OSA's Digital Library

Optics Express

Optics Express

  • Editor: Andrew M. Weiner
  • Vol. 21, Iss. 23 — Nov. 18, 2013
  • pp: 27631–27640
« Show journal navigation

Energy exchange between two noncollinear filament-forming laser pulses in air

Pengji Ding, Zeqing Guo, Xiaoshan Wang, Yu Cao, Mingze Sun, Peixi Zhao, Yanchao Shi, Shaohua Sun, Xiaoliang Liu, and Bitao Hu  »View Author Affiliations


Optics Express, Vol. 21, Issue 23, pp. 27631-27640 (2013)
http://dx.doi.org/10.1364/OE.21.027631


View Full Text Article

Acrobat PDF (1134 KB)





Browse Journals / Lookup Meetings

Browse by Journal and Year


   


Lookup Conference Papers

Close Browse Journals / Lookup Meetings

Article Tools

Share
Citations

Abstract

Energy exchange between two filament-forming pulses with initially free chirp in air was experimentally studied. It occurs because of the change of delayed nonlinear refractive index, which slightly chirps the incident filament-forming laser pulses. Accompanying energy exchange process, spectral characteristics of output laser pulses shows dramatic blueshift and supercontinuum generation. Nonlinear absorptive effect introduces an inbalance between energy exchange at the negative delays and that at the positive delays, and affects the energy exchange efficiency. These results may provide a more comprehensive understanding of energy exchange process between filament-forming laser pulses.

© 2013 OSA

1. Introduction

Femtosecond laser filamentation in air is an interesting phenomenon [1

1. A. Braun, G. Korn, X. Liu, D. Du, J. Squier, and G. Mourou, “Self-channeling of high-peak-power femtosecond laser pulses in air,” Opt. Lett. 20, 73–75 (1995).

3

3. S.L. Chin, T.–J. Wang, C. Marceau, J. Wu, J. S. Liu, O. Kosareva, N. Panov, Y. P. Chen, J.–F. Daigle, S. Yuan, A. Azarm, W. W. Liu, T. Seideman, H. P. Zeng, M. Richardson, R. Lic, and Z. Z. Xu, “Advances in intense femtosecond laser filamentation in air,” Laser Phys. 22, 1–53 (2011).

], and has intensive applications including few-cycle pulse generation, THz radiation source, remote-sensing of atmospheric pollution, lighting and discharge triggering, to name a few. During the femtosecond laser filamentation, the laser beam maintains, in general, a very high intensity over long distance, which is much larger than the optical Rayleigh length, leaving a weakly ionized plasma channel named as filament in its wakefield. Filament appears as a result of dynamic competition between laser beam focusing and plasma defocusing when the peak power exceeds the critical value Pcr=3.77λ02/8πn0n2, where λ0 is the laser central wavelength in vacuum, n0 and n2 are the linear refractive index and the nonlinear refractive index coefficient respectively. For applications of femtosecond laser filamentation, it is of great concern to control the propagation of incident ultra-intense and -short laser pulses and optimize the characteristics of filament such as length, diameter in the perpendicular plane, clamping intensity. One example is the formation of plasma grating by few filaments interaction, which introduces a periodically modulated change in the local refractive index of the medium. A stationary plasma grating can be used as an interceptor breaking up the propagation path of filament-forming pulses to enhance the efficiency of third-order harmonic generation [4

4. Y. Liu, M. Durand, A. Houard, B. Forestier, A. Couairon, and A. Mysyrowicz, “Efficient generation of third harmonic radiation in air filaments: A revisit,” Opt. Commun. 284, 4706–4713 (2011).

, 5

5. P. J. Ding, Z. Y. Liu, Y. C. Shi, S. H. Sun, X. L. Liu, X. Sh. Wang, Z. Q. Guo, Q. C. Liu, Y. H. Li, and B. T. Hu, “Spectral characterization of third-order harmonic generation assisted by a two-dimensional plasma grating in air,” Phys. Rev. A 87, 043828 (2013).

]. It can also diffract the laser pulses with different frequencies into directions deviating from its propagation direction [6

6. X. Yang, J. Wu, Y. Tong, L.’en Ding, Z. Xu, and H. Zeng, “Femtosecond laser pulse energy transfer induced by plasma grating due to filament interaction in air,” Appl. Phys. Lett. 97, 071108 (2010).

