE130100304.Author's contributions
Ion trap construction and experimental work was performed by M. Ghadimi, V. Blūms, B. G. Norton, P. M. Fisher, S. C. Connell, and D. Kielpinski with supervision by D. Kielpinski, M. Lobino, and E.W. Streed. The chip trap was fabricated by J. M. Amini, C. Volin, H. Hayden, and C. S. Pai at Georgia Tech Research Institute. The manuscript was prepared by M. Ghadimi, M. Lobino, and E.W. Streed in consultation with the other authors.Competing interests
The authors declare no competing interests.
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