Measurements of [Formula Presented] decays into vector-tensor final states
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Bai, J Z
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Ban, Y
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Bian, J G
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Cai, X
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Chang, J F
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Chen, H F
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Chen, H S
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Chen, H X
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Chen, J
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Chen, J C
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Chen, Jun
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Chen, M L
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Chen, Y B
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Chi, S P
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Chu, Y P
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Cui, X Z
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Dai, H L
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Dai, Y S
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Deng, Z Y
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Dong, L Y
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Du, S X
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Du, Z Z
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Fang, J
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Fang, S S
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Fu, C D
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Fu, L P
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Gao, C S
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Gao, M L
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Gao, Y N
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Gong, M Y
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Gong, W X
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Gu, S D
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Guo, Y N
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Guo, Y Q
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Guo, Z J
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Han, S W
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Harris, F A
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He, J
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He, K L
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He, M
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He, X
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Heng, Y K
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Hu, H M
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Hu, T
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Huang, G S
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Huang, L
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Huang, X P
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Ji, X B
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Jia, Q Y
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Jiang, C H
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Jiang, X S
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Jin, D P
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Jin, S
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Jin, Y
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Lai, Y F
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Li, F
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Li, G
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Li, H H
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Li, J
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Li, J C
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Li, Q J
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Li, R B
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Li, R Y
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Li, S M
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Li, W
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Li, W G
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Li, X L
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Li, X Q
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Li, X S
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Liang, Y F
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Liao, H B
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Liu, C X
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Liu, Fang
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Liu, F
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Liu, H M
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Liu, J B
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Liu, J P
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Liu, R G
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Liu, Y
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Liu, Z A
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Liu, Z X
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Lu, G R
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Lu, F
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Lu, J G
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Luo, C L
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Luo, X L
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Ma, F C
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Ma, J M
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Ma, L L
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Ma, X Y
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Mao, Z P
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Meng, X C
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Mo, X H
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Nie, J
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Nie, Z D
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Olsen, S L
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Peng, H P
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Qi, N D
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Qian, C D
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Qin, H
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Qiu, J F
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Ren, Z Y
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Rong, G
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Shan, L Y
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Shang, L
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Shen, D L
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Shen, X Y
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Sheng, H Y
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Shi, F
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Shi, X
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Song, L W
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Sun, H S
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Sun, S S
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Sun, Y Z
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Sun, Z J
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Tang, X
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Tao, N
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Tian, Y R
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Tong, G L
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Varner, G S
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Wang, D Y
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Wang, J Z
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Wang, L
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Wang, L S
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Wang, M
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Wang, Meng
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Wang, P
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Wang, P L
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Wang, S Z
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Wang, W F
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Wang, Y F
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Wang, Zhe
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Wang, Z
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Wang, Zheng
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Wang, Z Y
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Wei, C L
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Wu, N
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Wu, Y M
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Xia, X M
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Xie, X X
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Xin, B
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Xu, G F
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Xu, H
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Xu, Y
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Xue, S T
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Yan, M L
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Yan, W B
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Yang, F
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Yang, H X
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Yang, J
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Yang, S D
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Yang, Y X
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Yi, L H
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Yi, Z Y
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Ye, M
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Ye, M H
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Ye, Y X
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Yu, C S
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Yu, G W
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Yuan, C Z
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Yuan, J M
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Yuan, Y
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Yue, Q
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Zang, S L
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Zeng, Y
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Zhang, B X
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Zhang, B Y
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Zhang, C C
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Zhang, D H
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Zhang, H Y
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Zhang, J
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Zhang, J M
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Zhang, J Y
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Zhang, J W
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Zhang, L S
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Zhang, Q J
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Zhang, S Q
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Zhang, X M
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Zhang, X Y
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Zhang, Yiyun
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Zhang, Y J
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Zhang, Y Y
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Zhang, Z P
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Zhang, Z Q
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Zhao, D X
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Zhao, J B
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Zhao, J W
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Zhao, P P
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Zhao, W R
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Zhao, X J
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Zhao, Y B
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Zhao, Z G
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Zheng, H Q
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Zheng, J P
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Zheng, L S
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Zheng, Z P
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Zhong, X C
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Zhou, B Q
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Zhou, G M
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Zhou, L
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Zhou, N F
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Zhu, K J
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Zhu, Q M
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Zhu, Yingchun
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Zhu, Y C
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Zhu, Y S
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Zhu, Z A
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Zhuang, B A
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Zou, B S
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For the first three decays, we use the PDG recommended values of the (Formula presented) branching fractions. For (Formula presented) decay to (Formula presented) there is poor consistency between the existing measurement, Mark II, and DM2. Instead of the PDG average with 50% error, we use the data of DM2, which was a high statistics measurement, giving smaller errors and including the interference with (Formula presented)
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For the first three decays, we use the PDG recommended values of the (Formula presented) branching fractions. For (Formula presented) decay to (Formula presented) there is poor consistency between the existing measurement, Mark II, and DM2. Instead of the PDG average with 50% error, we use the data of DM2, which was a high statistics measurement, giving smaller errors and including the interference with (Formula presented)
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