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Journal articles on the topic 'Transient grating'

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Author: Grafiati

Published: 4 June 2021

Last updated: 11 March 2023

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1

Takata, Yoshiaki. "Conditions inducing reliable transient gratings of a LaCoO3 thin film using transient grating technique." Journal of Materials Research 19, no. 11 (November 1, 2004): 3149–51. http://dx.doi.org/10.1557/jmr.2004.0422.

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First, a grating decay rate and a thermal diffusion rate of the transient gratings are determined out of the energy-time trace observed by using a transient grating technique with 266-nm laser pulse inducing transient gratings in a LaCoO3 thin film. Second, the grating models aimed at studying two different thermal diffusion phenomena in contrast with the previous paper are described. The difference between both phenomena is attributable to the volume of photon scattering to characterize induced transient gratings. It is concluded that a reliable energy-time trace is observed when the transient gratings with a thickness smaller than a film are induced on the very surface of a thin film sample.

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2

Haynes, J. D., G. Roth, M. Stadler, and H. J. Heinze. "Neuromagnetic Correlates of Perceived Contrast in Primary Visual Cortex." Journal of Neurophysiology 89, no. 5 (May 1, 2003): 2655–66. http://dx.doi.org/10.1152/jn.00820.2002.

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When a target grating is flashed into a larger, surrounding grating, its contrast is perceived to be lower when both gratings are oriented collinearly rather than orthogonally. This effect can be used to dissociate the perceived contrast from the physical contrast of a target grating. We recorded the transient electric potentials and magnetic fields evoked by flashed target gratings and compared them with psychophysical judgments of perceived contrast. Both early (100 ms) and late (150 ms) transients were reduced in amplitude when targets were flashed into a collinear rather than orthogonal surround, thus paralleling the reduction in perceived contrast. Although targets in orthogonal backgrounds required 40% lower physical contrast to match the perceived contrast of collinear targets, the amplitudes of electrophysiological transients of matching stimuli were almost identical. Thus the responses correlated better with perceived than with physical target contrast. This holds especially for the late transient response. Source localization indicated that the transients in question may originate in primary visual cortex. Our results therefore identify the activity of primary visual cortex as one possible neural correlate of perceived contrast.

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3

Huang, Shubin, Zeyu Peng, Shi Rui, Renfu Zhang, Rui-Tao Wen, Xing Cheng, and Liang Guo. "Design and fabrication of diffraction grating with optimized efficiency for transient grating spectroscopy." Review of Scientific Instruments 93, no. 12 (December 1, 2022): 125112. http://dx.doi.org/10.1063/5.0116176.

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Transient grating spectroscopy (TGS) based on diffraction gratings is a powerful optical method for studying the transport of energy carriers such as phonons and electrons. The diffraction grating in a TGS system is a key component to form a large-area interference pattern, i.e., transient grating, and to study the mean free path distribution of energy carriers. In this work, a design method for polarization-insensitive diffraction gratings with periods in the range 2–50 µm for TGS by a combination of rigorous coupled wave analysis and genetic algorithm was discussed. The method was tested for pump/probe wavelength of 515/532 or 1030/808 nm. Each ±1st diffraction order carries 35%–40% of the incident energy and the diffraction efficiencies of the other orders are lower than 10%. The optimized diffraction gratings were fabricated by a combination of photolithography and inductively coupled plasma etching, with the processing parameters introduced in detail, and their optical characteristics were evaluated. Finally, as a demonstration, the diffraction gratings for 1030/808 nm were applied to TGS to study the thermal transport properties of Ge. This work provides a useful guide for future applications and the development of TGS.

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4

Ishihara, M. "Effect of Luminance Contrast on the Motion Aftereffect." Perception 26, no. 1_suppl (August 1997): 191. http://dx.doi.org/10.1068/v970311.

