• Chinese Optics Letters
  • Vol. 13, Issue 11, 112401 (2015)
Linguo Xie1, Xiaodong Qiu1, Jiangdong Qiu1, Zhiyou Zhang1、2、*, Jinglei Du1、2, and Fuhua Gao1、2
Author Affiliations
  • 1Key Laboratory of High Energy Density Physics and Technology of Ministry of Education, Sichuan University, Chengdu 610064, China
  • 2College of Physical Science and Technology, Sichuan University, Chengdu 610064, China
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    DOI: 10.3788/COL201513.112401 Cite this Article Set citation alerts
    Linguo Xie, Xiaodong Qiu, Jiangdong Qiu, Zhiyou Zhang, Jinglei Du, Fuhua Gao. Determination of the focused beam waist of lasers with weak measurements[J]. Chinese Optics Letters, 2015, 13(11): 112401 Copy Citation Text show less
    (a) Experimental setup: the light source is a He-Ne laser at 632.8 nm (Thorlabs HNL210L); HWP, half-wave plate for attenuating the light intensity; L1, short-focus lens (variable); P1 and P2, Glan polarizers; prism with refractive index n=1.515 (at 632.8 nm); L2, long-focus lens (150 mm); CCD, Coherent LaserCam HR. Dotted box: the schematic of the standard lock-in technology. PolM, polarization modulator; PSD, position sensitive detector; their frequencies keep synchronous. (b) and (c) denote the focused beam waist at different positions relative to the reflection surface.
    Fig. 1. (a) Experimental setup: the light source is a He-Ne laser at 632.8 nm (Thorlabs HNL210L); HWP, half-wave plate for attenuating the light intensity; L1, short-focus lens (variable); P1 and P2, Glan polarizers; prism with refractive index n=1.515 (at 632.8 nm); L2, long-focus lens (150 mm); CCD, Coherent LaserCam HR. Dotted box: the schematic of the standard lock-in technology. PolM, polarization modulator; PSD, position sensitive detector; their frequencies keep synchronous. (b) and (c) denote the focused beam waist at different positions relative to the reflection surface.
    ∂ΔH/∂ω0 (the sensitivity of the amplified shift to the beam waist) varies with incident and postselection angles. The extreme values are indicated by the black dashed lines.
    Fig. 2. ΔH/ω0 (the sensitivity of the amplified shift to the beam waist) varies with incident and postselection angles. The extreme values are indicated by the black dashed lines.
    Amplified shift changing with the postselection angle and the beam waist. Here, the beam waist is chosen as 15.96, 19.09, and 20.81 μm. The incident angle is 65°. The squares, circles, and triangles denote the experiment data corresponding to different beam waists. The curves are theoretical predictions from Eq. (7).
    Fig. 3. Amplified shift changing with the postselection angle and the beam waist. Here, the beam waist is chosen as 15.96, 19.09, and 20.81 μm. The incident angle is 65°. The squares, circles, and triangles denote the experiment data corresponding to different beam waists. The curves are theoretical predictions from Eq. (7).
    Linguo Xie, Xiaodong Qiu, Jiangdong Qiu, Zhiyou Zhang, Jinglei Du, Fuhua Gao. Determination of the focused beam waist of lasers with weak measurements[J]. Chinese Optics Letters, 2015, 13(11): 112401
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