Laser Apparatus For Excitation Of Rubidium Atoms In A Quantum Processor

    公开(公告)号:US20240364069A1

    公开(公告)日:2024-10-31

    申请号:US18685770

    申请日:2022-08-19

    Applicant: Pasqal

    Abstract: According to a first aspect, the present disclosure relates to a laser apparatus (210) for excitation of Rubidium (Rb) atoms in a quantum processor comprising an Er-doped DFB fiber laser (201) for emitting light at a wavelength of around 1560 nm; at least a first Yb-doped DFB fiber laser (202) for emitting light at a wavelength of around 1090 nm; a fiber-coupled laser source (203) for emitting light at a wavelength of around 1013 nm; a first fiber-coupled SHG device (301) configured to receive said light from said Yb-doped DFB fiber laser (202) and to produce light at a wavelength of around 545 nm; at least a first fiber-coupled DFG device (302) configured to receive a first part of said light from said Er-doped DFB fiber laser (201) and said light from said first fiber-coupled SHG device (301) and produce light at a wavelength of around 840 nm; a second fiber-coupled SHG device (303) configured to receive said light from said first fiber-coupled DFG device (302) and produce light at a wavelength of around 420 nm; a third fiber-coupled SHG device (304) configured to receive a second part of said light from said Er-doped DFB fiber laser (201) and produce light at a wavelength of around 780 nm, wherein said light at wavelength of around 780 nm is configured to produce MOT laser beams (111, 112, 113) for magneto-optical trapping of the Rb atoms and an optical pumping laser beam (120) for optical pumping of the Rb atoms; wherein said light at a wavelength of around 420 nm and said light at a wavelength of around 1013 nm are configured to produce Rydberg laser beams (141, 142) for transition of Rb atoms to Rydberg states.

    Compact fiber short pulse laser sources

    公开(公告)号:US09819141B2

    公开(公告)日:2017-11-14

    申请号:US15146675

    申请日:2016-05-04

    Abstract: Examples of robust self-starting passively mode locked fiber oscillators are described. In certain implementations, the oscillators are configured as Fabry-Perot cavities containing an optical loop mirror on one cavity end and a bulk mirror or saturable absorber on the other end. The loop mirror can be further configured with an adjustable line phase delay to optimize modelocking. All intra-cavity fiber(s) can be polarization maintaining. Dispersion compensation components such as, e.g., dispersion compensation fibers, bulk diffraction gratings or fiber Bragg gratings may be included. The oscillators may include a bandpass filter to obtain high pulse energies when operating in the similariton regime. The oscillator output can be amplified and used whenever high power short pulses are required. For example the oscillators can be configured as frequency comb sources or supercontinuum sources. In conjunction with repetition rate modulation, applications include dual scanning delay lines and trace gas detection.

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