DOUBLE DIFFERENTIAL AND INTEGRAL CROSS-SECTIONS OF (p,xp) AND (p,x  )

Содержание

1. DOUBLE DIFFERENTIAL AND INTEGRAL CROSS-SECTIONS OF (p,xp) AND (p,x  )
2. GOAL Investigation of the inclusive reaction cross
3. Set-up for the transport of accelerated particles
4. Main characteristics of the telescope and target
5. Block Scheme of Registration SystemAmp.#1,2 - spectroscopic
6. Experimental integral cross sections of 27Al(3He,x) reaction, at E3He=50,5 MeV
7. Contributions of different processes to formation of inclusive spectraBertrand-Peele, Phys.Rev. C8, 1045 (1973)
8. Two-component exciton modelBasic statement:The atomic nucleus is
9. Comparison of experimental integral cross sections of
10. Comparison of experimental integral cross sections of
11. Comparison of experimental integral cross sections of
12. Comparison of experimental integral cross sections of
13. Contributions of various mechanisms forming the integral
14. Experimental double-differential cross-section of reactions 59Co(p,xp) at Ep=30.0 MeV
15. Comparison of experimental integral cross sections of 59Co(p,xp) reaction with the calculations in the exciton model
16. Скачать презентанцию

GOAL Investigation of the inclusive reaction cross sections of nuclide 3He with the material of structural elements of nuclear energy systems for transmutation of radioactive waste, energy recovery and verification of

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DOUBLE DIFFERENTIAL AND INTEGRAL CROSS-SECTIONS OF (p,xp) AND (p,x  )

Слайды и текст этой презентации

Слайд 1

DOUBLE DIFFERENTIAL AND INTEGRAL CROSS-SECTIONS OF (p,xp) AND (p,x)

REACTIONS ON 59Co NUCLEUS
AT EP=30 MeV

«SPECTRA OF LIGHT PARTICLIES

FROM INTERACTION OF 50.5 MeV 3He IONS WITH 27Al »

Zholdybaev T.K., Duisebaev A., Duisebaev B.,
Sadykov B.M., Ismailov K.M.

Institute of nuclear physics, Almaty, Kazakhstan

DOUBLE DIFFERENTIAL AND INTEGRAL CROSS-SECTIONS OF (p,xp) AND (p,x) REACTIONS ON 59Co NUCLEUSAT EP=30 MeV «SPECTRA

Слайд 2

GOAL

Investigation of the inclusive reaction cross sections of

nuclide 3He with the material of structural elements of nuclear

energy systems for transmutation of radioactive waste, energy recovery and verification of the computer codes

GOAL Investigation of the inclusive reaction cross sections of nuclide 3He with the material of structural elements

Слайд 3
Set-up for the transport of accelerated particles to the scattering

chamber

Л - quadrupole lenses, М-1, М-2 - bending magnets,
М-3

- Diluting magnet, КМ - corrective magnets,
РК – scattering chamber

Set-up for the transport of accelerated particles to the scattering chamberЛ - quadrupole lenses, М-1, М-2

Слайд 4
Main characteristics of the telescope and target

Слайд 5
Block Scheme of Registration System

Amp.#1,2 - spectroscopic amplifier; SCA#1,2 -

single channel analyser;
Coinc. - scheme of coincidences; Counter -

counter scheme;
ADC#1,2 - analog-digital converter.

Block Scheme of Registration SystemAmp.#1,2 - spectroscopic amplifier; SCA#1,2 - single channel analyser; Coinc. - scheme of

Слайд 6
Experimental integral cross sections of 27Al(3He,x) reaction, at E3He=50,5 MeV

Слайд 7Contributions of different processes to formation of inclusive spectra
Bertrand-Peele, Phys.Rev.

