ライフサイエンスコーパス: charged particle

1 egatively charged protein and the negatively charged particle.

2 s a plasma wave (wakefield) that accelerates charged particles.

3 of energy between electromagnetic fields and charged particles.

4 dergo more rapid transport in CF sputum than charged particles.

5 electrostatic cohesion among the ensemble of charged particles.

6 is converted into heat and kinetic energy of charged particles.

7 distinct zones of trapped, highly energetic charged particles.

8 g of the stability of crystals of oppositely charged particles.

9 s that neutral particles diffuse faster than charged particles.

10 l trials compared treatments with or without charged particles.

11 barrier hindering transmembrane movement of charged particles.

12 is (GEMMA) separates nanometer-sized, single-charged particles according to their electrophoretic mob

13 Fluids of charged particles act as the supporting medium for chemi

14 g similarities with other curved crystals of charged particles and colloids.

15 used for coagulating and removing negatively charged particles and dissolved organic matter (DOM) fro

16 Through measurement of charged particles and electromagnetic fields with NASA's

17 Experimentally, the use of charged particles and low-ionic-strength solutions provi

18 ock to the planet, providing magnetic field, charged particle, and wave phenomena context for Juno's

19 action of ultraviolet light and high-energy charged particles, and compare rates, spectral propertie

20 Ioxaglate is composed of charged particles, and data are reported separately.

21 facilitates the translocation of negatively charged particles, and the free energy barrier for trans

22 h Gram-negative bacteria than are negatively charged particles, and this interaction occurs primarily

23 These results imply that charged particles are accelerated to very high energies

24 In the presence of magnetic fields, the charged particles are bound to their cyclotron orbits, w

25 Individual charged particles are dynamically confined into nanomete

26 In capture and release detection, charged particles are electrophoretically driven to the

27 In subsequent tests, all the charged particles are electrostatically removed from the

28 Charged particles are increasingly used in cancer radiot

29 ions encircling the Earth in which energetic charged particles are trapped inside the Earth's magneti

30 Cosmic rays are charged particles arriving at the Earth from space.

31 Nanometre- and micrometre-sized charged particles at aqueous interfaces are typically st

32 ce of area confinement, suggesting that like-charged particles at interfaces can also experience attr

33 electronic degrees of freedom are modeled by charged particles attached to the nuclei of their core a

34 By using the Columbia University charged particle beam in conjunction with a strip dish d

35 e laser pulse or an ultra-short relativistic charged particle beam.

36 High-efficiency acceleration of charged particle beams at high gradients of energy gain

37 n cells that are not directly traversed by a charged particle but are in close proximity to cells tha

38 l substorms is the acceleration of energetic charged particles, but no acceleration signatures were s

39 ance, a one-dimensional crystal of identical charged particles can accommodate an extra particle (int

40 act that the interaction of matter with fast charged particles can be described by its complete optic

41 Radiation therapy with charged particles can potentially deliver maximum doses

42 The charged particle community is looking for techniques exp

43 nce in the biological effects of high-energy charged particles compared with X-rays or gamma-rays is

44 The simple structures formed by charged particles confined in a harmonic potential have

45 relied on the gas-phase interaction between charged particles created by electrospray ionization (ES

46 We observed that charged particles damage tissue nonhomogenously, with si

47 particularly when comparing X-rays and heavy charged particles, due to the uncertainty in their Relat

48 le of the collisional breakup of a system of charged particles, e(-) + H --> H(+) + e(-) + e(-) (wher

49 We consider Charged-Particle Emission Tomography (CPET), which relie

50 rough over 80 years old, Cerenkov showed how charged particles emit shockwaves of light when moving f

51 ion-sensitive avalanche photodiode to detect charged particle-emitting probes within a microfluidic c

52 e particle detection efficiency (fraction of charged particles entering the inlet that are subsequent

53 Lack of charged-particle equilibrium at the luminal mucosa may c

54 This model was extended to charged particle exposures by integrating Monte Carlo ca

55 particles and measuring the current from the charged particle flux.

56 nated using mass selection to isolate singly charged particles for a specified electrical mobility di

57 fusion reaction, the fusion products are all charged particles for which direct conversion is feasibl

58 overall significance relative to the loss of charged particles from Jupiter's magnetosphere---were un

59 Magnetic fields, solar wind, and energetic charged particles from low-latitude sources reach all la

60 Strong interactions between the charged particles give rise to surprising dynamics such

61 The Aharonov-Bohm effects of charged particles have been experimentally demonstrated

62 Measurements of x-ray-driven implosions with charged particles have resulted in the quantitative char

63 The cyclotron frequency of a charged particle in a uniform magnetic field B is relate

64 emitted in the opposite direction of moving charged particles in a left-handed material.

65 g phenomena arise from the Lorentz force for charged particles in a magnetic field, such as the fract

66 atial distribution of DNA lesions induced by charged particles in a mouse model tissue.

67 ernative for the localization and control of charged particles in an aqueous environment.

68 fication of the spatial dose distribution of charged particles in biologically relevant material, and

69 in instruments dealing with ion packets and charged particles in gas phase such as the mass spectrom

70 standard way for gating or steering beams of charged particles in ion mobility spectrometry and time-

71 Charged particles in the aerosol are drawn through the a

72 cilitates efficient focusing and transfer of charged particles in the higher-pressure regions (e.g.,

73 We demonstrate that the charged particles in this quantum tunnelling system are

74 d primary beam that can consist of X-rays or charged particles in two different analytical setups.