].

As another promising nonlinear process for controlling the propagation of intensive ultra-short laser, energy exchange between few filament-forming pulses has been demonstrated in several experiments involving femtosecond laser filamentation in air and liquid [7

7. A. C. Bernstein, M. McCormick, G. M. Dyer, J. C. Sanders, and T. Ditmire, “Two-beam coupling between filament-forming beams in air,” Phys. Rev. Lett. 102, 123902 (2009).

9

9. Y. Liu, M. Durand, S. Chen, A. Houard, B. Prade, B. Forestier, and A. Mysyrowicz, “Energy exchange between femtosecond laser filaments in air,” Phys. Rev. Lett. 105, 055003 (2010).

]. Energy transfer occurs when linearly polarized laser beams are focused and spatiotemporally overlapped. It has been found that the magnitude and direction of energy transfer depend on the relative time delay, initial chirp, laser intensities, interacting location, intersecting angle and relative polarization. It is noticeable that in the first work [7

7. A. C. Bernstein, M. McCormick, G. M. Dyer, J. C. Sanders, and T. Ditmire, “Two-beam coupling between filament-forming beams in air,” Phys. Rev. Lett. 102, 123902 (2009).

] about energy exchange between laser pulses in the regime of femtosecond laser filamentation, the plasma generation or filament formation is an insignificant contribution desipite its presence. The possible reason is that the volume of filament under this condition was too samll compared to the area of the overall beam and the most of air molecules participate in the molecular rotational excitation rather than being ionized. Its results are well consistent with the classical two-beam coupling theory and attributed to impulsive stimulated Raman scattering (SRS). With a shorter focal length and higher incident laser power, the direction of energy transfer from the lower frequency pulse to the higher one was observed [9

9. Y. Liu, M. Durand, S. Chen, A. Houard, B. Prade, B. Forestier, and A. Mysyrowicz, “Energy exchange between femtosecond laser filaments in air,” Phys. Rev. Lett. 105, 055003 (2010).

]. This result is mediated by a moving plasma grating [10

10. M. Durand, Y. Liu, B. Forestier, A. Houard, and A. Mysyrowicz, “Experimental observation of a traveling plasma grating formed by two crossing filaments in gases,” Appl. Phys. Lett. 98, 121110 (2011).

], which is formed at the intersection region of the filaments. It is clearly different from that in a traditional Kerr nonlinearity mediated grating [7

7. A. C. Bernstein, M. McCormick, G. M. Dyer, J. C. Sanders, and T. Ditmire, “Two-beam coupling between filament-forming beams in air,” Phys. Rev. Lett. 102, 123902 (2009).

]. Efficient energy exchange was also reported and attributed to plasma-mediated forward SRS, facilitated by supercontinuum generation [8

8. Y. B. Zhao, T. E. Witt, and J. Gordon, “Efficient energy transfer between laser beams by stimulated Raman scattering,” Phys. Rev. Lett. 103, 173903 (2009).

]. In plasma-mediated SRS, the electromagnetic fields of two lasers are coupled by an electrostatic plasma wave. In the nonlinear regime involving filamentation, photons are transferred from one beam to another due to blueshift and supercontinuum generation in the plasma, resulting an energy difference between them. By using a motorized translation-stage setup with higher resolution, a fine spectral structure of energy exchange was also observed at small intersecting angles [11

11. B. D. Strycker, M. Springer, C. Trendafilova, X. Hua, M. Zhi, A. A. Kolomenskii, H. Schroeder, J. Strohaber, H. A. Schuessier, G. W. Kattawar, and A. V. Sokolov, “Energy transfer between laser filaments in liquid methanol,” Opt. Lett. 37, 16–18 (2012).

,12

12. G. Cheng, Y. H. Zheng, Y. Zhong, Z. N. Zeng, C. Li, X. C. Ge, R. X. Li, and Z. Z. Xu, “Energy transfer between few-cycle laser filaments in air,” Appl. Phys. Lett. 101, 251111 (2012).

], in which the direction of energy transfer varies with the spectral components of incident laser pulses.