C8, 1045 (1973)

Слайд 8
Two-component exciton model

Basic statement:
The atomic nucleus is considered as a

system of fermions with a weak two-particle residual interaction

The excited states are classified by the number of excitons n (n = p + h - the total number of excited particles p and holes n)
All states with the same number of excitons and a priori considered to be identical
Δn = 0, ± 2

Equilibration of the composite nucleus

Two-component exciton modelBasic statement:The atomic nucleus is considered as a system of fermions with a weak two-particle

Слайд 9
Comparison of experimental integral cross sections of 27Al(3He,xp) reaction with

the calculations in the frame of exciton model

Comparison of experimental integral cross sections of 27Al(3He,xp) reaction with the calculations in the frame of exciton

Слайд 10
Comparison of experimental integral cross sections of 27Al(3He,xd) reaction with

the calculations in the frame of exciton model

Comparison of experimental integral cross sections of 27Al(3He,xd) reaction with the calculations in the frame of exciton

Слайд 11
Comparison of experimental integral cross sections of 27Al(3He,xt) reaction with

the calculations in the frame of exciton model

Comparison of experimental integral cross sections of 27Al(3He,xt) reaction with the calculations in the frame of exciton

Слайд 12
Comparison of experimental integral cross sections of 27Al(3He,x) reaction with

the calculations in the frame of exciton model

Comparison of experimental integral cross sections of 27Al(3He,x) reaction with the calculations in the frame of exciton

Слайд 13
Contributions of various mechanisms forming the integral cross-sections of reactions

(3He,xd), (3He,xt) и (3He,x) on 27Al nucleus at E3He = 50,5 MeV

Contributions of various mechanisms forming the integral cross-sections of reactions (3He,xd), (3He,xt) и (3He,x) on 27Al nucleus

Слайд 14
Experimental double-differential cross-section of reactions 59Co(p,xp) at Ep=30.0 MeV

Слайд 15
Comparison of experimental integral cross sections of 59Co(p,xp) reaction with

the calculations in the exciton model

Скачать презентацию

Разделы презентаций

DOUBLE DIFFERENTIAL AND INTEGRAL CROSS-SECTIONS OF (p,xp) AND (p,x  )

Содержание

Слайды и текст этой презентации

Слайд 1

DOUBLE DIFFERENTIAL AND INTEGRAL CROSS-SECTIONS OF (p,xp) AND (p,x)

REACTIONS ON 59Co NUCLEUS
AT EP=30 MeV

«SPECTRA OF LIGHT PARTICLIES

Слайд 2

GOAL

Investigation of the inclusive reaction cross sections of

nuclide 3He with the material of structural elements of nuclear

Слайд 3
Set-up for the transport of accelerated particles to the scattering

chamber

Л - quadrupole lenses, М-1, М-2 - bending magnets,
М-3

Слайд 4
Main characteristics of the telescope and target

Слайд 5
Block Scheme of Registration System

Amp.#1,2 - spectroscopic amplifier; SCA#1,2 -

single channel analyser;
Coinc. - scheme of coincidences; Counter -

Слайд 6
Experimental integral cross sections of 27Al(3He,x) reaction, at E3He=50,5 MeV

Слайд 7Contributions of different processes to formation of inclusive spectra
Bertrand-Peele, Phys.Rev.

C8, 1045 (1973)

Слайд 8
Two-component exciton model

Basic statement:
The atomic nucleus is considered as a

system of fermions with a weak two-particle residual interaction

Слайд 9
Comparison of experimental integral cross sections of 27Al(3He,xp) reaction with

the calculations in the frame of exciton model

Слайд 10
Comparison of experimental integral cross sections of 27Al(3He,xd) reaction with

the calculations in the frame of exciton model

Слайд 11
Comparison of experimental integral cross sections of 27Al(3He,xt) reaction with

the calculations in the frame of exciton model

Слайд 12
Comparison of experimental integral cross sections of 27Al(3He,x) reaction with

the calculations in the frame of exciton model

Слайд 13
Contributions of various mechanisms forming the integral cross-sections of reactions

(3He,xd), (3He,xt) и (3He,x) on 27Al nucleus at E3He = 50,5 MeV

Слайд 14
Experimental double-differential cross-section of reactions 59Co(p,xp) at Ep=30.0 MeV

Слайд 15
Comparison of experimental integral cross sections of 59Co(p,xp) reaction with

the calculations in the exciton model

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Разделы презентаций

DOUBLE DIFFERENTIAL AND INTEGRAL CROSS-SECTIONS OF (p,xp) AND (p,x  )