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The effects of luminance contrast and spatial frequency in the transient channel were investigated by making use of the motion aftereffect (MAE) caused by adaptation to a drifting sinusoidal grating. Two experiments were performed. The PSE of the velocity was measured as an index of the MAE. The adapting grating was made to drift at a velocity of 2.28 deg s−1 and its spatial frequency was 0.8, 1.6, or 3.2 cycles deg−1. In the first experiment, the MAE caused by a luminance contrast grating or an equiluminous chromatic grating was measured. In the second experiment, luminance contrast gratings were used to measure the effect of the contrast differences between adapting and test gratings. The largest MAE was observed when a low-luminance-contrast grating or an equiluminous chromatic grating was presented as test stimulus after adaptation to a high-luminance-contrast grating in the low-spatial-frequency condition. Generally, the MAE increased with increasing adapting contrast and with decreasing test contrast or spatial frequency. Little MAE was observed at high test contrasts. The results may be explained by assuming that activity in the sustained channel (or parvocellular pathway) inhibits activity in the transient channel (or magnocellular pathway) owing to the domination of sustained channel activity when the test is a static high-luminance-contrast grating providing much information about position and form.

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5

Sahu, Kalyanasis, and Mark A. Berg. "Thermal gratings and phase in high-order, transient-grating spectroscopy." Journal of Chemical Physics 134, no. 14 (April 14, 2011): 144502. http://dx.doi.org/10.1063/1.3572332.

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6

Dong, Guan-Ting, Chun-Ta Wang, and Yu-Ju Hung. "Spatially Broadband Coupled-Surface Plasmon Wave Assisted Transmission Effect in Azo-Dye-Doped Liquid Crystal Cell." Nanomaterials 10, no. 7 (July 11, 2020): 1357. http://dx.doi.org/10.3390/nano10071357.

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Active tuning on a plasmonic structure is discussed in this report. We examined the transient transmission effects of an azo-dye-doped liquid crystal cell on a metallic surface grating. The transition between isotropic and nematic phases in liquid crystal generated micro-domains was shown to induce the dynamic scattering of light from a He-Ne laser, thereby allowing transmission through a non-transparent aluminum film overlaying a dielectric grating. Various grating pitches were tested in terms of transmission effects. The patterned gratings include stripe ones and circular forms. Our results indicate that surface plasmon polariton waves are involved in the transmission process. We also demonstrated how momentum diagrams of gratings and Surface Plasmon Polariton (SPP) modes combined with Mie scattering effects could explain the broadband coupling phenomenon. This noteworthy transition process could be applied to the development of spatially broadband surface plasmon polariton coupling devices.

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7

DeMarco, Paul J., Jonathan D. Nussdorf, Douglas A. Brockman, and Maureen K. Powers. "APB Selectively Reduces Visual Responses in Goldfish to High Spatiotemporal Frequencies." Visual Neuroscience 2, no. 1 (January 1989): 15–18. http://dx.doi.org/10.1017/s0952523800004272.

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AbstractVisual responses of goldfish to rotating square-wave gratings were recorded before and after intraocular injection of 2-amino-4-phosphonobutyric acid (APB). High doses of APB reduced the rate of optokinetic nystagmus (OKN) to a relatively high spatial frequency grating moving at a high temporal frequency. Responses to a low spatial frequency grating were not altered, nor were responses to the higher spatial frequency when it rotated slowly. The effects of APB were transient and lasted no longer than 3 d. We conclude that APB reduces OKN to high spatiotemporal frequencies in goldfish.

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8

Guo, Xiao-Zheng, Chang Liu, Yi Zhou, and Duan-Bin Luo. "All-optical logical gates based on photoinduced molecules reorientation in amorphous polymer films." Journal of Nonlinear Optical Physics & Materials 25, no. 01 (March 2016): 1650004. http://dx.doi.org/10.1142/s0218863516500041.

