Abstract

There has been growing interest both in studying high intensity ultrafast laser plasma interactions with adaptive control systems as well as using long wavelength driver beams. We demonstrate the coherent control of the dynamics of laser-wakefield acceleration driven by ultrashort (∼ 100 fs) mid-infrared (∼ 3.9 μm) laser pulses. The critical density at this wavelength is 7.3 × 1019 cm−3, which is achievable with an ordinary gas target system. Interactions between mid-infrared laser pulses and such near-critical-density plasma may be beneficial due to much higher absorption of laser energy. In addition, the normalized vector potential of the laser field a0 increases with longer laser wavelength, lowering the required peak laser intensity to drive non-linear laser-wakefield acceleration. Here, MeV level, collimated electron beams with non-thermal, peaked energy spectra are generated. Optimization of electron beam qualities are realized through adaptive control of the laser wavefront. A genetic algorithm controlling a deformable mirror improves the electron total charge, energy spectra, beam pointing and stability at various plasma density profiles. Particle-in-cell simulations reveal that the optimal wavefront causes an earlier injection on the density up-ramp and thus higher energy gain as well as less filamentation during the interaction, which leads to the improvement in electron beam collimation and energy spectra.

© 2019 Optical Society of America under the terms of the OSA Open Access Publishing Agreement

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2019 (1)

F. Albert, N. Lemos, J. L. Shaw, P. M. King, B. B. Pollock, C. Goyon, W. Schumaker, A. M. Saunders, K. A. Marsh, A. Pak, J. E. Ralph, J. L. Martins, L. D. Amorim, R. W. Falcone, S. H. Glenzer, J. D. Moody, and C. Joshi, “Betatron x-ray radiation in the self-modulated laser wakefield acceleration regime: Prospects for a novel probe at large scale laser facilities,” Nucl. Fusion 59, 032003 (2019).
[Crossref]

2018 (8)

A. Mitrofanov, D. Sidorov-Biryukov, M. Rozhko, S. Ryabchuk, A. Voronin, and A. Zheltikov, “High-order harmonic generation from a solid-surface plasma by relativistic-intensity sub-100-fs mid-infrared pulses,” Opt. letters 43, 5571–5574 (2018).
[Crossref]

A. Zheltikov and R. Nevels, “Intensity and wavelength scaling of laser-driven electron transition radiation: toward a table-top source of electromagnetic pulses,” Laser Phys. Lett. 16, 015401 (2018).
[Crossref]

M. Burger, P. J. Skrodzki, J. Lin, J. Nees, K. Krushelnick, and I. Jovanovic, “Intense laser filament-solid interactions from near-ultraviolet to mid-infrared,” Opt. express 26, 16456–16465 (2018).
[Crossref] [PubMed]

D. Woodbury, L. Feder, V. Shumakova, C. Gollner, R. Schwartz, B. Miao, F. Salehi, A. Korolov, A. Pugžlys, A. Baltuška, and H. M. Milchberg, “Laser wakefield acceleration with mid-ir laser pulses,” Opt. letters 43, 1131–1134 (2018).
[Crossref]

Y. Wang, T. Guo, J. Li, J. Zhao, Y. Yin, X. Ren, J. Li, Y. Wu, M. Weidman, Z. Chang, M. F. Jager, C. J. Kaplan, R. Geneaux, C. Ott, D. M. Neumark, and S. R. Leone, “Enhanced high-order harmonic generation driven by a wavefront corrected high-energy laser,” J. Phys. B: At. Mol. Opt. Phys. 51, 134005 (2018).
[Crossref]

J. Lin, J. H. Easter, K. Krushelnick, M. Mathis, J. Dong, A. Thomas, and J. Nees, “Focus optimization at relativistic intensity with high numerical aperture and adaptive optics,” Opt. Commun. 421, 79–82 (2018).
[Crossref]

C. Yu, J. Liu, W. Wang, W. Li, R. Qi, Z. Zhang, Z. Qin, J. Liu, M. Fang, K. Feng, Y. Wu, L. Ke, Y. Chen, C. Wang, Y. Xu, Y. Leng, C. Xia, R. Li, and Z. Xu, “Enhanced betatron radiation by steering a laser-driven plasma wakefield with a tilted shock front,” Appl. Phys. Lett. 112, 133503 (2018).
[Crossref]

M. J. Streeter, S. J. Dann, J. D. Scott, C. D. Baird, C. D. Murphy, S. Eardley, R. A. Smith, S. Rozario, J. N. Gruse, S. P. Mangles, Z. Najmudin, S. Tata, M. Krishnamurthy, S. V. Rahul, D. Hazra, P. Pourmoussavi, J. Osterhoff, J. Hah, N. Bourgeois, C. Thornton, C. D. Gregory, C. J. Hooker, O. Chekhlov, S. J. Hawkes, B. Parry, V. A. Marshall, Y. Tang, E. Springate, P. P. Rajeev, A. G. Thomas, and D. R. Symes, “Temporal feedback control of high-intensity laser pulses to optimize ultrafast heating of atomic clusters,” Appl. Phys. Lett. 112, 244101 (2018).
[Crossref]

2017 (3)

J. Hah, W. Jiang, Z. He, J. Nees, B. Hou, A. Thomas, and K. Krushelnick, “Enhancement of thz generation by feedback-optimized wavefront manipulation,” Opt. Express 25, 17271–17279 (2017).
[Crossref] [PubMed]

