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(2014) to obtain exact forms), Λœπœ™(𝛽)=πœ™ 0 + 𝐻(𝛽, πœ™ βˆ—(𝛽,Λ‡πœ)) βˆ’1𝑒(𝛽, Λœπœ™(𝛽)) βˆ’π‘’(𝛽, πœ™ 0) , where Λ‡πœis in the line segment between𝑒(𝛽, Λœπœ™(𝛽)) and 𝑒(𝛽, πœ™ 0)

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2025 1

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