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Optoelectronics Letters
Contents
2015
Volume: 11 Issue 5
18 Article(s)
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Research Article
Stable single-photon detection based on Si-avalanche photodiode in a large temperature variation range
Pei-qin YAN, Zhao-hui LI, Ya-fan SHI, Bai-cheng FENG, Bing-cheng DU, Yan-wei DU, Tian-le TAN, and Guang WU
In this paper, we present a stable single-photon detection method based on Si-avalanche photodiode (Si-APD) operating in Geiger mode with a large temperature variation range. By accurate temperature sensing and direct current (DC) bias voltage compensation, the single-photon detector can work stably in Geiger mode from
In this paper, we present a stable single-photon detection method based on Si-avalanche photodiode (Si-APD) operating in Geiger mode with a large temperature variation range. By accurate temperature sensing and direct current (DC) bias voltage compensation, the single-photon detector can work stably in Geiger mode from ?40 °C to 35 °C with an almost constant avalanche gain. It provides a solution for single-photon detection at outdoor operation in all-weather conditions..
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Optoelectronics Letters
Publication Date: Jan. 01, 1900
Vol. 11, Issue 5, 321 (2015)
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Switchable dual-wavelength erbium-doped fiber laser with tunable wavelength
Zheng-rong TONG, Meng-ying LIU, Ye CAO, Wei-hua ZHANG, and Xia HAO
A switchable dual-wavelength erbium-doped fiber laser (EDFL) with tunable wavelength is demonstrated. The ring cavity consists of two branches with a fiber Bragg grating (FBG) and a spherical-shape structure as fiber filters, respectively. By adjusting the variable optical attenuator (VOA), the laser can be switched be
A switchable dual-wavelength erbium-doped fiber laser (EDFL) with tunable wavelength is demonstrated. The ring cavity consists of two branches with a fiber Bragg grating (FBG) and a spherical-shape structure as fiber filters, respectively. By adjusting the variable optical attenuator (VOA), the laser can be switched between the single- wavelength mode and the dual-wavelength mode. The spherical-shape structure has good sensitivity to the temperature. When the temperature changes from 30 °C to 190 °C, the central wavelength of the EDFL generated by the branch of spherical-shape structure varies from 1 551.6 nm to 1 561.8 nm, which means that the wavelength interval is tunable..
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Optoelectronics Letters
Publication Date: Jan. 01, 1900
Vol. 11, Issue 5, 325 (2015)
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Improving the performance of inverted organic solar cells by adjusting the concentration of precursor solution of Al-doped ZnO
Xuan YU, Xiao-ming YU, Jian-jun ZHANG, and Hong-jun PAN
Al-doped ZnO (AZO) has been used as an electron transport and hole blocking buffer layer in inverted organic solar cells (IOSCs). In this paper, the AZO morphology, optical and structural properties and IOSCs performance are investigated as a function of precursor solution concentration from 0.1 mol/L to 1.0 mol/L. We
Al-doped ZnO (AZO) has been used as an electron transport and hole blocking buffer layer in inverted organic solar cells (IOSCs). In this paper, the AZO morphology, optical and structural properties and IOSCs performance are investigated as a function of precursor solution concentration from 0.1 mol/L to 1.0 mol/L. We demonstrate that the device with 0.1 mol/L precursor concentration of AZO buffer layers enhances the short-circuit current and the fill factor of IOSCs simultaneously. The resulting device shows that the power conversion efficiency is improved by 35.6% relative to that of the 1.0 mol/L device, due to the improved surface morphology and transmittance (300–400 nm) of AZO buffer layer..