However, the effect of plasma fromation has not been completely investigated. One effect affecting the energy exchange efficiency is the nonlinear absorption. Accompanying plasma formation in the intersecting region, the energy loss of lasers takes up, which should lead to an influence on the energy exchange process. In this work, we present experimental results on the energy exchange between two filament-forming pulses in air. Spectra of output laser pulses were measured in order to further understand energy exchange process. Different from reported literatures [7

7. A. C. Bernstein, M. McCormick, G. M. Dyer, J. C. Sanders, and T. Ditmire, “Two-beam coupling between filament-forming beams in air,” Phys. Rev. Lett. 102, 123902 (2009).

9

9. Y. Liu, M. Durand, S. Chen, A. Houard, B. Prade, B. Forestier, and A. Mysyrowicz, “Energy exchange between femtosecond laser filaments in air,” Phys. Rev. Lett. 105, 055003 (2010).

], the energy exchange efficiency is redefined concerning the inbalance between energy exchange at the negative delays and that at the positive delays. Its dependence on the incident laser power was also investigated.

2. Experimental setup

The schematic diagram of experimental setup is illustrated in Fig. 1(a). The laser system used is a Ti:sapphire pulse amplifier system which is capable of producing 43 fs pulses centered at 790 nm with energy of 3 mJ, at a repetition rate of 1 kHz. The chirp of laser pulse can be neglected, which has been confirmed by FROG measurement. The laser beam was split into two arms by a beamsplitter (splitting ratio 55:45). One arm is defined as the delay-tuned beam (Beam-1) and another arm defined the delay-fixed beam (Beam-2). Both beams were focused by two lens with focusing length of 400 mm to generate two filaments. A sensitive CCD was installed on the top of the filament intersecting region to record the fluorescence image of the plasma, which was collected by using an Al-coated concave mirror installed under the bottom of the filament intersecting region. Filament diameters were measured by CCD flurescent imaging technique to be approximately 100 μm. If the filaments interact without temporal overlap, they simply pass through each other as shown in Fig. 1(b). By tuning the delay-tuned beam passing through a motorized translation-stage setup (precision of 2.5 μm), the two beams can be spatiotemporally overlapped to generate a bright sparking spot accompanying blast sound as shown in Fig. 1(c). The minimal translation setup corresponds to a temporal resolution of 0.495 fs. By concerning the influence of effective interaction length, the crossing angle between the two beams marked as θ was fixed at 17 degree by referring to [8

8. Y. B. Zhao, T. E. Witt, and J. Gordon, “Efficient energy transfer between laser beams by stimulated Raman scattering,” Phys. Rev. Lett. 103, 173903 (2009).

]. The spectra of output filament-forming pulses were measured by a spectroscopy (USB4000). The energy of each beam is controlled by passing through several neutral density filters and measured by an energy meter.

Fig. 1 Schematic diagram of experimental setup (a) and images of the filament produced by the intersecting filament-forming laser pulses at the crossing angle of 17 degree, with (b) 0.15 ps and (c) zero time delay between the pulses. Apparatus components include two focusing lenses (L1, L2), a beam splitters (BS1), a delay line (DL), a neutral density filter (ND), a spectrograph (SM) and an energy monitor.

3. Results and discussion

Fig. 2 (a) The energy of two laser pulses versus the relative time delay with initial laser power of 0.7Pcr. (b)–(c) The transmission of Beam-1 as a function of the relative time delay when the initial laser powers are 3.0Pcr (b) and 6.6Pcr (c) respectively. The red solid (green dashed, blue dash-doted) line represents the best fit by using the formula T(τ) (T1(τ), T2(τ) + T3(τ)).

Fig. 3 The spectra of the delay-tuned Beam-1 (a) and delay-fixed Beam-2 (b) verse the relative time delay when the initial total energy was 0.52 mJ.
Fig. 4 The spectra of the delay-tuned Beam-1 verse the relative time delay when the initial total energy was 1.04 mJ.

From the two-beam coupling theory, the energy exchange vanishes if there is no difference in frequency, as is the case for unchirped laser pulses with identical carrier frequency. But in the pulsed experiments involving filamentation, the delayed nonlinear response such as the impulsive Raman nonlinear response and plasma formation can effectively chirp the involved laser pulse [8

8. Y. B. Zhao, T. E. Witt, and J. Gordon, “Efficient energy transfer between laser beams by stimulated Raman scattering,” Phys. Rev. Lett. 103, 173903 (2009).