H. Liang, P. Krogen, Z. Wang, H. Park, T. Kroh, K. Zawilski, P. Schunemann, J. Moses, L. F. Dimauro, F. X. Kärtner, and K. H. Hong, “High-energy mid-infrared sub-cycle pulse synthesis from a parametric amplifier,” Nat. Commun. 8, 141 (2017).
[Crossref]

F. Salehi, A. Goers, G. Hine, L. Feder, D. Kuk, B. Miao, D. Woodbury, K.-Y. Kim, and H. Milchberg, “Mev electron acceleration at 1 khz with< 10 mj laser pulses,” Opt. letters 42, 215–218 (2017).
[Crossref]

2016 (2)

A. C. Englesbe, Z. He, J. A. Nees, A. G. Thomas, A. Schmitt-Sody, and K. Krushelnick, “Control of the configuration of multiple femtosecond filaments in air by adaptive wavefront manipulation,” Opt. Express 24, 6071–6082 (2016).
[Crossref] [PubMed]

J. Ferri, X. Davoine, S. Fourmaux, J. Kieffer, S. Corde, K. T. Phuoc, and A. Lifschitz, “Effect of experimental laser imperfections on laser wakefield acceleration and betatron source,” Sci. reports 6, 27846 (2016).
[Crossref]

2015 (3)

Z.-H. He, B. Hou, V. Lebailly, J. Nees, K. Krushelnick, and A. Thomas, “Coherent control of plasma dynamics,” Nat. Commun. 6, 7156 (2015).
[Crossref] [PubMed]

T. D. Arber, K. Bennett, C. S. Brady, A. Lawrence-Douglas, M. G. Ramsay, N. J. Sircombe, P. Gillies, R. G. Evans, H. Schmitz, A. R. Bell, and C. P. Ridgers, “Contemporary particle-in-cell approach to laser-plasma modelling,” Plasma Phys. Control. Fusion 57, 113001 (2015).
[Crossref]

A. Goers, G. Hine, L. Feder, B. Miao, F. Salehi, J. Wahlstrand, and H. Milchberg, “Multi-mev electron acceleration by subterawatt laser pulses,” Phys. review letters 115, 194802 (2015).
[Crossref]

2014 (1)

J. Weisshaupt, V. Juvé, M. Holtz, S. Ku, M. Woerner, T. Elsaesser, S. Ališauskas, A. Pugžlys, and A. Baltuška, “High-brightness table-top hard x-ray source driven by sub-100-femtosecond mid-infrared pulses,” Nat. Photonics 8, 927 (2014).
[Crossref]

2013 (1)

G. Bussolino, A. Faenov, A. Giulietti, D. Giulietti, P. Koester, L. Labate, T. Levato, T. Pikuz, and L. Gizzi, “Electron radiography using a table-top laser-cluster plasma accelerator,” J. Phys. D: Appl. Phys. 46, 245501 (2013).
[Crossref]

2012 (1)

T. Popmintchev, M. C. Chen, D. Popmintchev, P. Arpin, S. Brown, S. Ališauskas, G. Andriukaitis, T. Balčiunas, O. D. Mücke, A. Pugzlys, A. Baltuška, B. Shim, S. E. Schrauth, A. Gaeta, C. Hernández-García, L. Plaja, A. Becker, A. Jaron-Becker, M. M. Murnane, and H. C. Kapteyn, “Bright coherent ultrahigh harmonics in the kev x-ray regime from mid-infrared femtosecond lasers,” Science 336, 1287–1291 (2012).
[Crossref] [PubMed]

2011 (2)

G. Andriukaitis, T. Balčiūnas, S. Ališauskas, A. Pugžlys, A. Baltuška, T. Popmintchev, M.-C. Chen, M. M. Murnane, and H. C. Kapteyn, “90 gw peak power few-cycle mid-infrared pulses from an optical parametric amplifier,” Opt. letters 36, 2755–2757 (2011).
[Crossref]

J. S. Liu, C. Q. Xia, W. T. Wang, H. Y. Lu, C. Wang, A. H. Deng, W. T. Li, H. Zhang, X. Y. Liang, Y. X. Leng, X. M. Lu, C. Wang, J. Z. Wang, K. Nakajima, R. X. Li, and Z. Z. Xu, “All-optical cascaded laser wakefield accelerator using ionization-induced injection,” Phys. Rev. Lett. 107, 035001 (2011).

2010 (1)

A. Popp, J. Vieira, J. Osterhoff, Z. Major, R. Hörlein, M. Fuchs, R. Weingartner, T. P. Rowlands-Rees, M. Marti, R. A. Fonseca, S. F. Martins, L. O. Silva, S. M. Hooker, F. Krausz, F. Grüner, and S. Karsch, “All-optical steering of laser-wakefield-accelerated electron beams,” Phys. review letters 105, 215001 (2010).
[Crossref]

2009 (2)

S. P. Mangles, G. Genoud, S. Kneip, M. Burza, K. Cassou, B. Cros, N. P. Dover, C. Kamperidis, Z. Najmudin, A. Persson, J. Schreiber, F. Wojda, and C. G. Wahlström, “Controlling the spectrum of x-rays generated in a laser-plasma accelerator by tailoring the laser wavefront,” Appl. Phys. Lett. 95, 181106 (2009).
[Crossref]

