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| 1 | Olfactory ensheathing cells genetically modified to secrete GDNF to promote spinal cord repair显示文摘Olfactory ensheathing cell (OEC) transplantation has emerged as a very promising therapy for spinal cord repair. In this study, we tested the ability of genetically modified OECs to secrete high levels of glial cell line-derived neu-rotrophic factor (GDNF) to promote spinal cord repair. The GDNF gene was transduced into OECs using | CAOLi LIULi CHENZhe-Yu WANGLi-Mei YEJun-Li QIUHai-Yan LUChang-Lin HECheng | 2004 | 第二军医大学学报2004，25，5： | 64 |
| 2 | Moments and Mean First—Passage Time of Parabolic—Bistable Potential System Driven by Colored Noise显示文摘A parabolic-bistable potential system driven by colored noise is studied. The exact analytical expressionsof the stationary probability distribution (SPD) and the moments of the system are derived. Furthermore, the meanfirst-passage time is calculated by the use of two approximate methods, respectively. It is found that (i) the double peaksof SPD are rubbed-down into a flat single peak with the increasing of noise intensity; (ii) a minimum occurs on the curve of the second-order moment of the system vs.noise intensity at the point DΓ=0.025;(iii)the results obtained by our approximate approach are in good agreement with the numerical calculations for either small or large correlation time Γ,while the conventional steepest descent apprximation leads to poor results. | LIANGGui-Yun CAOLi 等 | 2002 | Communications in Theoretical Physics2002，37，2： | 2 |
| 3 | Expression of PCNA and bcl-2 in basaloid squamous cell carcinoma of the larynx: a controlled study 显示文摘 | Deniz K Yuce I Caoli S | 2008 | Ear Nose Throat J2008，87，8： | 1 |
| 4 | 显示文摘 | 王艳(WangY) 黄剑锋(HuangJF) 曹丽云(CaoLY) 吴建鹏(WuJP) 贺海燕(HeHY) | 2010 | 陶瓷2010，19，： | 1 |
| 5 | InfluenceoftemGperatureonthemorphologyandphotocatalyticactivityofZnGa2O4crystallitespreparedbyhydrothermalmethod显示文摘 | LiuLL HuangJF CaoLY etal | 2013 | CeramicsInternational2013，39，3： | 1 |
| 6 | SynthesisofZnGGa2O4 octahedralcrystallite by hydrothermal methodwiththeaidofCTABanditsphotocatalyticactivity显示文摘 | LiuLL HuangJF CaoLY etal | 2013 | MaterialsLetters2013，95，： | 1 |
| 7 | Changes in Serum Interleukin-2,-6and-8 level Before and During Treatment with Risperidone and Haloperidol:Relationship to outcome in Schizophrenia显示文摘 | ZhangXY ZhouDF CaoLY | 2004 | J Clin Psychiatry2004，65，7： | 1 |
| 8 | Changesinseruminterleukin-2,-6,and-8levelsbeforeandduringtreatmentwithrisperi-doneandhaloperidol:relationshiptooutcomeinschizophrenia显示文摘 | ZhangXY ZhouDF CaoLY etal | 2004 | JClinPsychiatry2004，65，7： | 1 |
| 9 | The Research About Sustainable Development Based on Cultural Root: Take the Ecoal Yuan Conceptual Planning of Juewei Taiyuan as an Example显示文摘 | Weiwei Caoli | 2011 | Procedia Engineering2011，，： | 1 |
| 10 | Urinary tract abnormalities:initial experience with multi-detector row CT urography显示文摘 | Caoli E M Cohan R H Korobkin M | 2002 | Radiology2002，222，： | 1 |
| 11 | Analyses of Valid Range for the Linear Approximation in a Single-Mode Laser显示文摘Using the linear approximation method, we calculated the steady-state mean normalized intensity fluctu-ation for a loss-noise model of a single-mode laser driven by a pump noise and a quantum noise, whose real part andimaginary part are cross-correlated. We analyzed the valid range for thelinear approximation method by studying theinfluences on the steady-state mean normalized intensity fluctuation by the cross-correlation coefficient, the intensities ofthe quantum and pump noise, the net gain, and the amplitude and frequency of the input signal, and we found that thevalid range becomes wider when the cross-correlation between the real and imaginary part of quantum noise is weaker,the noise intensities of quantum and pump are weaker, the laser system is far from the threshold and the signal hassmaller amplitude and higher frequency. | CHENGQing-Hua CAOLi WANGJun WUDa-Jin | 2004 | Communications in Theoretical Physics2004，42，3X： | 1 |
| 12 | Intensity Correlation Function of a Single-Mode Laser Driven by Two Colored Noises with Colored Cross-Correlation显示文摘By using the linear approximation method, the intensity correlation function and the intensity correlation time are calculated in a gain-noise model of a single-mode laser driven by colored cross-correlated pump noise and quantum noise, each of which is colored. We detect that, when the cross-correlation between both noises is negative, the behavior of the intensity correlation function C(t) versus time t, in addition to decreasing monotonously, also exhibits several other cases, such as one maximum, one minimum, and two extrema (one maximum and one minimum), i.e., some parameters of the noises can greatly change the dependence of the intensity correlation function upon time. T3. | HANLi-Bo CAOLi WUDa-Jin WANGJun | 2004 | Communications in Theoretical Physics2004，42，1X： | 0 |
| 13 | Intensity Correlation Function of a Single-Mode Laser Driven by Colored Cross-Correlation Noises in Modulation of a Bias Signal显示文摘By using the linear approximation method, the intensity correlation function is calculated for a single-mode laser modulated by a bias signal and driven by colored pump and quantum noises with colored cross-correlation. We found that, when the correlation time between the two noises is very short, the behavior of the intensity correlation function versus the time, in addition to decreasing monotonously, also exhibits several cases, such as one maximum, one minimum, and two extrema. When the correlation time between the two noises is very long, the behavior of the intensity correlation function exhibits oscillation and the envelope is similar to the case of short cross-correlation time. | HANLi-Bo CAOLi YANGHong-Quan WUDa-Jin | 2005 | Communications in Theoretical Physics2005，43，4： | 0 |
