Yingpeng Zhao
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Research Subjects
Yingpeng Zhao has a total of 36 co-authors. Here are the top co-authors by number of shared publications:
- Qiang Lin
State Key Laboratory of Ocean Sensing, Institute of Quantum Sensing, School of Physics, Zhejiang University, Hangzhou 310058, China
6 shared publications - Bin Wu
Key Laboratory of Quantum Precision Measurement of Zhejiang Province, School of Physics, Zhejiang University of Technology, Hangzhou, China
4 shared publications - Xiaolong Wang
Key Laboratory of Quantum Precision Measurement of Zhejiang Province, College of Science, Zhejiang University of Technology, Hangzhou 310023, China
4 shared publications - Bing Cheng
Key Laboratory of Quantum Precision Measurement of Zhejiang Province, School of Physics, Zhejiang University of Technology, Hangzhou, China
3 shared publications - Bing Cheng
Zhejiang University of Technology
3 shared publications - Dianrong Li
Zhejiang Provincial Key Laboratory of Quantum Precision Measurement, College of Science, Zhejiang University of Technology, Hangzhou 310023, China
3 shared publications
Latest Publications
- Open Access
Realization of the Compact Magneto-Optical Trap Based on Single Laser with Frequency Modulation
In cold atom physics, the complexity of traditional magneto-optical trap system limits the use of their associated instruments for field applications in atomic physics, such as gravity mapping, space navigation and deep space exploration. This study introduces a novel compact MOT design that addresses these issues by simplifying the structure and reducing the size. The height of the unit is 0.7 m, the volume is and the mass is 11.32 kg. The new design utilizes a single laser to generate the two different frequencies needed for laser cooling by internally splitting the beam, shifting the frequency and then combining them, effectively controlling both the cooling and repumping beams. The compact vacuum chamber optical path, in conjunction with the magnetic field, facilitates the capture of 87Rb atoms in an ultra-high vacuum environment. Experimental results demonstrate an atom loading rate of up to 87Rb atoms per second, confirming the system’s effectiveness in capturing and cooling 87Rb atoms. This design provides a flexible and portable solution, offering valuable insights for the advancement of compact MOT and its applications in cold atom physics.Open AccessRealization of the Compact Magneto-Optical Trap Based on Single Laser with Frequency Modulation
In cold atom physics, the complexity of traditional magneto-optical trap system limits the use of their associated instruments for field applications in atomic physics, such as gravity mapping, space navigation and deep space exploration. This study introduces a novel compact MOT design that addresses these issues by simplifying the structure and reducing the size. The height of the unit is 0.7 m, the volume is and the mass is 11.32 kg. The new design utilizes a single laser to generate the two different frequencies needed for laser cooling by internally splitting the beam, shifting the frequency and then combining them, effectively controlling both the cooling and repumping beams. The compact vacuum chamber optical path, in conjunction with the magnetic field, facilitates the capture of 87Rb atoms in an ultra-high vacuum environment. Experimental results demonstrate an atom loading rate of up to 87Rb atoms per second, confirming the system’s effectiveness in capturing and cooling 87Rb atoms. This design provides a flexible and portable solution, offering valuable insights for the advancement of compact MOT and its applications in cold atom physics. - 25 October 2024
- Published by Institute of Electrical and Electronics Engineers (IEEE) in IEEE Sensors Journal
- Vol. 24 (24) , 40507-40517
The Implementation of a Compact Cold Atom Interference Gyroscope Based on Miniaturized Quartz Vacuum Chamber
The Cold Atom Interference Gyroscope (CAIG) offer substantial potential for rotation measurement due to the high sensitivity and stability. The CAIG with a fountain configuration realized by 4-pulse could provide a larger interference-loop area, and enhanced performance. However, this kind of CAIG is usually much larger and higher since it requires a vacuum chamber with sufficient height to achieve a long Raman pulse interval. We demonstrate a 4-pulse CAIG based on a miniaturized vacuum chamber that enables portable and transportable rotation rate measurements. The main vacuum chamber is realized by whole glass material. The height of the vacuum unit is 0.7 m, the volume is 8.86 × 10 4 cm 3 and the mass is 75 kg. Then, we estimated the performance of our portable CAIG in the environment of the underground laboratory and the fifth-floor office building. In the laboratory, the sensitivities of the homemade CAIG is 4.44 × 10 −6 rad/s/√Hz with an interrogation time of 55 ms and an interference area of 25 mm 2 . In addition, we measured the angular velocity of the Earth, the relative error is 2.4%. Furthermore, we transported the CAIG to the fifth floor of the office building, which is near the subway. Ultimately, the CAIG achieved a sensitivity of 5.47 × 10 −4 rad/s/√Hz. Additionally, the theoretical maximum interrogation time achieved by this CAIG is 124 ms corresponding to a sensitivity of 5.62 × 10 −8 /√Hz. Our new design of the compact CAIG could provide novel insights into the miniaturization of CAIGs, while also pointing out areas for further improvement.
