ライフサイエンスコーパス: specific heat

1 operties such as viscosity, molar weight, or specific heat.

2 ntropy of spin ice without an anomaly in the specific heat.

3 ergy and contribute to the anomalously large specific heat.

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

5 y, moderate temperature coefficients and low specific heat.

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

7 ction, and measurements of magnetization and specific heat.

8 al transition temperature, and its anomalous specific heat.

9 e of a graphene monolayer with extremely low specific heat(14) as the active material.

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

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

12 The calculated specific heat also compares very favorably with experime

13 Temperature-dependent specific heat and (31)P NMR measurements provide evidenc

14 We also find a T ln(1/T) specific heat and a rationale for the Planckian bound on

15 We use specific heat and ac magnetic susceptibility experiments

16 the second derivatives of Gibbs free energy (specific heat and compressibility) diverge at the transi

17 ivity and magnetic torque measurements, plus specific heat and DC magnetization data, we observed a r

18 ystematically investigate the magnetization, specific heat and electrical transport down to low tempe

19 spin susceptibility, and finite temperature-specific heat and entropy corroborate the gapped and gap

20 s doping, the temperature dependences of the specific heat and longitudinal resistivity display non-F

21 th the normal and superconducting states via specific heat and magnetic torque measurements and first

22 Thermal expansion, specific heat and magnetization measurements of the dope

23 Here we present our bulk magnetization, specific heat and neutron scattering studies on single c

24 Measurements of the specific heat and resistivity under pressure demonstrate

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

26 gnetic state is accompanied by a jump in the specific heat and the opening of a spectral gap(1).

27 To utilize the minute electronic specific heat and thermal conductivity of graphene, we d

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

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

30 tal CeRu(4)Sn(6) by magnetic susceptibility, specific heat, and inelastic neutron scattering experime

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

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

33 del for SmB(6) (mixed valent, with a peak in specific heat, and pressure induced magnetic phase trans

34 films such as thermal boundary conductance, specific heat, and sound speed from room temperature to

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

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

37 ase transition/crossover gives rise to large specific heat anomaly, both datasets point towards a lar

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

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

40 series of sharp double-peak features in the specific heat as a function of the magnetic field.

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

42 usly EuB(6) (possessing an anomalous peak in specific heat at low T, magnetic phase transitions, and

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

44 netic susceptibility, magnetoresistance, and specific heat at very low temperatures, we trace modific

45 Here we measure the specific heat C of the cuprates Eu-LSCO and Nd-LSCO at l

46 dy of quantum oscillations in the electronic specific heat C(el) in natural graphite.

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

48 sing the two-band model, the superconducting specific heat can be well described with two energy gaps

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

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

51 of these low-lying modes by low-temperature specific heat capacity measurement as well as Raman spec

52 p innovative correlations for estimating the specific heat capacity of mono-nanofluids.

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

54 e found to correlate strongly with gas phase specific heat capacity of the adsorbate.

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

56 ates and the device's electronic entropy and specific heat capacity.

57 Rather than finding an electronic specific heat characteristic of broad f-electron bands i

58 We performed specific heat characterization and T(c)-distribution ana

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

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

61 peratures, the temperature dependence of the specific-heat coefficient is logarithmically divergent a

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

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

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

65 Combining these specific heat data with existing longitudinal thermopowe

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

67 mperature susceptibility (down to 0.3 K) and specific heat (down to 0.055 K) of (NEt(4))(2)[Co(2)(H(2

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

69 s that key thermodynamic properties, such as specific heat, electron-phonon coupling and superfluid s

70 o [Formula: see text] corroborating previous specific heat experiments.

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

72 t this reanalysis implies an anomalously low specific heat for the metallic fluid that is clearly inc

73 ology that provides thermally tunable, tumor-specific heat generation.

74 erature glassy features in the corresponding specific heat (i.e., "boson peak" -BP-) and vibrational

75 near resistivity and a T log(1/T) electronic specific heat in a field-tuned quantum critical fan.

76 mechanism for the anomalous behavior of the specific heat in low-temperature amorphous solids.

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

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

79 Below T(c), the electronic specific heat initially decreases in T(3) behavior (1.5

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

81 ntly, the linear coefficient of the magnetic specific heat is large in the same temperature regime, i

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

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

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

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

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

87 Specific heat measurements also show magnetic correlatio

88 Here, we report on time-resolved specific heat measurements at filling factor 5/2, and we

89 Here, we show that thermal conductivity and specific heat measurements in insulating YbIr(3)Si(7) re

90 Electrical transport and specific heat measurements indicate a Curie temperature

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

92 Recent specific heat measurements show quantum oscillations in

93 Both magnetic susceptibility and specific heat measurements show that 1 does not undergo

94 Specific heat measurements show that these films, which

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

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

97 n scattering (VT-INS), DC susceptibility and specific heat measurements, high-field electron spin res

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

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

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

101 ration depth, nuclear magnetic resonance and specific heat measurements.

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

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

104 Specific-heat measurements demonstrated that a large por

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

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

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

108 ture of the nanoparticles is complemented by specific-heat measurements, which further support the la

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

110 holographic correspondence to determine the specific heat of a two-dimensional interacting gapless M

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

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

113 etermine the effect interactions have in the specific heat of the system at the zero temperature limi

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

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

116 gas-like states seen in the crossover of the specific heat on the dynamical length with a fixed inver

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

118 ific heat via spectroscopy and reproduce the specific heat peak at T(c), completing the missing link

119 c direction that manifests as a rather broad specific heat peak.

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

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

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

123 The resultant specific heat pumping power is ~ 1 Wg(-1), higher than t

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

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

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

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

128 sts a cross-over temperature above which the specific heat scales linearly with temperature, while be

129 A specific heating scheme is then applied to accelerate te

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

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

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

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

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

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

136 ntenance of pregnancy, whereas activation of specific heat shock protein mediated signaling may distu

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

138 We propose that suppression of specific heat shock proteins promotes maintenance of pre

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

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

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

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

143 Of the 74 specific heat-stable peptides detected in pure liver tis

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

145 c measurements also allow the detection of a specific heat step above 200 K, which is insensitive to

146 Hence, ant caste-specific heat stress resilience and extended longevity c

147 report extensive field-dependent electronic specific heat studies on [Formula: see text] up to an un

148 en theory and experiment for the phonons and specific heat suggests that the DFT (+OP) approach is ap

149 bits Pauli paramagnetism consistent with the specific heat, supporting the existence of a Fermi liqui

150 ween the magnetic T(c) and J(c), whereas the specific heat T(c)-distributions did provide valuable in

151 nset was always significantly lower than the specific heat T(c): although we partially ascribe the lo

152 te the ratio between thermal expansivity and specific heat (the Gruneisen parameter Gamma(s)) in supe

153 ling factor 5/2, and we examine the ratio of specific heat to temperature as a function of temperatur

154 ar Kerr effect and of two transitions in the specific heat upon entering the superconducting state, w

155 first probe the momentum-resolved electronic specific heat via spectroscopy and reproduce the specifi

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

157 And, from the field-dependent specific heat, we characterise the impact of fluctuation

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

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

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

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