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The recent developments in the theory of rapidly rotating Bose atoms have been reviewed in this article. Rotation leads to the development of quantized-vortices, that cluster into a vortex array, exactly to how superfluid helium behaves. Theoretically, a number of strongly correlated phases are projected to exist in this domain, which might be thought of as bosonic counterparts of fractional quantum Hall effect (FQHE). It is now possible for bosons associating with a short-range interaction to exhibit a FQHE, because the system of neutral bosons in a fast rotating atomic trap is analogous to charged bosons placed in a fictitious magnetic field. The neutral collective spin-conserving and spin-flip excitation for the rotating ultra-cold dilute Bose atoms in the FQHE domain are being discussed. We have introduced a realistic interaction between the Bose particles together with long-range interaction and presented a short review article about various fractional quantum Hall states and their spin conserving and spin reversed collective modes., Comment: Short review paper containing 29 pages, 11 figures accepted to Journal of Low Temperature Physics

We have studied the collective spin-conserving collective excitation spectra in rotating diluted ultra-cold Bose atoms. Double roton-minima have been observed in the fractional quantum Hall (FQH) states for the two filling fractions ($\nu$) of the first series of Jain's composite fermion sequences. The obtained roton-minima for $\nu$ = 1/4 are at the wave-vectors 1.26 and 2.38 and the roton-minima for $\nu$ = 1/6 have been shifted to 1.08 and 2.06. Such shift of roton-minima is attributed due to strong correlation between the particles in bosonic FQH-system. Moreover, the number of roton minima observed depends upon number of attached fluxes as well as the ranges of interaction between the particles., Comment: 6 pages, 4 figures, Accepted manuscript in Physica Scripta

We experimentally investigate spectral statistics in Anderson localization in two-dimensional amorphous disordered media. Intensity distributions captured over an ultrabroad wavelength range of $\sim 600$~nm and averaged over numerous configurations provided the Ioffe-Regel parameter to be $\sim2.5$ over the investigated wavelength range. The spectra of the disordered structures provided access to several quasimodes, whose widths and separations allowed to directly estimate the optical Thouless conductance $g_{Th}$, consistently observed to be below unity. The probability distribution of $g_{Th}$ was measured to be a log-normal. Despite being in the Anderson localization regime, the spacings of energy levels of the system was seen to follow a near Wigner-Dyson function. Theoretical calculations based on the tight-binding model, modified to include coupling to a bath, yielded results that were in excellent agreement with experiments. From the model, the level-spacing behavior was attributed to the degree of localization obtained in the optical disordered system., Comment: 6 pages, 7 figures in main manuscript, and 3 pages, 5 figures in Supplementary Document

Anderson localization is a striking phenomenon wherein transport of light is arrested due to the formation of disorder-induced resonances. Hitherto, Anderson localization has been demonstrated separately in two limits of disorder, namely, amorphous disorder and nearly-periodic disorder. However, transport properties in the two limits are yet unstudied, particularly in a statistically consistent manner. Here, we experimentally measure light transport across two-dimensional open mesoscopic structures, wherein the disorder systematically ranges from nearly-periodic to amorphous. We measure the generalized conductance, which quantifies the transport probability in the sample. Although localization was identified in both the limits, statistical measurements revealed a discrepant behavior in the generalized conductance fluctuations in the two disorder regimes. Under amorphous disorder, the generalized conductance remains below unity for any configuration of the disorder, attesting to the arrested nature of transport. Contrarily, at near-periodic disorder, the distribution of generalized conductance is heavy-tailed towards large conductance values, indicating that the overall transport is delocalized. Theoretical results from a model based on the tight-binding approximation, augmented to include open boundaries, are in excellent agreement with experiments, and also endorse the results over much larger ensembles. These results quantify the differences in the two disorder regimes, and advance the studies of disordered systems into actual consequences of Anderson localization in light transport., Comment: 27 pages, 15 figures, including Supplementary Information

Intrinsic charge trap capacitive non-volatile flash memories take a significant share of the semiconductor electronics market today. It is a challenge to create intrinsic traps in the dielectric layer without high temperature processing steps. While low temperature processed memory devices fabricated from polymers have been demonstrated as an alternative, their performance degrade rapidly after a few cycles of operation. Moreover conventional memory devices need the support of tunneling and blocking layers since the memory dielectric or polymer is incapable of preventing memory leakage. The main issue in designing a memory device is to optimize the leakage current and intrinsic trap density simultaneously. Here we report a tunable flash memory device without tunneling and blocking layer by combining the discovery of high intrinsic charge traps ($>$10$^{12}$ cm$^{-2}$) together with low leakage current($<$10$^{-7}$ A.cm$^{-2}$) in solution derived, inorganic, spin$-$coated dielectric films which were heated at 200$^\circ$C or below. In addition, the memory storage is tuned systematically upto 96% by controlling the trap density with increasing heating temperature.