, 13

13. S. Smolorz and F. Wise, “Femtosecond two-beam coupling energy transfer from Raman and electronic nonlinearities,” J. Opt. Soc. Am. B 17, 1636–1644 (2000).

]. In our case, the incident laser pulses have the same carrier frequency ω0, but due to chirp from the delayed nonlinear responses the instantaneous frequency varies over the pulse duration. The frequency difference Δω = ω1ω2 between the delay-fixed pulse and the delay-tuned one depends on their relative time delay τ, where ω1 and ω2 represent the frequency of delay-fixed pulse and delay-tuned pulse respectively. With this frequency difference, a phase shift occurs between the local optical interference pattern and the refractive index modulation. In the case where the nonlinear refractive index follows the Debye relaxation, the energy exchange between laser beams can be easily derivated from the wave propagation equation [14

14. R. W. Boyd, Nonlinear Optics, 3rd ed. (Academic, 2008).

]. As is well known, the generation of plasma introduces a retarded negative refractive index change by −ρ/2ρcr, where ρcr is the critical plasma density for 800 nm laser. This could negatively chirp the laser pulses. For pulses with negative chirp, Δω is negative for τ < 0 as the tail of Beam-1 and the front of Beam-2 overlap. Correspondingly, it is positive for τ > 0 as the tail of Beam-2 and the front of Beam-1 overlap. Though the decay process of nonlinear refractive index due to plasma generation is more complicated than a simple exponential law [15

15. M. Durand, A. Jarnac, Y. Liu, B. Prade, A. Houard, V. Tikhonchuk, and A. Mysyrowicz, ”Dynamics of plasma gratings in atomic and molecular gases,” Phys. Rev. E 86, 036405 (2012).

], but it doesn’t affect the validity of refractive grating dominating the energy exchange process. Therefore, according to the two-beam coupling theory [13

13. S. Smolorz and F. Wise, “Femtosecond two-beam coupling energy transfer from Raman and electronic nonlinearities,” J. Opt. Soc. Am. B 17, 1636–1644 (2000).

,16

16. A. Dogariu, T. Xia, D. J. Hagan, A. A. Said, and E. W. Van Stryland, “Purely refractive transient energy transfer by stimulated Rayleigh-wing scattering,” J. Opt. Soc. Am. B 14, 796–803 (1997).

,17

17. J. K. Wahlstrand, J. H. Odhner, E. T. McCole, Y.-H. Cheng, J. P. Palastro, R. J. Levis, and H. M. Milchberg, “Effect of two-beam coupling in strong-field optical pump-probe experiments,” Phys. Rev. A 87, 053801 (2013).

], one can expect that the delay-tuned pulse gain energy at negative delays and lose energy at positive delays because of plasma formation.

We use the time-domain theory for pump-probe experiments with chirped pulses [18

18. N. Tang and R. L. Sutherland, “Time-domain theory for pump-probe experiments with chirped pulses,” J. Opt. Soc. Am. B 14, 3412–3423 (1997).

] developed by N. Tang et al. to fit the transmission of Beam-1, as shown in Fig. 2. In our case involving femtosecond laser filamentation in air, the linear absorption can be neglected. Taking the temporal response function R(t) of air as exp(−t/τn), where τn is the exponential decay constant, the transmission of Beam-1 can be estimated as:
T(τ)=1+T1(τ)+T2(τ)+T3(τ),
(1)
T1(τ)=κπτpI02Bxxxx{Im[+dtu*(tτ)u(t)×tdtR(tt)u(tτ)u*(t)]},
(2)
T2(τ)=κπτpI02Bxxxx{Re+dtu*(tτ)u*(t)×tdtR(tt)u(tτ)u(t)]},
(3)
T3(τ)=κπτpI02Bxxxx{Re[+dtu*(tτ)u(t)×tdtR(tt)u(tτ)u*(t)]},
(4)
where τp the pulse duration, u(t) the time-dependent electric field, and I0=+|u(t)|2dt. T1(τ) represents the contribution from two beam-coupling, and the terms of T2(τ) and T3(τ) represent the nonlinear absorptive contributions. κ=24πkLeffEp/n2w2cτp, where k is the wave number for the incident laser wavelength in vacuum, Leff is the effective propagation length (3 cm), Ep is the pulse energy, and c is the light speed. The Gaussian beam radius w at the intersection region was estimated as 100 μm. Bxxxx and B′xxxx are the delayed contributions to the nonlinear refractive effects and the nonlinear absorptive effects respectively.

