ライフサイエンスコーパス: very low temperature

1 stems (TLS) govern the physics of glasses at very low temperature.

2 d (3)He conforms to this picture but only at very low temperature.

3 ly high electrical conductivity even down to very low temperatures.

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

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

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

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

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

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

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

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

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

13 due to limitations of equipment operating in very low temperatures.

14 (25) nanoclusters as primary active sites at very low temperatures.

15 exes, has largely constrained their study to very low temperatures.

16 on that is observed in most metals cooled to very low temperatures.

17 ameter destroy the Abrikosov lattice even at very low temperatures.

18 istivity over hundreds of degrees, except at very low temperatures.

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

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

21 ting the observation of important effects to very low temperatures(2,3).

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

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

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

25 to orthorhombic (alpha-MoO(3)) structure at very low temperature (90 degrees C), using a green solve

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

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

28 At very low temperatures, ac magnetic susceptibility data s

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

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

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

32 These detectors operate at very low temperatures and generate a minimum of excess n

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

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

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

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

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

38 extreme mechanical response upon cooling to very low temperatures are relatively rare in the chemica

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

40 ata show that a disordered fluid persists to very low temperatures at high concentrations.

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

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

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

44 on problem of the variational free energy at very low temperatures; ii) such a ground state can be ac

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

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

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

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

49 the "PEG dilemma", and the stability at only very low temperatures limit their efficiency.

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

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

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

53 idence (multinuclear solid-state NMR down to very low temperatures, synchrotron radiation XRD, gas so

54 (2), which has an antiferromagnetic order at very low temperature (T(N) ~ 148 mK), and observed a fin

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

56 ons around cooler profiles expose embryos to very low temperatures that inhibit development, and to f

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

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

59 blation is a therapeutic technique that uses very low temperatures to destroy cells; transcutaneous c

60 hnology that features the ability to utilize very low temperature waste heat (as low as 40 C).

61 ity, magnetoresistance, and specific heat at very low temperatures, we trace modifications of the ant

62 ogical transport phenomena usually appear at very low temperatures, which sets challenges for applica

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