ライフサイエンスコーパス: laser beam

1 ransit a finely focused, frequency-modulated laser beam.

2 acilitate sampling by a focused mid-infrared laser beam.

3 The spot is defined by the probe laser beam.

4 bution of paths taken through the excitation laser beam.

5 les traverse the full width of an excitation laser beam.

6 scence was selectively bleached by a focused laser beam.

7 e and locally photoactivated using a focused laser beam.

8 a moving observation volume by scanning the laser beam.

9 (PDT) drug in cells was activated by a HeNe laser beam.

10 on polymerization technique with a shaped UV laser beam.

11 to fluence variations in the profile of the laser beam.

12 PEG) that were solidified by the action of a laser beam.

13 ng selected cells to an adhesive film with a laser beam.

14 ondestructively probed within the excitation laser beam.

15 ed to microspheres using a single collimated laser beam.

16 approximately 2 micrometer diameter focused laser beam.

17 sample through the 1-microm-diameter focused laser beam.

18 nsion to move ions away from the path of the laser beam.

19 en they move in and out of the intracellular laser beam.

20 he study participants to fixate on a probing laser beam.

21 ass through a low power, focused, continuous laser beam.

22 by splitting and recombining a single Nd:YAG laser beam.

23 ct of self-focusing in the atmosphere on the laser beam.

24 ction of the electron bunch with the focused laser beam.

25 d from AuNPs under irradiation with a 355 nm laser beam.

26 th a continuous-wavelength laser or a pulsed laser beam.

27 attice beam is compensated by a blue-detuned laser beam.

28 an electrical gate rather than by a control laser beam.

29 respect to a nanosecond ultraviolet pumping laser beam.

30 passing through a 300/395 filter or a 405 nm laser beam.

31 es exerted by tightly focused high-intensity laser beams.

32 rmonic generation in the presence of intense laser beams.

33 rated by state-dependent forces induced with laser beams.

34 enerated by tightly focused ultrashort pulse laser beams.

35 rature and emits spatially coherent Gaussian laser beams.

36 d controlling optical phase singularities in laser beams.

37 ly-universe cosmology, and to engineering of laser beams.

38 er 0.8 microm) on the membrane with an Argon laser beam (488 nm) and following the fluorescence recov

39 A laser beam (488 nm) was attenuated by an acoustooptic mo

40 vacuum using a circularly polarized trapping laser beam--a microgyroscope.

41 quency comb is that it provides, in a single laser beam, about a million optical modes with very narr

42 The probe scanned the laser beam across a fan shape area by rotating the two G

43 ectral images were generated by scanning the laser beam across a sample surface.

44 rbide (SiC) substrates by scanning a focused laser beam across the GFET.

45 th via the voice coil actuator, scanning two laser beams across the channels on the microchip.

46 Use of a second nanosecond laser beam, adequately synchronized with the short laser

47 A collimated 980 nm laser beam afforded high local excitation densities to a

48 are vaporized in transmission geometry by a laser beam aligned with the atmospheric pressure inlet o

49 The apparatus translates a laser beam along the entire length of a fiber segment wi

50 oviding high-speed precision scanning of the laser beam along the sample surface.

51 optical train based on the interaction of a laser beam and an etched channel, consisting of two radi

52 250 ms every 5.00 s, to expose the dye to a laser beam and create a photobleached zone.

53 which a single spore is trapped in a focused laser beam and its Ca-DPA is quantitated from the intens

54 eria in aqueous solution in the focus of the laser beam and levitating the captured cell well off the

55 d to separate the individual components in a laser beam and map each mode onto its designated detecto

56 of fluorophores diffusing through a focused laser beam and provides a rigorous framework through whi

57 d fibrinogen with thrombin was captured by a laser beam and repeatedly brought into contact with surf

58 as spatial constraints exist to position the laser beam and the objective lens with the external beam

59 ted area by cutting rather than focusing the laser beam and to study the parameters affecting sensiti

60 riple-twist torons'--are generated by vortex laser beams and embed the localized three-dimensional (3

61 ransit time of a single molecule through the laser beam, and (iii) the number of detected molecules w

62 sis spore was optically trapped in a focused laser beam, and its Raman spectra were recorded sequenti

63 810 nm, 10-mW average power), 2-mm-diameter laser beam, and the detection optical fiber is 5 mm in d

64 nt field from a totally internally reflected laser beam, and the fluorescence arising from the IgE-co

65 ized in the injection channel using a shaped laser beam, and the sizing monolith was cast by photolit

66 h far-off-resonance blue-detuned swept sheet laser beams are used to make new types of high-density t

67 CROS consists of projecting a laser beam at an angle on the retina after injection of

68 By aiming a laser beam at the labeled retinal fibers demarcating the

69 generated by total internal reflection of a laser beam at the optical interface between the prism an

70 The complex is excited by focusing a laser beam at the pipet tip to produce a submicrometer l

71 erature gradient caused by the near-infrared laser beam at-a-distance was found to activate temperatu

72 oving either the trap or the stage along the laser beam axis, offer several potential benefits when s

73 sed on the rotation of the polarization of a laser beam by the nuclear spins in a liquid sample.

