\relax \ifx\hyper@anchor\@undefined \global \let \oldcontentsline\contentsline \gdef \contentsline#1#2#3#4{\oldcontentsline{#1}{#2}{#3}} \global \let \oldnewlabel\newlabel \gdef \newlabel#1#2{\newlabelxx{#1}#2} \gdef \newlabelxx#1#2#3#4#5#6{\oldnewlabel{#1}{{#2}{#3}}} \AtEndDocument{\let \contentsline\oldcontentsline \let \newlabel\oldnewlabel} \else \global \let \hyper@last\relax \fi \providecommand*\HyPL@Entry[1]{} \citation{Cirac1997} \citation{Kim2005} \citation{Harlander2010} \citation{Guthohrlein2001,Herskind2009a,Shu2010} \citation{Wilson2011} \citation{Streed2011} \citation{VanDevender2010,Brady2011} \citation{Herskind2010} \citation{Cirac1997,Kim2009} \citation{SchneiderCh2010} \citation{Herskind2010} \citation{Herskind2009} \citation{Blatt2008} \citation{Margolis2004} \citation{KimH2010} \HyPL@Entry{0<>} \newlabel{FirstPage}{{}{1}{\relax }{section*.1}{}} \@writefile{toc}{\contentsline {title}{Surface-electrode ion trap with integrated light source}{1}{section*.2}} \@writefile{toc}{\contentsline {abstract}{Abstract}{1}{section*.1}} \@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces (Color online) (a) Schematic of the surface-electrode ion trap with integrated optical fiber. The $^{88}$Sr$^+$ qubit laser is delivered axially (along $z$) through the fiber, while Doppler cooling beams propagate horizontally along $\mathaccentV {vec}17E{e}_x-\mathaccentV {vec}17E{e}_y$. (b) Alignment of the optical ferrule with respect to the trap electrodes. The ferrule is rotated until the fiber is aligned with the minor axis of the trap. (c) Fiber-trap system mounted on a CPGA and installed on the $8$ K basplate of a closed-cycle cryostat.}}{1}{figure.1}} \newlabel{fig:trap}{{1}{1}{(Color online) (a) Schematic of the surface-electrode ion trap with integrated optical fiber. The $^{88}$Sr$^+$ qubit laser is delivered axially (along $z$) through the fiber, while Doppler cooling beams propagate horizontally along $\vec {e}_x-\vec {e}_y$. (b) Alignment of the optical ferrule with respect to the trap electrodes. The ferrule is rotated until the fiber is aligned with the minor axis of the trap. (c) Fiber-trap system mounted on a CPGA and installed on the $8$ K basplate of a closed-cycle cryostat.\label {fig:trap}\relax }{figure.1}{}} \citation{Antohi2009} \citation{Brownnutt2007} \citation{Dehmelt1975} \citation{Berkeland1998} \citation{Herskind2009,VanDevender2010,KimH2010} \citation{Berkeland1998} \HyPL@Entry{1<>} \@writefile{lof}{\contentsline {figure}{\numberline {2}{\ignorespaces Shelving rate as a function of $674$\nobreakspace {}nm power coupled to the trap fiber. Inset: telegraph log of a single ion as it is shelved into the dark $4$D$_{5/2}$ state by $5.4\nobreakspace {}\mu $W of fiber light.}}{2}{figure.2}} \newlabel{fig:telegraph}{{2}{2}{Shelving rate as a function of $674$~nm power coupled to the trap fiber. Inset: telegraph log of a single ion as it is shelved into the dark $4$D$_{5/2}$ state by $5.4~\mu $W of fiber light.\label {fig:telegraph}\relax }{figure.2}{}} \@writefile{lof}{\contentsline {figure}{\numberline {3}{\ignorespaces (Color online) A circuit model for implementation of two in-phase RF drives through a capacitive network. Variable capacitor $C_v$ is used to adjust the RF ratio $\delta =V_2/V_1$.