ライフサイエンスコーパス: infrared laser

1 after oxidation, before imaging with a near infrared laser.

2 of graphene oxide flakes using a pulsed near-infrared laser.

3 ity was modulated by irradiation with a near-infrared laser.

4 ks from commercial polymer films using a CO2 infrared laser.

5 eased in a controllable fashion using a near-infrared laser.

6 umber of atoms--favors longer-wavelength mid-infrared lasers.

7 he upcoming next generation of multi-PW near-infrared lasers.

8 The sample was introduced using mid-infrared laser ablation of a water-rich target.

9 Here we report on a novel combination of infrared laser ablation with electrospray ionization (LA

10 imental setup for spatially resolved ambient infrared laser ablation-mass spectrometry (AIRLAB-MS) th

11 ength-dependence of collateral damage in mid-infrared laser ablation.

12 Infrared laser action spectroscopy is used to characteri

13 Infrared laser action spectroscopy is used to characteri

14 A near-infrared laser-activated "nanobomb" is synthesized using

15 loying an optimally synthesized 2-microm mid-infrared laser and a small amount of its third harmonic,

16 adiation conditions using a femtosecond near-infrared laser and found distinct damage site recruitmen

17 We induced pain using an infrared laser and recorded nociceptive laser-evoked pot

18 urther studies were conducted using a pulsed infrared laser as the excitation source to analyze BG ce

19 Ts can be activated remotely by a visible or infrared laser, avoiding the need for a detonating cord.

20 A quantum-cascade long-wavelength infrared laser based on superlattice active regions has

21 We present an infrared laser-based mass spectrometric strategy to diff

22 Optical tweezers (infrared laser-based optical traps) have emerged as a po

23 To overcome these problems, we used a diode infrared laser-based stimulator (wavelength: 980 nm) for

24 tial temperature gradient caused by the near-infrared laser beam at-a-distance was found to activate

25 Sample ionization is assisted by multipass infrared laser beam in the interface.

26 A 100-ps infrared laser beam operating at 1.06 microns was focuse

27 Raman spectral patterns excited by a near-infrared laser beam provide intrinsic molecular informat

28 ected, the probe is irradiated with a pulsed infrared laser beam to vaporize organic components, whic

29 tissues facilitate sampling by a focused mid-infrared laser beam.

30 cal traps or "tweezers" use high-power, near-infrared laser beams to manipulate and apply forces to b

31 engineered resonant surface and a low-power infrared laser can cause enough photoemission via electr

32 lack nanoparticles to nanosecond pulsed near-infrared laser causes intracellular delivery of molecule

33 l-cleaving annelid Capitella teleta, we used infrared laser cell deletions to dissect the role of ind

34 We present results for infrared laser desorption and ionization mass spectromet

35 e desorbed from whole bacterial spores using infrared laser desorption and no chemical matrix.

36 ted to be an efficient natural matrix for AP infrared laser desorption ionization.

37 Infrared laser desorption of hair strands was shown to p

38 Near-infrared laser desorption/ionization aerosol mass spectr

39 A new method, near-infrared laser desorption/ionization aerosol mass spectr

40 irect combination of gel electrophoresis and infrared laser desorption/ionization time-of-flight mass

41 tion unit, "Stheno II", coupled to a tunable infrared laser direct absorption spectroscopy (TILDAS) i

42 ative abundance of (13)CH3D by using tunable infrared laser direct absorption spectroscopy (TILDAS).

43 With use of a near-infrared laser, elevated perfusion associated with the m

44 hysical experiments that humans can perceive infrared laser emission as visible light.

45 Infrared laser evaporation of single aerosol particles i

46 hydrates, and other small biomolecules using infrared laser excitation.

47 use of a Raman microscope equipped with near-infrared laser excitation.

48 aesium (Cs) atoms in an intense 3,600-nm mid-infrared laser field.

49 sequential double ionization (NSDI) with mid-infrared laser fields, and compare with results from nea

50 r fields, and compare with results from near-infrared laser fields.

51 ization of clusters by intense, non-resonant infrared laser fields.

52 lution under a temperature gradient built by infrared laser focusing.

53 ydroxy fullerenes by exposing them to a near-infrared laser for a few seconds, and also ignited an ex

54 We present a method, using an infrared laser, for reproducible heat-dependent gene exp

55 ature surrounding the target cells, using an infrared laser heating system.

56 rtical cell bodies, apoptosis was induced by infrared laser illumination of A1.

57 Using mid-infrared laser-induced electron diffraction (LIED), we o

58 r the tumor temperature achieved during near-infrared laser-induced photothermal heating in vitro and

59 We conclude that nonablative infrared laser inhibited neointimal hyperplasia after PT

60 onductor CuS nanoparticles, followed by near-infrared laser irradiation 24 h later (12 W/cm(2) for 3

61 Upon near-infrared laser irradiation at 808 nm, the helical twist

62 eas its reverse process occurs upon the near-infrared laser irradiation at 980 nm.

63 temic administration of HPPH liposomes, near infrared laser irradiation induced vascular photodynamic

64 long-term effect of endoluminal nonablative infrared laser irradiation on neointimal hyperplasia in

65 the reduced collateral damage resulting from infrared laser irradiation through a mechanism involving

66 amic response of biological tissue to pulsed infrared laser irradiation was investigated by measuring

67 Under near-infrared laser irradiation, the molecule produces acid a

68 can be precisely controlled via dosing near infrared laser irradiation.

69 nas to specify tumor heating via remote near-infrared laser irradiation.

70 he cavity and the induced force by a 1550 nm infrared laser is found to be increased by an order of m

71 nsity targets, irradiated by an intense near-infrared laser is observed.

