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The one-dimensional position sensitive wire gaseous detector is developed for the synchrotron radiation diffraction, which consists of a single wire of gold-plated tungsten and 200 cathode strips as the readout. The induced signal is produced by the several adjacent cathode strips when X-ray is incident on anode wire with high voltage. Using the center gravity method to analyze the adjacent signals in one dimension, the primary ionization position of the X-ray can be obtained and the position resolution is 160 μm (FWHM). In Beijing Synchrotron Radiation Facility, the diffraction test is done at the experimental station. When the X-ray irradiates the crystal sample of SiO2, the different sizes of the diffraction rings can be produced. The diffraction angles are measured to be 11.148° and 14.201°, and the two-dimensional diffraction rings are reconstructed when the detector is moved and scanned with the several steps in the diffraction ring range. The diffraction aberration of one-dimensional wire chamber is very obvious. In the paper, the relevant influence factors of the detector construct are discussed. The thickness of the working gas and the width of active area window can give rise to the diffraction ring aberration. The theoretical calculation value of the diffraction aberration is larger than the position resolution value of the gaseous detector. The correction method is established based on the corresponding physical analysis, and by this method the value of the diffraction ring point is calculated. The relative aberration of diffraction position is improved by up to 7% with using the method, and the two-dimensional diffraction ring with no aberration can be reconstructed.
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Keywords:
- gas detector /
- diffraction measurements /
- synchrotron radiation /
- correction method
[1] Kosuke K, Shogo H, Masaaki K, Hiroshi W, Manabu F 1994 Nucl. Instrum. Meth. A 342 509
[2] Liu M 2013 M. S. Dissertation (Beijing: University of Chinese Academy of Sciences) (in Chinese) [刘梅 2013 硕士学位论文(北京: 中国科学院大学)]
[3] Liu M, Dai H L, Qi H R, Zhuang B A, Zhang J, Liu R G, Zhu Q M, Ouyang Q, Chen Y B, Jiang X S, Wang Y J, Liu P, Chang G C 2013 Chin. Phys. C 37 108001
[4] Owens A 2012 Nucl. Instrum. Meth. A 695 1
[5] Tolochko B P, Kulipanov G N, Mezentsev N A, Mishnev S I 2000 Nucl. Instrum. Meth. A 448 228
[6] Ramos-Lerate I, Beltran D, Magrans I, Martinez J C, Perlas J A, Bordas J 2003 Nucl. Instrum. Meth. A 513 197
[7] Liu S B, Feng C Q, Kang L F, An Q 2010 Nucl. Instrum. Meth. A 621 513
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[1] Kosuke K, Shogo H, Masaaki K, Hiroshi W, Manabu F 1994 Nucl. Instrum. Meth. A 342 509
[2] Liu M 2013 M. S. Dissertation (Beijing: University of Chinese Academy of Sciences) (in Chinese) [刘梅 2013 硕士学位论文(北京: 中国科学院大学)]
[3] Liu M, Dai H L, Qi H R, Zhuang B A, Zhang J, Liu R G, Zhu Q M, Ouyang Q, Chen Y B, Jiang X S, Wang Y J, Liu P, Chang G C 2013 Chin. Phys. C 37 108001
[4] Owens A 2012 Nucl. Instrum. Meth. A 695 1
[5] Tolochko B P, Kulipanov G N, Mezentsev N A, Mishnev S I 2000 Nucl. Instrum. Meth. A 448 228
[6] Ramos-Lerate I, Beltran D, Magrans I, Martinez J C, Perlas J A, Bordas J 2003 Nucl. Instrum. Meth. A 513 197
[7] Liu S B, Feng C Q, Kang L F, An Q 2010 Nucl. Instrum. Meth. A 621 513
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