The red solid lines in Fig. 2 are the best fitted curves by using T(τ) with the relevant pulse duration of 43 fs and energies. A good fit of Bxxxx = 9.0 × 10−6cm3/erg · s was obtained in Fig. 2(b). Also, as a dependent parameter, the temporal width of laser pulse was extracted as τp ≈ 60 fs, corresponding a chirp parameter C = 0.97. Then the delayed nonlinear refractive index coefficient n2,d can be extracted as 3.22 × 10−19cm2/W, which is perfectly consistent with the reported value of ∼ 3.01 × 10−19cm2/W in literatures [19

19. E. T. J. Nibbering, G. Grillon, M. A. Franco, B. S. Prade, and A. Mysyrowicz, “Determination of the inertial contribution to the nonlinear refractive index of air, N2, and O2by use of unfocused high-intensity femtosecond laser pulses,” J. Opt. Soc. Am. B 14, 650–660 (1997).

, 20

20. Y. E. Geints, A. M. Kabanov, A. A. Zemlyanov, E. E. Bykova, O. A. Bukin, and S. S. Golik, “Kerr-driven nonlinear refractive index of air at 800 and 400nm measured through femtosecond laser pulse filamentation,” Appl. Phys. Lett. 99, 181114 (2011).

]. The fit in Fig. 2(c) yields n2,d = 1.70 × 10−19cm2/W and the average of extracted n2,d for different laser powers is 2.78 × 10−19cm2/W, also close to the reported value. The combined contribution T2 + T3 originates from coherent interaction between the laser pulses and the air medium [18

18. N. Tang and R. L. Sutherland, “Time-domain theory for pump-probe experiments with chirped pulses,” J. Opt. Soc. Am. B 14, 3412–3423 (1997).

], which introduces a deep dip near zero time delay as shown in Fig. 2(b) and 2(c). This contribution was also termed the coherent artifact, coming from the absorptive nonlinearities. Any absorptive nonlinearity has a 90 degree phase shift in its polarization compared to the laser field. It leads to an energy exchange between the laser and the medium. Hence, when the laser intensity increases, the influence of absorptive nonlinearity becomes more important and then one can expect larger inbalance of energy exchange, as shown in Fig. 2(c).

Fig. 5 The energy exchange efficiency (a) and the corresponding time duration (b) as a function of the incident laser power.

These results can be qualitatively understood as follows: with a higher laser power, a larger volume plasma region and a higher refractive index contrast between the negative contribution due to the plasma formation and the positive contribution due to the delayed rotational Raman effect [9

9. Y. Liu, M. Durand, S. Chen, A. Houard, B. Prade, B. Forestier, and A. Mysyrowicz, “Energy exchange between femtosecond laser filaments in air,” Phys. Rev. Lett. 105, 055003 (2010).

] can be generated, which allows for more efficient energy exchange. Hence, it can be expected that more efficient energy exchange can be achieved at smaller crossing angles because of more effective interaction length. At the same time, the laser energy involving energy exchange process could be reduced by nonlinear absorption. With the competition of these two kinds of contributions, the energy exchange efficiency could reach a maximum value when the plasma density in the interacting region saturates, which also leads to a saturated interaction length. In this case, the laser power corresponding to the maximal efficiency is almost 3.0Pcr. After that, it decreases because of the second contribution, as shown in Fig. 5(a). However, the duration of energy exchange reflects the effective interaction length and has no close relation with strong plasma formation when the interaction length has saturated. Therefore, the duration of energy exchange remains an approximately constant level from P ∼ 3.0Pcr to P ∼ 6.6Pcr (Fig. 5(b)).

