Yb⁺
High power low noise laser for optical tweezers
| Real photos | Wavelength | Power | Introduction | Features |
 | 486.78nm | 0.05-6W | Used for Ytterbium atom Rydberg, magic wavelength, optical tweezers. Realized by thulium-doped fiber laser and frequency quadrupling. |
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 | 759nm | 1.5W-10W | Used in ytterbium atomic optical clocks, magic wavelength. Achieved by frequency summing of two low-noise lasers |
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Narrow linewidth lasers for quantum state manipulation and excitation of atoms
In order to achieve a laser covering multiple wavelengths from the ground state to the excited state of cesium atoms, Precilasers has launched a widely tunable laser that perfectly combines the wide tuning characteristics of external cavity diode lasers and the high power characteristics of fiber amplifiers.
| Real photos | Wavelength | Power | Introduction | Features |
 | 302nm | 0.1-1W | The 1974nm thulium-doped fiber DFB laser is frequency-doubled to produce a 987nm laser. The 1555nm fixed external cavity semiconductor laser seed passes through an erbium-doped fiber amplifier and then frequency-doubles with the 987nm laser to produce a 604nm laser. After cavity frequency doubling, a high-power 302nm laser is produced. |
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| 369nm | 0.5-4W | 1108nm Ytterbium-doped Fiber DFB Frequency Tripler |
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 | 399nm | 0.04-2W | The detection light of ytterbium atoms. The 1596nm fiber DFB laser can generate a high-power 798nm laser after single-pass frequency doubling. The 798nm single-pass frequency doubling can output 40mW of 399nm laser. For higher power, cavity frequency doubling is required to generate a 399nm laser with a maximum power of 1.5W. |
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 | 556nm | 0.5-20W | 1112nm Ytterbium-doped Fiber DFB Frequency Doubling |
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| | 578nm | 0.5-5W | The 1156nm fiber DFB seed laser passes through a low-noise Raman amplifier and then outputs a maximum of 5W of 578nm laser light in a single pass. |
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 | 639nm | 0.5-10W | Based on single-frequency seed laser, fiber laser amplification and high-efficiency frequency conversion technology, it can provide narrow linewidth laser of 639nm |
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| 770nm | 0.2-6W | High-power narrow-linewidth laser output based on high-power, low-noise erbium-doped fiber amplification and frequency doubling technology. |
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 | 1389nm | 1-15W | Used for Ytterbium atomic optical clock. The 1389nm fixed external cavity semiconductor laser is output after passing through the Raman amplifier. |
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 | 1539nm | 2-40W | The 1539nm fixed external cavity semiconductor laser seed is directly output after passing through the erbium-doped fiber amplifier |
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Widely tunable lasers
In order to achieve a laser covering multiple wavelengths from the ground state to the excited state of cesium atoms, Precilasers has launched a widely tunable laser that perfectly combines the wide tuning characteristics of external cavity semiconductor lasers and the high power characteristics of fiber amplifiers.
| Real photos | Wavelength | Power | Introduction | Features |
| | 302nm | 0.1W-1W | The 1974nm thulium-doped fiber DFB laser is frequency-doubled to produce a 987nm laser. The 1555nm wide-tuned external cavity diode laser seed passes through an erbium-doped fiber amplifier and then frequency-doubles with the 987nm laser to produce a 604nm laser. After cavity frequency doubling, a high-power 302nm laser is produced. |
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Frequency Stabilization and Other Accessories
The excitation of the Rydberg state of cesium atoms requires that the laser wavelength be accurately aligned with the transition spectrum of the atom and that the wavelength be kept stable for a long time. Precilasers has also launched corresponding frequency stabilization solutions.
| Real photos | name | Frequency stability | Introduction | Features |
 | Hertz level ultra-stable laser system | <0.5Hz/50Hz | Based on the PDH frequency stabilization method, the laser is locked to a high-precision and portable ultra-stable laser system to achieve the narrowing of the laser line width. |
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[1] Ma, S., Liu, G., Peng, P.et al.High-fidelity gates and mid-circuit erasure conversion in an atomic qubit.Nature622, 279–284 (2023).