论文列表

发表论文：（总引用超过2600，H因子25）

独立参加工作后所发表的论文：

2013年

1.  
P. Tang, X. Zhang, C. Zhao, Y. Wang, H. Zhang, D. Shen, S. Wen, D. Tang and D. Fan, “Topological Insulator: Bi2Te3 Saturable Absorber for the Passive Q-Switching Operation of an in-Band Pumped 1645-nm Er: YAG Ceramic Laser, ” IEEE Photon. J. 5(2), 1500707 (2013).

2.  Zhiteng Wang,     Shou-En Zhu,     Yu Chen,     Man Wu,    Chujun Zhao,  Han Zhang* , G.C.A.M.Janssen,     Shuangchun Wen, “Multilayergraphene for Q-switched mode-locking operation in an erbium-doped fiber laser”,Optics Communications, 300, 17–21, 2013.

3.  Shunbin Lu, Chujun Zhao, Yanhong Zou, Shuqing Chen, Yu Chen, Ying Li,  Han Zhang* , Shuangchun Wen, and Dingyuan Tang, "Third order nonlinear optical property of Bi2Se3," Opt. Express 21, 2072-2082 (2013)

4.Yu Feng Song, Lei Li, Han Zhang, De Yuan Shen, Ding Yuan Tang, and Kian Ping Loh, "Vector multi-soliton operation and interaction in a graphene mode-locked fiber laser," Opt. Express  21, 10010-10018 (2013)

5.   Yu Chen, Chujun Zhao, Huihui Huang, Shuqing Chen, Pinghua Tang, Zhiteng Wang, Shunbin Lu,  Han Zhang* ,Shuangchun Wen, and Dingyuan Tang,"Self-Assembled Topological Insulator: Bi₂Se₃ Membrane as a Passive Q-Switcher in an
Erbium-Doped Fiber Laser" IEEE JOURNAL OFLIGHTWAVE TECHNOLOGY, 31, 17, 2013.

6.  D. Y. Tang, L. Li, Y. F.Song, L. M. Zhao, H. Zhang, and D. Y. Shen, “Evidence of dark solitons inall-normal-dispersion-fiber lasers”, Phys. Rev. A 88, 013849 (2013)

7.   Qi Feng ; Yu Chen ; Chujun Zhao ; Ying Li ; Jianguo Wen ; Han Zhang,"Experimental study on the multisoliton pattern formation in an erbium-doped fiber laser passively mode-locked by graphene saturable absorber",Opt. Eng. 52(4), 044201 (Apr 15, 2013)

2012年

1.        Zhiteng Wang, Yu Chen,Chujun Zhao, Han Zhang*, and Shuangchun Wen, “Switchable Dual-Wavelength SynchronouslyQ-Switched Erbium-Doped Fiber Laser Based on Graphene Saturable Absorber,”IEEE Photonics Journal, 4,869, 2012.

2.  Chujun Zhao, Yanhong Zou, Yu Chen, Zhiteng Wang, Shunbin Lu, Han Zhang, Shuangchun Wen, and Dingyuan Tang, "Wavelength-tunable picosecond soliton fiber laser with Topological Insulator: Bi₂Se₃ as a mode locker," Opt. Express  20, 27888-27895 (2012)

3. Zhiwei Zheng, Chujun Zhao, Shunbin Lu, Yu Chen, Ying Li, Han Zhang*, and Shuangchun Wen, "Microwave and optical saturable absorption in graphene," Opt. Express  20, 23201-23214 (2012)

4. C. J. Zhao, H. Zhang*, X. Qi, Y. Chen, Z. T. Wang, S. C. Wen, and D. Y. Tang, “Ultra-short pulse generation by a topological insulator based saturable absorber,” Appl. Phys. Lett.101(21), 211106 (2012).

 5. Yu Chen ; Chujun Zhao ; Zhiteng Wang ; Jingchao Song ;  Han Zhang* ; Shuangchun Wen,"Erbium-doped fiber laser passively mode-locked by a position-adjustable graphene saturable absorber" Opt. Eng. 51(8), 084203 (2012).

 6. Yu Feng Song, Han Zhang, Ding Yuan Tang, and De Yuan Shen, "Polarization rotation vector solitons in a graphene mode-locked fiber laser," Opt. Express  20, 27283-27289 (2012).

博士及博士后期间的论文：

1)         Han Zhang*, Stephane Virally,Qiaoliang Bao, Kian Ping Loh, Serge Massar, Nicolas Godbout and PascalKockaert, “Z-scan measurement of the nonlinear refractive index of graphene,”Optics Letters,37, 1856, (2012).

2)         Han Zhang, Dingyuan Tang*,Luming Zhao, and Xuan Wu, “Dual-wavelength domain wall solitons in a fiber ringlaser,” Optics Express 19, 3525-3530 (2011).

3)         Han Zhang, Dingyuan Tang*,Luming Zhao, and Randall Knize, “Vector dark domain wall solitons in a fiberring laser,” Optics Express, 18, 4428 (2010).

