Time-dependent Schrödinger approach to sub-barrier fission
Abstract The time-dependent Schrödinger equation for the fission of213At through a one-dimensional potential barrier was solved numerically within a finite spatial grid. Several initial quasi-stationary vibrational states at and below the top of the barrier were considered. The time dependence of th...
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1994 |
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| Umfang: |
3 |
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| Reproduktion: |
Springer Online Journal Archives 1860-2002 |
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| Übergeordnetes Werk: |
in: The European physical journal - 1998, 349(1994) vom: März/Apr., Seite 353-355 |
| Übergeordnetes Werk: |
volume:349 ; year:1994 ; month:03/04 ; pages:353-355 ; extent:3 |
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NLEJ199011087 |
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| 245 | 1 | 0 | |a Time-dependent Schrödinger approach to sub-barrier fission |
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| 520 | |a Abstract The time-dependent Schrödinger equation for the fission of213At through a one-dimensional potential barrier was solved numerically within a finite spatial grid. Several initial quasi-stationary vibrational states at and below the top of the barrier were considered. The time dependence of the decay rate γ(t) was calculated. The non-exponential evolution of the process in the very early stages (≦10−20 s) differs considerably from the asymptotic (stationary) one. Fission is therefore delayed by the sum of this preexponential time, of the tunneling time and of the time necessary for the descent from the outer turning point to the scission point. These non-dissipative quantum times play the same role as the classical transient times usually included in the analyses of experimental data on pre-scission emission of light particles andγ rays. | ||
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| 700 | 1 | |a Serot, O. |4 oth | |
| 700 | 1 | |a Strottman, D. |4 oth | |
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(DE-627)NLEJ199011087 DE-627 ger DE-627 rakwb eng Time-dependent Schrödinger approach to sub-barrier fission 1994 3 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract The time-dependent Schrödinger equation for the fission of213At through a one-dimensional potential barrier was solved numerically within a finite spatial grid. Several initial quasi-stationary vibrational states at and below the top of the barrier were considered. The time dependence of the decay rate γ(t) was calculated. The non-exponential evolution of the process in the very early stages (≦10−20 s) differs considerably from the asymptotic (stationary) one. Fission is therefore delayed by the sum of this preexponential time, of the tunneling time and of the time necessary for the descent from the outer turning point to the scission point. These non-dissipative quantum times play the same role as the classical transient times usually included in the analyses of experimental data on pre-scission emission of light particles andγ rays. Springer Online Journal Archives 1860-2002 Carjan, N. oth Serot, O. oth Strottman, D. oth in The European physical journal 1998 349(1994) vom: März/Apr., Seite 353-355 (DE-627)NLEJ188987754 (DE-600)1459066-9 1434-601X nnns volume:349 year:1994 month:03/04 pages:353-355 extent:3 http://dx.doi.org/10.1007/BF01288994 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 349 1994 3/4 353-355 3 |
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(DE-627)NLEJ199011087 DE-627 ger DE-627 rakwb eng Time-dependent Schrödinger approach to sub-barrier fission 1994 3 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract The time-dependent Schrödinger equation for the fission of213At through a one-dimensional potential barrier was solved numerically within a finite spatial grid. Several initial quasi-stationary vibrational states at and below the top of the barrier were considered. The time dependence of the decay rate γ(t) was calculated. The non-exponential evolution of the process in the very early stages (≦10−20 s) differs considerably from the asymptotic (stationary) one. Fission is therefore delayed by the sum of this preexponential time, of the tunneling time and of the time necessary for the descent from the outer turning point to the scission point. These non-dissipative quantum times play the same role as the classical transient times usually included in the analyses of experimental data on pre-scission emission of light particles andγ rays. Springer Online Journal Archives 1860-2002 Carjan, N. oth Serot, O. oth Strottman, D. oth in The European physical journal 1998 349(1994) vom: März/Apr., Seite 353-355 (DE-627)NLEJ188987754 (DE-600)1459066-9 1434-601X nnns volume:349 year:1994 month:03/04 pages:353-355 extent:3 http://dx.doi.org/10.1007/BF01288994 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 349 1994 3/4 353-355 3 |
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(DE-627)NLEJ199011087 DE-627 ger DE-627 rakwb eng Time-dependent Schrödinger approach to sub-barrier fission 1994 3 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract The time-dependent Schrödinger equation for the fission of213At through a one-dimensional potential barrier was solved numerically within a finite spatial grid. Several initial quasi-stationary vibrational states at and below the top of the barrier were considered. The time dependence of the decay rate γ(t) was calculated. The non-exponential evolution of the process in the very early stages (≦10−20 s) differs considerably from the asymptotic (stationary) one. Fission is therefore delayed by the sum of this preexponential time, of the tunneling time and of the time necessary for the descent from the outer turning point to the scission point. These non-dissipative quantum times play the same role as the classical transient times usually included in the analyses of experimental data on pre-scission emission of light particles andγ rays. Springer Online Journal Archives 1860-2002 Carjan, N. oth Serot, O. oth Strottman, D. oth in The European physical journal 1998 349(1994) vom: März/Apr., Seite 353-355 (DE-627)NLEJ188987754 (DE-600)1459066-9 1434-601X nnns volume:349 year:1994 month:03/04 pages:353-355 extent:3 http://dx.doi.org/10.1007/BF01288994 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 349 1994 3/4 353-355 3 |
