ZD!"D2R.R. Lucchese(1-3[) T. Mazza(2-3[/ E. Gryzlova(2-3[)
\]^+K2 Chuncheng Wang (4-12 [/
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(a) NeAr
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1P)
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2+(3s
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*Ne
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2+(3p
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(c) NeAr
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2P)4p
1S)
*Ne+(2p
-1)-Ar
2+(3p
-23P) (d) NeAr
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2D)4d
3D,
1P,
3P)
*Ne
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(b) ` 3 ~'(uþzk«a~
+§ 3 '( ICD ÀÁ`E!"j«,-z.í:
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[1.1] T. Ouchi et al. Phys. Rev. A (in press).
[1.2] T. Ouchi et al. Submitted to Phys. Rev. Lett..
Fig. 1.1. Kinetic energy distribution for
Ne
+-Ar
2+.!"#$% &'()*+,%-.(ICD/01ETMD/0
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[2.1] K. Sakai et al. Phys. Rev. Lett. 106, 033401 (2011).
Fig. 2.2. Relationship between the ETMD electron energy and the total KER for the Ar
2+-Ar
2+fragmentation of the argon dimer.
See the caption of Fig. 2.1 for the details.
Fig. 2.1. (a) Relationship between the ICD electron energy and the total KER for the Ar
3+-Ar
+fragmentation of the argon dimer.
(b) Kinetic energy distribution of the ICD electrons detected in coincidence with Ar
3+-Ar
+pairs and in coincidence with Ar
+-Ar
+ion pairs are given by the solid line and the dashed line, respectively. The latter is scaled to match the former at high energy.
The latter gives the background coming
from the false co incidences because the
true electron signals in coincidence with
Ar
+-Ar
+ion pairs are expected to be zero
in this energy region. The result of the
background subtrac-tion is given by the
dots. (c) KER distribution between Ar
3+-Ar
+.
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aè:)î;!"sZ0M[3.1] M. Okunishi et al. Phys. Rev. Lett. 106, 063001 (2011).
Fig. 3.1. Comparison of experimentally extracted
electron-ion elastic scatting differential cross sectelectron-ions for O
2and
CO
2molecules with theoretical differential cross sections.
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[4.1] H. Fukuzawa et al. J. Phys. B
43,111001 (2010).
[4.2] R. Ma et al. to be submitted.
Fig. 4.1:
Photoelectron spectra around 20 eV: (a) experiment;(b) theory. The theoretical spectra were convoluted by a Gaussian function with the FWHM of 0.4 eV. Experimental and theoretical results are normalized to unity in the maximum.
0.2 0.4
0.6 0.8
1
30
210
60
240
90
270 120
300 150
330
180 0
Fig. 4.2: Angular distribution of the second photoelectron
e
2-emitted via resonant three photon double ionization at
hv=21.45 eV. 1
ststep, Ar + hv -> Ar
+(3p
5)+e
1-; 2
ndstep,
Ar
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5) + hv -> Ar
+(3p
43d),; 3
rdstep, Ar
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43d) + hv
-> Ar
+(3p
4 1S)+e
2-.
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[5.1] M. Tashiro et al. J. Chem. Phys.
132,184302 (2010).
[5.2] M. Tashiro et al. Chem. Phys. Lett. 496, 217 (2010).
[5.3] O. Takahashi et al. Chem. Phys. (in press).
[5.4] O. Takahashi et al. (in preparation).
[5.5] J.H.D. Eland et al. Phys. Rev. Lett.
105, 213005 (2010).
[5.6] P. Linusson et al. Phys. Rev. A
83,022506 (2011).
Fig. 5.1. Schematic picture of X-ray two-photon pho-toelectron spectroscopy and X-ray two-photon Auger electron spectroscopy. In this picture, it is assumed that the second photon is absorbed before Auger decay takes place.
Fig. 5.2. Nucleobases to be studied.
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