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Journal articles on the topic 'Pump-probe'

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Published: 4 June 2021
Last updated: 1 April 2023

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1

Schmidt, Aaron J. "PUMP-PROBE THERMOREFLECTANCE." Annual Review of Heat Transfer 16, no. 1 (2013): 159–81. http://dx.doi.org/10.1615/annualrevheattransfer.v16.60.

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2

Hoffmann, Roald. "Pulse, Pump & Probe." American Scientist 87, no. 4 (1999): 308. http://dx.doi.org/10.1511/1999.4.308.

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3

Hoffmann, Roald. "Pulse, Pump & Probe." American Scientist 87, no. 4 (1999): 308. http://dx.doi.org/10.1511/1999.30.308.

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4

Malý, Pavel, and Tobias Brixner. "Fluorescence‐Detected Pump–Probe Spectroscopy." Angewandte Chemie International Edition 60, no. 34 (July 16, 2021): 18867–75. http://dx.doi.org/10.1002/anie.202102901.

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5

Malý, Pavel, and Tobias Brixner. "Fluoreszenz‐detektierte Pump‐Probe‐Spektroskopie." Angewandte Chemie 133, no. 34 (July 16, 2021): 19015–24. http://dx.doi.org/10.1002/ange.202102901.

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6

Fushitani, Mizuho. "Applications of pump-probe spectroscopy." Annual Reports Section "C" (Physical Chemistry) 104 (2008): 272. http://dx.doi.org/10.1039/b703983m.

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7

Jiang, Jun, Warren S. Warren, and Martin C. Fischer. "Crossed-beam pump-probe microscopy." Optics Express 28, no. 8 (April 1, 2020): 11259. http://dx.doi.org/10.1364/oe.389004.

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8

Khitrova, Galina, Paul R. Berman, and Murray Sargent. "Theory of pump–probe spectroscopy." Journal of the Optical Society of America B 5, no. 1 (January 1, 1988): 160. http://dx.doi.org/10.1364/josab.5.000160.

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9

Parkhomenko, A. I., and A. M. Shalagin. "Ground-state pump-probe spectroscopy." Journal of Experimental and Theoretical Physics 105, no. 6 (December 2007): 1095–106. http://dx.doi.org/10.1134/s1063776107120011.

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10

Glownia, J. H., J. Misewich, and P. P. Sorokin. "Ultrafast ultraviolet pump–probe apparatus." Journal of the Optical Society of America B 3, no. 11 (November 1, 1986): 1573. http://dx.doi.org/10.1364/josab.3.001573.

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11

Inoue, Jun-ichi, and Akira Shimizu. "Pump Built-in Hamiltonian Method for Pump-Probe Spectroscopy." Journal of the Physical Society of Japan 68, no. 8 (August 15, 1999): 2534–37. http://dx.doi.org/10.1143/jpsj.68.2534.

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12

Buckup, Tiago, Janne Savolainen, Wendel Wohlleben, Jennifer L. Herek, Hideki Hashimoto, Ricardo R. B. Correia, and Marcus Motzkus. "Pump-probe and pump-deplete-probe spectroscopies on carotenoids with N=9–15 conjugated bonds." Journal of Chemical Physics 125, no. 19 (November 21, 2006): 194505. http://dx.doi.org/10.1063/1.2388274.

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13

Kovalev, V. I. "Effect of pump and probe radiation non-monochromaticity in pump-probe spectroscopy of Brillouin scattering." Journal of the Optical Society of America B 36, no. 4 (March 21, 2019): 1062. http://dx.doi.org/10.1364/josab.36.001062.

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14

Kaya, Gamze. "Field-free molecular alignment of carbon dioxide molecules measured with above-threshold ionization yields." Canadian Journal of Physics 98, no. 4 (April 2020): 390–94. http://dx.doi.org/10.1139/cjp-2019-0361.

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We present measurements of above-threshold ionization (ATI) of CO2 in a pump-probe experiment where the pump pulse creates a rotational wave packet and the linearly polarized probe pulse generates the ATI spectrum as a function of the pump-probe delay time, which sweeps over the revival time of field-free alignment and its quarter fractions. The observed alignment signals, which are the electron yields of ATI by a probe pulse as a function of a delay between the pump and probe pulse, are compared with the calculated alignment parameter [Formula: see text]. The results are explained by nuclear spin statistics and the wave packet evolution of the CO2 molecule in terms of the highest occupied molecular orbital.
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15

Weimer, Wayne A., and Norman J. Dovichi. "Optimization of Photothermal Refraction for Flowing Liquid Samples." Applied Spectroscopy 39, no. 6 (November 1985): 1009–13. http://dx.doi.org/10.1366/0003702854249394.

