The first application, to our knowledge, of an all-solid-state system of lasers to the study of a single cooled trapped Sr(+) ion is described. Quantum jumps have been observed by driving the 674-nm 5s(2)S(1/2)-4d(2)D(5/2) transition, and preliminary observations of the line shape are reported. An upper limit for the temperature of a single ion, derived from the 674-nm linewidth, was 200 mK. If non-Doppler sources of broadening such as unresolved Zeeman structure dominate, then the temperature limit would be even lower.
We performed laser spectroscopy of
In+ ions stored in a radio-frequency trap. The 5
s2 1S0\ensuremath{\rightarrow}5s5p
3P1 transition at 230.6 nm was excited and its hyperfine splitting and isotope shift have been measured. The lifetime of the
3P1 state was measured using intensity modulated laser excitation: \ensuremath{\tau}
(3P1)=0.44(4) \ensuremath{\mu}s. A single indium ion was laser cooled using this intercombination line and dark periods in the fluorescence were observed when the metastable
3P0 state was populated by a magnetic dipole decay from
3P1. The radiative lifetime of the forbidden transition
3P0${\ensuremath{\rightarrow}}^{1}$
S0 was determined from the duration of the dark periods: \ensuremath{\tau}
(3P0)=0.14(2) s. This value is compared to calculations based on perturbation theory. Prospects for an optical frequency standard using the narrow 5
s2 1S0\ensuremath{\rightarrow}5s5p
3P0 resonance at 236.5 nm of a single laser-cooled indium ion are discussed.
We performed laser spectroscopy of
In+ ions stored in a radio-frequency trap. The 5
s2 1S0\ensuremath{\rightarrow}5s5p
3P1 transition at 230.6 nm was excited and its hyperfine splitting and isotope shift have been measured. The lifetime of the
3P1 state was measured using intensity modulated laser excitation: \ensuremath{\tau}
(3P1)=0.44(4) \ensuremath{\mu}s. A single indium ion was laser cooled using this intercombination line and dark periods in the fluorescence were observed when the metastable
3P0 state was populated by a magnetic dipole decay from
3P1. The radiative lifetime of the forbidden transition
3P0${\ensuremath{\rightarrow}}^{1}$
S0 was determined from the duration of the dark periods: \ensuremath{\tau}
(3P0)=0.14(2) s. This value is compared to calculations based on perturbation theory. Prospects for an optical frequency standard using the narrow 5
s2 1S0\ensuremath{\rightarrow}5s5p
3P0 resonance at 236.5 nm of a single laser-cooled indium ion are discussed.
The quadrupole moment of the 4d (2)D(5/2) level in 88Sr+ has been measured to be 2.6(3)ea(2)(0), where a(0) is the Bohr radius and e the elementary charge. A single laser-cooled strontium ion was confined in an end cap trap with a variable dc quadrupole potential, and measurements were made on the 5s (2)S(1/2)-4d (2)D(5/2) transition at 674 nm using a femtosecond optical frequency comb. This work shows that measurements of the unperturbed 88Sr+ transition frequency with sub-Hz uncertainty are possible and is important in understanding the reproducibility of ion trap optical frequency standards.
We detect the radiatively driven electric quadrupole transition to the metastable
2D25 state in a single, laser-cooled Hg II ion by monitoring the abrupt cessation of the fluorescence signal from the laser-excited $^{2}S_{\frac{1}{2}}\ensuremath{\rightarrow}^{2}P_{\frac{1}{2}}$ first resonance line. When the ion "jumps" back from the metastable
D state to the ground
S state, the $S\ensuremath{\rightarrow}P$ resonance fluorescence signal immediately returns. The statistical properties of the quantum jumps are investigated; for example, photon antibunching in the emission from the
D state is observed with 100% efficiency.