3,670 research outputs found

    Ultrafast photoinduced enhancement of nonlinear optical response in 15-atom gold clusters on indium tin oxide conducting film

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    We show that the third order optical nonlinearity of 15-atom gold clusters is significantly enhanced when in contact with indium tin oxide (ITO) conducting film. Open and close aperture z-scan experiments together with non-degenerate pump-probe differential transmission experiments were done using 80 fs laser pulses centered at 395 nm and 790 nm on gold clusters encased inside cyclodextrin cavities. We show that two photon absorption coefficient is enhanced by an order of magnitude as compared to that when the clusters are on pristine glass plate. The enhancement for the nonlinear optical refraction coefficient is ~3 times. The photo-induced excited state absorption using pump-probe experiments at pump wavelength of 395 nm and probe at 790 nm also show an enhancement by an order of magnitude. These results attributed to the excited state energy transfer in the coupled gold cluster-ITO system are different from the enhancement seen so far in charge donor-acceptor complexes and nanoparticle-conjugate polymer composites.Comment: To appear in Optics Express (2013); http://dx.doi.org/10.1364/OE.21.00848

    Femtosecond Photoexcited Carrier Dynamics in Reduced Graphene Oxide Suspensions and Films

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    We report ultrafast response of femtosecond photoexcited carriers in single layer reduced graphene oxide flakes suspended in water as well as few layer thick film deposited on indium tin oxide coated glass plate using pump-probe differential transmission spectroscopy at 790 nm. The carrier relaxation dynamics has three components: ~200 fs, 1 to 2 ps, and ~25 ps, all of them independent of pump fluence. It is seen that the second component (1 to 2 ps) assigned to the lifetime of hot optical phonons is larger for graphene in suspensions whereas other two time constants are the same for both the suspension and the film. The value of third order nonlinear susceptibility estimated from the pump-probe experiments is compared with that obtained from the open aperture Z-scan results for the suspension.Comment: 4 pages, 4 figures, to appear in International Journal of Nanoscience (IJN), 201

    Jordan-Schwinger realizations of three-dimensional polynomial algebras

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    A three-dimensional polynomial algebra of order mm is defined by the commutation relations [P0,P±][P_0, P_\pm] == ±P±\pm P_\pm, [P+,P][P_+, P_-] == ϕ(m)(P0)\phi^{(m)}(P_0) where ϕ(m)(P0)\phi^{(m)}(P_0) is an mm-th order polynomial in P0P_0 with the coefficients being constants or central elements of the algebra. It is shown that two given mutually commuting polynomial algebras of orders ll and mm can be combined to give two distinct (l+m+1)(l+m+1)-th order polynomial algebras. This procedure follows from a generalization of the well known Jordan-Schwinger method of construction of su(2)su(2) and su(1,1)su(1,1) algebras from two mutually commuting boson algebras.Comment: 10 pages, LaTeX2

    Acoustic and optical phonon dynamics from femtosecond time-resolved optical spectroscopy of superconducting iron pnictide Ca(Fe_0.944Co_0.056)_2As_2

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    We report temperature evolution of coherently excited acoustic and optical phonon dynamics in superconducting iron pnictide single crystal Ca(Fe_0.944Co_0.056)_2As_2 across the spin density wave transition at T_SDW ~ 85 K and superconducting transition at T_SC ~20 K. Strain pulse propagation model applied to the generation of the acoustic phonons yields the temperature dependence of the optical constants, and longitudinal and transverse sound velocities in the temperature range of 3.1 K to 300 K. The frequency and dephasing times of the phonons show anomalous temperature dependence below T_SC indicating a coupling of these low energy excitations with the Cooper-pair quasiparticles. A maximum in the amplitude of the acoustic modes at T ~ 170 is seen, attributed to spin fluctuations and strong spin-lattice coupling before T_SDW.Comment: 6 pages, 4 figures (revised manuscript

    Ultrafast quasiparticle dynamics in superconducting iron pnictide CaFe1.89Co0.11As2

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    Nonequilibrium quasiparticle relaxation dynamics is reported in superconducting CaFe1.89Co0.11As2 single crystal using femtosecond time-resolved pump-probe spectroscopy. The carrier dynamics reflects a three-channel decay of laser deposited energy with characteristic time scales varying from few hundreds of femtoseconds to order of few nanoseconds where the amplitudes and time-constants of the individual electronic relaxation components show significant changes in the vicinity of the spin density wave (T_SDW ~ 85 K) and superconducting (T_SC ~ 20 K) phase transition temperatures. The quasiparticles dynamics in the superconducting state reveals a charge gap with reduced gap value of 2Δ\Delta_0/k_BT_SC ~ 1.8. We have determined the electron-phonon coupling constant \lemda to be ~ 0.14 from the temperature dependent relaxation time in the normal state, a value close to those reported for other types of pnictides. From the peculiar temperature-dependence of the carrier dynamics in the intermediate temperature region between the superconducting and spin density wave phase transitions, we infer a temperature scale where the charge gap associated with the spin ordered phase is maximum and closes on either side while approaching the two phase transition temperatures.Comment: 6 pages, 4 figures (revised manuscript); http://dx.doi.org/10.1016/j.ssc.2013.02.00

    Sponge Biodiversity in Kerala and its Biotechnological Potentials

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    Animals which exist today may be classified under two categories; I) Protozoa or s ingle celled animals 2) Metazoa or multicellular animals. Metazoam in tum, may be divided into two groups: a) Diploblastic, with two germ layers (ectoderm and endoderm) and b) Triploblastic, with three germ layers (eetoderm, mesoderm and endoderm). I n sponges thcre are no layers as seen in diploblastic or triobl.astic or triploblastic groups, but the 'layers', in sponges, are made of loosely arranged cells which can even change their location at will

    Pathological manifestations of sponge infestation in Perna indica Kuriakose & Nair 1976

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    Pathological manifestations of bioeroding sponges on the brown mussel, Perna indica were studied. The major manifestation was blister formation (46.3%). Nacre erosis was observed in 7.6% of the total infested population. Bifacial porosis was noted in 19.1% of infested shells; discolouration of shell was observed in 19.8 % and melanosis in 13.1 % of the infested population

    Large-amplitude chirped coherent phonons in tellurium mediated by ultrafast photoexcited carrier diffusion

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    We report femtosecond time-resolved reflectivity measurements of coherent phonons in tellurium performed over a wide range of temperatures (3K to 296K) and pump laser intensities. A totally symmetric A1_{1} coherent phonon at 3.6 THz responsible for the oscillations in the reflectivity data is observed to be strongly positively chirped (i.e, phonon time period decreases at longer pump-probe delay times) with increasing photoexcited carrier density, more so at lower temperatures. We show for the first time that the temperature dependence of the coherent phonon frequency is anomalous (i.e, increasing with increasing temperature) at high photoexcited carrier density due to electron-phonon interaction. At the highest photoexcited carrier density of \sim 1.4 ×\times 1021^{21}cm3^{-3} and the sample temperature of 3K, the lattice displacement of the coherent phonon mode is estimated to be as high as \sim 0.24 \AA. Numerical simulations based on coupled effects of optical absorption and carrier diffusion reveal that the diffusion of carriers dominates the non-oscillatory electronic part of the time-resolved reflectivity. Finally, using the pump-probe experiments at low carrier density of 6 ×\times 1018^{18} cm3^{-3}, we separate the phonon anharmonicity to obtain the electron-phonon coupling contribution to the phonon frequency and linewidth.Comment: 22 pages, 6 figures, submitted to PR
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