4)         Zhiwei Zheng, Chujun Zhao,Shunbin Lu, Yu Chen, Ying Li, HanZhang*, and Shuangchun Wen, “Microwave and opticalsaturable absorption in graphene, ”Optics Express. 20, 23201, 2012.

5)         Han Zhang,Dingyuan Tang*, Luming Zhao, Qiaoliang Bao, and KianPing Loh, “Graphene mode locked, wavelength-tunable, dissipative soliton fiberlaser,” Applied Physics Letters, 96, 111112 (2010).

6)         Han Zhang,Qiaoliang Bao, Dingyuan Tang*, Luming Zhao,and Kianping Loh, “Large energy soliton erbium-doped fiber laser with agraphene-polymer composite mode locker,” Applied Physics Letters, 95, 141103 (2009).  

7)         Han Zhang,Dingyuan Tang*, Luming Zhao and Wu Xuan, “Dark pulseemission of a fiber laser,’’ Physical Review A, 80, 045803 (2009).

8)         Han Zhang,  Dingyuan Tang*, Luming Zhao, Qiaoliang Bao,and Kianping Loh,“Largeenergy mode locking of an erbium-doped fiber laser with atomic layer graphene, ” Optics Express,17,17630-17635 (2009). 

9)         Han Zhang, Ding Yuan Tang, Luming Zhao andXuan Wu, “Observation of polarization domain wall solitons in weaklybirefringent cavity fiber lasers,” Physical Review B 80, 052302(2009).

10)     H. Zhang, D. Y. Tang, L. M. Zhao,X. Wu, “Multi-wavelength dissipative soliton operation of an erbium-doped fiberlaser,” Optics Express 17, 12692-12697 (2009).

11)     H. Zhang, D. Y. Tang, L. M. Zhaoand N. Xiang, “Coherentenergy exchange between components of a vector soliton in fiber lasers,”Optics Express,16, 12618-12623 (2008).

12)      H. Zhang,D. Y. Tang, L. M. Zhao and H. Y. Tam, “Induced solitons formed by cross polarization coupling in a birefringent cavity fiberlaser,” Optics Letters, 33, 2317-2319 (2008).

13)     H. Zhang, D. Y. Tang, L. M. Zhao,X. Wu and H. Y. Tam, “Dissipative vector solitons in a dispersion-managedcavity fiber laser with net positive cavity dispersion,” Optics Express, 17, 455-460 (2009).

14)     Han Zhang, Dingyuan Tang, LumingZhao, Qiaoliang Bao, Kian Ping Loh, “Vector Dissipative Solitons in GrapheneMode Locked Fiber Lasers,” Optics Communications, 283,3334-3338 (2010).

15)     Dingyuan Tang, Han Zhang, LumingZhao and Xuan Wu, “Observationof high-order polarization-locked vector solitons in a fiber laser,”Physical ReviewLetters, 101, 153904 (2008).

16)     Qiaoliang Bao, HanZhang, Bing Wang, Zhenhua Ni, Candy Haley Yi Xuan Lim, Ding Yuan Tang,Kian Ping Loh*, “Broadband Graphene Polarizer,” Nature Photonics,    411–415   (2011).

17)     H. Zhang, D. Y. Tang, L. M. Zhao,Q. L. Bao, K. P. Loh, B. Lin, and S. C. Tjin, “Compact graphene mode-lockedwavelength-tunable erbium-doped fiber lasers: from all anomalous dispersion toall normal dispersion,” Laser Physics Letters,DOI 10.1002/lapl.201010025 (2010).

18)      Qiaoliang Bao, Han Zhang, Jia-xiang Yang, ShuaiWang, Ding Yuan Tang, Rajan Jose, Seeram Ramakrishna, Chwee Teck Lim, and KianPing Loh*, “Graphene-Polymer Nanofiber Membrane for UltrafastPhotonics,” AdvancedFunctional Materials, 20, 782-791(2010).

19)     Qiaoliang Bao, Han Zhang, Yu Wang, Zhenhua Ni,Yongli Yan, Ze Xiang Shen, Kian Ping Loh* ,and Ding Yuan Tang*,“Atomic layer graphene as saturable absorber for ultrafast pulsedlasers, ” AdvancedFunctional materials, 19, 3077–3083(2009).

20)     Qiaoliang Bao*, Han Zhang*, Yu Wang, LakshminarayanaPolavarapu, Ding Yuan Tang, Qing-Hua Xu, and Kian Ping Loh, “SaturableAbsorption of Monolayer Graphene and Its Mode-locked Laser,” Nano Research, DOI: 10.1007/s12274-010-0082-9, 2010.  

21)     Bo Lin, Han Zhang,et al., “Inverse-Gaussian-Apodized Fiber Bragg Grating for Dual WavelengthLasing,”AppliedOptics, 49, 1373 (2010).

