9,027 research outputs found
A 0.8 V T Network-Based 2.6 GHz Downconverter RFIC
A 2.6 GHz downconverter RFIC is designed and implemented using a 0.18 μm CMOS standard process. An important goal of the design is to achieve the high linearity that is required in WiMAX systems with a low supply voltage. A passive T phase-shift network is used as an RF input stage in a Gilbert cell to reduce supply voltage. A single supply voltage of 0.8 V is used with a power consumption of 5.87 mW. The T network-based downconverter achieves a conversion gain (CG) of 5 dB, a single-sideband noise figure (NF) of 16.16 dB, an RF-to-IF isolation of greater than 20 dB, and an input-referred third-order intercept point (IIP3) of 1 dBm when the LO power of -13 dBm is applied
First passage times and asymmetry of DNA translocation
Motivated by experiments in which single-stranded DNA with a short hairpin
loop at one end undergoes unforced diffusion through a narrow pore, we study
the first passage times for a particle, executing one-dimensional brownian
motion in an asymmetric sawtooth potential, to exit one of the boundaries. We
consider the first passage times for the case of classical diffusion,
characterized by a mean-square displacement of the form , and for the case of anomalous diffusion or subdiffusion, characterized by a
mean-square displacement of the form with
. In the context of classical diffusion, we obtain an expression
for the mean first passage time and show that this quantity changes when the
direction of the sawtooth is reversed or, equivalently, when the reflecting and
absorbing boundaries are exchanged. We discuss at which numbers of `teeth'
(or number of DNA nucleotides) and at which heights of the sawtooth potential
this difference becomes significant. For large , it is well known that the
mean first passage time scales as . In the context of subdiffusion, the
mean first passage time does not exist. Therefore we obtain instead the
distribution of first passage times in the limit of long times. We show that
the prefactor in the power relation for this distribution is simply the
expression for the mean first passage time in classical diffusion. We also
describe a hypothetical experiment to calculate the average of the first
passage times for a fraction of passage events that each end within some time
. We show that this average first passage time scales as in
subdiffusion.Comment: 10 pages, 4 figures We incorporated reviewers' suggestions from
Physical Review E. We reformulated a few paragraphs in the introduction and
further clarified the issue of the (a)symmetry of passage times. In the
results section, we re-expressed the results in a form that manifest the
important features. We also added a few references concerning anomalous
diffusion. The look (but not the content) of figure 1 was also change
Recommended from our members
Polaronic effect in the x-ray absorption spectra of La1-x Ca x MnO3 manganites.
X-ray absorption spectroscopy (XAS) is performed to study changes in the electronic structures of colossal magnetoresistance (CMR) and charged ordered (CO) La1-x Ca x MnO3 manganites with respect to temperature. The pre-edge features in O and Mn K-edge XAS spectra, which are highly sensitive to the local distortion of MnO6 octahedral, exhibit contrasting temperature dependence between CMR and CO samples. The seemingly counter-intuitive XAS temperature dependence can be reconciled in the context of polarons. These results help identify the most relevant orbital states associated with polarons and highlight the crucial role played by polarons in understanding the electronic structures of manganites
Cryogenic-coolant He4-superconductor dynamic and static interactions
A composite superconducting material (NbTi-Cu) was evaluated with emphasis on post quench solid cooling interaction regimes. The quasi-steady runs confirm the existence of a thermodynamic limiting thickness for insulating coatings. Two distinctly different post quench regimes of coated composites are shown to relate to the limiting thickness. Only one regime,, from quench onset to the peak value, revealed favorable coolant states, in particular in He2. Transient recovery shows favorable recovery times from this post quench regime (not drastically different from bare conductors) for both single coated specimens and a coated conductor bundle
Quantum Bit Regeneration
Decoherence and loss will limit the practicality of quantum cryptography and
computing unless successful error correction techniques are developed. To this
end, we have discovered a new scheme for perfectly detecting and rejecting the
error caused by loss (amplitude damping to a reservoir at T=0), based on using
a dual-rail representation of a quantum bit. This is possible because (1)
balanced loss does not perform a ``which-path'' measurement in an
interferometer, and (2) balanced quantum nondemolition measurement of the
``total'' photon number can be used to detect loss-induced quantum jumps
without disturbing the quantum coherence essential to the quantum bit. Our
results are immediately applicable to optical quantum computers using single
photonics devices.Comment: 4 pages, postscript only, figures available at
http://feynman.stanford.edu/qcom
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