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A model has been developed for photothermal refraction using flowing liquid samples. In photothermal refraction, a cylindrical thermal lens is formed within the sample because of the temperature rise produced by the absorbance of a pump laser beam. This cylindrical thermal lens is intersected at right angles with a second probe laser. For static samples, the maximum signal results when the pump and probe beams are coplanar. Defocusing of the probe beam by the cylindrical thermal lens is detected as a change in the far-field probe beam center intensity. Flow acts to distort the temperature distribution by transporting heat down stream. For flowing samples, the optimum signal is found when the probe beam is located about one pump beam spot size down stream from the pump beam axis.
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16

Foing, J. P., M. Joffre, J. L. Oudar, and D. Hulin. "Coherence effects in pump–probe experiments with chirped pump pulses." Journal of the Optical Society of America B 10, no. 7 (July 1, 1993): 1143. http://dx.doi.org/10.1364/josab.10.001143.

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17

Kang, Heung-Sik, and In Soo Ko. "Attosecond XFEL for pump–probe experiments." Nature Photonics 14, no. 1 (December 20, 2019): 7–8. http://dx.doi.org/10.1038/s41566-019-0570-8.

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18

Benka, Stephen. "Optical pump-probe diagnosis for melanoma?" Physics Today 64, no. 7 (July 2011): 18. http://dx.doi.org/10.1063/pt.3.1154.

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19

Massaro, Eric S., Andrew H. Hill, and Erik M. Grumstrup. "Super-Resolution Structured Pump–Probe Microscopy." ACS Photonics 3, no. 4 (March 7, 2016): 501–6. http://dx.doi.org/10.1021/acsphotonics.6b00140.

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20

Robles, Francisco E., Prathyush Samineni, Jesse W. Wilson, and Warren S. Warren. "Pump-probe nonlinear phase dispersion spectroscopy." Optics Express 21, no. 8 (April 9, 2013): 9353. http://dx.doi.org/10.1364/oe.21.009353.

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21

Fischer, Martin C., Jesse W. Wilson, Francisco E. Robles, and Warren S. Warren. "Invited Review Article: Pump-probe microscopy." Review of Scientific Instruments 87, no. 3 (March 2016): 031101. http://dx.doi.org/10.1063/1.4943211.

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22

Korobchevskaya, Kseniya, Paolo Bianchini, Silvia Galiani, Marco Scotto d'Abbusco, Colin Sheppard, and Alberto Diaspro. "Development of Pump-Probe Nanoscopy Architecture." Biophysical Journal 106, no. 2 (January 2014): 201a. http://dx.doi.org/10.1016/j.bpj.2013.11.1185.

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23

SHIGEKAWA, Hidemi, Shoji YOSHIDA, and Osamu TAKEUCHI. "Optical Pump-Probe Scanning Tunneling Microscopy." Hyomen Kagaku 35, no. 12 (2014): 656–61. http://dx.doi.org/10.1380/jsssj.35.656.

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24

Farrow, Darcie A., Anchi Yu, and David M. Jonas. "Spectral relaxation in pump–probe transients." Journal of Chemical Physics 118, no. 20 (May 22, 2003): 9348–56. http://dx.doi.org/10.1063/1.1564058.

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25

Elzinga, Paul A., Fred E. Lytle, Yanan Jian, Galen B. King, and Normand M. Laurendeau. "Pump/Probe Spectroscopy by Asynchronous Optical Sampling." Applied Spectroscopy 41, no. 1 (January 1987): 2–4. http://dx.doi.org/10.1366/0003702874868025.

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We report the first results from a new pump/probe technique called asynchronous optical sampling (ASOPS). The method employs a mode-locked, frequency-doubled Nd:YAG laser operating at a repetition rate of 81.5970000 MHz as the pump laser, and a synchronously pumped dye laser (R6G) operating at a repetition rate of 81.5870000 MHz as the probe laser system. The 10-kHz beat frequency produces a repetitive relative phase walk-out of the pump and probe pulses which replaces the optical delay line used in conventional instruments. Studies of rhodamine B in methanol demonstrate that the instrument response is proportional to pump power, probe power, and sample absorptance. The fluorescence lifetime of 4 × 10−5 M rhodamine B is determined to be 2.3 ns.
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26

Kee, Tak W. "Femtosecond Pump–Push–Probe and Pump–Dump–Probe Spectroscopy of Conjugated Polymers: New Insight and Opportunities." Journal of Physical Chemistry Letters 5, no. 18 (September 8, 2014): 3231–40. http://dx.doi.org/10.1021/jz501549h.

