We have set up a STIRAP excitation mechanism for helium from the metastable 23S state into Rydberg states, via the intermediate level 33P . A uv laser at 389 nm and an ir laser at 780-815nm are used as the pump and Stokes beams respectively. Our purposes is to examine how well STIRAP works to efficiently produce the Rydberg atoms, and also to apply STIRAP for further coherent manipulations of helium. To examine the efficiency of the STIRAP process, we use the state selectivity of the light force on atoms to physically separate atoms with different internal states. We use the bichromatic force on a transition different from those used for Rydberg excitation. We do not measure an excitation efficiency close to the ~100% theoretical optimum but instead only about 50%. To gain more insight into this coherent process, an excitation path interferometer is envisioned that showes the expected interference, via the final population of the Rydberg level.We have set up a STIRAP excitation mechanism for helium from the metastable 23S state into Rydberg states, via the intermediate level 33P . A uv laser at 389 nm and an ir laser at 780-815nm are used as the pump and Stokes beams respectively. Our purposes is to examine how well STIRAP works to efficiently produce the Rydberg atoms, and also to apply STIRAP for further coherent manipulations of helium. To examine the efficiency of the STIRAP process, we use the state selectivity of the light force on atoms to physically separate atoms with different internal states. We use the bichromatic force on a transition different from those used for Rydberg excitation. We do not measure an excitation efficiency close to the ~100% theoretical optimum but instead only about 50%. To gain more insight into this coherent process, an excitation path interferometer is envisioned that showes the expected interference, via the final population of the Rydberg level.

Bulletin of the American Physical SocietyJun 16, 20110 citations

Measurement of the binding energy of ultracold Rb87Cs133 molecules using an offset-free optical frequency comb

Peter K. Molony, Avinash Kumar, Philip D. Gregory +6 more

We report the binding energy of $^{87}\mathrm{Rb}^{133}\mathrm{Cs}$ molecules in their rovibrational ground state measured using an offset-free optical frequency comb based on difference frequency generation technology. We create molecules in the absolute ground state using stimulated Raman adiabatic passage (STIRAP) with a transfer efficiency of 88%. By measuring the absolute frequencies of our STIRAP lasers, we find the energy-level difference from an initial weakly bound Feshbach state to the rovibrational ground state with a resolution of $\ensuremath{\sim}5$ kHz over an energy-level difference of more than $114\phantom{\rule{0.28em}{0ex}}\mathrm{T}\mathrm{Hz}$ ; this lets us discern the hyperfine splitting of the ground state. Combined with theoretical models of the Feshbach-state binding energies and ground-state hyperfine structure, we determine a zero-field binding energy of $h\ifmmode\times\else\texttimes\fi{}114\phantom{\rule{0.16em}{0ex}}268\phantom{\rule{0.16em}{0ex}}135.24(4)(3)\phantom{\rule{0.28em}{0ex}}\mathrm{M}\mathrm{Hz}$. To our knowledge, this is the most accurate determination to date of the dissociation energy of a molecule.We report the binding energy of $^{87}\mathrm{Rb}^{133}\mathrm{Cs}$ molecules in their rovibrational ground state measured using an offset-free optical frequency comb based on difference frequency generation technology. We create molecules in the absolute ground state using stimulated Raman adiabatic passage (STIRAP) with a transfer efficiency of 88%. By measuring the absolute frequencies of our STIRAP lasers, we find the energy-level difference from an initial weakly bound Feshbach state to the rovibrational ground state with a resolution of $\ensuremath{\sim}5$ kHz over an energy-level difference of more than $114\phantom{\rule{0.28em}{0ex}}\mathrm{T}\mathrm{Hz}$; this lets us discern the hyperfine splitting of the ground state. Combined with theoretical models of the Feshbach-state binding energies and ground-state hyperfine structure, we determine a zero-field binding energy of $h\ifmmode\times\else\texttimes\fi{}114\phantom{\rule{0.16em}{0ex}}268\phantom{\rule{0.16em}{0ex}}135.24(4)(3)\phantom{\rule{0.28em}{0ex}}\mathrm{M}\mathrm{Hz}$. To our knowledge, this is the most accurate determination to date of the dissociation energy of a molecule.

arXiv:1605.08557Physical Review AAug 15, 201619 citations

Coherent population transfer of ground-state atoms into Rydberg states

T. Cubel, Boon-Keng Kevin Teo, Vladimir S. Malinovsky +5 more

The technique of stimulated Raman adiabatic passage (STIRAP) is used to excite laser-cooled rubidium atoms from the $^{85}\mathrm{Rb}\phantom{\rule{0.3em}{0ex}}5{S}_{1∕2}$ ground state to the $44{D}_{5∕2}$ Rydberg state through the $5{P}_{3∕2}$ state. The utilized double-STIRAP scheme allows for an accurate determination of the absolute excitation efficiency. Experimental data are compared with results of a detailed theoretical model, and good agreement is found. It is concluded that at the center of the excitation region an excitation efficiency of 70% is achieved.The technique of stimulated Raman adiabatic passage (STIRAP) is used to excite laser-cooled rubidium atoms from the $^{85}\mathrm{Rb}\phantom{\rule{0.3em}{0ex}}5{S}_{1∕2}$ ground state to the $44{D}_{5∕2}$ Rydberg state through the $5{P}_{3∕2}$ state. The utilized double-STIRAP scheme allows for an accurate determination of the absolute excitation efficiency. Experimental data are compared with results of a detailed theoretical model, and good agreement is found. It is concluded that at the center of the excitation region an excitation efficiency of 70% is achieved.

Physical Review AAug 8, 200580 citations

Measurement of Population Dynamics in STIRAP

M. A. Gearba, M. L. Trachy, G. Veshapidze +4 more

APSJun 1, 20070 citations

We report the binding energy of

^{87}\mathrm{Rb}^{133}\mathrm{Cs}

molecules in their rovibrational ground state measured using an offset-free optical frequency comb based on difference frequency generation technology. We create molecules in the absolute ground state using stimulated Raman adiabatic passage (STIRAP) with a transfer efficiency of 88%. By measuring the absolute frequencies of our STIRAP lasers, we find the energy-level difference from an initial weakly bound Feshbach state to the rovibrational ground state with a resolution of $\ensuremath{\sim}5$ kHz over an energy-level difference of more than

114\phantom{\rule{0.28em}{0ex}}\mathrm{T}\mathrm{Hz}

; this lets us discern the hyperfine splitting of the ground state. Combined with theoretical models of the Feshbach-state binding energies and ground-state hyperfine structure, we determine a zero-field binding energy of $h\ifmmode\times\else\texttimes\fi{}114\phantom{\rule{0.16em}{0ex}}268\phantom{\rule{0.16em}{0ex}}135.24(4)(3)\phantom{\rule{0.28em}{0ex}}\mathrm{M}\mathrm{Hz}$. To our knowledge, this is the most accurate determination to date of the dissociation energy of a molecule.

The technique of stimulated Raman adiabatic passage (STIRAP) is used to excite laser-cooled rubidium atoms from the

^{85}\mathrm{Rb}\phantom{\rule{0.3em}{0ex}}5{S}_{1∕2}

ground state to the

44{D}_{5∕2}

Rydberg state through the

5{P}_{3∕2}

state. The utilized double-STIRAP scheme allows for an accurate determination of the absolute excitation efficiency. Experimental data are compared with results of a detailed theoretical model, and good agreement is found. It is concluded that at the center of the excitation region an excitation efficiency of 70% is achieved.