4. Summary

In summary, energy exchange between two initially chirp-free femtosecond pulses in air was experimentally studied. The transmission of the delay-tuned beam around the zero time delay were measured. Accompanying energy exchange process, spectral characteristics of output laser pulses shows dramatic blueshift and supercontinuum generation. Because of the inbalance between energy exchange at the negative delays and that at the positive delays caused by nonlinear absorption, the energy exchange efficiency was redefined. When the incident laser power is varied from 0.7Pcr to 3.0Pcr, the energy exchange efficiency increases from 8% to 45%. With higher incident laser power, the exchange efficiency slightly decreases. With a time-domain two-beam coupling model, the experimental results were fitted and the delayed nonlinear coefficient was extracted. These experiments were performed in air, and a higher energy exchange efficiency could be achieved in gaseous media with longer molecule response time. The results may be promising for some applications like filament control and ultra-intense laser propagation.

Acknowledgments

We would like to acknowledge the support of the National Natural Science Foundation of China (Grants No. 11135002, No. 11075069, No. 91026021, No. 11075068, and No. 11175076) and Scholarship Award for Excellent Doctoral Student granted by Ministry of Education.

References and links

1.

A. Braun, G. Korn, X. Liu, D. Du, J. Squier, and G. Mourou, “Self-channeling of high-peak-power femtosecond laser pulses in air,” Opt. Lett. 20, 73–75 (1995).

2.

A. Couairon and A. Mysyrowicz, “Femtosecond filamentation in transparent media,” Phys. Rep. 441, 47–189 (2007).

3.

S.L. Chin, T.–J. Wang, C. Marceau, J. Wu, J. S. Liu, O. Kosareva, N. Panov, Y. P. Chen, J.–F. Daigle, S. Yuan, A. Azarm, W. W. Liu, T. Seideman, H. P. Zeng, M. Richardson, R. Lic, and Z. Z. Xu, “Advances in intense femtosecond laser filamentation in air,” Laser Phys. 22, 1–53 (2011).

4.

Y. Liu, M. Durand, A. Houard, B. Forestier, A. Couairon, and A. Mysyrowicz, “Efficient generation of third harmonic radiation in air filaments: A revisit,” Opt. Commun. 284, 4706–4713 (2011).

5.

P. J. Ding, Z. Y. Liu, Y. C. Shi, S. H. Sun, X. L. Liu, X. Sh. Wang, Z. Q. Guo, Q. C. Liu, Y. H. Li, and B. T. Hu, “Spectral characterization of third-order harmonic generation assisted by a two-dimensional plasma grating in air,” Phys. Rev. A 87, 043828 (2013).

6.

X. Yang, J. Wu, Y. Tong, L.’en Ding, Z. Xu, and H. Zeng, “Femtosecond laser pulse energy transfer induced by plasma grating due to filament interaction in air,” Appl. Phys. Lett. 97, 071108 (2010).

7.

A. C. Bernstein, M. McCormick, G. M. Dyer, J. C. Sanders, and T. Ditmire, “Two-beam coupling between filament-forming beams in air,” Phys. Rev. Lett. 102, 123902 (2009).

8.

Y. B. Zhao, T. E. Witt, and J. Gordon, “Efficient energy transfer between laser beams by stimulated Raman scattering,” Phys. Rev. Lett. 103, 173903 (2009).

9.

Y. Liu, M. Durand, S. Chen, A. Houard, B. Prade, B. Forestier, and A. Mysyrowicz, “Energy exchange between femtosecond laser filaments in air,” Phys. Rev. Lett. 105, 055003 (2010).

10.

M. Durand, Y. Liu, B. Forestier, A. Houard, and A. Mysyrowicz, “Experimental observation of a traveling plasma grating formed by two crossing filaments in gases,” Appl. Phys. Lett. 98, 121110 (2011).

11.

B. D. Strycker, M. Springer, C. Trendafilova, X. Hua, M. Zhi, A. A. Kolomenskii, H. Schroeder, J. Strohaber, H. A. Schuessier, G. W. Kattawar, and A. V. Sokolov, “Energy transfer between laser filaments in liquid methanol,” Opt. Lett. 37, 16–18 (2012).

12.

G. Cheng, Y. H. Zheng, Y. Zhong, Z. N. Zeng, C. Li, X. C. Ge, R. X. Li, and Z. Z. Xu, “Energy transfer between few-cycle laser filaments in air,” Appl. Phys. Lett. 101, 251111 (2012).

13.

S. Smolorz and F. Wise, “Femtosecond two-beam coupling energy transfer from Raman and electronic nonlinearities,” J. Opt. Soc. Am. B 17, 1636–1644 (2000).