E. Esarey, C. Schroeder, and W. Leemans, “Physics of laser-driven plasma-based electron accelerators,” Rev. modern physics 81, 1229 (2009).
[Crossref]

2007 (3)

K. C. Nowack, F. Koppens, Y. V. Nazarov, and L. Vandersypen, “Coherent control of a single electron spin with electric fields,” Science 318, 1430–1433 (2007).
[Crossref] [PubMed]

W. Lu, M. Tzoufras, C. Joshi, F. Tsung, W. Mori, J. Vieira, R. Fonseca, and L. Silva, “Generating multi-gev electron bunches using single stage laser wakefield acceleration in a 3d nonlinear regime,” Phys. Rev. Special Top. Beams 10, 061301 (2007).
[Crossref]

J. Werschnik and E. Gross, “Quantum optimal control theory,” J. Phys. B: At. Mol. Opt. Phys. 40, R175 (2007).
[Crossref]

2006 (3)

Y. Glinec, J. Faure, A. Guemnie-Tafo, V. Malka, H. Monard, J. Larbre, V. De Waele, J. Marignier, and M. Mostafavi, “Absolute calibration for a broad range single shot electron spectrometer,” Rev. scientific instruments 77, 103301 (2006).
[Crossref]

S. P. Mangles, B. R. Walton, Z. Najmudin, A. E. Dangor, K. Krushelnick, V. Malka, M. Manclossi, N. Lopes, C. Carias, G. Mendes, and F. Dorchies, “Table-top laser-plasma acceleration as an electron radiography source,” Laser Part. Beams 24, 185–190 (2006).
[Crossref]

W. P. Leemans, B. Nagler, A. J. Gonsalves, C. Toth, K. Nakamura, C. G. Geddes, E. Esarey, C. Schroeder, and S. Hooker, “Gev electron beams from a centimetre-scale accelerator,” Nat. physics 2, 696 (2006).
[Crossref]

2004 (4)

S. P. Mangles, C. D. Murphy, Z. Najmudin, A. G. Thomas, J. L. Collier, A. E. Dangor, E. J. Divall, P. S. Foster, J. G. Gallacher, C. J. Hooker, D. A. Jaroszynski, A. J. Langley, W. B. Mori, P. A. Norreys, F. S. Tsung, R. Viskup, B. R. Walton, and K. Krushelnick, “Monoenergetic beams of relativistic electrons from intense laser-plasma interactions,” Nature 431, 535 (2004).
[Crossref] [PubMed]

C. Geddes, C. Toth, J. Van Tilborg, E. Esarey, C. Schroeder, D. Bruhwiler, C. Nieter, J. Cary, and W. Leemans, “High-quality electron beams from a laser wakefield accelerator using plasma-channel guiding,” Nature 431, 538 (2004).
[Crossref] [PubMed]

J. Faure, Y. Glinec, A. Pukhov, S. Kiselev, S. Gordienko, E. Lefebvre, J.-P. Rousseau, F. Burgy, and V. Malka, “A laser–plasma accelerator producing monoenergetic electron beams,” Nature 431, 541 (2004).
[Crossref] [PubMed]

S.-W. Bahk, P. Rousseau, T. Planchon, V. Chvykov, G. Kalintchenko, A. Maksimchuk, G. Mourou, and V. Yanovsky, “Generation and characterization of the highest laser intensities (10 22 w/cm 2),” Opt. letters 29, 2837–2839 (2004).
[Crossref]

2000 (1)

1999 (1)

Y. Nakamura, Y. A. Pashkin, and J. Tsai, “Coherent control of macroscopic quantum states in a single-cooper-pair box,” nature 398, 786 (1999).
[Crossref]

1998 (3)

D. Meshulach and Y. Silberberg, “Coherent quantum control of two-photon transitions by a femtosecond laser pulse,” Nature 396, 239 (1998).
[Crossref]

N. H. Bonadeo, J. Erland, D. Gammon, D. Park, D. Katzer, and D. Steel, “Coherent optical control of the quantum state of a single quantum dot,” Science 282, 1473–1476 (1998).
[Crossref] [PubMed]

A. Assion, T. Baumert, M. Bergt, T. Brixner, B. Kiefer, V. Seyfried, M. Strehle, and G. Gerber, “Control of chemical reactions by feedback-optimized phase-shaped femtosecond laser pulses,” Science 282, 919–922 (1998).
[Crossref] [PubMed]

1997 (1)

A. Haché, Y. Kostoulas, R. Atanasov, J. Hughes, J. Sipe, and H. Van Driel, “Observation of coherently controlled photocurrent in unbiased, bulk gaas,” Phys. review letters 78, 306 (1997).
[Crossref]

1979 (1)

T. Tajima and J. M. Dawson, “Laser electron accelerator,” Phys. Rev. Lett. 43, 267 (1979).
[Crossref]

Albert, F.

F. Albert, N. Lemos, J. L. Shaw, P. M. King, B. B. Pollock, C. Goyon, W. Schumaker, A. M. Saunders, K. A. Marsh, A. Pak, J. E. Ralph, J. L. Martins, L. D. Amorim, R. W. Falcone, S. H. Glenzer, J. D. Moody, and C. Joshi, “Betatron x-ray radiation in the self-modulated laser wakefield acceleration regime: Prospects for a novel probe at large scale laser facilities,” Nucl. Fusion 59, 032003 (2019).
[Crossref]

Albert, O.

Ališauskas, S.