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27

Chen, Huajun. "Controllable Fast and Slow Light in Photonic-Molecule Optomechanics with Phonon Pump." Micromachines 12, no. 9 (September 4, 2021): 1074. http://dx.doi.org/10.3390/mi12091074.

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We theoretically investigate the optical output fields of a photonic-molecule optomechanical system in an optomechanically induced transparency (OMIT) regime, in which the optomechanical cavity is optically driven by a strong pump laser field and a weak probe laser field and the mechanical mode is driven by weak coherent phonon driving. The numerical simulations indicate that when the driven frequency of the phonon pump equals the frequency difference of the two laser fields, we show an enhancement OMIT where the probe transmission can exceed unity via controlling the driving amplitude and pump phase of the phonon driving. In addition, the phase dispersion of the transmitted probe field can be modified for different parametric regimes, which leads to a tunable delayed probe light transmission. We further study the group delay of the output probe field with numerical simulations, which can reach a tunable conversion from slow to fast light with the manipulation of the pump laser power, the ratio parameter of the two cavities, and the driving amplitude and phase of the weak phonon pump.
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28

Yuan, Chao, Riley Hanus, and Samuel Graham. "A review of thermoreflectance techniques for characterizing wide bandgap semiconductors’ thermal properties and devices’ temperatures." Journal of Applied Physics 132, no. 22 (December 14, 2022): 220701. http://dx.doi.org/10.1063/5.0122200.

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Thermoreflectance-based techniques, such as pump–probe thermoreflectance (pump–probe TR) and thermoreflectance thermal imaging (TTI), have emerged as the powerful and versatile tools for the characterization of wide bandgap (WBG) and ultrawide bandgap (UWBG) semiconductor thermal transport properties and device temperatures, respectively. This Review begins with the basic principles and standard implementations of pump–probe TR and TTI techniques, illustrating that when analyzing WBG and UWBG materials or devices with pump–probe TR or TTI, a metal thin-film layer is often required. Due to the transparency of the semiconductor layers to light sources with sub-bandgap energies, these measurements directly on semiconductors with bandgaps larger than 3 eV remain challenging. This Review then summarizes the general applications of pump–probe TR and TTI techniques for characterizing WBG and UWBG materials and devices where thin metals are utilized, followed by introducing more advanced approaches to conventional pump–probe TR and TTI methods, which achieve the direct characterizations of thermal properties on GaN-based materials and the channel temperature on GaN-based devices without the use of thin-film metals. Discussions on these techniques show that they provide more accurate results and rapid feedback and would ideally be used as a monitoring tool during manufacturing. Finally, this Review concludes with a summary that discusses the current limitations and proposes some directions for future development.
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29

Dakovski, Georgi L., Brian Kubera, Song Lan, and Jie Shan. "Finite pump-beam-size effects in optical pump-terahertz probe spectroscopy." Journal of the Optical Society of America B 23, no. 1 (January 1, 2006): 139. http://dx.doi.org/10.1364/josab.23.000139.

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30

MAJUMDAR, INDRANI, and PRATIMA SEM. "PUMP-PROBE SPECTROSCOPIC ANALYSIS OF FREE INDUCTION DECAY IN GaAs/AlxGa1-xAs QUANTUM WELL STRUCTURES." Journal of Nonlinear Optical Physics & Materials 08, no. 04 (December 1999): 443–54. http://dx.doi.org/10.1142/s021886359900031x.

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The theoretical formulation for pump-probe spectroscopic analysis of free induction decay has been made using semiclassical time dependent perturbation technique in GaAs/AlxGa1-xAs quantum well structure. The pump pulse is considered to be tuned below the band edge and the excitation intensity is assumed to be in the moderate power regime so that the only many-body effect that dominates is the excitonic effect. The probe transmission spectrum features the characteristic resonance frequencies of the system concerned. The temporal nature of the transmitted probe signal is also found to characterize the ultrafast free induction decay of the pump induced polarization, which is recorded by the low intensity probe transmission in the system.
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31

So, P. T. C., C. Y. Dong, C. Buhler, and E. Gratton. "Time-Resolved Stimulated-Emission Fluorescence Microscope." Proceedings, annual meeting, Electron Microscopy Society of America 54 (August 11, 1996): 278–79. http://dx.doi.org/10.1017/s042482010016385x.