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Optoelectronics Letters
Publication Date: Jan. 01, 1900
Vol. 11, Issue 5, 329 (2015)
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Effects of transparent MPTMS/Ag/MoO
3
structure as anode on the performance of green organic light-emitting diodes
Jun-tao HU, Ya-fei DENG, Wen-juan MEI, and Jing-song YANG
A transparent 3-mercaptopropyl trimethoxysilane (MPTMS)/Ag/MoO3composite anode is introduced to fabricate green organic light-emitting diodes (OLEDs). Effects of the composite anode on brightness and operating voltage of OLEDs are researched. By optimizing the thickness of each layer of the MPTMS/Ag/MoO3structure, the
A transparent 3-mercaptopropyl trimethoxysilane (MPTMS)/Ag/MoO
3
composite anode is introduced to fabricate green organic light-emitting diodes (OLEDs). Effects of the composite anode on brightness and operating voltage of OLEDs are researched. By optimizing the thickness of each layer of the MPTMS/Ag/MoO
3
structure, the transmittance of MPTMS/Ag (8 nm)/MoO
3
(30 nm) reaches over 75% at about 520 nm. The sheet resistance is 3.78 Ω/□, corresponding to this MPTMS/Ag (8 nm)/MoO
3
(30 nm) structure. For the OLEDs with the optimized anode, the maximum electroluminescence (EL) current efficiency reaches 4.5 cd/A, and the maximum brightness is 37 036 cd/m
2
. Moreover, the OLEDs with the optimized anode exhibit a very low operating voltage (2.6 V) for obtaining brightness of 100 cd/m
2
. We consider that the improved device performance is mainly attributed to the enhanced hole injection resulting from the reduced hole injection barrier height. Our results indicate that employing the MPTMS/Ag/MoO
3
as a composite anode can be a simple and promising technique in the fabrication of low-operating voltage and high-brightness OLEDs..
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Optoelectronics Letters
Publication Date: Jan. 01, 1900
Vol. 11, Issue 5, 333 (2015)
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Tunable thin-film filter with low angle sensitivity
Kan YU, Jia-qi BAO, and Juan-juan YIN
Conventional angle-tuned thin-film filters have serious angle sensitivity for their low spacer effective refractive index, and it is difficult to fabricate their angle control system. In this paper, we propose and fabricate a novel 100 GHz angletuned thin-film filter stack with low angle sensitivity, which uses the hig
Conventional angle-tuned thin-film filters have serious angle sensitivity for their low spacer effective refractive index, and it is difficult to fabricate their angle control system. In this paper, we propose and fabricate a novel 100 GHz angletuned thin-film filter stack with low angle sensitivity, which uses the high refractive index material TiO2
2
as the spacer, and its incident angle can be expanded to 25°. Compared with the traditional Ta
2
O
5
-SiO
2
thin-film filter stack, the novel stack has fewer layers. Using the polarization beam splitters and the half wave plates, the polarization sensitivity of the angle-tuned filter can also be suppressed. Simulation results and the experiments show that the thin-film filter with low angle sensitivity has an effective tuning range of 33 nm, which can cover the whole C-band, and its angle control system is easy to be fabricated..
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Optoelectronics Letters
Publication Date: Jan. 01, 1900
Vol. 11, Issue 5, 338 (2015)
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Rabi oscillation generation in the microring resonator system with double-series ring resonators
Ahmad Noorden Ahmad Fakhrurrazi, Chaudhary Kashif, Bahadoran Mahdi, Aziz Muhammad Safwan, Jalil Muhammad Arif, Tiong Ong Chee, Ali Jalil, and Yupapin Preecha
In this paper, a microring resonator (MRR) system using double-series ring resonators is proposed to generate and investigate the Rabi oscillations. The system is made up of silicon-on-insulator and attached to bus waveguide which is used as propagation and oscillation medium. The scattering matrix method is employed t
In this paper, a microring resonator (MRR) system using double-series ring resonators is proposed to generate and investigate the Rabi oscillations. The system is made up of silicon-on-insulator and attached to bus waveguide which is used as propagation and oscillation medium. The scattering matrix method is employed to determine the output signal intensity which acts as the input source between two-level Rabi oscillation states, where the increase of Rabi oscillation frequency with time is obtained at the resonant state. The population probability of the excited state is higher and unstable at the optical resonant state due to the nonlinear spontaneous emission process. The enhanced spontaneous emission can be managed by the atom (photon) excitation, which can be useful for atomic related sensors and single-photon source applications..
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Optoelectronics Letters
Publication Date: Jan. 01, 1900
Vol. 11, Issue 5, 342 (2015)
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Effects of Mg-doping concentration on the characteristics of InGaN based solar cells
Gang LU, Bo WANG, and Yun-wang GE
A major challenge in GaN based solar cell design is the lack of holes compared with electrons in the multiple quantum wells (MQWs). We find that GaN based MQW photovoltaic devices with five different Mg-doping concentrations of 0 cm-3, 5×1017 cm-3, 2×1018 cm-3, 4×1018 cm-3and 7×1018 cm-3in GaN barri
A major challenge in GaN based solar cell design is the lack of holes compared with electrons in the multiple quantum wells (MQWs). We find that GaN based MQW photovoltaic devices with five different Mg-doping concentrations of 0 cm
-3
, 5×10
17
cm
-3
, 2×10
18
cm
-3
, 4×10
18
cm
-3
and 7×10
18
cm
-3
in GaN barriers can lead to different hole concentrations in quantum wells (QWs). However, when the Mg-doping concentration is over 1×10
18
cm
-3
, the crystal quality degrades, which results in the reduction of the external quantum efficiency (EQE), short circuit current density and open circuit voltage. As a result, the sample with a slight Mg-doping concentration of 5×10
17
cm
-3
exhibits the highest conversion efficiency..