}}{2}{figure.3}} \newlabel{fig:phasediag}{{3}{2}{(Color online) A circuit model for implementation of two in-phase RF drives through a capacitive network. Variable capacitor $C_v$ is used to adjust the RF ratio $\delta =V_2/V_1$.\label {fig:phasediag}\relax }{figure.3}{}} \citation{Harlander2010} \citation{Cirac1997,Kim2009} \bibcite{Cirac1997}{{1}{1997}{{Cirac\ \emph {et~al.}}}{{Cirac, Zoller, Kimble,\ and\ Mabuchi}}} \bibcite{Kim2005}{{2}{2005}{{Kim~et al.}}{{}}} \bibcite{Harlander2010}{{3}{2010}{{Harlander\ \emph {et~al.}}}{{Harlander, Brownnutt, Hansel,\ and\ Blatt}}} \bibcite{Guthohrlein2001}{{4}{2001}{{Guthohrlein\ \emph {et~al.}}}{{Guthohrlein, Keller, Hayasaka, Lange,\ and\ Walther}}} \bibcite{Herskind2009a}{{5}{2009{}}{{Herskind\ \emph {et~al.}}}{{Herskind, Dantan, Marler, Albert,\ and\ Drewsen}}} \bibcite{Shu2010}{{6}{2010}{{Shu\ \emph {et~al.}}}{{Shu, Kurz, Dietrich,\ and\ Blinov}}} \bibcite{Wilson2011}{{7}{2011}{{Wilson~et al.}}{{}}} \bibcite{Streed2011}{{8}{2011}{{Streed\ \emph {et~al.}}}{{Streed, Norton, Jechow, Weinhold,\ and\ Kielpinski}}} \bibcite{VanDevender2010}{{9}{2010}{{VanDevender\ \emph {et~al.}}}{{VanDevender, Colombe, Amini, Leibfried,\ and\ Wineland}}} \bibcite{Brady2011}{{10}{2011}{{Brady~et al.}}{{}}} \bibcite{Herskind2010}{{11}{2010}{{Herskind\ \emph {et~al.}}}{{Herskind, Wang, Shi, Ge, Cetina,\ and\ Chuang}}} \bibcite{Kim2009}{{12}{2009}{{Kim\ and\ Kim}}{{}}} \bibcite{SchneiderCh2010}{{13}{2010}{{Schneider\ \emph {et~al.}}}{{Schneider, Enderlein, Huber,\ and\ Schaetz}}} \bibcite{Herskind2009}{{14}{2009{}}{{Herskind\ \emph {et~al.}}}{{Herskind, Dantan, Albert, Marler,\ and\ Drewsen}}} \bibcite{Blatt2008}{{15}{2008}{{Blatt\ and\ Wineland}}{{}}} \bibcite{Margolis2004}{{16}{2004}{{Margolis\ \emph {et~al.}}}{{Margolis, Barwood, Huang, Klein, Lea, Szymaniec,\ and\ Gill}}} \bibcite{KimH2010}{{17}{2010}{{Kim\ \emph {et~al.}}}{{Kim, Herskind, Kim, Kim,\ and\ Chuang}}} \bibcite{Antohi2009}{{18}{2009}{{Antohi~et al.}}{{}}} \bibcite{Brownnutt2007}{{19}{2007}{{Brownnutt~et al.}}{{}}} \bibcite{Dehmelt1975}{{20}{1975}{{Dehmelt}}{{}}} \bibcite{Berkeland1998}{{21}{1998}{{Berkeland\ \emph {et~al.}}}{{Berkeland, Miller, Bergquist, Itano,\ and\ Wineland}}} \bibstyle{apsrev4-1} \HyPL@Entry{2<>} \@writefile{lof}{\contentsline {figure}{\numberline {4}{\ignorespaces Measurement of the mode profile of the integrated fiber using the ion as a probe. The dashed line is a fit to a Gaussian profile showing good qualitative agreement with the expected profile. Calibrating the transverse displacement by an independent measurement of the fiber mode, the initial fiber-ion offset is approximately $160\nobreakspace {}\mu $m. Images show the relative position of a single ion and an unfocused image of the fiber.}}{3}{figure.4}} \newlabel{fig:modemeas}{{4}{3}{Measurement of the mode profile of the integrated fiber using the ion as a probe. The dashed line is a fit to a Gaussian profile showing good qualitative agreement with the expected profile. Calibrating the transverse displacement by an independent measurement of the fiber mode, the initial fiber-ion offset is approximately $160~\mu $m. Images show the relative position of a single ion and an unfocused image of the fiber.\label {fig:modemeas}\relax }{figure.4}{}} \newlabel{LastBibItem}{{21}{3}{\relax }{figure.4}{}} \newlabel{LastPage}{{}{3}{}{}{}}