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Time-resolved stimulated-emission fluorescence microscopy is a novel technique for obtaining super-diffraction limited spatial resolution and sub-nanosecond time resolution using a multi-photon process. This technique is inspired by traditional asynchronous stimulated-emission pump-probe spectroscopy. Fluorescence sample is first excited by a pump laser pulse, tuned to the molecular absorption band of the molecule. Within the chromophore lifetime, a second probe pulse, tuned to the emission band, stimulates fluorescence emission.The spatial resolution enhancement originates from the bilinear dependence of the stimulated emission efficiency on both the pump and probe beam intensities. At the objective focal point, the stimulated emission point spread function is the product of the point spread functions of the pump and probe beams. This situation is mathematically equivalent to both the confocal and the two-photon methods. 3-D depth discrimination and superior spatial resolution is expected.
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32

Meyer, S., C. Meier, and V. Engel. "Photoelectron distributions from femtosecond pump/probe excitation with chirped probe pulses." Journal of Chemical Physics 108, no. 18 (May 8, 1998): 7631–36. http://dx.doi.org/10.1063/1.476198.

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33

SINGH, ASHA, SALAHUDDIN KHAN, PODILI SIVASANKARAIAH, J. JAYABALAN, and RAMA CHARI. "Tunable third-harmonic probe for non-degenerate ultrafast pump–probe measurements." Pramana 82, no. 2 (February 2014): 413–17. http://dx.doi.org/10.1007/s12043-014-0699-4.

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34

Peng, Wanyue, and Richard B. Wilson. "Thermal model for time-domain thermoreflectance experiments in a laser-flash geometry." Journal of Applied Physics 131, no. 13 (April 7, 2022): 134301. http://dx.doi.org/10.1063/5.0082549.

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Time-domain thermoreflectance (TDTR) is a well-established pump–probe method for measuring thermal conductivity and interface conductance of multilayers. Interpreting signals in a TDTR experiment requires a thermal model. In standard front/front TDTR experiments, both pump and probe beams typically irradiate the surface of a multilayer. As a result, existing thermal models for interpreting thermoreflectance experiments assume that the pump and probe beams both interact with the surface layer. Here, we present a frequency-domain solution to the heat-diffusion equation of a multilayer in response to nonhomogeneous laser heating. This model allows analysis of experiments where the pump and probe beams irradiate opposite sides of a multilayer. We call such a geometry a front/back experiment to differentiate such experiments from standard TDTR experiments. As an example, we consider a 60nm amorphous Si film. We consider how signals differ in a front/front vs front/back geometry and compare thermal model predictions to experimental data.
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35

Fuertes Marrón, D. "Modulation above Pump Beam Energy in Photoreflectance." International Journal of Photoenergy 2017 (2017): 1–4. http://dx.doi.org/10.1155/2017/4894127.

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Photoreflectance is used for the characterisation of semiconductor samples, usually by sweeping the monochromatized probe beam within the energy range comprised between the highest value set up by the pump beam and the lowest absorption threshold of the sample. There is, however, no fundamental upper limit for the probe beam other than the limited spectral content of the source and the responsivity of the detector. As long as the modulation mechanism behind photoreflectance does affect the complete electronic structure of the material under study, sweeping the probe beam towards higher energies from that of the pump source is equally effective in order to probe high-energy critical points. This fact, up to now largely overseen, is shown experimentally in this work. E1 and E0 + Δ0 critical points of bulk GaAs are unambiguously resolved using pump light of lower energy. This type of upstream modulation may widen further applications of the technique.
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36

Khos-Ochir, Tsogvoo, Purevdorj Munkhbaatar, Tsermaa Baatarchuluun, Norovsambuu Tuvjargal, Bat-Erdene Ulziibayar, Ganbold Erdene-Ochir, Gombosuren Munkhbayar, Myagmar Otgonbaatar, Ojiyed Tegus, and Jav Davaasambuu. "Femtosecond Pump Probe Spectroscopy Implementation for Semiconductors." Solid State Phenomena 288 (March 2019): 148–52. http://dx.doi.org/10.4028/www.scientific.net/ssp.288.148.