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Optoelectronics Letters
Publication Date: Jan. 01, 1900
Vol. 11, Issue 5, 348 (2015)
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Uncooled InAs
0.09
Sb
0.91
photoconductors with cutoff wavelength extended to 11.5 μm
Yu-zhu GAO, Xiu-ying GONG, Ran ZHOU, Ji-jun LI, Yan-bin FENG, Makino Takamitsu, and Kan Hirofumi
Uncooled InAsSb photoconductors were fabricated. The photoconductors were based on InAs0.09Sb0.91and InAs0.09Sb0.91thick epilayers grown on InAs substrates by melt epitaxy (ME). Ge immersion lenses were set on the photoconductors. The cutoff wavelength of InAs0.09Sb0.91detectors is obviously extended to 11.5 μm, and th
Uncooled InAsSb photoconductors were fabricated. The photoconductors were based on InAs
0.09
Sb
0.91
and InAs
0.09
Sb
0.91
thick epilayers grown on InAs substrates by melt epitaxy (ME). Ge immersion lenses were set on the photoconductors. The cutoff wavelength of InAs
0.09
Sb
0.91
detectors is obviously extended to 11.5 μm, and that of InAs
0.09
Sb
0.95
detectors is 8.3 μm. At room temperature, the peak detectivity of D
λp
*
at wavelength of 6.8 μm and modulation frequency of 1 200 Hz is 1.08×10
9
cm·Hz
1/2
·W
-1
for InAs
0.09
Sb
0.91
photoconductors, the detectivity D
*
at wavelength of 9 μm is 7.56×10
8
cm·Hz
1/2
·W
-1
, and that at 11 μm is 3.92×10
8
cm·Hz
1/2
·W
-1
. The detectivity of InAs
0.09
Sb
0.91
detectors at the wavelengths longer than 9 μm is about one order of magnitude higher than that of InAs
0.09
Sb
0.95
detectors, which rises from the increase of arsenic (As) composition in InAs
0.09
Sb
0.91
materials..
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Optoelectronics Letters
Publication Date: Jan. 01, 1900
Vol. 11, Issue 5, 352 (2015)
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Growth and optical properties of Dy
3+
/Eu
3+
co-doped NaYF
4
single crystals with cubic lattice for white LED application
Dong-sheng JIANG, Yong-zhang JIANG, Hai-ping XIA, Jia-zhong ZHANG, Shuo YANG, Xue-mei GU, Hao-chuan JIANG, and Bao-jiu CHEN
Dy3+/Eu3+co-doped cubic lattice NaYF4single crystal with high quality in the size of ~Φ1.0 cm×10.0 cm was grown by an improved Bridgman method using potassium fluoride (KF) as assistant flux. X-ray diffraction (XRD), absorption spectra, excitation spectra and emission spectra are measured to investigate the phase
Dy
3+
/Eu
3+
co-doped cubic lattice NaYF
4
single crystal with high quality in the size of ~Φ1.0 cm×10.0 cm was grown by an improved Bridgman method using potassium fluoride (KF) as assistant flux. X-ray diffraction (XRD), absorption spectra, excitation spectra and emission spectra are measured to investigate the phase and luminescent properties of the crystal. The effects of excitation wavelength and concentrations of Dy
3+
and EuEu
3+
ions on the luminescent characteristics are analyzed. The NaYF
4
single crystal with the doping molar concentrations of 1.205% Dy
3+
and 0.366% Eu3+ exhibits an excellent white light emission with chromaticity coordinates of x=0.321, y=0.332. It indicates that the Dy
3+
/Eu
3+
co-doped cubic lattice NaYF
4
single crystal can be a potential luminescent material for the ultraviolet (UV) light excited white light emitting diode (w-LED)..