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A type of all-optical logical gate based on two kinds of refractive index grating in azo-dye doped polymer film is studied in this paper. Using interference recording method with two 532[Formula: see text]nm laser beams, the transient refractive gratings can be formed in poly(methyl methacrylate) (PMMA) films containing azo-dye Disperse Red 13 (DR13). The characteristics of the transient gratings in films which are recorded by two 532[Formula: see text]nm laser beams with different polarization states are investigated by monitoring the first-order diffraction intensity of the readout He–Ne laser beam (632.8[Formula: see text]nm). It is found that the transient gratings in the polymeric films can be established and decayed in several seconds. Furthermore, we realize XOR and XNOR all-optical logical operation based on the relationship among the polarization states of the recording beams, the reading beam, and the diffraction beam.

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9

Wang, F., and R. Schwarz. "Electrically detected transient photocarrier grating method." Applied Physics Letters 65, no. 7 (August 15, 1994): 884–86. http://dx.doi.org/10.1063/1.112189.

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10

Bisht, Prem B. "Relaxation processes using transient grating technique." Research on Chemical Intermediates 27, no. 4-5 (July 2001): 539–47. http://dx.doi.org/10.1163/156856701104202192.

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11

Park, June-Sik, and Taiha Joo. "Coherent interactions in femtosecond transient grating." Journal of Chemical Physics 120, no. 11 (March 15, 2004): 5269–74. http://dx.doi.org/10.1063/1.1647534.

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12

Svetina, C., R. Mankowsky, G. Knopp, F. Koch, G. Seniutinas, B. Rösner, A. Kubec, et al. "Towards X-ray transient grating spectroscopy." Optics Letters 44, no. 3 (January 24, 2019): 574. http://dx.doi.org/10.1364/ol.44.000574.

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13

Sweetser, John N., David N. Fittinghoff, and Rick Trebino. "Transient-grating frequency-resolved optical gating." Optics Letters 22, no. 8 (April 15, 1997): 519. http://dx.doi.org/10.1364/ol.22.000519.

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14

Katayama, K., Q. Shen, T. Toyoda, M. Yamaguchi, and T. Sawada. "Lens-free heterodyne transient grating technique." Journal de Physique IV (Proceedings) 125 (June 2005): 349–53. http://dx.doi.org/10.1051/jp4:2005125082.

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15

Tanaka, Keiji. "Transient‐grating study of amorphous As2S3films." Journal of Applied Physics 65, no. 5 (March 1989): 2042–46. http://dx.doi.org/10.1063/1.342872.

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16

Taschin, A., P. Bartolini, M. Ricci, and R. Torre. "Transient grating experiment on supercooled water." Philosophical Magazine 84, no. 13-16 (May 2004): 1471–79. http://dx.doi.org/10.1080/14786430310001644233.

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17

Katayama, Kenji, Kazuo Sato, Hisashi Sugiya, and Takafumi Shoji. "Near-field heterodyne transient grating spectroscopy." Chemical Physics Letters 479, no. 4-6 (September 2009): 306–9. http://dx.doi.org/10.1016/j.cplett.2009.08.025.

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18

Evesque, P., J. Duran, and A. Bourdon. "TRANSIENT GRATING EXPERIMENTS IN PERCOLATION FRACTALS." Le Journal de Physique Colloques 46, no. C7 (October 1985): C7–45—C7–49. http://dx.doi.org/10.1051/jphyscol:1985709.

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19

Garrity, D. K., and J. L. Skinner. "Exciton dynamics and transient grating experiments." Journal of Chemical Physics 82, no. 1 (January 1985): 260–69. http://dx.doi.org/10.1063/1.448951.

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20

Maly, P., A. Svoboda, and P. Busa. "Picosecond Transient Concentration Grating in Silicon." physica status solidi (a) 121, no. 2 (October 16, 1990): K223—K226. http://dx.doi.org/10.1002/pssa.2211210257.