- 25 October 2024
- Published by Institute of Electrical and Electronics Engineers (IEEE) in IEEE Sensors Journal
- Vol. 24 (24) , 40507-40517
The Implementation of a Compact Cold Atom Interference Gyroscope Based on Miniaturized Quartz Vacuum Chamber
The Cold Atom Interference Gyroscope (CAIG) offer substantial potential for rotation measurement due to the high sensitivity and stability. The CAIG with a fountain configuration realized by 4-pulse could provide a larger interference-loop area, and enhanced performance. However, this kind of CAIG is usually much larger and higher since it requires a vacuum chamber with sufficient height to achieve a long Raman pulse interval. We demonstrate a 4-pulse CAIG based on a miniaturized vacuum chamber that enables portable and transportable rotation rate measurements. The main vacuum chamber is realized by whole glass material. The height of the vacuum unit is 0.7 m, the volume is 8.86 × 10 4 cm 3 and the mass is 75 kg. Then, we estimated the performance of our portable CAIG in the environment of the underground laboratory and the fifth-floor office building. In the laboratory, the sensitivities of the homemade CAIG is 4.44 × 10 −6 rad/s/√Hz with an interrogation time of 55 ms and an interference area of 25 mm 2 . In addition, we measured the angular velocity of the Earth, the relative error is 2.4%. Furthermore, we transported the CAIG to the fifth floor of the office building, which is near the subway. Ultimately, the CAIG achieved a sensitivity of 5.47 × 10 −4 rad/s/√Hz. Additionally, the theoretical maximum interrogation time achieved by this CAIG is 124 ms corresponding to a sensitivity of 5.62 × 10 −8 /√Hz. Our new design of the compact CAIG could provide novel insights into the miniaturization of CAIGs, while also pointing out areas for further improvement.
- Open Access
- 10 June 2024
- Published by Institute of Electrical and Electronics Engineers (IEEE) in IEEE Sensors Journal
- Vol. 24 (15) , 23527-23536
Construction of Absolute Gravity Benchmark Offshore With an Atomic Gravimeter
Marine gravity survey is of great significance to the fields of geophysics research, marine geological mapping, and so on. Usually, accuracy calibration is required since the gravity measurements remain relative at present. For this application, the absolute gravity reference point is necessary, which can be established with classical optical absolute gravimeters. In this paper, an absolute gravity benchmark is constructed through a gravity measurement system based on a homemade atomic gravimeter at the quay of Zhoushan Archipelago. Even in the rugged environment of seaboard, a measurement sensitivity of 0.76 mGal/√Hz is obtained. Besides, the estimated absolute accuracy of gravity is better than 30 μGal. Interestingly, it is found that the accuracy has been affected greatly by the ocean tidal loading (OTL) effect, especially the absence of an accurate OTL model in the observation region. In order to further investigate the OTL effect, the continuous absolute gravity observations are carried out for 7 days, collecting tidal heights as well. Notably, a peak-to-peak amplitude of approximately 170 μGal is obtained even when the gravity variations caused by solid tide effect have been corrected. However, the calculated values with the existing OTL models seem much smaller than the actual gravity variation data. To solve this problem, an optimized OTL model for offshore gravity measurement has been proposed through an analysis of the existing models. With the improved model of OTL, the calculated results agree well the experimental data. These findings offer valuable insights for the high-precision calibration of marine gravimeters.