75 s every 2 months) to re-align the Low-Energy Charged Particle instrument on board Voyager 1 so that i

76 dendritic morphology observed after low dose charged particle irradiation by providing accurate descr

77 Charged-particle irradiation constitutes an alternative

78 coherent Cerenkov radiation due to a moving charged particle is associated with a velocity threshold

79 The mobility distribution of these charged particles is then measured in air in a different

80 nergy transfer (LET) IR (such as high energy charged particles) killing more cells at the same dose a

81 present study, using the Columbia University charged particle microbeam, we found that mitochondrial

82 Using a precision charged particle microbeam, we show here that irradiatio

83 A charged-particle microbeam was used, allowing irradiatio

84 the effects of single alpha particles uses a charged-particle microbeam, which irradiates individual

85 As well as charged particle microbeams, X-ray microprobes have been

86 t describes electromagnetic radiation from a charged particle moving in a medium with a uniform veloc

87 In the Cherenkov effect a charged particle moving with a velocity faster than the

88 The impact of the charged particles on the surface produces gaseous ions o

89 ements of energetic (>40 kiloelectron volts) charged particles on Voyager 1 from the interface region

90 ve different surface charges, and positively charged particles only show nonspecific DNA adsorption.

91 gy transfer (LET) radiation from space heavy charged particles or a heavier ion radiotherapy machine

92 atmosphere is exposed to a flow of energetic charged particles or solar radiation.

93 n two facts: (1) The equilibrium height of a charged particle over a charged surface depends on the e

94 Global imaging of the magnetospheric charged particle population can be achieved by remote me

95 Charged particle radiation is emitted as a byproduct of

96 O3, produced by the action of ultraviolet or charged-particle radiation on O2, was also not predicted

97 the comparative effectiveness and safety of charged-particle radiation therapy in cancer is needed t

98 In 243 eligible articles, charged-particle radiation therapy was used alone or in

99 Laboratory studies of the interaction of charged-particle radiation with water ice predicted the

100 he model presented has applications within a charged particle radiotherapy optimization framework as

101 occurs in a variety of situations, including charged particle radiotherapy, radiological accidents, a

102 such as thermotherapy, plaque radiotherapy, charged-particle radiotherapy, and local resection.

103 therapy offers 97% tumor control, similar to charged-particle radiotherapy.

104 Charged particles ranging from micro- to nanoscale are d

105 ation-sensitive catheter, optimized to sense charged particle rather than gamma or x-radiation, speci

106 e ionized gas composed of neutral particles, charged particles, reactive species, and electrons.

107 onsecutive poly(anion)/poly(cation) pairs of charged particles result in the formation of three-dimen

108 consists of a short one-dimensional chain of charged particles (rRNA antecedent) interacting with a p

109 Planetary aurorae are formed by energetic charged particles streaming along the planet's magnetic

110 Charged particles such as protons and carbon ions are an

111 field of a plasma wake excited by a bunch of charged particles (such as electrons) is used to acceler

112 Our scheme applies to any beams of charged particles, such as protons and ion beams.Vortex

113 Electrically charged particles, such as the electron, are ubiquitous.

114 s is found at saturation coverage due to the charged particle surface resulting in a repulsive intera

115 A key component for the description of charged particle systems is the screening of the Coulomb

116 high linear energy transfer radiation (e.g. charged particles) than by low linear energy transfer X-

117 e electromagnetic field fluctuations and the charged particles that comprise an undamped kinetic Alfv

118 the magnetosphere which accelerate energetic charged particles that hit the upper atmosphere.

119 s and identify a new stable configuration of charged particles that we call a quantum droplet.

120 he passage of an ultra-relativistic bunch of charged particles (the drive bunch) through a plasma.

121 is excited by an ultra-relativistic bunch of charged particles (the drive bunch).

122 iously unmeasured populations of neutral and charged particles, the homopause altitude at approximate

123 ompared event rates of combined outcomes for charged particle therapy and photon therapy using an int

124 Compared with photon therapy, charged particle therapy could be associated with better

125 Median follow-up for the charged particle therapy group was 38 months (range 5-73

126 Charged particle therapy is generally regarded as cuttin

127 e-free survival was significantly higher for charged particle therapy than for photon therapy (1.93,

128 ival was significantly higher at 5 years for charged particle therapy than for photon therapy (relati

129 06, 0.68-1.67; p=0.79) but it was higher for charged particle therapy than for photon therapy at long

130 e clinical outcomes of patients treated with charged particle therapy with those of individuals recei

131 However, charged-particle therapy is limited by the availability

132 cles in asymmetric silicon pores, as well as charged particles through artificial pores and arrays of

133 logic effects consequent to the traversal of charged particles through mammalian cells are explored w

134 izing radiation from high-energy photons and charged particles through mechanisms including radiolumi

135 ol size analyzer allows the removal of small charged particles to improve the signal-to-noise ratio.

136 ors, capable of energizing a large number of charged particles to relativistic speeds.

137 elerators (LPAs) are capable of accelerating charged particles to very high energies in very compact

138 Neutral-particle and charged-particle traps are widely used for studying both

139 aviolet and blue light that is produced by a charged particle traveling through a dielectric medium f

140 Charged particles traveling through matter at speeds lar

141 e (CL) arises from the interaction between a charged particle travelling faster than the phase veloci

142 r cells have been exposed to low fluences of charged particles, where only a few percent are exposed.

143 two-slit interference experiment with highly charged particles which argues that the consistency of e

144 s can lead to correlated motions of multiple charged particles, which can induce important many-body

145 Neutrally charged particles with a diameter <200 nm undergo more r

146 residue and other poorly focused neutral or charged particles with very high mass-to-charge ratios.

147 ortant challenge has been to explain how the charged particles within these belts are accelerated to