We calculate the light field in metal-coated optical fiber probes under illumination of femtosecond laser pulses with the three-dimensional finite-difference time-domain method. By choosing the maximum of the calculated light field data in the time period of one light wave cycle at each spatial point, we obtain the amplitude distributions instead of the conventional light field distribution of a time instant. It is found that with an incident plane wave pulse of y-polarization, the output amplitude distributions of y-polarization have roughly a circled-cross-like pattern with two arc-like zero-amplitude zones. By analyzing the y-polarized waveforms versus time at the points near the arc-like zero-amplitude zones, we find that waveform distortions appear at points in the neighborhood of the zero amplitude lines and in the time intervals when two wave-packets overlap.
We calculate the light field in metal-coated optical fiber probes under illumination of femtosecond laser pulses with the three-dimensional finite-difference time-domain method. By choosing the maximum of the calculated light field data in the time period of one light wave cycle at each spatial point, we obtain the amplitude distributions instead of the conventional light field distribution of a time instant. It is found that with an incident plane wave pulse of y-polarization, the output amplitude distributions of y-polarization have roughly a circled-cross-like pattern with two arc-like zero-amplitude zones. By analyzing the y-polarized waveforms versus time at the points near the arc-like zero-amplitude zones, we find that waveform distortions appear at points in the neighborhood of the zero amplitude lines and in the time intervals when two wave-packets overlap.
[1] Müller R and Lienau C 2000 Appl. Phys. Lett. 76 3367 [2] Pack A, Hietschold M and Wannemacher R 2002 Ultramicroscopy 92 251 [3] Baida F I, Labeke D. Van and Pagani Y 2003 Opt. Commun. 225 241 [4] Hwang D J, Chimmalgi A and Grigoropoulos CP 2006 J. Appl. Phys. 99 044905 [5] Wen S B and Greif R 2009 J. Phys. D 42 075502 [6] Zorba V, Mao X L, Russo R E 2009 Appl. Phys. Lett. 95 041110 [7] Milner A A, Zhang K and Prior Y 2008 Nano Lett. 8 2017 [8] Hwang D, Ryu S G and Misra N et al 2009 Appl. Phys. A 96 289 [9] Müller R and Lienau C 2001 J. Microscopy 202 339 [10] Yee K S 1996 IEEE Trans. Anten. Propagat. 14 302 [11] Liu M, Cheng C F and Song H S et al 2009 Acta Phys. Sin. 58 5376 (in Chinese) [12] Burresi M, Engelen R J P, Opheij A, van Oosten D, Mori D, Baba T and Kuipers L 2009 Phys. Rev. Lett. 102 033902 [13] Liu M, Song H S, Chen X Y et al 2010 Chin. Phys. Lett. 27 034202 [14] Liu GY, Teng S Y, Cheng C F et al 2009 Acta Phys. Sin. 58 7613 (in Chinese) [15] Teng S Y, Tan Y G and Cheng C F 2008 J. Opt. Soc. Am. A 25 2945