· . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg...

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Page 1:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

ΣT

Page 2:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7
Page 3:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

✿ Fe– Fe

Page 4:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

D + T → n(14.1MeV) + 4He(3.5MeV)

n + 6Li → 4He(2.1MeV) + T(2.7MeV)

Page 5:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

10keV 1

Page 6:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

– T10keV

– n– t

– (J. D. Lawson, 1957)

n tt = 1014 s/cm3 for D-T fusion

110-26

T [keV]

<ssv>

[m3 /s

]

10 100

10-24

10-22

Page 7:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

–✿

– n = 1000 , t = 3 mm !–

n ~ 1014 1/cm3, tt ~ 1 s

n ~ 1025 1/cm3, tt ~ 10-11 s

Page 8:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

Elaser

✿ Elaserµ 1/n21000

100✿

Page 9:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

(1)

(2)

(3)

(4)

Page 10:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

Page 11:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

––

–––

Page 12:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

NIF : National Ignition FacilityLawrence Livermore National Laboratory✿ 2009 5 8

Page 13:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

NIF : National Ignition FacilityLawrence Livermore National Laboratory

✿ Star Trek Into Darkness

Page 14:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

NIF : National Ignition FacilityLawrence Livermore National Laboratory

Page 15:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

NIF : National Ignition FacilityLawrence Livermore National Laboratory✿ 50%

Page 16:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

NIF : National Ignition FacilityLawrence Livermore National Laboratory✿

50kJ

*O. Hurricane, invited talk at ICPP2018, Vancouver, Canada, June 4 - 8 (2018).

Page 17:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

Chirped Pulse Amplification

(1)

(2)(3)

Page 18:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

✿ (10keV) (1000 )

––

Page 19:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

Page 20:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

– XII 12 10kJ/2ns/0.53µm– 1983

Page 21:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

✿ LFEX– 4– 10kJ/10ps/1.06µm

XII

Page 22:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

FIREX

500 µm

Fast Ignition Realization EXperiment

5[keV]

Page 23:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

–ns vs. ps mm vs. µm

vs. vs. –

Page 24:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

FI3Fast Ignition Integrated Interconnecting code

Page 25:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

by✿

Page 26:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

Page 27:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

by✿

Page 28:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

(quiver)––

Plasma WakeField Acceleration (PWFA)

–Radiation Pressure Acceleration (RPA)

Target Normal Sheath field Acceleration (TNSA)

Page 29:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

ne=10ncr, IL=1020 [W/cm2]

Page 30:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

ni=25ncr, IL=1021 [W/cm2]

Page 31:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

*A. Macchi, et al., Rev. Mod. Phys. 85, 751 (2013).

Page 32:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

ne=20ncr, IL=1020 [W/cm2]

Page 33:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

/NIRS

Page 34:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

✿ 42m

/NIRS

~6m ~5m

Compact Heavy-Ion (Carbon Ion) Synchrotron

100TW Laser Target Chamber toFocus the Laser Beam

Dipole MagnetsElectron Beam Cooler

Carbon (200MeV)

RF Acceleration Cavity

100 TW Laser Ion Source

Inner Ring

RF Acceleration Cavity

Induction Accelerator

Outer Ring

RF Acceleration Cavity

RF Cavity forPhase Rotation

Page 35:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

SEM*M. Hashida, et al., Proc. 9th Symp. Microjoining and Assembly Technology in Electronics, 9, 517-522 (2003).

Page 36:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7
Page 37:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

nthin = 0.7ncr

jxe / encrc BZ [MG]ne / ncr

t = 150 [fs]

t = 200 [fs]

Page 38:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

X

Page 39:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

Page 40:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

*T. N. Kato, et al., APJ 681, L93 (2008).

jxe

BZ

ne

Page 41:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

Page 42:  · . & 4x; ! pb qyf 8ivl / (0d6#uh !qy . & $)-% e laser @7r3m j e laserµ1/n2 aeg =aeg*,'+#8i vl 1000o 1b " qy $)-% 100ts 2 ! w2 pb :vl1b#3m ! – c5n !1b z[k @7

✿ 3 3