72 A polarized infrared laser is then used to determine the directions

73 toinduced evaporation of these atoms when an infrared laser is tuned to a vibrational resonance.

74 orm of subwavelength microscopy, in which an infrared laser is used to optically trap and scan a nano

75 of a temperature field produced by the near-infrared laser light absorption.

76 ific dimensions enabling them to absorb near-infrared laser light have been widely used.

77 Previous work showed that infrared laser light selectively excited neural activity

78 tential of strongly coupled superlattices as infrared laser materials for high-power sources in which

79 Infrared laser-mediated injury mechanisms may be importa

80 In the current study, we used a near-infrared laser microirradiation system to directly study

81 om skin surface and exposure of skin to near-infrared laser, nanoshells localized in the follicles ab

82 process, excitons are created by a weak near-infrared laser of frequency f(NIR).

83 te reaction system, were immobilized with an infrared laser optical trap or by adhesion to modified b

84 ve developed a microscopy technique based on infrared laser overtone/combination band absorption to h

85 ied in a time-of-flight mass spectrometer by infrared laser photodissociation spectroscopy in the C-H

86 ight mass spectrometer and investigated with infrared laser photodissociation spectroscopy using the

87 ation (HHG) traditionally combines ~100 near-infrared laser photons to generate bright, phase-matched

88 A picosecond infrared laser (PIRL) is capable of cutting through biol

89 The infrared laser power required to sample the core of the

90 Low infrared laser powers incompletely vaporize particles an

91 a single, moderately powerful (10-kilowatt) infrared laser, producing 12-nanosecond-duration pulses.

92 induced during a contraction by applying an infrared laser pulse (lambda = 1.32 micro, 0.2 ms) to th

93 T-jumps were induced by an infrared laser pulse (wavelength 1.32 microns, pulse dur

94 Our infrared laser pulses produce high density avalanches of

95 long-distance transmission of ultrashort mid-infrared laser pulses through atmospheric air, probing a

96 The spectrograms of ultrashort mid-infrared laser pulses transmitted over a distance of 60

97 within our reach: Using intense ultra-short infrared laser pulses we can now deposit a very large en

98 The interaction of intense near- and mid-infrared laser pulses with rare gases has produced burst

99 Compared with near-infrared laser pulses, blue-IRIS enhances both achievabl

100 g of CED in clusters ionized by intense near-infrared laser pulses, our observation of CED in the XUV

101 ns of different alcohols were excited by mid-infrared laser pulses, vibrational energy was observed t

102 beam, state specific reactant preparation by infrared laser pumping, and ultrahigh vacuum surface ana

103 e delivery of short pulses of high-intensity infrared laser radiation, in a process known as laser ab

104 re only observed in the area exposed to near-infrared laser radiation.

105 A new infrared laser resonant desorption (LRD) technique has b

106 Using an ultrafast infrared laser source to create a coherent superposition

107 nanoimaging techniques and state-of-art mid-infrared laser sources, we have succeeded in demonstrati

108 nventional IRMS technique and by the new mid-infrared laser spectrometer agree remarkably well within

109 high precision with the use of a tunable far-infrared laser spectrometer.

110 Infrared laser spectroscopy is used to study the four lo

111 High-resolution infrared laser spectroscopy was used to obtain rotationa

112 The method combines infrared laser spectroscopy with mass spectrometry to se

113 isolated water trimer is investigated by far-infrared laser spectroscopy.

114 n vivo using transcutaneous, fiber-based mid-infrared laser spectroscopy.

115 nder a range of light intensities, using mid-infrared laser spectroscopy.

116 phase, size-selected, and investigated with infrared laser spectroscopy.

117 ed by high-resolution polarization-modulated infrared laser spectroscopy.

118 Upon irradiation by a near-infrared laser, the phase-change material is melted due

119 Transcranial near infrared laser therapy (NILT) improves behavioral outcom

120 mechanical and thermal repeatability for an infrared laser to achieve both accurate and precise open

121 tes such correlation by using a pulsed, near-infrared laser to create defined fiducial marks in three

122 Using computer vision, FlyMAD targets an infrared laser to freely walking flies.

123 rapping apparatus, we used a tightly focused infrared laser to heat single molecules of Escherichia c

124 ce-activated cell sorter (microFACS) uses an infrared laser to laterally deflect cells into a collect

125 , we use the scattering force from a focused infrared laser to levitate cells of interest from their

126 In the first method, we used a 975 nm infrared laser to raise the temperature 5.6 degrees C/10

127 nology for applications ranging from tunable infrared lasers to biological labels.

128 ticles were displaced 10-100 nm using a near-infrared laser trap with a trap constant of 0.0001 N/m.

129 uNR@G-P-aspirin complexes were used for near-infrared laser-triggered photothermal ablation of solid

130 amine (Tryp) is examined in the gas phase by infrared laser-vibrational predissociation spectroscopy

131 An infrared laser was used to ablate material from tissue s

132 A femtosecond, tunable near-infrared laser was used to generate both nonresonant and

133 cope equipped with a femtosecond-pulsed near-infrared laser was used to simultaneously excite second

134 er with the emerging high-repetition MHz mid-infrared lasers, we anticipate efficiency of harmonic yi

135 Mice were then treated with near-infrared laser, which elevated tumor temperature by 20.7

136 We induced acute pain with an infrared laser while human participants looked either at

137 The CuO matrix is locally heated with an infrared laser while it is contained within a sealed cha

138 capture all sample-associated ions using an infrared laser with a 20 Hz repetition rate.

139 An infrared laser with a noncontact temperature sensing sys

140 The reader contains a miniaturized, 1-W, infrared laser with peak emission at 980 nm.

141 device and a rapidly switched moderate-power infrared laser with the laser beam focused on the nano-c