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1
The variation, in polar representation, of the fourfold differential cross section in atomic units equation (1), scaled by 105, of the photo-double ionization of H2 obtained by the velocity gauge (left) and the length gauge (right)
The variation, in polar representation, of the fourfold differential cross section in atomic units equation (1), scaled by 105, of the photo-double ionization of H2 obtained by the velocity gauge (left) and the length gauge (right)
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The variation, in polar representation, of the fourfold differential cross section in atomic units equation (1), scaled by 105, of the photo-double ionization of H2 obtained by the velocity gauge (left) and the length gauge (right)

A A Bulychev ; O Chuluunbaatar ; A A Gusev ; B Joulakian

IOP Publishing 2014

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2
Same as in figure 7 but with a fixed value of θ1 = 60
Same as in figure 7 but with a fixed value of θ1 = 60
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Same as in figure 7 but with a fixed value of θ1 = 60

A A Bulychev ; O Chuluunbaatar ; A A Gusev ; B Joulakian

IOP Publishing 2014

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3
Same as in figure 1, for { f k}_1perp { oldsymbol epsilon }; ρ
Same as in figure 1, for { f k}_1perp { oldsymbol epsilon }; ρ
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Same as in figure 1, for { f k}_1perp { oldsymbol epsilon }; ρ

A A Bulychev ; O Chuluunbaatar ; A A Gusev ; B Joulakian

IOP Publishing 2014

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4
Same as in figure 1, for { oldsymbol epsilon }uparrow uparrow { f k}_1; k
Same as in figure 1, for { oldsymbol epsilon }uparrow uparrow { f k}_1; k
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Same as in figure 1, for { oldsymbol epsilon }uparrow uparrow { f k}_1; k

A A Bulychev ; O Chuluunbaatar ; A A Gusev ; B Joulakian

IOP Publishing 2014

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5
Same as in figure 7 but with a fixed value of θ1 = 90
Same as in figure 7 but with a fixed value of θ1 = 90
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Same as in figure 7 but with a fixed value of θ1 = 90

A A Bulychev ; O Chuluunbaatar ; A A Gusev ; B Joulakian

IOP Publishing 2014

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6
Polar representation of the variation of the TDCS in atomic units, scaled by 104, of the photo-double ionization of the 3σg orbital of N2 obtained by the velocity gauge
Polar representation of the variation of the TDCS in atomic units, scaled by 104, of the photo-double ionization of the 3σg orbital of N2 obtained by the velocity gauge
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Polar representation of the variation of the TDCS in atomic units, scaled by 104, of the photo-double ionization of the 3σg orbital of N2 obtained by the velocity gauge

A A Bulychev ; O Chuluunbaatar ; A A Gusev ; B Joulakian

IOP Publishing 2014

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7
Same as in figure 1, for { oldsymbol ho }perp { oldsymbol epsilon }
Same as in figure 1, for { oldsymbol ho }perp { oldsymbol epsilon }
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Same as in figure 1, for { oldsymbol ho }perp { oldsymbol epsilon }

A A Bulychev ; O Chuluunbaatar ; A A Gusev ; B Joulakian

IOP Publishing 2014

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8
Left: greyscale representation (colourscale in the online version) of the variation of the TDCS in atomic units equation (2), scaled by 104, of the photo-double ionization of the 3σg level of N2 obtained by the velocity gauge in terms of the two ejection angles θ1 and θ2
Left: greyscale representation (colourscale in the online version) of the variation of the TDCS in atomic units equation (2), scaled by 104, of the photo-double ionization of the 3σg level of N2 obtained by the velocity gauge in terms of the two ejection angles θ1 and θ2
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Left: greyscale representation (colourscale in the online version) of the variation of the TDCS in atomic units equation (2), scaled by 104, of the photo-double ionization of the 3σg level of N2 obtained by the velocity gauge in terms of the two ejection angles θ1 and θ2

A A Bulychev ; O Chuluunbaatar ; A A Gusev ; B Joulakian

IOP Publishing 2014

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9
The variation, in polar representation, of the FDCS in atomic units equation (2), scaled by 105, of the photo-double ionization of H2 in the velocity gauge obtained by the Turbiner–Guevara wave function
The variation, in polar representation, of the FDCS in atomic units equation (2), scaled by 105, of the photo-double ionization of H2 in the velocity gauge obtained by the Turbiner–Guevara wave function
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The variation, in polar representation, of the FDCS in atomic units equation (2), scaled by 105, of the photo-double ionization of H2 in the velocity gauge obtained by the Turbiner–Guevara wave function

A A Bulychev ; O Chuluunbaatar ; A A Gusev ; B Joulakian

IOP Publishing 2014

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10
Same as in figure 7 but with a fixed value of θ1 = 180
Same as in figure 7 but with a fixed value of θ1 = 180
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Same as in figure 7 but with a fixed value of θ1 = 180

A A Bulychev ; O Chuluunbaatar ; A A Gusev ; B Joulakian

IOP Publishing 2014

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  • Realização: ABCD-USP USP   Logos de Redes Sociais: Freepik

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