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A connection-level call admission control using genetic algorithm for MultiClass multimedia services in wireless networks
Call admission control in a wireless cell in a personal communication system (PCS) can be modeled as an M/M/C/C queuing system with m classes of users. Semi-Markov Decision Process (SMDP) can be used to optimize channel utilization with upper bounds on handoff blocking probabilities as Quality of Service constraints. However, this method is too time-consuming and therefore it fails when state space and action space are large. In this paper, we apply a genetic algorithm approach to address the situation when the SMDP approach fails. We code call admission control decisions as binary strings, where a value of “1” in the position i (i=1,…m) of a decision string stands for the decision of accepting a call in class-i; a value of “0” in the position i of the decision string stands for the decision of rejecting a call in class-i. The coded binary strings are feed into the genetic algorithm, and the resulting binary strings are founded to be near optimal call admission control decisions. Simulation results from the genetic algorithm are compared with the optimal solutions obtained from linear programming for the SMDP approach. The results reveal that the genetic algorithm approximates the optimal approach very well with less complexity
Illumination and annealing characteristics of two-dimensional electron gas systems in metal-organic vapor-phase epitaxy grown AlGaN/AlN/GaN heterostructures
We studied the persistent photoconductivity (PPC) effect in AlGaN/AlN/GaN
heterostructures with two different Al-compositions (x=0.15 and x=0.25). The
two-dimensional electron gas formed at the AlN/GaN heterointerface was
characterized by Shubnikov-de Haas and Hall measurements. Using optical
illumination, we were able to increase the carrier density of the
Al0.15Ga0.85N/AlN/GaN sample from 1.6x10^{12} cm^{-2} to 5.9x1012 cm^{-2},
while the electron mobility was enhanced from 9540 cm2/Vs to 21400 cm2/Vs at T
= 1.6 K. The persistent photocurrent in both samples exhibited a strong
dependence on illumination wavelength, being highest close to the bandgap and
decreasing at longer wavelengths. The PPC effect became fairly weak for
illumination wavelengths longer than 530 nm and showed a more complex response
with an initial negative photoconductivity in the infrared region of the
spectrum (>700 nm). The maximum PPC-efficiency for 390 nm illumination was
0.011% and 0.005% for Al0.25Ga0.75N/AlN/GaN and Al0.15Ga0.85N/AlN/GaN samples,
respectively. After illumination, the carrier density could be reduced by
annealing the sample. Annealing characteristics of the PPC effect were studied
in the 20-280 K temperature range. We found that annealing at 280 K was not
sufficient for full recovery of the carrier density. In fact, the PPC effect
occurs in these samples even at room temperature. Comparing the measurement
results of two samples, the Al0.25Ga0.75N/AlN/GaN sample had a larger response
to illumination and displayed a smaller recovery with thermal annealing. This
result suggests that the energy scales of the defect configuration-coordinate
diagrams for these samples are different, depending on their Al-composition.Comment: 27 pages, 8 figure
Performance of Photosensors in the PandaX-I Experiment
We report the long term performance of the photosensors, 143 one-inch
R8520-406 and 37 three-inch R11410-MOD photomultipliers from Hamamatsu, in the
first phase of the PandaX dual-phase xenon dark matter experiment. This is the
first time that a significant number of R11410 photomultiplier tubes were
operated in liquid xenon for an extended period, providing important guidance
to the future large xenon-based dark matter experiments.Comment: v3 as accepted by JINST with modifications based on reviewers'
comment
Design and experimentation of sensitive element of piezoelectric crystal sensor array for grain cleaning loss
This study described the optimal design for the sensitive element of the piezoelectric crystal sensor array for grain cleaning loss. To improve the signal-to-noise and resolution of grain cleaning loss, the dynamic model for grain collision sensor array was established by using elastic thin plate theory and also the best structural parameters of sensitive element were determined to make out the grain and the stems momentum. The structural parameters of the thin plate were length of 300 mm, width of 200 mm, thickness of 1.5 mm, plate structural style and four corners fixed. Then, the experiment that grain impacted the sensitive elements with the thickness of 0.5, 1.5 and 2.5 mm was established on the test bench to verify the overall performance of the sensitive element. The results showed that the stiffness of the sensitive element designed was moderate, grain collision signal amplitude was about 1.2 V and decay time was within 1s, which was easily separated from other signals generated from the glumes and the straws. The sensitive element not only had high resolution between grain and stems, but also measured the highest frequency of grain impact, which significantly improved the overall performance of grain cleaning loss sensor.Key words: Grain cleaning loss, sensor array, sensitive element, elastic thin plate theory, structural parameters
Commuting Quantum Circuits with Few Outputs are Unlikely to be Classically Simulatable
We study the classical simulatability of commuting quantum circuits with n
input qubits and O(log n) output qubits, where a quantum circuit is classically
simulatable if its output probability distribution can be sampled up to an
exponentially small additive error in classical polynomial time. First, we show
that there exists a commuting quantum circuit that is not classically
simulatable unless the polynomial hierarchy collapses to the third level. This
is the first formal evidence that a commuting quantum circuit is not
classically simulatable even when the number of output qubits is exponentially
small. Then, we consider a generalized version of the circuit and clarify the
condition under which it is classically simulatable. Lastly, we apply the
argument for the above evidence to Clifford circuits in a similar setting and
provide evidence that such a circuit augmented by a depth-1 non-Clifford layer
is not classically simulatable. These results reveal subtle differences between
quantum and classical computation.Comment: 19 pages, 6 figures; v2: Theorems 1 and 3 improved, proofs modifie
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