J. Weisshaupt, V. Juvé, M. Holtz, S. Ku, M. Woerner, T. Elsaesser, S. Ališauskas, A. Pugžlys, and A. Baltuška, “High-brightness table-top hard x-ray source driven by sub-100-femtosecond mid-infrared pulses,” Nat. Photonics 8, 927 (2014).
[Crossref]

T. Popmintchev, M. C. Chen, D. Popmintchev, P. Arpin, S. Brown, S. Ališauskas, G. Andriukaitis, T. Balčiunas, O. D. Mücke, A. Pugzlys, A. Baltuška, B. Shim, S. E. Schrauth, A. Gaeta, C. Hernández-García, L. Plaja, A. Becker, A. Jaron-Becker, M. M. Murnane, and H. C. Kapteyn, “Bright coherent ultrahigh harmonics in the kev x-ray regime from mid-infrared femtosecond lasers,” Science 336, 1287–1291 (2012).
[Crossref] [PubMed]

G. Andriukaitis, T. Balčiūnas, S. Ališauskas, A. Pugžlys, A. Baltuška, T. Popmintchev, M.-C. Chen, M. M. Murnane, and H. C. Kapteyn, “90 gw peak power few-cycle mid-infrared pulses from an optical parametric amplifier,” Opt. letters 36, 2755–2757 (2011).
[Crossref]

Amorim, L. D.

F. Albert, N. Lemos, J. L. Shaw, P. M. King, B. B. Pollock, C. Goyon, W. Schumaker, A. M. Saunders, K. A. Marsh, A. Pak, J. E. Ralph, J. L. Martins, L. D. Amorim, R. W. Falcone, S. H. Glenzer, J. D. Moody, and C. Joshi, “Betatron x-ray radiation in the self-modulated laser wakefield acceleration regime: Prospects for a novel probe at large scale laser facilities,” Nucl. Fusion 59, 032003 (2019).
[Crossref]

Andriukaitis, G.

T. Popmintchev, M. C. Chen, D. Popmintchev, P. Arpin, S. Brown, S. Ališauskas, G. Andriukaitis, T. Balčiunas, O. D. Mücke, A. Pugzlys, A. Baltuška, B. Shim, S. E. Schrauth, A. Gaeta, C. Hernández-García, L. Plaja, A. Becker, A. Jaron-Becker, M. M. Murnane, and H. C. Kapteyn, “Bright coherent ultrahigh harmonics in the kev x-ray regime from mid-infrared femtosecond lasers,” Science 336, 1287–1291 (2012).
[Crossref] [PubMed]

G. Andriukaitis, T. Balčiūnas, S. Ališauskas, A. Pugžlys, A. Baltuška, T. Popmintchev, M.-C. Chen, M. M. Murnane, and H. C. Kapteyn, “90 gw peak power few-cycle mid-infrared pulses from an optical parametric amplifier,” Opt. letters 36, 2755–2757 (2011).
[Crossref]

Arber, T. D.

T. D. Arber, K. Bennett, C. S. Brady, A. Lawrence-Douglas, M. G. Ramsay, N. J. Sircombe, P. Gillies, R. G. Evans, H. Schmitz, A. R. Bell, and C. P. Ridgers, “Contemporary particle-in-cell approach to laser-plasma modelling,” Plasma Phys. Control. Fusion 57, 113001 (2015).
[Crossref]

Arpin, P.

T. Popmintchev, M. C. Chen, D. Popmintchev, P. Arpin, S. Brown, S. Ališauskas, G. Andriukaitis, T. Balčiunas, O. D. Mücke, A. Pugzlys, A. Baltuška, B. Shim, S. E. Schrauth, A. Gaeta, C. Hernández-García, L. Plaja, A. Becker, A. Jaron-Becker, M. M. Murnane, and H. C. Kapteyn, “Bright coherent ultrahigh harmonics in the kev x-ray regime from mid-infrared femtosecond lasers,” Science 336, 1287–1291 (2012).
[Crossref] [PubMed]

Assion, A.

A. Assion, T. Baumert, M. Bergt, T. Brixner, B. Kiefer, V. Seyfried, M. Strehle, and G. Gerber, “Control of chemical reactions by feedback-optimized phase-shaped femtosecond laser pulses,” Science 282, 919–922 (1998).
[Crossref] [PubMed]

Atanasov, R.

A. Haché, Y. Kostoulas, R. Atanasov, J. Hughes, J. Sipe, and H. Van Driel, “Observation of coherently controlled photocurrent in unbiased, bulk gaas,” Phys. review letters 78, 306 (1997).
[Crossref]

Bahk, S.-W.

S.-W. Bahk, P. Rousseau, T. Planchon, V. Chvykov, G. Kalintchenko, A. Maksimchuk, G. Mourou, and V. Yanovsky, “Generation and characterization of the highest laser intensities (10 22 w/cm 2),” Opt. letters 29, 2837–2839 (2004).
[Crossref]

Baird, C. D.

M. J. Streeter, S. J. Dann, J. D. Scott, C. D. Baird, C. D. Murphy, S. Eardley, R. A. Smith, S. Rozario, J. N. Gruse, S. P. Mangles, Z. Najmudin, S. Tata, M. Krishnamurthy, S. V. Rahul, D. Hazra, P. Pourmoussavi, J. Osterhoff, J. Hah, N. Bourgeois, C. Thornton, C. D. Gregory, C. J. Hooker, O. Chekhlov, S. J. Hawkes, B. Parry, V. A. Marshall, Y. Tang, E. Springate, P. P. Rajeev, A. G. Thomas, and D. R. Symes, “Temporal feedback control of high-intensity laser pulses to optimize ultrafast heating of atomic clusters,” Appl. Phys. Lett. 112, 244101 (2018).
[Crossref]

Balciunas, T.