- 10 June 2024
- Published by Institute of Electrical and Electronics Engineers (IEEE) in IEEE Sensors Journal
- Vol. 24 (15) , 23527-23536
Open AccessConstruction of Absolute Gravity Benchmark Offshore With an Atomic Gravimeter
Marine gravity survey is of great significance to the fields of geophysics research, marine geological mapping, and so on. Usually, accuracy calibration is required since the gravity measurements remain relative at present. For this application, the absolute gravity reference point is necessary, which can be established with classical optical absolute gravimeters. In this paper, an absolute gravity benchmark is constructed through a gravity measurement system based on a homemade atomic gravimeter at the quay of Zhoushan Archipelago. Even in the rugged environment of seaboard, a measurement sensitivity of 0.76 mGal/√Hz is obtained. Besides, the estimated absolute accuracy of gravity is better than 30 μGal. Interestingly, it is found that the accuracy has been affected greatly by the ocean tidal loading (OTL) effect, especially the absence of an accurate OTL model in the observation region. In order to further investigate the OTL effect, the continuous absolute gravity observations are carried out for 7 days, collecting tidal heights as well. Notably, a peak-to-peak amplitude of approximately 170 μGal is obtained even when the gravity variations caused by solid tide effect have been corrected. However, the calculated values with the existing OTL models seem much smaller than the actual gravity variation data. To solve this problem, an optimized OTL model for offshore gravity measurement has been proposed through an analysis of the existing models. With the improved model of OTL, the calculated results agree well the experimental data. These findings offer valuable insights for the high-precision calibration of marine gravimeters.
- Open Access
- 16 February 2024
- Published by Institute of Electrical and Electronics Engineers (IEEE) in IEEE Sensors Journal
- Vol. 24 (7) , 9536-9544
Construction of a Test Field for Relative Gravimeters in a Cave With a Cold Atom Gravimeter
The Earth’s gravity field is complex and variable. Performance evaluation of gravimeter requires gravity fields with well-known absolute gravity values. The aim of this study is to utilize an in-house developed Cold Atom Gravimeter (CAG-E) in conjunction with CG-5 to establish a comprehensive test field consisting of 13 gravity datums at different altitudes. This absolute gravity field can be used for testing multiple relative gravimeters at the same time. The additional theoretical model calculations of this test field can provide a reference for gravity values at different heights, and a three-dimensional test field can be constructed in the future. In addition, a detailed performance evaluation of CAG-E was performed where the accuracy of the instrument repeatability was found to be 4.8 μGal. Finally, a correction of the geological density of the mountain was carried out using the absolute gravity values, and a minimum gravity difference residual of 0.9 μGal was obtained. These results verify the reliability of this test field for relative gravimeters.
- 16 February 2024
- Published by Institute of Electrical and Electronics Engineers (IEEE) in IEEE Sensors Journal
- Vol. 24 (7) , 9536-9544
Open AccessConstruction of a Test Field for Relative Gravimeters in a Cave With a Cold Atom Gravimeter
The Earth’s gravity field is complex and variable. Performance evaluation of gravimeter requires gravity fields with well-known absolute gravity values. The aim of this study is to utilize an in-house developed Cold Atom Gravimeter (CAG-E) in conjunction with CG-5 to establish a comprehensive test field consisting of 13 gravity datums at different altitudes. This absolute gravity field can be used for testing multiple relative gravimeters at the same time. The additional theoretical model calculations of this test field can provide a reference for gravity values at different heights, and a three-dimensional test field can be constructed in the future. In addition, a detailed performance evaluation of CAG-E was performed where the accuracy of the instrument repeatability was found to be 4.8 μGal. Finally, a correction of the geological density of the mountain was carried out using the absolute gravity values, and a minimum gravity difference residual of 0.9 μGal was obtained. These results verify the reliability of this test field for relative gravimeters.