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Optoelectronics Letters
Publication Date: Jan. 01, 1900
Vol. 11, Issue 5, 356 (2015)
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Enhancement of fluorescence emission and signal gain at 1.53 μm in Er
3+
/Ce
3+
co-doped tellurite glass fiber
Feng-jing YANG, Bo HUANG, Li-bo WU, Ya-wei QI, Sheng-xi PENG, Jun LI, and Ya-xun ZHOU
Er3+/Ce3+co-doped tellurite glasses with composition of TeO2-GeO2-Li2O-Nb2O5were prepared using conventional melt-quenching technique for potential applications in Er3+-doped fiber amplifier (EDFA). The absorption spectra, up-conversion spectra and 1.53 μm band fluorescence spectra of glass samples were measured. It is
Er
3+
/Ce
3+
co-doped tellurite glasses with composition of TeO
2
-GeO
2
-Li
2
O-Nb
2
O
5
were prepared using conventional melt-quenching technique for potential applications in Er
3+
-doped fiber amplifier (EDFA). The absorption spectra, up-conversion spectra and 1.53 μm band fluorescence spectra of glass samples were measured. It is shown that the 1.53 μm band fluorescence emission intensity of Er
3+
-doped tellurite glass fiber is improved obviously with the introduction of an appropriate amount of Ce
3+
, which is attributed to the energy transfer (ET) from Er
3+
to Ce
3+
. Meanwhile, the 1.53 μm band optical signal amplification is simulated based on the rate and power propagation equations, and an increment in signal gain of about 2.4 dB at 1 532 nm in the Er
3+
/Ce
3+
co-doped tellurite glass fiber is found. The maximum signal gain reaches 29.3 dB on a 50 cm-long fiber pumped at 980 nm with power of 100 mW. The results indicate that the prepared Er
3+
/Ce
3+
co-doped tellurite glass is a good gain medium applied for 1.53 μm broadband and high-gain EDFA..
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Optoelectronics Letters
Publication Date: Jan. 01, 1900
Vol. 11, Issue 5, 361 (2015)
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Improved luminescent properties of SrZn
2
(PO
4
)
2
:Sm
3+
doped with Li
+
, Na
+
and K
+
ions
Wei LU, Yu-fei LIU, Ying WANG, Zhi-jun WANG, and Li-bin PANG
SrZn2(PO4)2:Sm3+phosphor was synthesized by a high temperature solid-state reaction in atmosphere. SrZn2(PO4)2:Sm3+phosphor is efficiently excited by ultraviolet (UV) and blue light, and the emission peaks are assigned to the transitions of 4G5/2-6H5/2(563 nm), 4G5/2-6H7/2(597 nm and 605 nm) and 4G5/2-6H9/2(644 nm and
SrZn
2
(PO
4
)
2
:Sm
3+
phosphor was synthesized by a high temperature solid-state reaction in atmosphere. SrZn
2
(PO
4
)
2
:Sm
3+
phosphor is efficiently excited by ultraviolet (UV) and blue light, and the emission peaks are assigned to the transitions of
4
G
5/2
-
6
H
5/2
(563 nm),
4
G
5/2
-
6
H
7/2
(597 nm and 605 nm) and
4
G
5/2
-
6>H
9/2
(644 nm and 653 nm). The emission intensities of SrZn
2
(PO
4
)
2
:Sm
3+
are influenced by Sm
3+
concentration, and the concentration quenching effect of SrZn
2
(PO
4
)
2
:Sm
3+
is also observed. When doping A
+
(A=Li, Na and K) ions, the emission intensity of SrZn
2
(PO
4
)
2
:Sm
3+
can be obviously enhanced. The Commission Internationale de l'Eclairage (CIE) color coordinates of SrZn
2
(PO
4
)
2
:Sm
3+
locate in the orange-red region. The results indicate that the phosphor has a potential application in white light emitting diodes (LEDs)..