22)     Bo Lin, Swee Chuan Tjin, HanZhang, et al., “Dual-Wavelength Single-Longitudinal-Mode Erbium-DopedFiber Laser Based on Inverse-Gaussian Apodized Fiber Bragg Grating and ItsApplication in Microwave Generation,” Optical Fiber Technology,accepted, (2011).

23)     Yu Zhang, Bo Lin, Swee Chuan Tjin, Han Zhang, Guanghui Wang, Ping Shum,and Xinliang Zhang,“Refractive index sensing based on higher-order mode reflection of a microfiberBragg grating,” OpticsExpress, 18, 26345 (2010).

24)     Bo Lin, Swee ChuanTjin, Han Zhang, DingyuanTang, Jianzhong Hao, Bo Dong, and Sheng Liang, “Switchable dual-wavelengthsingle-longitudinal-mode erbium-doped fiber laser using an inverse-Gaussianapodized fiber Bragg grating filter and a low-gain semiconductor opticalamplifier,” AppliedOptics, 49, 6855-6860 (2010).

25)     X. Wu, D. Y. Tang, L. M. Zhao and H. Zhang, “Mode-locking of fiber lasers induced by residualpolarization dependent loss of cavity components,” Laser Physics, 20, 1913-1917, (2010).

26)     L. M. Zhao, D. Y. Tang, H.Zhang, X. Wu, Qiaoliang Bao, and Kian Ping Loh, “Dissipative soliton operationof an ytterbium-doped fiber laser mode locked with atomic multilayer graphene,”Optics Letters, 35, 3622-3624 (2010).

27)     Luming Zhao, Dingyuan Tang, Xuan Wu, and Han Zhang, "Dissipative soliton generation in Yb-fiberlaser with an invisible intracavity bandpass filter," Optics Letters, 35, 2756-2758 (2010).        

28)     Qiaoliang Bao, HanZhang, Chunxu Pan. “Simulationfor growth of multi-walled carbon nanotubes in electric field,” ComputationalMaterials Science, 39 616-626 (2007).

29)     Qiaoliang Bao, HanZhang, Chunxu Pan. “Electric-field-inducedmicrostructural transformation of carbon nanotubes”, Applied PhysicsLetters,89 063124 (2006).

30)     D. Y. Tang, L. M. Zhao, X. Wu, and H. Zhang, “Soliton modulation instability in fiber lasers,” Physical Review A, 80,013804 (2009).

31)     X. Wu, D. Y. Tang, L. M. Zhao, and H. Zhang, “Effective cavity dispersion shiftinduced by nonlinearity in a fiber laser,” Physical Review A,80, 013804 (2009).

32)     L. M. Zhao, D. Y. Tang, H.Zhang, X. Wu, “Bunch ofrestless vector solitons in a fiber laser with SESAM,” Optics Express, 17, 8103-8108 (2009)

33)     X. Wu, D. Y. Tang, H.Zhang, and L. M. Zhao, “Dissipativesoliton resonance in an all-normal-dispersion erbium-doped fiber laser,”Optics Express,17, 5580-5584 (2009).

34)     L. M. Zhao, D. Y. Tang, H.Zhang, X. Wu, and N. Xiang, “Soliton trapping in fiber lasers,” Optics Express, 16, 9528-9533.(2008).

35)     L. M. Zhao, D. Y. Tang, H. Zhang, X. Wu, “Polarizationrotation locking of vector solitons in a fiber ring laser,” Optics Express, 16, 10053-10058 (2008).

36)     L. M. Zhao, D. Y. Tang, H. Zhang, T. H. Cheng, H. Y. Tam, and C. Lu, “Dynamics of gain-guided solitons inan all-normal-dispersion fiber laser,” Optics Letter, 32, 1806-1808 (2007).

37)     L. M. Zhao, D. Y. Tang, X. Wu, H. Zhang, H. Y. Tam, “Coexistence of polarization-locked andpolarization-rotating vector solitons in a fiber laser with SESAM,” Optics Letters,34, 3059-3061 (2009).

38)     L. M. Zhao, D. Y. Tang, X. Wu, H. Zhang, C. Lu, and H. Y. Tam, “Observation of dip-typesidebands in a soliton fiber laser,” Optics Communications, 283, 340-343 (2010).

39)     L. M. Zhao, D. Y. Tang, H. Zhang, X. Wu, C. Lu and H. Y. Tam, “Period-doublingof vector solitons in a ring fiber laser,” Optics Communications, 281,5614-5617 (2008).

40)     L. M. Zhao, D. Y. Tang, X. Wu, H. Zhang, “Period-doubling of gain-guidedsolitons in fiber lasers of large net normal dispersion,” Optics Communications, 281, 3557-3560 (2008).

41)     L. M. Zhao, D. Y. Tang, X. Wu, H. Zhang, C. Lu and H. Y. Tam, “Dynamics of gain-guided solitons in adispersion-managed fiber laser with large normal cavity dispersion,”Optics Communications,281, 3324-3326 (2008).