ライフサイエンスコーパス: infrared laser

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

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

3 aphene induced by a continuous-wave (CW) mid-infrared laser.

4 the photothermal effect induced by a pulsed infrared laser.

5 ing (d-3DPLM) using a nanosecond pulsed near-infrared laser.

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

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

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

9 portance of the nonadiabatic effects for mid-infrared lasers.

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

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

12 ir was performed using a tunable 100 fs near-infrared laser (1100 nm-2400 nm).

13 ing plasma accelerator driven by a long-wave-infrared laser: a chirped-pulse-amplified CO(2) laser (l

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

15 tform was tested using aerosol formed by the infrared laser ablation of tissues.

16 intact gold nanoparticle (Au NP) tags using infrared laser ablation single-particle inductively coup

17 We developed an infrared laser ablation system capable of thermally lesi

18 herapy (EPIT) was performed using fractional infrared laser ablation to generate micropores in the sk

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

20 Using nanosecond infrared laser ablation, the region of interest can be t

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

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

23 esent a novel modality, atmospheric-pressure infrared laser-ablation plasma postionization (AP-IR-LA-

24 presents the design and application of a mid-infrared laser absorption spectroscopy (LAS) diagnostic

25 This study highlights the potential of mid-infrared laser absorption spectroscopy (LAS) for analyzi

26 Here we demonstrate actively tunable mid-infrared laser action in group-IV nanomechanical oscilla

27 Infrared laser action spectroscopy is used to characteri

28 Infrared laser action spectroscopy is used to characteri

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

30 al trial of low-power, continuous-wave, near-infrared laser adjuvant treatment, representing the firs

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

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

33 ntegrates a high-power, high-repetition-rate infrared laser and ion trap MS.

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

35 holes generated in semiconductors by a near-infrared laser are accelerated to a high kinetic energy

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

37 ose (TRD) were determined using a high-power infrared laser (at 1064 nm) trap by single and multiple

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

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

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

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

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

43 in the blue-green is challenging for current infrared-laser-based technology.

44 An infrared laser beam (2.94 mum) was used to irradiate the

45 An infrared laser beam (2.94 um) was used to irradiate the

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

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

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

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

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

51 In contrast, LAESI using a 3.4 mum infrared laser beam was able to detect and map hydrocarb

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

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

54 ssible from LWFAs driven by femtosecond near-infrared lasers by up to three orders of magnitude.

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

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

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

58 ctivation of these nanoparticles with a near infrared laser could selectively detect and kill biofilm

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

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

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

62 rapid tumor characterization with Picosecond infrared laser desorption mass spectrometry (PIRL-MS) fo

63 Infrared laser desorption of hair strands was shown to p

64 Near-infrared laser desorption/ionization aerosol mass spectr

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

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

67 We have adapted a tunable infrared laser differential absorption spectrometer (TIL

68 Recently, tunable infrared laser direct absorption spectroscopy (TILDAS) h

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

70 2)) in natural methane samples using tunable infrared laser direct absorption spectroscopy (TILDAS).

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

72 on Delta'(17)O analysis of CO(2) via tunable infrared laser direct absorption spectroscopy that is co

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

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

75 ser used was a gallium arsenide laser with 4 infrared laser emitters and 4 red laser emitters, 4 J/cm

76 Infrared laser evaporation of single aerosol particles i

77 ed upside-down isomer (CO-Na(+)) produced by infrared laser excitation and obtain well-resolved infra

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

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

80 that may span the gap between petawatt-class infrared laser facilities and x-ray free-electron lasers

81 attosecond pulses in the presence of a weak infrared laser field.

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

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

84 d works without the presence of superimposed infrared laser fields.

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

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

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

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

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

90 emble of randomly oriented molecules with an infrared laser, half of the molecules will undergo the v

91 high power ultrafast short-wave and mid-wave infrared lasers has enabled gas-phase high harmonic gene

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

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

94 Local infrared laser illumination produces a temperature gradi

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

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

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

98 ive of the tape is converted by a commercial infrared laser into a homogeneous porous SiO(x) layer de

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

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

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

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

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

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

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

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

107 SEMS) was produced to conduct PTT under near-infrared laser irradiation.

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

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

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

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

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

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

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

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

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

117 echanistic insight into the effect of pulsed infrared laser light on astroglial cells.

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

119 r barcoding via microparticles emitting near-infrared laser light to track and repeatedly measure eac

120 itizer (2p-PDT) using ~100 fs pulses of near-infrared laser light.

121 ng, making the particles susceptible to near-infrared laser light.

122 filing of biological tissues with picosecond infrared laser mass spectrometry (PIRL-MS) has enabled t

123 Picosecond infrared laser mass spectrometry (PIRL-MS) is shown, thr

124 Picosecond infrared laser mass spectrometry (PIRL-MS) using a hand-

125 ing interface for dual imaging of Picosecond Infrared Laser Mass Spectrometry (PIRL-MS) with DESI-MS.

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

127 Infrared laser-mediated injury mechanisms may be importa

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

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

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

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

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

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

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

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

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

137 those attained for typical single-pulse near-infrared laser plasmas but with the advantage of substan

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

139 Low infrared laser powers incompletely vaporize particles an

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

141 An unfocused pulsed infrared laser provided contactless sample desorption fr

142 nces, and their interrogation with a tunable infrared laser provides vibrational fingerprints for una

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

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

145 A near-infrared laser pulse enables triggered readout of the tr

146 jection into a wakefield bubble driven by an infrared laser pulse in structured CNT targets, similar

147 gating of the electron pulse mediated by an infrared laser pulse, and exploit the sensitivity of ine

148 d critical point of the LLPT by an ultrafast infrared laser pulse, following which we measure the str

149 Using an additional circularly polarized infrared laser pulse, we created a clock to time-resolve

150 after the quench of superconductivity by an infrared laser pulse.

151 arbon-based flexible film that converts near-infrared laser pulses into a localized acoustic field wi

152 Our infrared laser pulses produce high density avalanches of

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

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

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

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

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

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

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

160 Using short trains of mid-infrared laser pulses, we demonstrate the controllable f

161 r highly efficient HHG driven by intense mid-infrared laser pulses: an ultra-thin resonant gallium ph

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

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

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

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

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

167 Compared with excitation with infrared laser sources, the vibrational polariton conden

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

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

170 his processed sample is then delivered to an infrared laser spectrometer for measuring the amount fra

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

172 Infrared laser spectroscopy is used to study the four lo

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

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

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

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

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

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

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

180 riven by widely available 100s TW-class near-infrared laser systems have been shown to produce GeV-le

181 s has so far been limited to the use of near-infrared lasers that are down-converted to the mmWave re

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

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

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

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

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

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

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

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

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

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

192 citation microscopy employs ultrafast pulsed infrared lasers to image fluorophores at high-resolution

193 h) and 2-photon excitation using pulsed near-infrared lasers to reversibly silence metabotropic gluta

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

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

196 A pilot clinical trial of a near-infrared laser vaccine adjuvant: safety, tolerability, a

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

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

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

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

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

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

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

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

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

206 An infrared laser with a noncontact temperature sensing sys

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

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

209 ipse Tribrid mass spectrometer coupled to an infrared laser within a high-pressure linear ion trap.

210 Here we demonstrate a non-reciprocal near-infrared laser-writing technique for reconfigurable thre