T. Popmintchev, M. C. Chen, D. Popmintchev, P. Arpin, S. Brown, S. Ališauskas, G. Andriukaitis, T. Balčiunas, O. D. Mücke, A. Pugzlys, A. Baltuška, B. Shim, S. E. Schrauth, A. Gaeta, C. Hernández-García, L. Plaja, A. Becker, A. Jaron-Becker, M. M. Murnane, and H. C. Kapteyn, “Bright coherent ultrahigh harmonics in the kev x-ray regime from mid-infrared femtosecond lasers,” Science 336, 1287–1291 (2012).
[Crossref] [PubMed]

G. Andriukaitis, T. Balčiūnas, S. Ališauskas, A. Pugžlys, A. Baltuška, T. Popmintchev, M.-C. Chen, M. M. Murnane, and H. C. Kapteyn, “90 gw peak power few-cycle mid-infrared pulses from an optical parametric amplifier,” Opt. letters 36, 2755–2757 (2011).
[Crossref]

Baltuška, A.

D. Woodbury, L. Feder, V. Shumakova, C. Gollner, R. Schwartz, B. Miao, F. Salehi, A. Korolov, A. Pugžlys, A. Baltuška, and H. M. Milchberg, “Laser wakefield acceleration with mid-ir laser pulses,” Opt. letters 43, 1131–1134 (2018).
[Crossref]

J. Weisshaupt, V. Juvé, M. Holtz, S. Ku, M. Woerner, T. Elsaesser, S. Ališauskas, A. Pugžlys, and A. Baltuška, “High-brightness table-top hard x-ray source driven by sub-100-femtosecond mid-infrared pulses,” Nat. Photonics 8, 927 (2014).
[Crossref]

T. Popmintchev, M. C. Chen, D. Popmintchev, P. Arpin, S. Brown, S. Ališauskas, G. Andriukaitis, T. Balčiunas, O. D. Mücke, A. Pugzlys, A. Baltuška, B. Shim, S. E. Schrauth, A. Gaeta, C. Hernández-García, L. Plaja, A. Becker, A. Jaron-Becker, M. M. Murnane, and H. C. Kapteyn, “Bright coherent ultrahigh harmonics in the kev x-ray regime from mid-infrared femtosecond lasers,” Science 336, 1287–1291 (2012).
[Crossref] [PubMed]

G. Andriukaitis, T. Balčiūnas, S. Ališauskas, A. Pugžlys, A. Baltuška, T. Popmintchev, M.-C. Chen, M. M. Murnane, and H. C. Kapteyn, “90 gw peak power few-cycle mid-infrared pulses from an optical parametric amplifier,” Opt. letters 36, 2755–2757 (2011).
[Crossref]

Baumert, T.

A. Assion, T. Baumert, M. Bergt, T. Brixner, B. Kiefer, V. Seyfried, M. Strehle, and G. Gerber, “Control of chemical reactions by feedback-optimized phase-shaped femtosecond laser pulses,” Science 282, 919–922 (1998).
[Crossref] [PubMed]

Becker, A.

T. Popmintchev, M. C. Chen, D. Popmintchev, P. Arpin, S. Brown, S. Ališauskas, G. Andriukaitis, T. Balčiunas, O. D. Mücke, A. Pugzlys, A. Baltuška, B. Shim, S. E. Schrauth, A. Gaeta, C. Hernández-García, L. Plaja, A. Becker, A. Jaron-Becker, M. M. Murnane, and H. C. Kapteyn, “Bright coherent ultrahigh harmonics in the kev x-ray regime from mid-infrared femtosecond lasers,” Science 336, 1287–1291 (2012).
[Crossref] [PubMed]

Bell, A. R.

T. D. Arber, K. Bennett, C. S. Brady, A. Lawrence-Douglas, M. G. Ramsay, N. J. Sircombe, P. Gillies, R. G. Evans, H. Schmitz, A. R. Bell, and C. P. Ridgers, “Contemporary particle-in-cell approach to laser-plasma modelling,” Plasma Phys. Control. Fusion 57, 113001 (2015).
[Crossref]

Bennett, K.

T. D. Arber, K. Bennett, C. S. Brady, A. Lawrence-Douglas, M. G. Ramsay, N. J. Sircombe, P. Gillies, R. G. Evans, H. Schmitz, A. R. Bell, and C. P. Ridgers, “Contemporary particle-in-cell approach to laser-plasma modelling,” Plasma Phys. Control. Fusion 57, 113001 (2015).
[Crossref]

Bergt, M.

A. Assion, T. Baumert, M. Bergt, T. Brixner, B. Kiefer, V. Seyfried, M. Strehle, and G. Gerber, “Control of chemical reactions by feedback-optimized phase-shaped femtosecond laser pulses,” Science 282, 919–922 (1998).
[Crossref] [PubMed]

Bonadeo, N. H.

N. H. Bonadeo, J. Erland, D. Gammon, D. Park, D. Katzer, and D. Steel, “Coherent optical control of the quantum state of a single quantum dot,” Science 282, 1473–1476 (1998).
[Crossref] [PubMed]

Bourgeois, N.