| 14 | Stationary Intensity Distribution of Single-Mode Laser Driven by Additive and Multiplicative Colored Noises with Colored Cross-Correlation显示文摘Applying the approximate Fokker-Planck equation we derived, we obtain the analytic expression of the stationary laser intensity distribution Pst(l) by studying the single-mode laser cubic model subject to colored cross-correlation additive and multiplicative noise, each of which is colored. Based on it, we discuss the effects on the stationary laser intensity distribution Pot(I) by cross-correlation between noises and 'color' of noises (non-Markovian effect) when the laser system is above the threshold. In detail, we analyze two cases: One is that the three correlation-times (i.e.the self-correlation and cross-correlation times of the additive and multiplicative noise) are chosen to be the same value(Tl=T2=T3=T). For this case, the effect of noise cross-correlation is investigated emphatically, and we detect that only when λ≠ 0 can the noise-induced transition occur in the Pst (I) curve, and only when T≠ 0 and λ≠0, can the 'reentrant noise-induced transition' occur. The other case is that the three correlation times are not the same value,T1≠T2≠T3. For this case, we find that the noise-induced transition occurring in the Pst(I) curve is entirely different when the values of T1,T2, and T3 are changed respectively. In particular, when T2 (serf-correlation time of additive noise) is cha^g~g, the ratio of the two maximums of the Pst( I) curve R exhibits an interesting phenomenon,'reentrant noise-induced transition', which demonstrates the effect of noise 'color' (non-Markovian effect). | CAOLi WANGJun WuDa-Jin LIANGGui-Yun | 2003 | Communications in Theoretical Physics2003，40，1X： | 0 |
| 15 | Steady-State Analysis of a Single-Mode Laser Driven by Colored Pump Noise withCross-Correlation Between Real and Imaginary Parts of Quantum Noise显示文摘Applying the method of the unified colored noise approximation and phase lock, we study in this paper the stationary intensity distribution of the single-mode laser driven by colored pump noise with cross-correlation between the real and imaginary parts of the quantum noise. We present a thorough discussion of how the cross-correlation λq between the realand imaginary parts of the quantum noise and the self-correlation time τ of the pump noise determine the behaviors of the stationary distribution Qst(I), the mean (I), and the variance λ2(0) of the laser intensity. It is shown that cross-correlation intensity λq of the complex quantum noise can induce a first-order-like transition. When the pump noise is colored noise (τ≠ 0), improving the pump parameters monotonously will make the curves of Qst(I)exhibit reentrant phase transition. The fluctuations of laser intensity are strongly influenced by λq and τ when the laser is operated near or below threshold. Especially when τ≠ 0, the heights of the peaks of the curves of λ2(0)-a0 and λ3(0)-a0, (here a0 is the net gain coefficient) go up as λq increases. However the entire curves of λ2(0)-a0 and λ3(0)-a0are abruptly suppressed when λq = 1, in similarity to phase transition of stationary intensity distribution. | ZHANGLi CAOLi WUDa-Jin | 2003 | Communications in Theoretical Physics2003，40，6X： | 0 |
| 16 | Coherence Resonance in the System with Periodical Potential and Driven by Correlated Noises显示文摘We study the ratchet model with both thermal and potential fluctuations, discussing analytically the coherence resonance of the particle moving in such a potential field. It is found that the correlation between the thermal and potential fluctuations has significant effect on the coherence of the system, i.e. negative correlation enhances the coherence of the system greatly, and with positive correlation, there appears the phenomenon that the coherence suppression and enhancement occur alternatively as the additive noise becomes larger. | YANGMing LIXiang-Lian CAOLi WUDa-Jin | 2004 | Chinese Physics Letters2004，21，7： | 0 |
| 17 | Stochastic Resonance in a Single-Mode Laser Driven by Pump Noise and QuantumNoise with Cross-Correlated Real and Imaginary Parts显示文摘We present an analytic investigation of the signal-to-noise ratio (SNR) by studying a signal modulated model of a single-mode laser system driven by pump noise and quantum noise with correlated real and imaginary parts,and find there is a maximum in the curve of the dependence of SNR upon the cross-correlation coefficient λq between the real part and the imaginary part, i.e., stochastic resonance appears in the SNR vs. λq curve. Moreover, when the SNR is at the maximum, the cross-correlation coefficient λq = 0, which is coincidentally at the minimum of the mean normalized intensity fluctuation. The influences on stochastic resonance by the intensities of the pump and the quantum noise, the amplitude of the modulation signal, and the net gain of the laser are also studied. Furthermore, in order to ensure that the results obtained in this paper is reliable, the valid range for the linear approximation method is discussed. | CHENGQing-Hua CAOLi WANGJun WUDa-Jin | 2004 | Communications in Theoretical Physics2004，42，4X： | 0 |
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