ライフサイエンスコーパス: specific heat

1 y, moderate temperature coefficients and low specific heat.

2 s in phase space, leading to a small jump of specific heat.

3 ction, and measurements of magnetization and specific heat.

4 ng the phonon mean free path or reducing the specific heat.

5 al transition temperature, and its anomalous specific heat.

6 tical "soup." Here, we report a study of the specific heat across the phase diagram of the model syst

7 easurements of the magnetocaloric effect and specific heat allows a comprehensive study of the entrop

8 o 2 K from single crystal X-ray diffraction, specific heat and susceptibility measurements.

9 measurements of the magnetic susceptibility, specific heat, and electrical resistivity in the layered

10 as revealed through magnetic susceptibility, specific heat, and EPR.

11 Electrical resistivity, specific heat, and magnetization measurements to tempera

12 Using dc magnetization, ac susceptibility, specific heat, and neutron diffraction, we have studied

13 temperature, the anomalous structure in the specific heat, and the existence of multiple gaps in thi

14 e, where the order responsible for the sharp specific heat anomaly at T(0) = 17 K has remained uniden

15 We show that liquid energy and specific heat are given, to a very good approximation, b

16 ding resistivity, Hall coefficient (RH), and specific heat are reported.

17 thermal expansion coefficient, enthalpy and specific heat at constant pressure.

18 under cooling is more sudden and the jump of specific heat at the glass transition is generally large

19 ed pair separation fluctuation Delta(B), the specific heat C(v), the internal energy of the system E,

20 , where rho denotes density and C(P) denotes specific heat capacity at constant pressure.

21 Our results imply that the specific heat capacity change during channel gating is a

22 f sign in deltaCp(o)(T)(reaction) (change in specific heat capacity of reaction at constant pressure)

23 ese changes contribute to a reduction in the specific heat capacity upon binding.

24 romagnetically ordered state, the electronic-specific heat coefficient gamma approximately 1 J/mol x

25 del with a large zero-temperature electronic-specific heat coefficient that decreases with increasing

26 In terms of the implications for practice, specific heating conditions can be found to maintain a r

27 RNA folding parameters including specific heat, contact maps, simulation trajectories, gy

28 powder diffraction, dielectric constant, and specific heat data show that 1 undergoes an order-disord

29 tions of this system with susceptibility and specific-heat data, we show that both energy-level split

30 e as T4 and that the first correction to the specific heat due to this varies as T7; these are quite

31 maximum-entropy principle predicts negative specific heat for a stationary, magnetically self-confin

32 dependence of the electrical resistivity and specific heat in the paramagnetic state are consistent w

33 The electronic-specific heat in the paramagnetic state can be described

34 An anomaly in the specific heat is a classic signature of this phenomenon.

35 The second derivative, a specific heat-like quantity, shows a peak around a mean

36 ed temperature data displayed variability at specific heating loads resulting in larger variance of c

37 tween the dynamic crossover and the locus of specific heat maxima C(P)(max) ("Widom line") emanating

38 s to the presence at ambient pressure of two specific heat maxima.

39 that it produces a major contribution to the specific heat maximum at the Widom line.

40 expansion, magnetostriction, dielectric, and specific heat measurements on polycrystalline FeCr2S4 in

41 Recent specific heat measurements show quantum oscillations in

42 , electrical resistivity, magnetization, and specific heat measurements were performed on URu2-xFexSi

43 is probed via a combination of magnetometry, specific heat measurements, elastic and inelastic neutro

44 ntal techniques, including magnetization and specific heat measurements, inelastic neutron scattering

45 K are studied with X-ray powder diffraction, specific heat measurements, transmission electron micros

46 ANES) spectroscopy and making comparisons to specific heat measurements, we demonstrate the presence

47 O6+delta that is not identified in available specific heat measurements.

48 resistivity, AC magnetic susceptibility, and specific heat measurements.

49 Specific-heat measurements demonstrated that a large por

50 Here we present specific-heat measurements of Ce3Bi4Pt3 in d.c. and puls

51 Here we report specific-heat measurements of the pressure-tuned unconve

52 Here we present low-temperature specific-heat measurements of ultrastable glasses of ind

53 ude to describe approximately the electronic specific heat near the superconducting transition temper

54 re gain from artery to brain tissue, and the specific heat of blood, decreased by 45 +/- 11 % in para

55 egime by measuring the temperature-dependent specific heat of purified single-wall nanotubes.

56 idual nanotubes and differ markedly from the specific heat of two-dimensional graphene or three-dimen

57 One potential advantage of Mo is its higher specific heat of vaporization, which could lead to reduc

58 ange of experimentally accessible volumetric specific heats, our detection scheme should allow us to

59 equency and magnetic field dependence of the specific heat power produced during field-driven hystere

60 on-induced enhancement or suppression of the specific heat power, dependent on the intrinsic statisti

61 The melting temperatures from the specific heat profiles are in good agreement with the av

62 We conclude that an interaction between specific HEAT repeats in ATM and the C-terminal FXF/Y do

63 nd the flanking kinase-docking motif to bind specific HEAT repeats in Rad3.

64 we also derive the critical behavior of the specific heat, resistivity, thermopower, magnetization a

65 We show that the specific heat saturates in high magnetic fields.

66 In addition, specific heat, Seebeck coefficient, electric conductivit

67 Inhibition of proliferation was pathogen specific, heat sensitive, and multiplicity of infection

68 eed to determine the mortality projection of specific heat-sensitive diseases to provide more detaile

69 s reveals that the mutants have growth stage-specific heat sensitivity.

70 HSF2 heterotrimeric complexes recruited to a specific heat shock element in the AIRAP promoter.

71 Both systems modulate the induction of specific heat shock genes.

72 adjuvant (OVA/aluminum hydroxide) and CD8(+)-specific heat shock protein-based (gp96-Ig) vaccine appr

73 t HSR induction with increased expression of specific heat shock proteins that was variable across ti

74 of the supercritical state and discover that specific heat shows a crossover between two different re

75 The temperature dependence of the specific heat shows that the folding temperature (T(F))

76 A set of 25 species and protein-specific heat stable peptide markers has been detected i

77 rapid and is insensitive to PKI, the highly specific heat-stable protein kinase inhibitor.

78 me-series analyses to estimate the community-specific heat wave-mortality relation over lags of 0-10

79 ermal conductivity, thermal diffusivity, and specific heat were determined.

80 Thermal conductivity and specific heat were, respectively 0.14 +/- 0.007 W/mK and

81 greement between calculated and experimental specific heat with no free-fitting parameters.

82 We also compare the measured specific heat with some usual types of transitions, whic