ライフサイエンスコーパス: very low temperature

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1 s generated by a vibrating grid resonator at very low temperatures.

2 m for the emergence of quantum turbulence at very low temperatures.

3 acterized in the gas phase or in matrices at very low temperatures.

4 en when the Michael addition is performed at very low temperatures.

5 act as a single electron-accepting moiety at very low temperatures.

6 o indicated that So1648 may function only at very low temperatures.

7 ssful isolation and X-ray crystallography at very low temperatures.

8 Mg(2+), and Ca(2+) form weaker complexes at very low temperatures.

9 h, in suspended insulating nanostructures at very low temperatures.

10 with a well-defined coiled-coil developed at very low temperatures.

11 es, unlike those of homeotherms, assemble at very low temperatures (-1.8 degrees C).

12 Depositions of 1 and 2 at very low temperatures (380-450 degrees C) produce near s

13 Rectification persisted at very low temperature (7 K), and was activationless betwe

14 The materials were extremely active at very low temperature (-80 degrees C) and also highly sta

15 At very low temperature, a modest beta-selectivity could be

16 At very low temperatures, a kinetic trap arising from the i

17 At very low temperatures, ac magnetic susceptibility data s

18 escribed are multinuclear NMR experiments at very low temperatures aimed at defining solution structu

19 At very low temperatures, an extra point contact feature wh

20 currently possible for individual isomers at very low temperature and observations of isomer mixtures

21 (within 2 kilometers of the seafloor), where very low temperatures and pressures exist.

22 d on the basis of experiments carried out at very low temperatures and shunt reactions, but their pre

23 e conclude that the CW state is preferred at very low temperatures and that it is relatively more hig

24 stance to probe both the insulating state at very low temperatures and the presence of superconductin

25 s make the proposed mechanism viable even at very low temperatures and under single-collision conditi

26 hexamer are the lowest energy structures at very low temperatures, as temperature is increased the c

27 rovement for the production of antimatter at very low temperatures (below 1 K).

28 ergy transfer prevails in a glassy matrix at very low temperature, but this is augmented by Dexter-ty

29 e we are familiar with hexagonal ice, but at very low temperature ice can exist in a different struct

30 ion has been observed by NMR spectroscopy at very low temperature in isopropyladamantane, 1-tert-buty

31 ibit slow relaxation of the magnetization at very low temperatures in a dc field.

32 two-dimensional electron system is cooled to very low temperatures, indicating that it arises from de

33 s from an insulating to a metallic state; at very low temperatures, it even transforms to a supercond

34 h materials include silicon and germanium at very low temperature (<100 K) and, at room temperature,

35 Work to date has required very low temperatures (on the order of -40 degrees C or

36 ty, proximity to the ferromagnetic state and very low temperatures required to test the theory defini

37 tructured W-Cr alloy, sintering sets on at a very low temperature that is commensurate with phase sep

38 ental data available for selected isomers at very low temperature, the present results provide quanti

39 Because the latter reaction occurs at very low temperature, the proton is most likely taken fr

40 Cooling spins to a very low temperature without cooling the environment cou

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