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21

Huang Pei, Fang Shao-Bo, Huang Hang-Dong, Zhao Kun, Teng Hao, Hou Xun, and Wei Zhi-Yi. "Attosecond relative delay measurement using transient-grating frequency-resolved optical grating." Acta Physica Sinica 67, no. 21 (2018): 214202. http://dx.doi.org/10.7498/aps.67.20181570.

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22

Hao, Luguo, Hongzhen Jing, Ying Xiang, Andrey Iljin, Yao Wang, Hao Li, Qinyuan Li, Jinghui Peng, and Michal Kohout. "Transient optically induced grating and underlying transport process in bent-core nematics." Journal of Applied Physics 132, no. 6 (August 14, 2022): 065108. http://dx.doi.org/10.1063/5.0096106.

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In this paper, we have applied a holographic time-of-flight technique with a nanosecond laser pulse to perform time-resolved measurements of optically induced gratings in bent-core nematics formed by a new kind of liquid crystal (LC). The effects of the electric field, laser pulse energy, temperature, and light intensity pattern on the photocharge transport process were investigated systematically. The results indicate that some peculiar features, such as high photosensitivity, relatively large mobility, and negative conductivity anisotropy, were present in the studied soft-matter system. Furthermore, a coupling between the optically induced grating and electrically induced convection was observed, which revealed a competitive state between them via the transport process. Thus, a better understanding of the carrier transport process involving photosensitivity and response time will help to tailor LC devices toward novel optical applications.

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23

Punzi, Angela, Pierre Brodard, and Eric Vauthey. "Transient Grating Investigations at Liquid–Liquid Interfaces." CHIMIA International Journal for Chemistry 59, no. 3 (March 1, 2005): 116–18. http://dx.doi.org/10.2533/000942905777676777.

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24

Lu, Baozhu, Mykola Abramchuk, Fazel Tafti, and Darius H. Torchinsky. "Transient grating measurements at ultralow probe power." Journal of the Optical Society of America B 37, no. 2 (January 28, 2020): 433. http://dx.doi.org/10.1364/josab.377545.

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25

McEwan, K. J., and Paul A. Madden. "Transient grating effects in absorbing colloidal suspensions." Journal of Chemical Physics 97, no. 11 (December 1992): 8748–59. http://dx.doi.org/10.1063/1.463393.

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26

Loring, Roger F., and Shaul Mukamel. "Microscopic theory of the transient grating experiment." Journal of Chemical Physics 83, no. 9 (November 1985): 4353–59. http://dx.doi.org/10.1063/1.449050.

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27

GRAC, R., J. L. IEHL, and M. PUGNET. "ELECTRON-HOLE PLASMA GRATINGS RELATED TO THE URBACH TAIL IN POLAR SEMICONDUCTORS." Journal of Nonlinear Optical Physics & Materials 05, no. 04 (October 1996): 631–36. http://dx.doi.org/10.1142/s0218863596000453.

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We have studied the optical index modulation in the Urbach tail of Cd 0.96 Zn 0.04 Te , using the transient grating technique in the subnanosecond domain. We have shown that the screening of the electric field due to LO-phonons by free carriers can explain the main features of picosecond transient grating experiments in the spectral region of the Urbach tail in CdZnTe. We can explain simultaneously the following features: the existence of a break in the kinetics, the saturation of the diffraction efficiency with the pump energy, the possibility of grating erasure and finally the order of magnitude of the experimental diffraction efficiency.

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28

Terazima, Masahide, Koichi Okamoto, and Noboru Hirota. "Translational diffusion of transient radicals studied by the transient grating method." Journal of Molecular Liquids 65-66 (November 1995): 401–4. http://dx.doi.org/10.1016/0167-7322(95)00885-3.

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29

Dewi, Arkidianabela Anggara, Teguh Prakoso, and Aghus Sofwan. "ARRAYED WAVEGUIDE GRATING PADA DENSE WAVELENGTH DIVISION MULTIPLEXING." TRANSIENT 7, no. 1 (March 26, 2018): 179. http://dx.doi.org/10.14710/transient.7.1.179-185.

