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Intense few-cycle pulses are widely used in transient light synthesis,high harmonic generation (HHG) and especially in isolated attosecond pulse generation.To obtain intense few-cycle pulses,the intense supercontinuum is needed.The traditional way to generate intense supercontinuum is using rare gas filled hollow-core fibers.Since the input energy of hollow-core fiber system is limited to a level of tens of mJ,it is necessary to find new ways to achieve energy scaling.In this paper we demonstrate the efficient generation of supercontinuum by solid thin plates,compression and its application in HHG. The Ti:sapphire laser used in the present experiment emits 0.8 mJ in energy with a duration of 30 fs at 1 kHz.After passing through a 3:1 telescope,the beam has a diameter changed from 12 mm to 4 mm.Then the laser is focused by an f=2000 mm lens into a 600 m-diameter spot.After propagating through 7 fused silica plates placed at Brewster's angle (55.5) with a thickness of 0.1 mm,the 0.7 mJ octave spanning supercontinuum is achieved,corresponding to an efficiency of 87.5%.The first three plates are placed at 31,11,2.5 mm in front of the beam waist,and the last four plates are placed at 2,7,12,17 mm behind the beam waist respectively.With a pair of wedges and 4 pairs of chirped mirrors,the 0.68 mJ supercontinuum is compressed to a duration of 6.3 fs,which is measured by TG-FROG. The 0.5 mJ,6.3 fs pulse is used to perform high-harmonic generation experiment.The beam diameter is 150 m when focused by an f=400 mm lens,with a laser intensity of 8.11014 W/cm2.The 1 mm Ne gas jet is used to perform HHG experiment with a back pressure of 300 mbar.To block the near-infrared light,a 150 m Zirconium foil is placed behind the gas jet.Then the XUV spectrum is detected by a spectrometer,which consists of a flat field grating and a CCD camera.For driving pulses of few-cycle regime without dispersion,the cutoff spectrum of HHG is continuous.But when the pulse is stretched by positive or negative dispersion,the cutoff spectrum turns discrete.The HHG result is that the cutoff region is continuous when the wedge is in a certain place.Then by increasing or reducing the insertion of the wedge,the cutoff spectrum becomes discrete.Our result is consistent with HHG generated by few-cycle pulses. In conclusion,we demonstrate high-harmonic generation based on supercontinuum generated by solid thin plates. The 0.7 mJ supercontinuum is achieved when 0.8 mJ pulses are injected to 7 thin fused silica plates.The supercontinuum is compressed to 0.68 mJ,6.3 fs.The 0.5 mJ,6.3 fs pulse is used to perform HHG experiments.The HHG result was consistent with few-cycle driving pulses.Our research indicates that solid state supercontinuum has great potential applications in HHG and isolated attosecond pulse generation.
[1] Telle H R, Steinmeyer G, Dunlop A E, Stenger J, Sutter D H, Keller U 1999 Appl. Phys. B 69 327
[2] Wirth A, Hassan M, Grgura I, Gagnon J, et al. 2011 Science 334 195
[3] McPherson A, Gibson G, Jara H, et al. 1987 J. Opt. Soc. Am. B 4 595
[4] Baltuka A, Udem T, Uiberacker M, et al. 2003 Nature 421 611
[5] Zhao K, Zhang Q, Chini M, Wu Y, Wang X, Chang Z 2012 Opt. Lett. 37 3891
[6] Mashiko H, Gilbertson S, Li C, Moon E, Chang Z 2008 Phys. Rev. A 77 063423
[7] Kim I J, Kim C M, Kim H T, Lee G H, Lee Y S, Park J Y, Cho D J, Nam C H 2005 Phys. Rev. Lett. 94 243901
[8] Chini M, Zhao K, Chang Z 2014 Nat. Photonics 8 178
[9] Shimizu F 1967 Phys. Rev. Lett. 19 1097
[10] Yang G, Shen Y R 1984 Opt. Lett. 9 510
[11] Nisoli M, De Silvestri S, Svelto O 1996 Appl. Phys. Lett. 68 2793
[12] Cardin V, Thir N, Beaulieu S, Wanie V, Lgar F, Schmidt B E 2015 Appl. Phys. Lett. 107 181101
[13] Lu C H, Tsou Y J, Chen H Y, Chen B H, Cheng Y C, Yang S D, Chen M C, Hsu C C, Kung A H 2014 Optica 1 400
[14] He P, Liu Y Y, Zhao K, et al. 2017 Opt. Lett. 42 474
[15] Sweetser J N, Fittinghoff D N, Trebino R 1997 Opt. Lett. 22 519
[16] Ye P 2014 Ph. D. Dissertation (Beijing:Institute of Physics, Chinese Academy of Sciences) (in Chinese)[叶蓬 2014 博士学位论文 (北京:中国科学院物理研究所)]
[17] Wang X W, l Chini M, Cheng Y, Wu Y, Chang Z H 2013 Appl. Opt. 52 323
[18] Tatsuo H, Kaoru T, Hideo S, Andrzej O 1999 Appl. Opt. 38 2743
[19] Corkum P B 1993 Phys. Rev. Lett. 71 1994
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[1] Telle H R, Steinmeyer G, Dunlop A E, Stenger J, Sutter D H, Keller U 1999 Appl. Phys. B 69 327
[2] Wirth A, Hassan M, Grgura I, Gagnon J, et al. 2011 Science 334 195
[3] McPherson A, Gibson G, Jara H, et al. 1987 J. Opt. Soc. Am. B 4 595
[4] Baltuka A, Udem T, Uiberacker M, et al. 2003 Nature 421 611
[5] Zhao K, Zhang Q, Chini M, Wu Y, Wang X, Chang Z 2012 Opt. Lett. 37 3891
[6] Mashiko H, Gilbertson S, Li C, Moon E, Chang Z 2008 Phys. Rev. A 77 063423
[7] Kim I J, Kim C M, Kim H T, Lee G H, Lee Y S, Park J Y, Cho D J, Nam C H 2005 Phys. Rev. Lett. 94 243901
[8] Chini M, Zhao K, Chang Z 2014 Nat. Photonics 8 178
[9] Shimizu F 1967 Phys. Rev. Lett. 19 1097
[10] Yang G, Shen Y R 1984 Opt. Lett. 9 510
[11] Nisoli M, De Silvestri S, Svelto O 1996 Appl. Phys. Lett. 68 2793
[12] Cardin V, Thir N, Beaulieu S, Wanie V, Lgar F, Schmidt B E 2015 Appl. Phys. Lett. 107 181101
[13] Lu C H, Tsou Y J, Chen H Y, Chen B H, Cheng Y C, Yang S D, Chen M C, Hsu C C, Kung A H 2014 Optica 1 400
[14] He P, Liu Y Y, Zhao K, et al. 2017 Opt. Lett. 42 474
[15] Sweetser J N, Fittinghoff D N, Trebino R 1997 Opt. Lett. 22 519
[16] Ye P 2014 Ph. D. Dissertation (Beijing:Institute of Physics, Chinese Academy of Sciences) (in Chinese)[叶蓬 2014 博士学位论文 (北京:中国科学院物理研究所)]
[17] Wang X W, l Chini M, Cheng Y, Wu Y, Chang Z H 2013 Appl. Opt. 52 323
[18] Tatsuo H, Kaoru T, Hideo S, Andrzej O 1999 Appl. Opt. 38 2743
[19] Corkum P B 1993 Phys. Rev. Lett. 71 1994
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