TY - JOUR
T1 - A tunable low-drift laser stabilized to an atomic reference
AU - Leopold, Tobias
AU - Schmöger, Lisa
AU - Feuchtenbeiner, Stefanie
AU - Grebing, Christian
AU - Micke, Peter
AU - Scharnhorst, Nils
AU - Leroux, Ian D.
AU - López-Urrutia, José R.Crespo
AU - Schmidt, Piet Oliver
N1 - Funding Information:
We acknowledge support from DFG through QUEST. I.D.L. acknowledges a fellowship from the Alexander von Humboldt Foundation. This work was funded by PTB.
PY - 2016/8/27
Y1 - 2016/8/27
N2 - We present a laser system with a linewidth and long-term frequency stability at the 50 kHz level. It is based on a Ti:Sapphire laser emitting radiation at 882 nm which is referenced to an atomic transition. For this, the length of an evacuated transfer cavity is stabilized to a reference laser at 780 nm locked to the 85Rb D2-line via modulation transfer spectroscopy. Gapless frequency tuning of the spectroscopy laser is realized using the sideband-locking technique to the transfer cavity. In this configuration , the linewidth of the spectroscopy laser is derived from the transfer cavity, while the long-term stability is derived from the atomic resonance. Using an optical frequency comb, the frequency stability and linewidth of both lasers are characterized by comparison against an active hydrogen maser frequency standard and an ultra-narrow linewidth laser, respectively. The laser system presented here will be used for spectroscopy of the 1s22s22p2P1/2-2P3/2 transition in sympathetically cooled Ar13 + ions at 441 nm after frequency doubling.
AB - We present a laser system with a linewidth and long-term frequency stability at the 50 kHz level. It is based on a Ti:Sapphire laser emitting radiation at 882 nm which is referenced to an atomic transition. For this, the length of an evacuated transfer cavity is stabilized to a reference laser at 780 nm locked to the 85Rb D2-line via modulation transfer spectroscopy. Gapless frequency tuning of the spectroscopy laser is realized using the sideband-locking technique to the transfer cavity. In this configuration , the linewidth of the spectroscopy laser is derived from the transfer cavity, while the long-term stability is derived from the atomic resonance. Using an optical frequency comb, the frequency stability and linewidth of both lasers are characterized by comparison against an active hydrogen maser frequency standard and an ultra-narrow linewidth laser, respectively. The laser system presented here will be used for spectroscopy of the 1s22s22p2P1/2-2P3/2 transition in sympathetically cooled Ar13 + ions at 441 nm after frequency doubling.
UR - https://www.scopus.com/pages/publications/84983749199
U2 - 10.48550/arXiv.1602.04169
DO - 10.48550/arXiv.1602.04169
M3 - Article
AN - SCOPUS:84983749199
SN - 0946-2171
VL - 122
JO - Applied Physics B: Lasers and Optics
JF - Applied Physics B: Lasers and Optics
IS - 9
M1 - 236
ER -