• Chinese Optics Letters
  • Vol. 13, Issue 5, 052101 (2015)
Wangzi Ma1, Dawei Zhang2, Linwei Zhu1, and Jiannong Chen1、*
Author Affiliations
  • 1School of Physics and Optoelectronic Engineering, Ludong University, Yantai 264025, China
  • 2Engineering Research Center of Optical Instruments and Systems, Ministry of Education, Shanghai Key Lab of Modern Optical Systems, School of Optical-Electrical and Computer Engineering, University of Shanghai for Science and Technology, Shanghai 200093, China
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    DOI: 10.3788/COL201513.052101 Cite this Article Set citation alerts
    Wangzi Ma, Dawei Zhang, Linwei Zhu, Jiannong Chen. Super-long longitudinal magnetization needle generated by focusing an azimuthally polarized and phase-modulated beam[J]. Chinese Optics Letters, 2015, 13(5): 052101 Copy Citation Text show less
    (a) Annular vortex filter composed of two annular belts with π shift radially between adjacent belts; (b) an azimuthally divided annular vortex filter with additional phase for moving the magnetization needle along the positive and negative direction of the z axis.
    Fig. 1. (a) Annular vortex filter composed of two annular belts with π shift radially between adjacent belts; (b) an azimuthally divided annular vortex filter with additional phase for moving the magnetization needle along the positive and negative direction of the z axis.
    Longitudinal magnetization distribution along the z axis at different θ1, θ2, and Δz. The green line is obtained when θ1=1.19, θ2=1.21; blue line is obtained when θ1=1.19, θ2=1.23; red line is obtained when θ1=1.17, θ2=1.21; and yellow line is obtained when θ1=1.17, θ2=1.19. (a) Δz=1.90λ; (b) Δz=1.95λ; (c) Δz=2.00λ; (d) Δz=2.05λ.
    Fig. 2. Longitudinal magnetization distribution along the z axis at different θ1, θ2, and Δz. The green line is obtained when θ1=1.19, θ2=1.21; blue line is obtained when θ1=1.19, θ2=1.23; red line is obtained when θ1=1.17, θ2=1.21; and yellow line is obtained when θ1=1.17, θ2=1.19. (a) Δz=1.90λ; (b) Δz=1.95λ; (c) Δz=2.00λ; (d) Δz=2.05λ.
    Normalized longitudinal magnetization distribution along the radial direction at z=0 and z=9λ. The red line is obtained when θ1=1.17, θ2=1.21 and. The green line is obtained when θ1=1.19, θ2=1.21 and Δz=2.00λ. The FWHM in all cases are 0.27λ.
    Fig. 3. Normalized longitudinal magnetization distribution along the radial direction at z=0 and z=9λ. The red line is obtained when θ1=1.17, θ2=1.21 and. The green line is obtained when θ1=1.19, θ2=1.21 and Δz=2.00λ. The FWHM in all cases are 0.27λ.
    Two-dimensional intensity distribution of (a) the electric field and (b) longitudinal magnetization in the longitudinal plane of the focal volume. The parameters are θ1=1.17, θ2=1.21, and Δz=1.95λ.
    Fig. 4. Two-dimensional intensity distribution of (a) the electric field and (b) longitudinal magnetization in the longitudinal plane of the focal volume. The parameters are θ1=1.17, θ2=1.21, and Δz=1.95λ.
    Three-dimensional half-maximum surface of the electric field (left panel) and longitudinal magnetization needle (right panel) in the focal volume.
    Fig. 5. Three-dimensional half-maximum surface of the electric field (left panel) and longitudinal magnetization needle (right panel) in the focal volume.
    Wangzi Ma, Dawei Zhang, Linwei Zhu, Jiannong Chen. Super-long longitudinal magnetization needle generated by focusing an azimuthally polarized and phase-modulated beam[J]. Chinese Optics Letters, 2015, 13(5): 052101
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