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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 77 (1995), S. 4935-4940 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The real and imaginary parts of the linear electro-optic (EO) constants of four dyes, i.e., N,N-dimethylaminonitrostilbene (DANS), 4-[N-(2-hydroxyethyl)-N-ethyl]amino-4'-nitroazo- benzene [disperse red 1 (DR1)], N,N-dimentylindoaniline [phenol blue (PB)], and 1,1',3,3,3',3'-hexamethylindotricarbocyanine iodide (HITCI) in polymethylmethacrylate (PMMA) films were determined using a Mach–Zehnder interferometer. The electronic transitions of DANS, DR1, PB, and HITCI are off-resonant, near-resonant, and resonant on the higher and lower energy sides with a He-Ne laser wavelength (632.8 nm), respectively. The different ratios of the real and imaginary parts of the EO constants of four dyes including their signs are successfully explained in terms of detuning energy. © 1995 American Institute of Physics.
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 110 (1999), S. 5844-5850 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We observed the ultrafast response of exciton (S1-exciton) and excited-exciton (S2-exciton) in one-dimensional J-aggregates of three-level porphyrin molecules by femtosecond pump–probe spectroscopy. The decay profiles of the nonlinear response can be fitted to a sum of instantaneous response and two exponential decay components with time constants of 1.3±0.1 and 40±1 ps. The former and latter were found to correspond to the lifetimes of S2- and S1-excitons, respectively. The origins of the nonlinearity were attributed to the following three contributions: (1) coherent effects between the pump and probe via one-photon virtual S1-exciton, (2) induced absorption of real S2-excitons generated by two photons, and (3) induced absorption of real S1-exciton. © 1999 American Institute of Physics.
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  • 3
    ISSN: 1520-6041
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
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  • 4
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Biochemistry 25 (1986), S. 3356-3363 
    ISSN: 1520-4995
    Source: ACS Legacy Archives
    Topics: Biology , Chemistry and Pharmacology
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 63 (1988), S. 5491-5494 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The tunneling process of photogenerated carriers in AlAs/GaAs double quantum well structures in which two wells have different widths (60 and 80 A(ring)) was studied by steady-state and time-resolved photoluminescence spectra. The tunneling process was found to play an important role for a barrier thickness narrower than about 40 A(ring). The tunneling rate was determined as 2×1010 s−1 for a 30-A(ring) barrier. The quantum-mechanical penetration depth of the wave function into an AlAs barrier was estimated as 6 A(ring) from the barrier width dependence of luminescence intensity ratio between the two wells. The tunneling rate and penetration depth are consistent with a simple envelope function approximation with no Γ-X mixing.
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 64 (1988), S. 2625-2629 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A new method is proposed for the determination of the electro-optic constants and relevant nonlinear susceptibilities. It was applied to polycarbonate films doped with 4-diethylamino-4'-nitrostilbene. The real and imaginary parts of the third-order nonlinear susceptibility X(3) (−ω;ω, 0,0) of the film were determined by the method between 600 and 800 nm at room temperature. X(3) (−ω;ω, 0,0) is (6+4i)×10−12 esu or quadratic electro-optic constant R is (−1−0.7i)×10−20 m2/V2 at 597 nm.
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 62 (1987), S. 1010-1016 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The time-resolved luminescence spectra from excited conduction subbands in three samples of multi-quantum-well GaAs/AlxGa1−xAs (x=0.3 and 1) semiconductors with several well widths and barrier heights were obtained under high-density excitations by a 30-ps pulsed laser at 532 nm, which generated electron–hole pairs to the concentration of 1010–1013/cm2 per well per pulse at 77 K. The temperature and the Fermi energy of electron were determined by fitting best the constructed time-resolved spectrum to the observed, and the time-dependent electron energy was obtained by using these parameters. The energy-loss rates of hot electrons are at least twice smaller than the calculated ones induced by the electron-polar phonon scattering, including the screening effect due to the high carrier density.
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  • 8
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 75 (1994), S. 382-387 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: An exciton with a massive hole trapped at an arbitrary position in a semiconductor quantum dot (QD) is studied theoretically. The energy spectra, wave functions, and dipole moments are obtained in the effective mass approximation. The contour maps of the density of the lowest state obtained clearly show the development of the wave function from the strong to weak confinement limit. The energy minimum for the lowest state is found for the trapped hole position from the center of a QD. The dipole moment of an exciton with the hole trapped on the surface is found to be proportional to R0 for small R0 and nearly constant for large R0.
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  • 9
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 85 (1986), S. 1211-1219 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The time-resolved Sn–S1 and Tn–T1 resonance Raman spectra of highly purified chrysene in tetrahydrofuran were observed at room temperature using the third harmonic of a Q-switched Nd:YAG laser as an electronic excitation pulse and a dye laser pumped by the second harmonic of another Q-switched Nd:YAG laser as a Raman probe pulse. We observed the Raman lines attributed to the S1 state at 1549, 1369, 1344, 1110, and 990 cm−1, and to the T1 state at 1528, 1494, 1353, 1199, 1110, 990, 678, 554, 472, and 286 cm−1. The decay time of 1369 cm−1 (S1) line, the formation time of 1528 cm−1 (T1) line, that of 1199 cm−1 (T1) line, and the fluorescence lifetime were obtained to be 35+6−5, 51+19−12, 41+10−7, and 41+− 1 ns, respectively. The observed Sn–S1 and Tn–T1 resonance Raman spectra were compared with the previously reported fluorescence and phosphorescence spectra in Shpolskii matrices, Sn–S1 and Tn–T1 resonance CARS spectra, and Tn–T1 spontaneous resonance Raman spectra. Discussion was made on the geometrical changes in the excited states on the assumption that the changes were not very large for the rigid molecular structure. We came to the following conclusions: (1) The resonance-coupled excited singlet state is different from the ground state in geometry mainly along the normal coordinates of the vibrational modes which have the Sn–S1 resonance Raman peaks at 1549 and 1344 cm−1. (2) The geometry of the resonance-coupled excited triplet state differs from that of the ground state mainly along five coordinates. Four of them correspond to the vibrational bands observed in the Tn–T1 resonance Raman spectrum at 1528, 1353, 1110, and 990 cm−1. The other corresponds to the vibrational bands observed in the Shpolskii spectrum of phosphorescence at 1385 cm−1 in literature. (3) The S1 and T1 states differ along the normal coordinates of the modes which have the Tn–T1 resonance Raman bands at 678, 554,472, and 286 cm−1.
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  • 10
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 116 (2002), S. 184-195 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Dynamics of excited states in porphyrin J-aggregates has been investigated using femtosecond time-resolved fluorescence and absorption spectroscopies. An ultrafast relaxation process due to internal conversion (IC) from the S2-exciton state to the S1-exciton state is observed as an S2-fluorescence and a recovery from a bleaching of the S2-exciton state. The S2-fluorescence shows a sharp spectrum with almost no Stokes shift with a decay-time constant of 360±70 fs. In the transient absorption spectrum, the bleaching of the S2-exciton state disappears with a time constant of about 300 fs, which is in agreement with the result of the time-resolved fluorescence data. Relaxation dynamics of the S1-exciton following S2→S1IC is also studied and several relaxation processes such as an intra-aggregate vibrational energy redistribution, vibrational and phase-space coolings are investigated. © 2002 American Institute of Physics.
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