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DWDM (Dense Wavelength Division Multiplexing) adalah suatu teknik multiplexing yang mampu mentransmisikan lebih dari 400 panjang gelombang dalam satu serat optik. Laju pengiriman data menggunakan media serat optik dapat mencapai 1 Tbps atau 1.000 Gbps. DWDM merupakan suatu perbaikan dari WDM. Inti perbaikan yang dimiliki oleh teknologi DWDM terletak pada jenis filter, serat optik dan penguat amplifier. Jenis filter yang umum dipergunakan salah satunya adalah Array Waveguide Grating (AWG). Pada Penelitian ini dianalisis kinerja suatu Array Waveguide Filters (AWG) yang mampu digunakan pada DWDM. Pada Penelitian ini dilakukan dengan menggunkan 2 software. Pertama, menggunakan software Optisystem 7 untuk memodelkan sistem DWDM. Kedua, menggunakan software OptiBPM untuk verifikasi AWG. Pada Optisystem didapatkan nilai konfigurasi DWDM yang optimal yaitu pada C Band dengan spasi kanal 50GHz dan jumlah wavelength 64. Sedangkan pada OptiBPM didapatkan untuk konfigurasi DWDM tersebut diperlukan AWG dengan dengan sudut orientasi 53 derajat, panjang FSR 1500um, lebar angular 11,4 derajat dengan ukuran 15000x10000um sehingga didapatkan nilai BER, Q-factor dan crosstalk yang memiliki perbedaan namun telah mencapai kriteria yaitu dengan Q factor antara 8,43 sampai dengan 14,09 sedangkan untuk BER dari 1,719x10-40 sampai dengan 1,19x10-17 dan crosstalk antara -149 dB sampai dengan -40,8 dB.

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30

Toscano, John P., Matthew S. Platz, Valerij Nikolaev, Yanni Cao, and Matthew B. Zimmt. "The Lifetime of Formylcarbene Determined by Transient Absorption and Transient Grating Spectroscopy." Journal of the American Chemical Society 118, no. 14 (January 1996): 3527–28. http://dx.doi.org/10.1021/ja953810x.

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31

Ajdarzadeh, Ahmad, Cristina Consani, Olivier Bräm, Andreas Tortschanoff, Andrea Cannizzo, and Majed Chergui. "Ultraviolet transient absorption, transient grating and photon echo studies of aqueous tryptophan." Chemical Physics 422 (August 2013): 47–52. http://dx.doi.org/10.1016/j.chemphys.2013.01.036.

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32

Choi, Jungkweon, Cheolhee Yang, Jeongho Kim, and Hyotcherl Ihee. "Protein Folding Dynamics of CytochromecSeen by Transient Grating and Transient Absorption Spectroscopies." Journal of Physical Chemistry B 115, no. 12 (March 31, 2011): 3127–35. http://dx.doi.org/10.1021/jp106588d.

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33

Sharif, S. M., and K. Ogusu. "Enhanced and Constant-value Transient Diffraction Efficiency from a Recorded Grating in a BaTiO₃ Crystal." Journal of Scientific Research 3, no. 2 (April 28, 2011): 217–24. http://dx.doi.org/10.3329/jsr.v3i2.5593.

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A simple method has been proposed here to get an enhanced and constant-value transient diffraction efficiency for a large time scale from a recorded grating in an undoped BaTiO3 crystal. After writing a steady-state grating by two cw recording beams (λ=514.5 nm), when the recording beams are switched off, the recorded grating as well as the diffraction efficiency decreases at a faster rate initially, and thereafter reaches to almost a stationary level for some few seconds. The diffraction efficiency for this level is very small compared to that for a steady-state grating and it becomes smaller slowly with time. We can increase (about twice the initial stationary-level value) this small diffraction efficiency from its any initial value and have this value (increased) constantly for a large time scale by using a suitable backward-pulsed reading beam containing the same properties as the recording beams.Keywords: Photorefractive effect; Transient diffraction efficiency; Steady-state volume grating; Ferroelectric perovskite crystal.© 2011 JSR Publications. ISSN: 2070-0237 (Print); 2070-0245 (Online). All rights reserved.doi:10.3329/jsr.v3i2.5593 J. Sci. Res. 3 (2), 217-224 (2011)

