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In this section, we consider the total active average energy consumption in a cycle of active and sleep modes, denoted by Ecycle.
We obtain the normal modes, denoted by the N × N matrix M m, i α, by diagonalizing the vibrational Hamiltonian K α, M m, i α K m m ′ α M m ′, i ′ α = ω m α 2 δ i, i ′. (27).
The null set is a set consisting of all independent elementary modes, denoted by.
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The phonons in the system are counted by n ˆ m = a ˆ m † a ˆ m, for each mode denoted by m.
Since it has been JPEG compressed with quality factor QF1, D m, n AJ k would be a multiple of the quantization step of the (m,n th DCT mode (denoted by qm,n(QF1)).
The mode‐n product of X ∈ C I 1 × ⋯ × I N with A ∈ C J n × I n along the n th mode, denoted by X × n A, gives the tensor of order N and dimensions I1×⋯×In-1×J n ×In+1×⋯×I N, such as[47] y i 1, …, i n - 1, j n, i n + 1, …, i N = ∑ i n = 1 I n a j n, i n x i 1, …, i n - 1, i n, i n + 1, …, i N (12).
Then, the EEs of the DT mode and the TWRT mode are denoted by e dand e t, respectively.
The ECRs of the DT mode and the TWRT mode are denoted by η dand η t.
The EEs of the DT mode and the TWRT mode are denoted by e dand e t.
The average energy consumed per unit time switching from phase R of the active mode to the sleep mode is denoted by E RS.
The average energy consumed per unit time switching from the sleep mode to phase R of active mode is denoted by E SR.
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