74 The angle of the incident laser beam can be changed automatically and reliably fro

75 The laser beam can trap such particles not only at their cen

76 Furthermore, laser beams can be tailored to match the absorption prof

77 In this approach, a tightly focused pulsed laser beam capable of promoting protein photo-cross-link

78 on of the incident angle by 2 degrees of the laser beam caused a swing between the two features.

79 A switching laser beam causes this pattern to rotate even when the p

80 grating is promising to find applications in laser beam combining systems.

81 made under optimal polarization of incident laser beam, corroborated the proposed carotenoid orienta

82 It consists of laser beams counterpropagating through a warm rubidium v

83 Folding proteins pass through a focused UV laser beam, creating OH radicals that label the select p

84 er plume, and it can be controlled by proper laser beam delivery.

85 ualified by the possibility to tune both the laser beam diameter and the acquisition camera field of

86 The imaging parameters, such as the laser beam diameter and the translation stage movement,

87 es and reduced sample volume with decreasing laser beam diameter.

88 ed spontaneous emission (SASE) nature of the laser beam does not affect the dynamics of the ions.

89 ntional three-electrode measurement, and the laser beam does not perturb the electrochemical process.

90 e controlled by irradiation with one or more laser beams during individual bimolecular collisions or

91 rent solar radiation into a bright, coherent laser beam enables the application of nonlinear optics t

92 conds to nanoseconds are utilized at varying laser beam energies and pulse lengths, and enable the re

93 lection interference fringe FPR, interfering laser beams enter a 1.65-numercial aperture (NA) Olympus

94 The vertically and a horizontally polarized laser beam exiting a Wollaston prism are focused into th

95 We find that, by using two laser beams far detuned from an optical cavity resonance

96 time constant shows linear dependence on the laser beam fluence.

97 tched moderate-power infrared laser with the laser beam focused on the nano-coating, enabling heating

98 applications, such as MALDI MS imaging where laser beam focusing as fine as possible (5-10 mum) is se

99 t heat loads were simulated using long pulse laser beams for two different grades of ultrafine-graine

100 After bleaching by a focused laser beam, GFP-CFTR fluorescence in the bleached membra

101 In the zone farthest from the laser beam (> 60 microns under these conditions), nearly

102 smaller than the diffraction-limited focused laser beam have been used to confine single molecules in

103 ing ultranarrow, precisely controlled ion or laser beams have enabled assembly of architectures of un

104 hundred and ninety-two simultaneously fired laser beams heat ignition-emulate hohlraums to radiation

105 In LSR, a coherent laser beam illuminates the specimen and a high-speed cam

106 om one adjacent flow to the other causes the laser beam, impinging orthogonal to the RIG through the

107 ished by using acoustic waves to deflect the laser beam in a manner that is dependent on the acoustic

108 On irradiation of the labeled tissue by the laser beam in a raster pattern, the mass tags are libera

109 aneously by rapidly directing the excitation laser beam in a uniform (circular) scan across the bilay

110 s to assess the nonlinear propagation of the laser beam in order to predict the optimal range of proc

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

112 one were subjected to multiple passes of the laser beam in the same line of incision at energy densit

113 obe system to focus displaced pump and probe laser beams in a microfabricated flow channel and to det

114 We demonstrate that laser beams in these fluids can generate anisotropic opt

115 erimentally creating combinations of optical laser beams in which these dark threads form stable loop

116 ace is generated by reflecting an elliptical laser beam incident from the top by 90 degrees with a sm

117 A diode laser beam, incident upon and illuminating the entire wi

118 s and an x, y translator, the 10.6-microm IR laser beam, initially 3.5 mm in diameter, is focused int

119 The laser beam initiates a cascade of reactions in the regio

120 particle is created by either modulating the laser beam intensity during the scan or by using an asym

121 Reaction plume formation at the precursor/laser beam interface initiates confined-plume, chemical

122 light modulator to split a high-power femto-laser beam into multiple subbeams.