Содержание

Слайды и текст этой презентации

Слайд 1 DOUBLE DIFFERENTIAL AND INTEGRAL CROSS-SECTIONS OF (p,xp) AND (p,x)

REACTIONS ON 59Co NUCLEUSAT EP=30 MeV «SPECTRA OF LIGHT PARTICLIES

Слайд 2GOAL Investigation of the inclusive reaction cross sections of

nuclide 3He with the material of structural elements of nuclear

Слайд 3Set-up for the transport of accelerated particles to the scattering

chamberЛ - quadrupole lenses, М-1, М-2 - bending magnets, М-3

Слайд 4Main characteristics of the telescope and target

Слайд 5Block Scheme of Registration SystemAmp.#1,2 - spectroscopic amplifier; SCA#1,2 -

single channel analyser; Coinc. - scheme of coincidences; Counter -

Слайд 6Experimental integral cross sections of 27Al(3He,x) reaction, at E3He=50,5 MeV

Слайд 7Contributions of different processes to formation of inclusive spectraBertrand-Peele, Phys.Rev.

C8, 1045 (1973)

Слайд 8Two-component exciton modelBasic statement:The atomic nucleus is considered as a

system of fermions with a weak two-particle residual interaction

Слайд 9Comparison of experimental integral cross sections of 27Al(3He,xp) reaction with

the calculations in the frame of exciton model

Слайд 10Comparison of experimental integral cross sections of 27Al(3He,xd) reaction with

the calculations in the frame of exciton model

Слайд 11Comparison of experimental integral cross sections of 27Al(3He,xt) reaction with

the calculations in the frame of exciton model

Слайд 12Comparison of experimental integral cross sections of 27Al(3He,x) reaction with

the calculations in the frame of exciton model

Слайд 13Contributions of various mechanisms forming the integral cross-sections of reactions

(3He,xd), (3He,xt) и (3He,x) on 27Al nucleus at E3He = 50,5 MeV

Слайд 14Experimental double-differential cross-section of reactions 59Co(p,xp) at Ep=30.0 MeV

Слайд 15Comparison of experimental integral cross sections of 59Co(p,xp) reaction with

the calculations in the exciton model

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Обратная связь

Что такое TheSlide.ru?

Слайд 1

DOUBLE DIFFERENTIAL AND INTEGRAL CROSS-SECTIONS OF (p,xp) AND (p,x)

REACTIONS ON 59Co NUCLEUS
AT EP=30 MeV

«SPECTRA OF LIGHT PARTICLIES

Слайд 2

GOAL

Investigation of the inclusive reaction cross sections of

Слайд 3
Set-up for the transport of accelerated particles to the scattering

chamber

Л - quadrupole lenses, М-1, М-2 - bending magnets,
М-3

Слайд 4
Main characteristics of the telescope and target

Слайд 5
Block Scheme of Registration System

Amp.#1,2 - spectroscopic amplifier; SCA#1,2 -

single channel analyser;
Coinc. - scheme of coincidences; Counter -

Слайд 6
Experimental integral cross sections of 27Al(3He,x) reaction, at E3He=50,5 MeV

Слайд 7Contributions of different processes to formation of inclusive spectra
Bertrand-Peele, Phys.Rev.

Слайд 8
Two-component exciton model

Basic statement:
The atomic nucleus is considered as a

Слайд 9
Comparison of experimental integral cross sections of 27Al(3He,xp) reaction with

Слайд 10
Comparison of experimental integral cross sections of 27Al(3He,xd) reaction with

Слайд 11
Comparison of experimental integral cross sections of 27Al(3He,xt) reaction with

Слайд 12
Comparison of experimental integral cross sections of 27Al(3He,x) reaction with

Слайд 13
Contributions of various mechanisms forming the integral cross-sections of reactions

Слайд 14
Experimental double-differential cross-section of reactions 59Co(p,xp) at Ep=30.0 MeV

Слайд 15
Comparison of experimental integral cross sections of 59Co(p,xp) reaction with