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34

Heeger, D. J. "Modeling simple-cell direction selectivity with normalized, half-squared, linear operators." Journal of Neurophysiology 70, no. 5 (November 1, 1993): 1885–98. http://dx.doi.org/10.1152/jn.1993.70.5.1885.

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1. A longstanding view of simple cells is that they sum their inputs linearly. However, the linear model falls short of a complete account of simple-cell direction selectivity. We have developed a nonlinear model of simple-cell responses (hereafter referred to as the normalization model) to explain a larger body of physiological data. 2. The normalization model consists of an underlying linear stage along with two additional nonlinear stages. The first is a half-squaring nonlinearity; half-squaring is half-wave rectification followed by squaring. The second is a divisive normalization non-linearity in which each model cell is suppressed by the pooled activity of a large number of cells. 3. By comparing responses with counterphase (flickering) gratings and drifting gratings, researchers have demonstrated that there is a nonlinear contribution to simple-cell responses. Specifically they found 1) that the linear prediction from counterphase grating responses underestimates a direction index computed from drifting grating responses, 2) that the linear prediction correctly estimates responses to gratings drifting in the preferred direction, and 3) that the linear prediction overestimates responses to gratings drifting in the nonpreferred direction. 4. We have simulated model cell responses and derived mathematical expressions to demonstrate that the normalization model accounts for this empirical data. Specifically the model behaves as follows. 1) The linear prediction from counterphase data underestimates the direction index computed from drifting grating responses. 2) The linear prediction from counterphase data overestimates the response to gratings drifting in the nonpreferred direction. The discrepancy between the linear prediction and the actual response is greater when using higher contrast stimuli. 3) For an appropriate choice of contrast, the linear prediction from counterphase data correctly estimates the response to gratings drifting in the preferred direction. For higher contrasts the linear prediction overestimates the actual response, and for lower contrasts the linear prediction underestimates the actual response. 5. In addition, the normalization model is qualitatively consistent with data on the dynamics of simple-cell responses. Tolhurst et al. found that simple cells respond with an initial transient burst of activity when a stimulus first appears. The normalization model behaves similarly; it takes some time after a stimulus first appears before the model cells are fully normalized. We derived the dynamics of the model and found that the transient burst of activity in model cells depends in a particular way on stimulus contrast. The burst is short for high-contrast stimuli and longer for low-contrast stimuli.(ABSTRACT TRUNCATED AT 400 WORDS)

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35

Rao, D. Narayana, Ryszard Burzynski, Xin Mi, and Paras N. Prasad. "Picosecond transient grating studies of polymeric thin films." Applied Physics Letters 48, no. 6 (February 10, 1986): 387–89. http://dx.doi.org/10.1063/1.96560.

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36

Mairesse, Y., N. Dudovich, D. Zeidler, M. Spanner, D. M. Villeneuve, and P. B. Corkum. "Phase sensitivity of high harmonic transient grating spectroscopy." Journal of Physics B: Atomic, Molecular and Optical Physics 43, no. 6 (March 2, 2010): 065401. http://dx.doi.org/10.1088/0953-4075/43/6/065401.

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37

Farrell, J. P., L. S. Spector, M. B. Gaarde, B. K. McFarland, P. H. Bucksbaum, and M. Gühr. "Strongly dispersive transient Bragg grating for high harmonics." Optics Letters 35, no. 12 (June 9, 2010): 2028. http://dx.doi.org/10.1364/ol.35.002028.

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38

TERAZIMA, MASAHIDE. "A transient grating detection method of circular dichroism." Molecular Physics 88, no. 5 (August 10, 1996): 1223–36. http://dx.doi.org/10.1080/00268979609484507.