14.

R. W. Boyd, Nonlinear Optics, 3rd ed. (Academic, 2008).

15.

M. Durand, A. Jarnac, Y. Liu, B. Prade, A. Houard, V. Tikhonchuk, and A. Mysyrowicz, ”Dynamics of plasma gratings in atomic and molecular gases,” Phys. Rev. E 86, 036405 (2012).

16.

A. Dogariu, T. Xia, D. J. Hagan, A. A. Said, and E. W. Van Stryland, “Purely refractive transient energy transfer by stimulated Rayleigh-wing scattering,” J. Opt. Soc. Am. B 14, 796–803 (1997).

17.

J. K. Wahlstrand, J. H. Odhner, E. T. McCole, Y.-H. Cheng, J. P. Palastro, R. J. Levis, and H. M. Milchberg, “Effect of two-beam coupling in strong-field optical pump-probe experiments,” Phys. Rev. A 87, 053801 (2013).

18.

N. Tang and R. L. Sutherland, “Time-domain theory for pump-probe experiments with chirped pulses,” J. Opt. Soc. Am. B 14, 3412–3423 (1997).

19.

E. T. J. Nibbering, G. Grillon, M. A. Franco, B. S. Prade, and A. Mysyrowicz, “Determination of the inertial contribution to the nonlinear refractive index of air, N2, and O2by use of unfocused high-intensity femtosecond laser pulses,” J. Opt. Soc. Am. B 14, 650–660 (1997).

20.

Y. E. Geints, A. M. Kabanov, A. A. Zemlyanov, E. E. Bykova, O. A. Bukin, and S. S. Golik, “Kerr-driven nonlinear refractive index of air at 800 and 400nm measured through femtosecond laser pulse filamentation,” Appl. Phys. Lett. 99, 181114 (2011).

OCIS Codes
(190.5330) Nonlinear optics : Photorefractive optics
(190.7070) Nonlinear optics : Two-wave mixing
(320.2250) Ultrafast optics : Femtosecond phenomena

ToC Category:
Nonlinear Optics

History
Original Manuscript: August 26, 2013
Revised Manuscript: October 18, 2013
Manuscript Accepted: October 21, 2013
Published: November 4, 2013

Citation
Pengji Ding, Zeqing Guo, Xiaoshan Wang, Yu Cao, Mingze Sun, Peixi Zhao, Yanchao Shi, Shaohua Sun, Xiaoliang Liu, and Bitao Hu, "Energy exchange between two noncollinear filament-forming laser pulses in air," Opt. Express 21, 27631-27640 (2013)
http://www.opticsinfobase.org/oe/abstract.cfm?URI=oe-21-23-27631


