Mixed experience sampling for off-policy reinforcement learning
Yu, Jiayu, Li, Jingyao, Lü, Shuai, Han, Shuai
Published in Expert systems with applications (01.10.2024)
Published in Expert systems with applications (01.10.2024)
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Consistency regularization-based mutual alignment for source-free domain adaptation
Lü, Shuai, Li, Zongze, Zhang, Xinyu, Li, Jingyao
Published in Expert systems with applications (01.05.2024)
Published in Expert systems with applications (01.05.2024)
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Construction of emissive ruthenium(II) metallacycle over 1000 nm wavelength for in vivo biomedical applications
Xu, Yuling, Li, Chonglu, Lu, Shuai, Wang, Zhizheng, Liu, Shuang, Yu, Xiujun, Li, Xiaopeng, Sun, Yao
Published in Nature communications (14.04.2022)
Published in Nature communications (14.04.2022)
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Explorer-Actor-Critic: Better actors for deep reinforcement learning
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Published in Information sciences (01.03.2024)
Published in Information sciences (01.03.2024)
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Formation of Planar Chiral Platinum Triangles via Pillar[5]arene for Circularly Polarized Luminescence
Zhu, Huangtianzhi, Li, Qi, Shi, Bingbing, Xing, Hao, Sun, Yan, Lu, Shuai, Shangguan, Liqing, Li, Xiaopeng, Huang, Feihe, Stang, Peter J
Published in Journal of the American Chemical Society (14.10.2020)
Published in Journal of the American Chemical Society (14.10.2020)
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Guided deterministic policy optimization with gradient-free policy parameters information
Shen, Chun, Zhu, Sheng, Han, Shuai, Gong, Xiaoyu, Lü, Shuai
Published in Expert systems with applications (30.11.2023)
Published in Expert systems with applications (30.11.2023)
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Entropy regularization methods for parameter space exploration
Han, Shuai, Zhou, Wenbo, Lü, Shuai, Zhu, Sheng, Gong, Xiaoyu
Published in Information sciences (01.04.2023)
Published in Information sciences (01.04.2023)
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Sampling diversity driven exploration with state difference guidance
Lu, Jiayi, Han, Shuai, Lü, Shuai, Kang, Meng, Zhang, Junwei
Published in Expert systems with applications (01.10.2022)
Published in Expert systems with applications (01.10.2022)
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