M. J. Streeter, S. J. Dann, J. D. Scott, C. D. Baird, C. D. Murphy, S. Eardley, R. A. Smith, S. Rozario, J. N. Gruse, S. P. Mangles, Z. Najmudin, S. Tata, M. Krishnamurthy, S. V. Rahul, D. Hazra, P. Pourmoussavi, J. Osterhoff, J. Hah, N. Bourgeois, C. Thornton, C. D. Gregory, C. J. Hooker, O. Chekhlov, S. J. Hawkes, B. Parry, V. A. Marshall, Y. Tang, E. Springate, P. P. Rajeev, A. G. Thomas, and D. R. Symes, “Temporal feedback control of high-intensity laser pulses to optimize ultrafast heating of atomic clusters,” Appl. Phys. Lett. 112, 244101 (2018).
[Crossref]

Brady, C. S.

T. D. Arber, K. Bennett, C. S. Brady, A. Lawrence-Douglas, M. G. Ramsay, N. J. Sircombe, P. Gillies, R. G. Evans, H. Schmitz, A. R. Bell, and C. P. Ridgers, “Contemporary particle-in-cell approach to laser-plasma modelling,” Plasma Phys. Control. Fusion 57, 113001 (2015).
[Crossref]

Brixner, T.

A. Assion, T. Baumert, M. Bergt, T. Brixner, B. Kiefer, V. Seyfried, M. Strehle, and G. Gerber, “Control of chemical reactions by feedback-optimized phase-shaped femtosecond laser pulses,” Science 282, 919–922 (1998).
[Crossref] [PubMed]

Brown, S.

T. Popmintchev, M. C. Chen, D. Popmintchev, P. Arpin, S. Brown, S. Ališauskas, G. Andriukaitis, T. Balčiunas, O. D. Mücke, A. Pugzlys, A. Baltuška, B. Shim, S. E. Schrauth, A. Gaeta, C. Hernández-García, L. Plaja, A. Becker, A. Jaron-Becker, M. M. Murnane, and H. C. Kapteyn, “Bright coherent ultrahigh harmonics in the kev x-ray regime from mid-infrared femtosecond lasers,” Science 336, 1287–1291 (2012).
[Crossref] [PubMed]

Bruhwiler, D.

C. Geddes, C. Toth, J. Van Tilborg, E. Esarey, C. Schroeder, D. Bruhwiler, C. Nieter, J. Cary, and W. Leemans, “High-quality electron beams from a laser wakefield accelerator using plasma-channel guiding,” Nature 431, 538 (2004).
[Crossref] [PubMed]

Burger, M.

Burgy, F.

J. Faure, Y. Glinec, A. Pukhov, S. Kiselev, S. Gordienko, E. Lefebvre, J.-P. Rousseau, F. Burgy, and V. Malka, “A laser–plasma accelerator producing monoenergetic electron beams,” Nature 431, 541 (2004).
[Crossref] [PubMed]

Burza, M.

S. P. Mangles, G. Genoud, S. Kneip, M. Burza, K. Cassou, B. Cros, N. P. Dover, C. Kamperidis, Z. Najmudin, A. Persson, J. Schreiber, F. Wojda, and C. G. Wahlström, “Controlling the spectrum of x-rays generated in a laser-plasma accelerator by tailoring the laser wavefront,” Appl. Phys. Lett. 95, 181106 (2009).
[Crossref]

Bussolino, G.

G. Bussolino, A. Faenov, A. Giulietti, D. Giulietti, P. Koester, L. Labate, T. Levato, T. Pikuz, and L. Gizzi, “Electron radiography using a table-top laser-cluster plasma accelerator,” J. Phys. D: Appl. Phys. 46, 245501 (2013).
[Crossref]

Carias, C.

S. P. Mangles, B. R. Walton, Z. Najmudin, A. E. Dangor, K. Krushelnick, V. Malka, M. Manclossi, N. Lopes, C. Carias, G. Mendes, and F. Dorchies, “Table-top laser-plasma acceleration as an electron radiography source,” Laser Part. Beams 24, 185–190 (2006).
[Crossref]

Cary, J.

C. Geddes, C. Toth, J. Van Tilborg, E. Esarey, C. Schroeder, D. Bruhwiler, C. Nieter, J. Cary, and W. Leemans, “High-quality electron beams from a laser wakefield accelerator using plasma-channel guiding,” Nature 431, 538 (2004).
[Crossref] [PubMed]

Cassou, K.

S. P. Mangles, G. Genoud, S. Kneip, M. Burza, K. Cassou, B. Cros, N. P. Dover, C. Kamperidis, Z. Najmudin, A. Persson, J. Schreiber, F. Wojda, and C. G. Wahlström, “Controlling the spectrum of x-rays generated in a laser-plasma accelerator by tailoring the laser wavefront,” Appl. Phys. Lett. 95, 181106 (2009).
[Crossref]

Chang, Z.

Y. Wang, T. Guo, J. Li, J. Zhao, Y. Yin, X. Ren, J. Li, Y. Wu, M. Weidman, Z. Chang, M. F. Jager, C. J. Kaplan, R. Geneaux, C. Ott, D. M. Neumark, and S. R. Leone, “Enhanced high-order harmonic generation driven by a wavefront corrected high-energy laser,” J. Phys. B: At. Mol. Opt. Phys. 51, 134005 (2018).
[Crossref]

O. Albert, H. Wang, D. Liu, Z. Chang, and G. Mourou, “Generation of relativistic intensity pulses at a kilohertz repetition rate,” Opt. Lett. 25, 1125–1127 (2000).
[Crossref]

Chekhlov, O.