Sort:  Author  |  Year  |  Journal  |  Reset  

References

  1. A. Braun, G. Korn, X. Liu, D. Du, J. Squier, and G. Mourou, “Self-channeling of high-peak-power femtosecond laser pulses in air,” Opt. Lett.20, 73–75 (1995).
  2. A. Couairon and A. Mysyrowicz, “Femtosecond filamentation in transparent media,” Phys. Rep.441, 47–189 (2007).
  3. S.L. Chin, T.–J. Wang, C. Marceau, J. Wu, J. S. Liu, O. Kosareva, N. Panov, Y. P. Chen, J.–F. Daigle, S. Yuan, A. Azarm, W. W. Liu, T. Seideman, H. P. Zeng, M. Richardson, R. Lic, and Z. Z. Xu, “Advances in intense femtosecond laser filamentation in air,” Laser Phys.22, 1–53 (2011).
  4. Y. Liu, M. Durand, A. Houard, B. Forestier, A. Couairon, and A. Mysyrowicz, “Efficient generation of third harmonic radiation in air filaments: A revisit,” Opt. Commun.284, 4706–4713 (2011).
  5. P. J. Ding, Z. Y. Liu, Y. C. Shi, S. H. Sun, X. L. Liu, X. Sh. Wang, Z. Q. Guo, Q. C. Liu, Y. H. Li, and B. T. Hu, “Spectral characterization of third-order harmonic generation assisted by a two-dimensional plasma grating in air,” Phys. Rev. A87, 043828 (2013).
  6. X. Yang, J. Wu, Y. Tong, L.’en Ding, Z. Xu, and H. Zeng, “Femtosecond laser pulse energy transfer induced by plasma grating due to filament interaction in air,” Appl. Phys. Lett.97, 071108 (2010).
  7. A. C. Bernstein, M. McCormick, G. M. Dyer, J. C. Sanders, and T. Ditmire, “Two-beam coupling between filament-forming beams in air,” Phys. Rev. Lett.102, 123902 (2009).
  8. Y. B. Zhao, T. E. Witt, and J. Gordon, “Efficient energy transfer between laser beams by stimulated Raman scattering,” Phys. Rev. Lett.103, 173903 (2009).
  9. Y. Liu, M. Durand, S. Chen, A. Houard, B. Prade, B. Forestier, and A. Mysyrowicz, “Energy exchange between femtosecond laser filaments in air,” Phys. Rev. Lett.105, 055003 (2010).
  10. M. Durand, Y. Liu, B. Forestier, A. Houard, and A. Mysyrowicz, “Experimental observation of a traveling plasma grating formed by two crossing filaments in gases,” Appl. Phys. Lett.98, 121110 (2011).
  11. B. D. Strycker, M. Springer, C. Trendafilova, X. Hua, M. Zhi, A. A. Kolomenskii, H. Schroeder, J. Strohaber, H. A. Schuessier, G. W. Kattawar, and A. V. Sokolov, “Energy transfer between laser filaments in liquid methanol,” Opt. Lett.37, 16–18 (2012).
  12. G. Cheng, Y. H. Zheng, Y. Zhong, Z. N. Zeng, C. Li, X. C. Ge, R. X. Li, and Z. Z. Xu, “Energy transfer between few-cycle laser filaments in air,” Appl. Phys. Lett.101, 251111 (2012).
  13. S. Smolorz and F. Wise, “Femtosecond two-beam coupling energy transfer from Raman and electronic nonlinearities,” J. Opt. Soc. Am. B17, 1636–1644 (2000).
  14. R. W. Boyd, Nonlinear Optics, 3rd ed. (Academic, 2008).
  15. M. Durand, A. Jarnac, Y. Liu, B. Prade, A. Houard, V. Tikhonchuk, and A. Mysyrowicz, ”Dynamics of plasma gratings in atomic and molecular gases,” Phys. Rev. E86, 036405 (2012).
  16. A. Dogariu, T. Xia, D. J. Hagan, A. A. Said, and E. W. Van Stryland, “Purely refractive transient energy transfer by stimulated Rayleigh-wing scattering,” J. Opt. Soc. Am. B14, 796–803 (1997).
  17. J. K. Wahlstrand, J. H. Odhner, E. T. McCole, Y.-H. Cheng, J. P. Palastro, R. J. Levis, and H. M. Milchberg, “Effect of two-beam coupling in strong-field optical pump-probe experiments,” Phys. Rev. A87, 053801 (2013).
  18. N. Tang and R. L. Sutherland, “Time-domain theory for pump-probe experiments with chirped pulses,” J. Opt. Soc. Am. B14, 3412–3423 (1997).
  19. E. T. J. Nibbering, G. Grillon, M. A. Franco, B. S. Prade, and A. Mysyrowicz, “Determination of the inertial contribution to the nonlinear refractive index of air, N2, and O2by use of unfocused high-intensity femtosecond laser pulses,” J. Opt. Soc. Am. B14, 650–660 (1997).
  20. Y. E. Geints, A. M. Kabanov, A. A. Zemlyanov, E. E. Bykova, O. A. Bukin, and S. S. Golik, “Kerr-driven nonlinear refractive index of air at 800 and 400nm measured through femtosecond laser pulse filamentation,” Appl. Phys. Lett.99, 181114 (2011).

Cited By

Alert me when this paper is cited

OSA is able to provide readers links to articles that cite this paper by participating in CrossRef's Cited-By Linking service. CrossRef includes content from more than 3000 publishers and societies. In addition to listing OSA journal articles that cite this paper, citing articles from other participating publishers will also be listed.

Figures

Fig. 1 Fig. 2 Fig. 3
 
Fig. 4 Fig. 5
 

« Previous Article  |  Next Article »

OSA is a member of CrossRef.

CrossCheck Deposited