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Optoelectronics Letters
Publication Date: Jan. 01, 1900
Vol. 11, Issue 5, 366 (2015)
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White light emission in Pr
3+
, Tb
3+
:CaYAlO
4
phosphor
Qiao-ling CHEN, and Shao-zhen Lü
In this work, the synthesis and photoluminescence characteristics of two new phosphors Pr3+: CaYAlO4(CYA) and Pr3+/Tb3+: CYA for light emitting diodes (LEDs) are investigated. 0.5% (atom percentage) Pr3+: CYA exhibits the largest bright yellow emission by varying the Pr3+concentration, owing to the cross-relaxation pro
In this work, the synthesis and photoluminescence characteristics of two new phosphors Pr
3+
: CaYAlO
4
(CYA) and Pr
3+
/Tb
3+
: CYA for light emitting diodes (LEDs) are investigated. 0.5% (atom percentage) Pr
3+
: CYA exhibits the largest bright yellow emission by varying the Pr
3+
concentration, owing to the cross-relaxation process of
3
P
0
+
3
H
4
→
1
G
4
+
1
G
4
. The energy level diagram in Pr
3+
: CYA, especially the positions of 4f5d level and 1S0 level, is discussed. By co-doping Tb
3+
ions, the color coordinates of Pr
3+
/Tb
3+
: CYA phosphor can be tuned from yellow to white region. Finally, the strongest luminescence emission with color coordinates of (0.339, 0.364) located in the white region can be obtained in 0.3%Tb
3+
/0.5%Pr
3+
: CYA phosphor..
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Optoelectronics Letters
Publication Date: Jan. 01, 1900
Vol. 11, Issue 5, 370 (2015)
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A novel TS-EIA-PTS PAPR reduction algorithm for optical OFDM systems
Jian-guo YUAN, Zhang-chao LI, Jun MA, Yong WANG, Jin-zhao LIN, and Yu PANG
Because the partial transmit sequence (PTS) peak-to-average power ratio (PAPR) reduction technology for optical orthogonal frequency division multiplexing (O-OFDM) systems has higher computational complexity, a novel two-stage enhanced-iterative-algorithm PTS (TS-EIA-PTS) PAPR reduction algorithm with lower computation
Because the partial transmit sequence (PTS) peak-to-average power ratio (PAPR) reduction technology for optical orthogonal frequency division multiplexing (O-OFDM) systems has higher computational complexity, a novel two-stage enhanced-iterative-algorithm PTS (TS-EIA-PTS) PAPR reduction algorithm with lower computational complexity is proposed in this paper. The simulation results show that the proposed TS-EIA-PTS PAPR reduction algorithm can reduce the computational complexity by 18.47% in the condition of the original signal sequence partitioned into 4 sub-blocks at the remaining stage of n-d=5. Furthermore, it has almost the same PAPR reduction performance and the same bit error rate (BER) performance as the EIA-PTS algorithm, and with the increase of the subcarrier number, the computational complexity can be further reduced. As a result, the proposed TS-EIA-PTS PAPR reduction algorithm is more suitable for the practical O-OFDM systems..
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Optoelectronics Letters
Publication Date: Jan. 01, 1900
Vol. 11, Issue 5, 375 (2015)
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An optical fiber magnetic field sensor based on fiber spherical structure interferometer coated by magnetic fluid
Feng-tian XU, Pan-pan LUAN, Ke-song JIA, and Ai-ling ZHANG
A novel magnetic field sensor based on optical fiber Mach-Zehnder interferometer (MZI) coated by magnetic fluid (MF) is proposed. The MZI consists of two spherical structures formed on standard single mode fiber (SMF). The interference wavelength and the power of the sensing structure are sensitive to the external refr
A novel magnetic field sensor based on optical fiber Mach-Zehnder interferometer (MZI) coated by magnetic fluid (MF) is proposed. The MZI consists of two spherical structures formed on standard single mode fiber (SMF). The interference wavelength and the power of the sensing structure are sensitive to the external refractive index (RI). Since RI of the MF is sensitive to the magnetic field, the magnetic field measurement can be realized by detecting the variation of the interference spectrum. Experimental results show that the wavelength and the power of interference dip both increase with the increase of magnetic field intensity..
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Optoelectronics Letters
Publication Date: Jan. 01, 1900
Vol. 11, Issue 5, 379 (2015)
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Miniature Fabry-Perot interferometric sensor for temperature measurement based on photonic crystal fiber
Xing-hu FU, Hai-yang XIE, Feng WANG, Peng JIANG, FUGuang-wei , and Wei-hong BI
A novel miniature Fabry-Perot interferometric (FPI) temperature sensor is proposed and demonstrated experimentally. The modal interferometer is fabricated by just splicing a section of photonic crystal fiber (PCF) with a single-mode fiber (SMF). The air holes of the PCF are fully collapsed by the discharge arc during t
A novel miniature Fabry-Perot interferometric (FPI) temperature sensor is proposed and demonstrated experimentally. The modal interferometer is fabricated by just splicing a section of photonic crystal fiber (PCF) with a single-mode fiber (SMF). The air holes of the PCF are fully collapsed by the discharge arc during the splicing procedure to enhance the reflection coefficient of the splicing point. The transmission spectra with different temperatures are measured, and the experimental results show that the linear response of 11.12 pm/°C in the range of 30–80 °C is obtained. This sensor has potential applications in temperature measurement field..
