ライフサイエンスコーパス: decay to (the|a)

1 membrane suspensions at 35 degrees C and its decay to a 380 nm absorbing species being less complete

2 rmed that this mechanism couples CsrB/C sRNA decay to the availability of a preferred carbon source.

3 d as a ferric-(hydro)peroxo species, and its decay to the carboxylate-ligated ferric [Fe(NHis)(4)(SCy

4 sequent fluorescence enhancement upon (64)Cu decay to the daughter isotopes (64)Ni and (64)Zn.

5 us HuNoV, results ranged from no significant decay to a decay rate constant ("k") of 2.2 day(-1).

6 Instead, diversity will decay to a depauperate steady state in two phases.

7 The decay to a diamagnetic state is complete and no paramagn

8 ter, and (iv) the diiron(III,IV) core and W* decay to the diiron(III) product by a common mechanism.

9 enerated multiple carriers, which ultimately decay to the edges of the dispersive bands by means of I

10 n isolated base pair initiates non-radiative decay to the electronic ground state.

11 lves from an initial regime of slow capacity decay to a fast decay regime, due to catastrophic electr

12 The peroxy species decay to a ferryl intermediate, with a peak at 578 nm ve

13 However, the transient decay to the fixed point depends highly on initial condi

14 e biradical 1-OS displayed an unusually slow decay to the ground state (1-CS) due to a large energy b

15 Decay to the ground state in 100 ns is the primary loss

16 The decay to the ground state occurs along a second reaction

17 However, this state does not decay to the ground state of [Formula: see text]Tb, nega

18 try in 39 fs, followed by a multiexponential decay to the ground state on the 1-100 ps time scale.

19 at subsequently undergoes rapid nonradiative decay to the ground state via a short-lived intermediate

20 ctrons into the conduction band, the rate of decay to the ground state, and dimensions of the ferroel

21 complex to the ZnP subunit, competitive with decay to the ground state, leads to the isoenergetic lon

22 tural relaxation, and the MLCT excited-state decay to the ground state, respectively.

23 iscuss the proposed mechanisms for ultrafast decay to the ground state, that involve conical intersec

24 from high CT state energies through a slower decay to the ground state.

25 e charge-separated state is competitive with decay to the ground state.

26 hat arise due to energy transfer and loss by decay to the ground state.

27 uanine which are necessary for the ultrafast decay to the ground state.

28 the protein in red light and by its thermal decay to the L intermediate.

29 ur interpretation and indicate an electronic decay to the npi* state.

30 were present, some subjects exhibited rapid decay to the original baseline, while others persisted i

31 ot to a level > 1 microM, followed by a slow decay to a plateau of approximately 0.5 microM.

32 an initial peak (mean 1.6 pA/pF) followed by decay to the point that submembrane [Ca(2+)] reached ~10

33 with one axial ligand from each protein and decay to the products with rate constants of 0.4-3 s(-1)

34 ve intermediate (NI), which undergoes a slow decay to the resting enzyme in the absence of substrate.

35 MD2, and UPF3 inhibit nonsense-mediated mRNA decay to the same extent; and an analysis of the possibl

36 high-dimensional firing-rate vectors rapidly decay to a single mode.

37 ference in 1 hr, followed by a slow activity decay to a stable, level plateau approximately 30-40% be

38 permeability with an early peak, followed by decay to a steady level.

39 piking frequency (Fi) followed by a variable decay to a steady-state firing frequency (Fss).

40 reactive singlet state of oxygen (O(2)) can decay to the triplet ground state nonradiatively in the