M. J. Streeter, S. J. Dann, J. D. Scott, C. D. Baird, C. D. Murphy, S. Eardley, R. A. Smith, S. Rozario, J. N. Gruse, S. P. Mangles, Z. Najmudin, S. Tata, M. Krishnamurthy, S. V. Rahul, D. Hazra, P. Pourmoussavi, J. Osterhoff, J. Hah, N. Bourgeois, C. Thornton, C. D. Gregory, C. J. Hooker, O. Chekhlov, S. J. Hawkes, B. Parry, V. A. Marshall, Y. Tang, E. Springate, P. P. Rajeev, A. G. Thomas, and D. R. Symes, “Temporal feedback control of high-intensity laser pulses to optimize ultrafast heating of atomic clusters,” Appl. Phys. Lett. 112, 244101 (2018).
[Crossref]

Chen, M. C.

T. Popmintchev, M. C. Chen, D. Popmintchev, P. Arpin, S. Brown, S. Ališauskas, G. Andriukaitis, T. Balčiunas, O. D. Mücke, A. Pugzlys, A. Baltuška, B. Shim, S. E. Schrauth, A. Gaeta, C. Hernández-García, L. Plaja, A. Becker, A. Jaron-Becker, M. M. Murnane, and H. C. Kapteyn, “Bright coherent ultrahigh harmonics in the kev x-ray regime from mid-infrared femtosecond lasers,” Science 336, 1287–1291 (2012).
[Crossref] [PubMed]

Chen, M.-C.

G. Andriukaitis, T. Balčiūnas, S. Ališauskas, A. Pugžlys, A. Baltuška, T. Popmintchev, M.-C. Chen, M. M. Murnane, and H. C. Kapteyn, “90 gw peak power few-cycle mid-infrared pulses from an optical parametric amplifier,” Opt. letters 36, 2755–2757 (2011).
[Crossref]

Chen, Y.

C. Yu, J. Liu, W. Wang, W. Li, R. Qi, Z. Zhang, Z. Qin, J. Liu, M. Fang, K. Feng, Y. Wu, L. Ke, Y. Chen, C. Wang, Y. Xu, Y. Leng, C. Xia, R. Li, and Z. Xu, “Enhanced betatron radiation by steering a laser-driven plasma wakefield with a tilted shock front,” Appl. Phys. Lett. 112, 133503 (2018).
[Crossref]

Chvykov, V.

S.-W. Bahk, P. Rousseau, T. Planchon, V. Chvykov, G. Kalintchenko, A. Maksimchuk, G. Mourou, and V. Yanovsky, “Generation and characterization of the highest laser intensities (10 22 w/cm 2),” Opt. letters 29, 2837–2839 (2004).
[Crossref]

Collier, J. L.

S. P. Mangles, C. D. Murphy, Z. Najmudin, A. G. Thomas, J. L. Collier, A. E. Dangor, E. J. Divall, P. S. Foster, J. G. Gallacher, C. J. Hooker, D. A. Jaroszynski, A. J. Langley, W. B. Mori, P. A. Norreys, F. S. Tsung, R. Viskup, B. R. Walton, and K. Krushelnick, “Monoenergetic beams of relativistic electrons from intense laser-plasma interactions,” Nature 431, 535 (2004).
[Crossref] [PubMed]

Corde, S.

J. Ferri, X. Davoine, S. Fourmaux, J. Kieffer, S. Corde, K. T. Phuoc, and A. Lifschitz, “Effect of experimental laser imperfections on laser wakefield acceleration and betatron source,” Sci. reports 6, 27846 (2016).
[Crossref]

Cros, B.

S. P. Mangles, G. Genoud, S. Kneip, M. Burza, K. Cassou, B. Cros, N. P. Dover, C. Kamperidis, Z. Najmudin, A. Persson, J. Schreiber, F. Wojda, and C. G. Wahlström, “Controlling the spectrum of x-rays generated in a laser-plasma accelerator by tailoring the laser wavefront,” Appl. Phys. Lett. 95, 181106 (2009).
[Crossref]

Dangor, A. E.

S. P. Mangles, B. R. Walton, Z. Najmudin, A. E. Dangor, K. Krushelnick, V. Malka, M. Manclossi, N. Lopes, C. Carias, G. Mendes, and F. Dorchies, “Table-top laser-plasma acceleration as an electron radiography source,” Laser Part. Beams 24, 185–190 (2006).
[Crossref]

S. P. Mangles, C. D. Murphy, Z. Najmudin, A. G. Thomas, J. L. Collier, A. E. Dangor, E. J. Divall, P. S. Foster, J. G. Gallacher, C. J. Hooker, D. A. Jaroszynski, A. J. Langley, W. B. Mori, P. A. Norreys, F. S. Tsung, R. Viskup, B. R. Walton, and K. Krushelnick, “Monoenergetic beams of relativistic electrons from intense laser-plasma interactions,” Nature 431, 535 (2004).
[Crossref] [PubMed]

Dann, S. J.