- Open Access
Improved Accuracy for Measurement of Filament Diameter Based on Image-Based Fitting Method
Laser diffraction (LD) has many obvious advantages for measuring. However, the measurement accuracy is limited by a number of factors, such as imaging noise, sensor threshold, and fitting methods. In this paper, we present a novel method for measuring filament diameter based on image-based fitting, which maintains more information. Before fitting the diffraction image, image processing is applied to solve the problem of image noise and the non-linear response of the charge-coupled device (CCD). Then, a fitting formula is established based on the distribution of laser intensity on a diffraction image, and the fitted results are solved with the Levenberg–Marquardt (LM) algorithm. Finally, the initial parameters of a fit are obtained by calculation, which speeds up the calculation and improves the accuracy of the fitting. The measurement accuracy of this method is verified by experimental and theoretical analysis. In experiments, the filament diameters of 125 and 125.2 μm are measured with a relative error of approximately 0.12%, Furthermore, the superiority of this method is demonstrated by comparing the measurements with other methods. To verify the stability of the measurements, filament diameters of 110–180 μm are chosen to be measured with a relative standard deviation of less than 0.14%.
Open AccessImproved Accuracy for Measurement of Filament Diameter Based on Image-Based Fitting Method
Laser diffraction (LD) has many obvious advantages for measuring. However, the measurement accuracy is limited by a number of factors, such as imaging noise, sensor threshold, and fitting methods. In this paper, we present a novel method for measuring filament diameter based on image-based fitting, which maintains more information. Before fitting the diffraction image, image processing is applied to solve the problem of image noise and the non-linear response of the charge-coupled device (CCD). Then, a fitting formula is established based on the distribution of laser intensity on a diffraction image, and the fitted results are solved with the Levenberg–Marquardt (LM) algorithm. Finally, the initial parameters of a fit are obtained by calculation, which speeds up the calculation and improves the accuracy of the fitting. The measurement accuracy of this method is verified by experimental and theoretical analysis. In experiments, the filament diameters of 125 and 125.2 μm are measured with a relative error of approximately 0.12%, Furthermore, the superiority of this method is demonstrated by comparing the measurements with other methods. To verify the stability of the measurements, filament diameters of 110–180 μm are chosen to be measured with a relative standard deviation of less than 0.14%.
- Open Access
A Simplified Laser System for Atom Interferometry Based on a Free-Space EOM
In this paper, a compact laser system for 87Rb atom interferometry based on only one free-space electro-optic modulator (EOM) was realized, where repumping and Raman beams were generated with a free-space EOM. In addition, this laser system does not require a laser amplifier compared to fibered EOM since fibered EOM cannot transmit high-power lasers. However, due to the narrow modulation linewidth of free-space EOM, it is impossible to obtain the frequencies of repumping and Raman beams separately, which would lead to some complicated effects. Therefore, a theoretical analysis was carried out to solve this problem, and a new frequency scheme for AI is proposed. For the experiment, the laser system of AI was built up. Moreover, the atomic interference fringes were obtained with a contrast of 20.7% (T = 60 ms) and the fitted phase resolution is approximately 1.25 mrad. The presented laser system could provide a new solution for compact AI systems in the future.
Open AccessA Simplified Laser System for Atom Interferometry Based on a Free-Space EOM
In this paper, a compact laser system for 87Rb atom interferometry based on only one free-space electro-optic modulator (EOM) was realized, where repumping and Raman beams were generated with a free-space EOM. In addition, this laser system does not require a laser amplifier compared to fibered EOM since fibered EOM cannot transmit high-power lasers. However, due to the narrow modulation linewidth of free-space EOM, it is impossible to obtain the frequencies of repumping and Raman beams separately, which would lead to some complicated effects. Therefore, a theoretical analysis was carried out to solve this problem, and a new frequency scheme for AI is proposed. For the experiment, the laser system of AI was built up. Moreover, the atomic interference fringes were obtained with a contrast of 20.7% (T = 60 ms) and the fitted phase resolution is approximately 1.25 mrad. The presented laser system could provide a new solution for compact AI systems in the future.