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Two different pump-probe (PP) setups were developed successfully with different femtosecond pulse lasers. Using a PP setup with an ultra-short pulse laser, the excitation of coherent phonons in GaAs was measured for a calibration and an accuracy test of the developed setup. The frequencies of the coherent phonon modes were in good agreement with reported values [1, 2]. The setups for ZnSe and GaAs were transmission and reflection–type, respectively. When using the ultra-short pulse laser, the signal in the PP experiment was measured by a balanced photo diode.In the other PP experimental setup, built to measure the transient transmittance of bulk ZnSe, the light source and detector differed from the previous PP setup. A strong pulse laser was successfully used for the spectrally resolved pump probe experimental setup. A broadband, high-resolution spectrometer (HR4000CG-UV-NIR) was used as the detector.
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37

Cabrera, Jose A., Craig R. Bieler, Benjamin C. Olbricht, Wytze E. van der Veer, and Kenneth C. Janda. "Time-dependent pump-probe spectra of NeBr2." Journal of Chemical Physics 123, no. 5 (August 2005): 054311. http://dx.doi.org/10.1063/1.1990118.

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38

Wang Zhi-Guo, Luo Hui, Fan Zhen-Fang, and Xie Yuan-Ping. "Research on an pump-probe rubidium magnetometer." Acta Physica Sinica 65, no. 21 (2016): 210702. http://dx.doi.org/10.7498/aps.65.210702.

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39

Chen Cong, Liang Pan, Hu Rong-Rong, Jia Tian-Qing, Sun Zhen-Rong, and Feng Dong-Hai. "Pump-orientation-probe technique and its applications." Acta Physica Sinica 67, no. 9 (2018): 097201. http://dx.doi.org/10.7498/aps.67.20180244.

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40

Fain, B., V. Khidekel, and S. H. Lin. "Phase-dependent amplification in pump-probe experiments." Physical Review A 49, no. 2 (February 1, 1994): 1498–501. http://dx.doi.org/10.1103/physreva.49.1498.

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41

Cho, Minhaeng. "Two-dimensional circularly polarized pump–probe spectroscopy." Journal of Chemical Physics 119, no. 14 (October 8, 2003): 7003–16. http://dx.doi.org/10.1063/1.1599344.

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42

Popov, S. V., Yu P. Svirko, and N. I. Zheludev. "Pump–probe reflective polarization-sensitive nonlinear optics." Journal of the Optical Society of America B 13, no. 12 (December 1, 1996): 2729. http://dx.doi.org/10.1364/josab.13.002729.

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43

Berman, P. R., and B. Bian. "Pump-probe spectroscopy approach to Bragg scattering." Physical Review A 55, no. 6 (June 1, 1997): 4382–85. http://dx.doi.org/10.1103/physreva.55.4382.

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44

Ochoa, Maicol A., Yoram Selzer, Uri Peskin, and Michael Galperin. "Pump–Probe Noise Spectroscopy of Molecular Junctions." Journal of Physical Chemistry Letters 6, no. 3 (January 21, 2015): 470–76. http://dx.doi.org/10.1021/jz502484z.

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45

Saikan, Seishiro. "Vibronic quantum beat in pump-probe experiments." Physical Review A 38, no. 9 (November 1, 1988): 4669–72. http://dx.doi.org/10.1103/physreva.38.4669.

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46

White, Richard T., and Iain T. McKinnie. "Pump-probe switching in gain-switched lasers." Optics Express 3, no. 8 (October 12, 1998): 298. http://dx.doi.org/10.1364/oe.3.000298.

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47

Berman, P. R., B. Dubetsky, and J. Guo. "Recoil-induced resonances in pump-probe spectroscopy." Physical Review A 51, no. 5 (May 1, 1995): 3947–58. http://dx.doi.org/10.1103/physreva.51.3947.

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48

Nechay, B. A., U. Siegner, M. Achermann, H. Bielefeldt, and U. Keller. "Femtosecond pump-probe near-field optical microscopy." Review of Scientific Instruments 70, no. 6 (June 1999): 2758–64. http://dx.doi.org/10.1063/1.1149841.

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49

Wintner, E. "Numerical evaluation of optical pump‐probe experiments." Journal of Applied Physics 57, no. 5 (March 1985): 1533–37. http://dx.doi.org/10.1063/1.334467.

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50

Eberly, J. H., and V. D. Popov. "Phase-dependent pump-probe line-shape formulas." Physical Review A 37, no. 6 (March 1, 1988): 2012–16. http://dx.doi.org/10.1103/physreva.37.2012.

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