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39

Li, Ming, John P. Nibarger, Chunlei Guo, and George N. Gibson. "Dispersion-free transient-grating frequency-resolved optical gating." Applied Optics 38, no. 24 (August 20, 1999): 5250. http://dx.doi.org/10.1364/ao.38.005250.

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40

Simoni, Francesco, Francesco Bloisi, and Luciano Vicari. "Transient Amplitude Grating in Polymer Dispersed Liquid Crystals." Molecular Crystals and Liquid Crystals Science and Technology. Section A. Molecular Crystals and Liquid Crystals 223, no. 1 (January 1992): 169–79. http://dx.doi.org/10.1080/15421409208048250.

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41

Wen, Xiaoming, Lap Van Dao, Peter Hannaford, Eun-Chel Cho, Young H. Cho, and Martin A. Green. "Ultrafast Transient Grating Spectroscopy in Silicon Quantum Dots." Journal of Nanoscience and Nanotechnology 9, no. 8 (August 1, 2009): 4575–79. http://dx.doi.org/10.1166/jnn.2009.1084.

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42

Wu, Pengfei, Li Wang, Jiren Xu, Bingsuo Zou, Xiong Gong, Guilan Zhang, Guoqing Tang, Wenju Chen, and Wei Huang. "Transient biphotonic holographic grating in photoisomerizative azo materials." Physical Review B 57, no. 7 (February 15, 1998): 3874–80. http://dx.doi.org/10.1103/physrevb.57.3874.

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43

Taschin, A., R. Cucini, C. Ziparo, P. Bartolini, and R. Torre. "Transient grating experiments on CCl4-filled porous glasses." Philosophical Magazine 87, no. 3-5 (January 21, 2007): 715–22. http://dx.doi.org/10.1080/14786430600910756.

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44

Brewer, Timothy R., John T. Fourkas, and M. D. Fayer. "Flame temperature measurement using picosecond transient grating experiments." Chemical Physics Letters 203, no. 4 (February 1993): 344–48. http://dx.doi.org/10.1016/0009-2614(93)85579-d.

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45

Park, Sohyun, June-Sik Park, and Taiha Joo. "Solvation Dynamics by Coherence Period Resolved Transient Grating." Journal of Physical Chemistry A 115, no. 16 (April 28, 2011): 3973–79. http://dx.doi.org/10.1021/jp108495t.

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46

Maznev, A. A., Jeremy A. Johnson, and Keith A. Nelson. "Non-equilibrium transient thermal grating relaxation in metal." Journal of Applied Physics 109, no. 7 (April 2011): 073517. http://dx.doi.org/10.1063/1.3569731.

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47

Harata, A., H. Nishimura, Q. Shen, T. Tanaka, and T. Sawada. "Transient reflecting grating study of ion-implanted semiconductors." Le Journal de Physique IV 04, no. C7 (July 1994): C7–159—C7–162. http://dx.doi.org/10.1051/jp4:1994738.

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48

Alam, M., R. E. Imhof, and B. Zhang. "Transient surface grating technique for thermal diffusivity measurement." Le Journal de Physique IV 04, no. C7 (July 1994): C7–299—C7–302. http://dx.doi.org/10.1051/jp4:1994771.

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Tang, Y., J. P. Schmidt, and S. A. Reid. "Nanosecond transient grating studies of jet-cooled NO2." Journal of Chemical Physics 110, no. 12 (March 22, 1999): 5734–44. http://dx.doi.org/10.1063/1.478472.

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Kawashima, Hitoshi, Fumio Sasaki, Shunsuke Kobayashi, and Toshiro Tani. "Excitation of Phonon-Polaritons with Asymmetric Transient Grating." Japanese Journal of Applied Physics 36, Part 1, No. 11 (November 15, 1997): 6764–67. http://dx.doi.org/10.1143/jjap.36.6764.

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