123 Here, by introducing a laser beam into the combination of piezoresponse force m

124 unt is assembled and installed to direct the laser beam into the objective lens of a standard inverte

125 cus has been mainly on investigating various laser beams irradiating initially overdense flat interfa

126 (DLMF) is a procedure in which a high-power laser beam is directed onto a metal powder bed and progr

127 In this microscope, the exciting laser beam is first split into multiple beams and each b

128 When a terawatt-peak-power laser beam is focused into a gas jet, an electron plasma

129 The laser beam is incident at a surface plasmon resonance (S

130 arge-coupled device camera when a collimated laser beam is projected on the mouse to stimulate fluore

131 from a single DNA molecule passing through a laser beam is proportional to the size (contour length)

132 In these schemes, a laser beam is rapidly scanned along a line in the focal

133 When a tunable IR laser beam is reflected off a surface coated with target

134 The laser beam is scanned over a 2 X 2-mm area to generate 4

135 The trajectory of a second probe laser beam is then continuously tuned in the experiment.

136 urement spot size defined by the size of the laser beam is ~10 microm.

137 colloidal particles trapped by two coherent laser beams is measured by phase-sensitive detection.

138 Obliteration of matter by pulsed laser beams is not only prevalent in science fiction mov

139 samples were photographed with a helium-neon laser beam (lambda = 633 nm).

140 ion of flow was used to focus the excitation laser beam (lambda exc = 532 nm) in the solution and als

141 lecules in a volume smaller than the focused laser beam leads to a Gaussian distribution of single mo

142 believed that angiogensis stimulation by the laser beam may be responsible for the relief of angina.

143 asurements assumes bleaching with a circular laser beam of a Gaussian intensity profile.

144 an optical beam deflection system using two laser beams of different wavelengths.

145 ermined by measuring the displacement of the laser beam on a quadrant photodiode.

146 focusing lens, appropriate alignment of the laser beam on the capillary, and use of appropriate opti

147 rmed on a monolith electrode by scanning the laser beam on the electrode.

148 doscopic probe was developed to guide an OCT laser beam onto human cadaver eye tissue samples to dete

149 By focusing a pulsed laser beam onto one or more selected membrane positions,

150 sing a spatial light modulator, we split the laser beam onto several neurons and performed simultaneo

151 A 100-ps infrared laser beam operating at 1.06 microns was focused onto a

152 ovides solutions for both Dirac and Gaussian laser beam (or fluorescence-labeled biomacromolecule) pr

153 ethod that does not require high voltages, a laser beam, or applied heat and depends only the proper

154 ramic coatings are produced by rastering the laser beam over a sample specimen.

155 /A output voltages drive the scanning of the laser beam over all channels, the software can define ad

156 Consideration of laser beam parameters (spot size, rastering across the s

157 plasma-particle interactions as opposed to a laser beam-particle interaction.

158 constructed in which one of two interfering laser beams passed through a flow chamber containing the

159 In DCDB MIBD, a He-Ne laser beam passes through a half-wave plate onto the cro

160 le while maintaining it in the center of the laser beam path and within the laser focus, thus maximiz

161 tically-guided electrokinetic forces, vortex laser beams, plasmonics, and optofluidics.

162 ssing of the photoacoustic signal and higher laser beam power, should further increase the instrument

163 e grating and (2) the refraction of a narrow laser beam projected through the lens.

164 ntensity feature of the axially nonsymmetric laser beam propagates along a bent trajectory, leaving a

165 To achieve MRSFG, a collinear laser beam propagation geometry was adopted and trapezoi

166 spectral patterns excited by a near-infrared laser beam provide intrinsic molecular information for r

167 In this method, a large diameter laser beam rasters across the surface of a partly aligne

168 longated condensate to a single off-resonant laser beam resulted in the observation of highly directi

169 cence from two spatially separate excitation laser beams resulted in cross-correlation functions that

170 of particles that have entered and left the laser beam sample volume during large dwell times.

171 Conditions including laser fluence, laser beam scan rate, and carrier gas flow rate were opt

172 Laser beam scanning driven by an acousto-optical deflect

173 While fast laser beam scanning for LIF detection on capillary or mi

174 eat flow directions are examined for various laser beam scanning patterns based on numerical modeling

175 bright, phase-matched emission also support laser beam self-confinement, further enhancing the x-ray

176 allows the approach to take into account the laser beam shape, beam aberrations, and the laser-solid

177 This improvement became possible by laser beam shaping using a 4:1 beam expander and a circu

178 ximately 12 mum was achieved by reducing the laser beam size by using an optical fiber with 25 mum co

179 showed a dependence on two laser parameters: laser beam spot size and wavelength.

