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arXiv:0706.3374 · Physical Review A

Laser ablation loading of a surface-electrode ion trap

David R. Leibrandt, Robert Clark, Jaroslaw Labaziewicz, Paul Antohi, Waseem Bakr, Kenneth R. Brown, Isaac L. Chuang

Published Nov 8, 2007• 61 citations
arXivHTMLPDF

Abstract

We demonstrate loading of $^{88}\mathrm{Sr}^{+}$ ions by laser ablation into a mm-scale surface-electrode ion trap. The laser used for ablation is a pulsed, frequency-tripled Nd:YAG with pulse energies of $1--10\phantom{\rule{0.3em}{0ex}}\mathrm{mJ}$ and durations of $4\phantom{\rule{0.3em}{0ex}}\mathrm{ns}$. An additional laser is not required to photoionize the ablated material. The efficiency and lifetime of several candidate materials for the laser ablation target are characterized by measuring the trapped ion fluorescence signal for a number of consecutive loads. Additionally, laser ablation is used to load traps with a trap depth $(40\phantom{\rule{0.3em}{0ex}}\mathrm{meV})$ below where electron impact ionization loading is typically successful $(\ensuremath{\gtrsim}500\phantom{\rule{0.3em}{0ex}}\mathrm{meV})$.

DOI
10.1103/physreva.76.055403

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We demonstrate loading of 88Sr+^{88}\mathrm{Sr}^{+}88Sr+ ions by laser ablation into a mm-scale surface-electrode ion trap. The laser used for ablation is a pulsed, frequency-tripled Nd:YAG with pulse energies of 1−−10mJ1--10\phantom{\rule{0.3em}{0ex}}\mathrm{mJ}1−−10mJ and durations of 4ns4\phantom{\rule{0.3em}{0ex}}\mathrm{ns}4ns. An additional laser is not required to photoionize the ablated material. The efficiency and lifetime of several candidate materials for the laser ablation target are characterized by measuring the trapped ion fluorescence signal for a number of consecutive loads. Additionally, laser ablation is used to load traps with a trap depth (40meV)(40\phantom{\rule{0.3em}{0ex}}\mathrm{meV})(40meV) below where electron impact ionization loading is typically successful (\ensuremath≳500meV)(\ensuremath{\gtrsim}500\phantom{\rule{0.3em}{0ex}}\mathrm{meV})(\ensuremath≳500meV).
Atomic cadmium ions are loaded into radiofrequency ion traps by photoionization of atoms in a cadmium vapor with ultrafast laser pulses. The photoionization is driven through an intermediate atomic resonance with a frequency-quadrupled mode-locked Ti:sapphire laser that produces pulses of either $100\text{\ensuremath{-}}\mathrm{fs}$ or $1\text{\ensuremath{-}}\mathrm{ps}$ duration at a central wavelength of 229nm229\phantom{\rule{0.3em}{0ex}}\mathrm{nm}229nm. The large bandwidth of the pulses photoionizes all velocity classes of the Cd vapor, resulting in a high loading efficiency compared to previous ion trap loading techniques. Measured loading rates are compared with a simple theoretical model, and we conclude that this technique can potentially ionize every atom traversing the laser beam within the trapping volume. This may allow the operation of ion traps with lower levels of background pressures and less trap electrode surface contamination. The technique and laser system reported here should be applicable to loading most laser-cooled ion species.
Abstract Trapped-ion quantum technologies have been developed for decades toward applications such as precision measurement, quantum communication and quantum computation. Coherent manipulation of ions’ oscillatory motions in an ion trap is important for quantum information processing by ions, however, unwanted decoherence caused by fluctuating electric-field environment often hinders stable and high-fidelity operations. One way to avoid this is to adopt pulsed laser ablation for ion loading, a loading method with significantly reduced pollution and heat production. Despite the usefulness of the ablation loading such as the compatibility with cryogenic environment, randomness of the number of loaded ions is still problematic in realistic applications where definite number of ions are preferably loaded with high probability. In this paper, we demonstrate an efficient loading of a single strontium ion into a surface electrode trap generated by laser ablation and successive photoionization. The probability of single-ion loading into a surface electrode trap is measured to be 82%, and such a deterministic single-ion loading allows for loading ions into the trap one-by-one. Our results open up a way to develop more functional ion-trap quantum devices by the clean, stable, and deterministic ion loading.
Trapped-ion quantum information processing may benefit from qubits encoded in isotopes that are practically available in only small quantities, e.g., due to low natural abundance or radioactivity. Laser ablation provides a method of controllably liberating neutral atoms or ions from low-volume targets, but energetic ablation products can be difficult to confine in the small ion-electrode distance, micron-scale microfabricated traps amenable to high-speed, high-fidelity manipulation of ion arrays. Here, we investigate ablation-based ion loading into surface-electrode traps of different sizes to test a model describing ion loading probability as a function of effective trap volume and other trap parameters. We characterize loading of ablated barium from a metallic source in two cryogenic surface-electrode traps with 730 and 50 μm ion-electrode distances. Our loading rate agrees with a predictive analytical model, providing insight for the confinement of limited-quantity species of interest for quantum computing, simulation, and sensing.
The 133Ba+^{133}\mathrm{Ba}^{+}133Ba+ ion is a promising candidate as a high-fidelity qubit, and the 137Ba+^{137}\mathrm{Ba}^{+}137Ba+ isotope is promising as a high-fidelity qudit (d>2)(d>2)(d>2). Barium metal is very reactive, and 133Ba+^{133}\mathrm{Ba}^{+}133Ba+ is radioactive and can only be sourced in small quantities, so the most commonly used loading method, oven heating, is less suited for barium and is currently not possible for 133Ba+^{133}\mathrm{Ba}^{+}133Ba+. Pulsed laser ablation solves both of these problems by utilizing compound barium sources while also giving some distinct advantages, such as fast loading, less displaced material, and lower heat load near the ion trap. Because of the relatively low abundances of the isotopes of interest, a two-step photoionization technique is used, which gives us the ability to selectively load isotopes. Characterization of the ablation process for our BaCl2{\mathrm{BaCl}}_{2}BaCl2​ targets are presented, including observation of neutral and ion ablation-fluence regimes, preparation and conditioning, lifetimes of ablation spots, and plume velocity distributions. We show that by using laser ablation on BaCl2{\mathrm{BaCl}}_{2}BaCl2​ salt targets with a two-step photoionization method, we can produce and trap barium ions reliably. Furthermore, we demonstrate that with our photoionization method, we can trap 137Ba+^{137}\mathrm{Ba}^{+}137Ba+ with an enhanced selectivity compared to its natural abundance.
We produce large numbers of low-energy ions by photoionization of laser-cooled atoms inside a surface-electrode-based Paul trap. The isotope-selective trap's loading rate of $4\ifmmode\times\else\texttimes\fi{}{10}^{5}\phantom{\rule{0.3em}{0ex}}{\mathrm{Yb}}^{+}\phantom{\rule{0.3em}{0ex}}\mathrm{ions}∕\mathrm{s}$ exceeds that attained by photoionization (electron-impact ionization) of an atomic beam by three (six) orders of magnitude. Traps as shallow as 0.13eV0.13\phantom{\rule{0.3em}{0ex}}\mathrm{eV}0.13eV are easily loaded with this technique. The ions are confined in the same spatial region as the laser-cooled atoms, which will allow the experimental investigation of interactions between cold ions and cold atoms or Bose-Einstein condensates.