M. J. Streeter, S. J. Dann, J. D. Scott, C. D. Baird, C. D. Murphy, S. Eardley, R. A. Smith, S. Rozario, J. N. Gruse, S. P. Mangles, Z. Najmudin, S. Tata, M. Krishnamurthy, S. V. Rahul, D. Hazra, P. Pourmoussavi, J. Osterhoff, J. Hah, N. Bourgeois, C. Thornton, C. D. Gregory, C. J. Hooker, O. Chekhlov, S. J. Hawkes, B. Parry, V. A. Marshall, Y. Tang, E. Springate, P. P. Rajeev, A. G. Thomas, and D. R. Symes, “Temporal feedback control of high-intensity laser pulses to optimize ultrafast heating of atomic clusters,” Appl. Phys. Lett. 112, 244101 (2018).
[Crossref]

Davoine, X.

J. Ferri, X. Davoine, S. Fourmaux, J. Kieffer, S. Corde, K. T. Phuoc, and A. Lifschitz, “Effect of experimental laser imperfections on laser wakefield acceleration and betatron source,” Sci. reports 6, 27846 (2016).
[Crossref]

Dawson, J. M.

T. Tajima and J. M. Dawson, “Laser electron accelerator,” Phys. Rev. Lett. 43, 267 (1979).
[Crossref]

De Waele, V.

Y. Glinec, J. Faure, A. Guemnie-Tafo, V. Malka, H. Monard, J. Larbre, V. De Waele, J. Marignier, and M. Mostafavi, “Absolute calibration for a broad range single shot electron spectrometer,” Rev. scientific instruments 77, 103301 (2006).
[Crossref]

Deng, A. H.

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Figures (8)

Fig. 1
Fig. 1 Schematic of the setup: Deformable mirror: AOA Xenitics 37-channel 2 inch; OAP: f/2.7; Gas jet: 150μm orifice diameter nozzle; CCD: The Imaging Source DMK41BU02.H Charged Particle Device (CCD) camera; Lanex: LANEX Regular screen.
Fig. 2
Fig. 2 Improvement charts using different figure of merit (FOM) functions: (a) total charge collected in the region of interest on CCD image after background subtraction; (b) the fitness function defined in Eq. (2) with n=2. Both optimizations started from initializing the deformable mirror to a flat surface. The shaded area refers to the variation of 5 best genes in each iteration. The number of iteration was limited by the experimental time considering the system repetition rate was as low as 1 Hz. The figure of merit values were calibrated to real units taking into account the geometry and the efficiency of optics, LANEX [36] and CCD.
Fig. 3
Fig. 3 Comparison of electron beam energy spectra: (a)–(c) before and after optimization; (d),(e) at front, center and back of the gas jet. 20 consecutive images were taken in each case. The shot-to-shot variation is shown in (a)–(c) while the statistic mean was shown in (d),(e). Examples of raw spectra with non-thermal peak features are shown in (f), in which the optimal laser wavefront found by the genetic algorithm was focused at back, center and front of the gas jet. Note that peaks do not occur on all shots.
Fig. 4
Fig. 4 Electron beam profile optimization using the image moment as figure of merit, defined in Eq. (2). (a) and (b): 30 consecutive raw images before and after optimization. The circular edge, due to a collimation tube in front of the LANEX, corresponds to a solid angle of 550 mrad. (c) – (f) are the visualization of beam quality in terms of total beam charge, peak charge density, divergence angle and beam pointing, respectively. Each dot represents one shot.
Fig. 5
Fig. 5 Reconstruct the laser wavefront propagation for three cases. (a–c): wavefront for the optimal electron beam, (d–f): wavefront from a flat mirror surface, and (g–i): perfect Gaussian wavefront. Wavefronts leaving the DM, propagating 4.5m and focused by the OAP are shown in the first, second and third column. First 50 Zernike coefficients are included in the reconstruction.
Fig. 6
Fig. 6 Laser field evolution and electron beam qualities with different laser wavefronts in PIC simulations. (a) Evolution of peak laser field strength with different wavefronts in vacuum and plasma, respectively. (b) and (c) Electron spectra and angular distributions at the end of the simulation (t = 2 ps) with different laser wavefronts and the same plasma profile showing in (a).
Fig. 7
Fig. 7 Snapshot for plasma density and electron beam distribution with (a) Gaussian, (b) flat mirror and (c) optimized wavefront at the same time, t = 1 ps. Self-injection has occurred with optimized wavefront in (c) while not in the other two cases.
Fig. 8
Fig. 8 Snapshots of PIC simulations with different wavefronts. Laser field distribution at t = 1.5 ps for (a) Gaussian, (c) Flat mirror and (e) Optimized wavefront, respectively. Plasma density distribution at t = 1.64 ps for (b) Gaussian, (d) Flat mirror and (f) Optimized wavefront, respectively. Spatial distribution of accelerated electron macro-particles are overlaid on the plasma density distribution where color scale represents longitudinal momentum of the particles.

Equations (6)

Equations on this page are rendered with MathJax. Learn more.

P cr = 17.4 n cr / n e [ GW ] F p = m e γ c 2 ( a 2 / 2 )
FOM = ( i , j ) r i j r 0 I i j | r i j r 0 | n
Δ ϕ = j = 1 200 A j Z j
A j = i = 1 37 C i j V i
ϕ = ϕ laser + 2 × ϕ SHG ϕ Gaussian
ϕ opt = ϕ laser + 2 × ϕ DM

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