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(DE-627)NLEJ199011087 DE-627 ger DE-627 rakwb eng Time-dependent Schrödinger approach to sub-barrier fission 1994 3 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract The time-dependent Schrödinger equation for the fission of213At through a one-dimensional potential barrier was solved numerically within a finite spatial grid. Several initial quasi-stationary vibrational states at and below the top of the barrier were considered. The time dependence of the decay rate γ(t) was calculated. The non-exponential evolution of the process in the very early stages (≦10−20 s) differs considerably from the asymptotic (stationary) one. Fission is therefore delayed by the sum of this preexponential time, of the tunneling time and of the time necessary for the descent from the outer turning point to the scission point. These non-dissipative quantum times play the same role as the classical transient times usually included in the analyses of experimental data on pre-scission emission of light particles andγ rays. Springer Online Journal Archives 1860-2002 Carjan, N. oth Serot, O. oth Strottman, D. oth in The European physical journal 1998 349(1994) vom: März/Apr., Seite 353-355 (DE-627)NLEJ188987754 (DE-600)1459066-9 1434-601X nnns volume:349 year:1994 month:03/04 pages:353-355 extent:3 http://dx.doi.org/10.1007/BF01288994 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 349 1994 3/4 353-355 3 |
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(DE-627)NLEJ199011087 DE-627 ger DE-627 rakwb eng Time-dependent Schrödinger approach to sub-barrier fission 1994 3 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract The time-dependent Schrödinger equation for the fission of213At through a one-dimensional potential barrier was solved numerically within a finite spatial grid. Several initial quasi-stationary vibrational states at and below the top of the barrier were considered. The time dependence of the decay rate γ(t) was calculated. The non-exponential evolution of the process in the very early stages (≦10−20 s) differs considerably from the asymptotic (stationary) one. Fission is therefore delayed by the sum of this preexponential time, of the tunneling time and of the time necessary for the descent from the outer turning point to the scission point. These non-dissipative quantum times play the same role as the classical transient times usually included in the analyses of experimental data on pre-scission emission of light particles andγ rays. Springer Online Journal Archives 1860-2002 Carjan, N. oth Serot, O. oth Strottman, D. oth in The European physical journal 1998 349(1994) vom: März/Apr., Seite 353-355 (DE-627)NLEJ188987754 (DE-600)1459066-9 1434-601X nnns volume:349 year:1994 month:03/04 pages:353-355 extent:3 http://dx.doi.org/10.1007/BF01288994 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 349 1994 3/4 353-355 3 |
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Abstract The time-dependent Schrödinger equation for the fission of213At through a one-dimensional potential barrier was solved numerically within a finite spatial grid. Several initial quasi-stationary vibrational states at and below the top of the barrier were considered. The time dependence of the decay rate γ(t) was calculated. The non-exponential evolution of the process in the very early stages (≦10−20 s) differs considerably from the asymptotic (stationary) one. Fission is therefore delayed by the sum of this preexponential time, of the tunneling time and of the time necessary for the descent from the outer turning point to the scission point. These non-dissipative quantum times play the same role as the classical transient times usually included in the analyses of experimental data on pre-scission emission of light particles andγ rays. |
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Abstract The time-dependent Schrödinger equation for the fission of213At through a one-dimensional potential barrier was solved numerically within a finite spatial grid. Several initial quasi-stationary vibrational states at and below the top of the barrier were considered. The time dependence of the decay rate γ(t) was calculated. The non-exponential evolution of the process in the very early stages (≦10−20 s) differs considerably from the asymptotic (stationary) one. Fission is therefore delayed by the sum of this preexponential time, of the tunneling time and of the time necessary for the descent from the outer turning point to the scission point. These non-dissipative quantum times play the same role as the classical transient times usually included in the analyses of experimental data on pre-scission emission of light particles andγ rays. |
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Abstract The time-dependent Schrödinger equation for the fission of213At through a one-dimensional potential barrier was solved numerically within a finite spatial grid. Several initial quasi-stationary vibrational states at and below the top of the barrier were considered. The time dependence of the decay rate γ(t) was calculated. The non-exponential evolution of the process in the very early stages (≦10−20 s) differs considerably from the asymptotic (stationary) one. Fission is therefore delayed by the sum of this preexponential time, of the tunneling time and of the time necessary for the descent from the outer turning point to the scission point. These non-dissipative quantum times play the same role as the classical transient times usually included in the analyses of experimental data on pre-scission emission of light particles andγ rays. |
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