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Optoelectronics Letters
Publication Date: Jan. 01, 1900
Vol. 11, Issue 5, 382 (2015)
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Characteristics of strong-coupling bipolaron qubit in two-dimensional quantum dot in electric field
Ying ZHANG, Chao HAN, and Eerdunchaolu
Based on Lee-Low-Pines (LLP) unitary transformation, this article adopts the variational method of the Pekar type and gets the energy and wave functions of the ground state and the first excited state of strong-coupling bipolaron in two-dimensional quantum dot in electric field, thus constructs a bipolaron qubit. The n
Based on Lee-Low-Pines (LLP) unitary transformation, this article adopts the variational method of the Pekar type and gets the energy and wave functions of the ground state and the first excited state of strong-coupling bipolaron in two-dimensional quantum dot in electric field, thus constructs a bipolaron qubit. The numerical results represent that the time oscillation period T0 of probability density of the two electrons in qubit decreases with the increasing electric field intensity F and dielectric constant ratio of the medium η; the probability density Q of the two electrons in qubit oscillates periodically with the increasing time t; the probability of electron appearing near the center of the quantum dot is larger, while that appearing away from the center of the quantum dot is much smaller..
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Optoelectronics Letters
Publication Date: Jan. 01, 1900
Vol. 11, Issue 5, 386 (2015)
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A stereo matching algorithm based on SIFT feature and homography matrix
Zong-yan LI, Li-mei SONG, Jiang-tao XI, Qing-hua GUO, Xin-jun ZHU, and Ming-lei CHEN
Aiming at the low speed of traditional scale-invariant feature transform (SIFT) matching algorithm, an improved matching algorithm is proposed in this paper. Firstly, feature points are detected and the speed of feature points matching is improved by adding epipolar constraint; then according to the matching feature po
Aiming at the low speed of traditional scale-invariant feature transform (SIFT) matching algorithm, an improved matching algorithm is proposed in this paper. Firstly, feature points are detected and the speed of feature points matching is improved by adding epipolar constraint; then according to the matching feature points, the homography matrix is obtained by the least square method; finally, according to the homography matrix, the points in the left image can be mapped into the right image, and if the distance between the mapping point and the matching point in the right image is smaller than the threshold value, the pair of matching points is retained, otherwise discarded. Experimental results show that with the improved matching algorithm, the matching time is reduced by 73.3% and the matching points are entirely correct. In addition, the improved method is robust to rotation and translation..
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Optoelectronics Letters
Publication Date: Jan. 01, 1900
Vol. 11, Issue 5, 390 (2015)
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Tumor segmentation in lung CT images based on support vector machine and improved level set
Xiao-peng WANG, Wen ZHANG, and Ying CUI
In lung CT images, the edge of a tumor is frequently fuzzy because of the complex relationship between tumors and tissues, especially in cases that the tumor adheres to the chest and lung in the pathology area. This makes the tumor segmentation more difficult. In order to segment tumors in lung CT images accurately, a
In lung CT images, the edge of a tumor is frequently fuzzy because of the complex relationship between tumors and tissues, especially in cases that the tumor adheres to the chest and lung in the pathology area. This makes the tumor segmentation more difficult. In order to segment tumors in lung CT images accurately, a method based on support vector machine (SVM) and improved level set model is proposed. Firstly, the image is divided into several block units; then the texture, gray and shape features of each block are extracted to construct eigenvector and then the SVM classifier is trained to detect suspicious lung lesion areas; finally, the suspicious edge is extracted as the initial contour after optimizing lesion areas, and the complete tumor segmentation can be obtained by level set model modified with morphological gradient. Experimental results show that this method can efficiently and fast segment the tumors from complex lung CT images with higher accuracy..
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Optoelectronics Letters
Publication Date: Jan. 01, 1900
Vol. 11, Issue 5, 395 (2015)
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