180 for instance graduate-level familiarity with laser beam steering and optical components, this protoco

181 roscientists by using fast three-dimensional laser beam steering enabling an image-guided "point-and-

182 de gel and then irradiated with a converging laser beam targeting the rear of the gel.

183 With a focused 633-nm laser beam that acts as a 'paintbrush' and the photoswit

184 arization modulation of an ultra-short pulse laser beam that can simultaneously determine collagen fi

185 abilities in addition to a highly focused UV laser beam that is utilized for laser ablation of sample

186 image the sample using a number of modulated laser beams that correspond to the number of GNP species

187 nto quasicrystalline arrays by using intense laser beams that create quasi-periodic optical standing-

188 ng the propagation direction of the trapping laser beam (the axial direction).

189 broad-band source is added to a narrow-band laser beam, the intensity of the Raman signal is amplifi

190 ct is placed between two opposed, nonfocused laser beams, the total force acting on the object is zer

191 ring CO2 laser micromachining by passing the laser beam through a stainless steel pinhole.

192 The propagation of such powerful laser beams through the atmosphere reveals many novel in

193 g the molecule in the axial direction of the laser beam, thus avoiding limiting artifacts from steric

194 The prototype probe focused the laser beam to a working distance of approximately 1.4 mm

195 ic deflectors to steer a focused, ultra-fast laser beam to arbitrary locations in three-dimensional s

196 ng the frequency input to the AOD allows the laser beam to be addressed accurately on a microchip.

197 Here, we have used a focused femtosecond laser beam to create a small transient hole in the cellu

198 al time and space by focusing an addressable laser beam to differentially heat a platinum (110) singl

199 A spatial light modulator splits a laser beam to generate an m x n multifocal array.

200 elation spectroscopy (FCS) uses a stationary laser beam to illuminate a small sample volume and analy

201 multiphoton excitation, using the attenuated laser beam to measure fluorescence recovery as fresh unb

202 s by using spectral multiplexing of a single laser beam to perform tomographic imaging over a continu

203 se techniques either require an illuminating laser beam to resolve to 70 nm in the visible spectrum o

204 dimensions under a focused mid-infrared (IR) laser beam to transfer material to the target slide via

205 e probe is irradiated with a pulsed infrared laser beam to vaporize organic components, which are the

206 d a dichroic filter, which directed the dual-laser beams to an objective.

207 or "tweezers" use high-power, near-infrared laser beams to manipulate and apply forces to biological

208 d cycle of the tracking routine (32 ms), the laser beam traces four circular orbits surrounding the p

209 stream produce substantial scattering of the laser beam used to measure cantilever deflection.

210 ded as a function of incident angle of He-Ne laser beam using a laboratory assembled SPR setup.

211 Modulation of each laser beam using acousto-optic modulators allowed the in

212 3D) nuclide distribution mapping beyond the laser beam waist are described.

213 rspacings smaller than the dimensions of the laser beam waist, onto the sample surface, thus oversamp

214 Therefore, a nanosecond Nd:YAG laser beam was focused into a flux of helium charged wit

215 A laser beam was launched into the side of the chip, which

216 The laser beam was masked to produce a beam 2 mm by 1 mm.

217 ls were streamed into an X-ray free-electron laser beam we found that scattering from other cell comp

218 By controlling the polarization of the laser beams, we were able to assign unambiguously the os

219 We used pulsed laser beam welding method to join Pd43Cu27Ni10P20 (at.%)

220 Our results reveal that pulsed laser beam welding under appropriate processing paramete

221 es the second step, where a nanosecond pulse laser beam welds the nanowires.

222 ost fields elicited by co-stimulation of two laser beams were well explained by linear combination of

223 e atoms are guided by horizontal red-detuned laser beams which cross with an angle of roughly 90 degr

224 eraction of the particle with the ionization laser beam, which affect the absolute peak areas in the

225 array of magneto-optical traps with a single laser beam, which will be utilised for future cold atom

226 tical forces produced by the interference of laser beams, which allow NPs to migrate to lower-energy

227 and experimentally demonstrate a new complex laser beam with inhomogeneous polarization distributions

228 asured by merging a tunable narrow-bandwidth laser beam with the ions.

229 ctric field distributions of tightly focused laser beams with different polarizations.

230 ssibility of controlling high-power coherent laser beams with low-power incoherent light sources such