Double refraction and reflection of sequential crystal interfaces with arbitrary orientation of the optic axis and application to optimum design /Type /Page 11.9559 TL /R376 239 0 R /Contents 136 0 R n /R373 236 0 R 3 0 obj 203.593 0 Td /Pages 1 0 R /R356 218 0 R 1446.11 904.148 l << /R8 32 0 R /R11 11.9552 Tf Depending on the polarization the light must travel in different directions for the two dots to appear. 87.273 33.801 l /R84 78 0 R endobj
The calcite crystal presented in Figure 3(b) is positioned over the capital letter A on a white sheet of paper demonstrating a double image observed through the crystal. @�T�7z�].`�ǝ���/5���1g���6ðEz�[�
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/CA 1 BT To find out more, see our, Browse more than 70 science journal titles, Read the very best research published in IOP journals, Read open access proceedings from science conferences worldwide, Published under licence by IOP Publishing Ltd, Babinet's principle in double-refraction systems, Bounds and zeros in reflection and refraction by uniaxial crystals, Inhibited reflection: longitudinal and transverse displacement of the reflectedray, Propagation of Gaussian beams in anisotropic media, Evolution of optical phase and polarization vortices in birefringent media, Circularly and linearly polarized light in the totalreflection region at isotropic medium-uniaxial crystalinterfaces, Features Editor, Physics World (Maternity Cover). >> stream [ (from\055focus) -263 (\1335\135\054) -265.994 (and) -263.009 (depth\055from\055refraction) -262.99 (\13320\054) -263.005 (4\054) -263.008 (7\054) -263.008 (1\135\056) -348.996 (Al\055) ] TJ /R306 373 0 R /R118 152 0 R |��� &� +F0)ʂ��ހ�x�X��n��DŽEa�O0*D(g�Y��P.� D. /XObject << q /Contents 188 0 R /R317 379 0 R /R11 37 0 R endstream
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