On the production mechanism of deuterons in proton-nucleus interactions at 400 GeV/c
Summary The deuteron production in the interactions of protons with emulsion nuclei at 400 GeV/c has been studied. Different theoretical models proposed for explaining the production mechanism of light fragments have been used. It has been found that most of the deuterons in the energy range (60÷260...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Aggarwal, M. M. [verfasserIn] |
|---|
| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1980 |
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| Schlagwörter: |
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| Anmerkung: |
© tbc 1980 |
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| Übergeordnetes Werk: |
Enthalten in: Journal of otolaryngology, head & neck surgery - London : BioMed Central, 2008, 56(1980), 4 vom: 01. Apr., Seite 422-434 |
|---|---|
| Übergeordnetes Werk: |
volume:56 ; year:1980 ; number:4 ; day:01 ; month:04 ; pages:422-434 |
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10.1007/BF02732094 |
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| 520 | |a Summary The deuteron production in the interactions of protons with emulsion nuclei at 400 GeV/c has been studied. Different theoretical models proposed for explaining the production mechanism of light fragments have been used. It has been found that most of the deuterons in the energy range (60÷260) MeV are produced due to the pick-up of the target nucleon inside the nucleus by the recoil nucleon. To explain the production of deuterons of energy (260÷760) MeV, the theoretical model proposed $ for^{3} $He nuclei production by Egliet al. (where pick-up amongst recoil nucleons takes place) has been extended. We tried to explain the results with this model and also on the basis of the NN collision model where deuteron production takes place as a result of reactions of the type N(N, π)d. | ||
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10.1007/BF02732094 doi (DE-627)SPR050054570 (SPR)BF02732094-e DE-627 ger DE-627 rakwb eng Aggarwal, M. M. verfasserin aut On the production mechanism of deuterons in proton-nucleus interactions at 400 GeV/c 1980 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © tbc 1980 Summary The deuteron production in the interactions of protons with emulsion nuclei at 400 GeV/c has been studied. Different theoretical models proposed for explaining the production mechanism of light fragments have been used. It has been found that most of the deuterons in the energy range (60÷260) MeV are produced due to the pick-up of the target nucleon inside the nucleus by the recoil nucleon. To explain the production of deuterons of energy (260÷760) MeV, the theoretical model proposed $ for^{3} $He nuclei production by Egliet al. (where pick-up amongst recoil nucleons takes place) has been extended. We tried to explain the results with this model and also on the basis of the NN collision model where deuteron production takes place as a result of reactions of the type N(N, π)d. Production Mechanism (dpeaa)DE-He213 AgBr (dpeaa)DE-He213 Recoil Proton (dpeaa)DE-He213 Target Nucleon (dpeaa)DE-He213 Proton Yield (dpeaa)DE-He213 Lamba, J. P. aut Mittra, I. S. aut Singh, J. B. aut Sood, P. M. aut Enthalten in Journal of otolaryngology, head & neck surgery London : BioMed Central, 2008 56(1980), 4 vom: 01. Apr., Seite 422-434 (DE-627)572078080 (DE-600)2436698-5 1916-0216 nnns volume:56 year:1980 number:4 day:01 month:04 pages:422-434 https://dx.doi.org/10.1007/BF02732094 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER AR 56 1980 4 01 04 422-434 |
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10.1007/BF02732094 doi (DE-627)SPR050054570 (SPR)BF02732094-e DE-627 ger DE-627 rakwb eng Aggarwal, M. M. verfasserin aut On the production mechanism of deuterons in proton-nucleus interactions at 400 GeV/c 1980 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © tbc 1980 Summary The deuteron production in the interactions of protons with emulsion nuclei at 400 GeV/c has been studied. Different theoretical models proposed for explaining the production mechanism of light fragments have been used. It has been found that most of the deuterons in the energy range (60÷260) MeV are produced due to the pick-up of the target nucleon inside the nucleus by the recoil nucleon. To explain the production of deuterons of energy (260÷760) MeV, the theoretical model proposed $ for^{3} $He nuclei production by Egliet al. (where pick-up amongst recoil nucleons takes place) has been extended. We tried to explain the results with this model and also on the basis of the NN collision model where deuteron production takes place as a result of reactions of the type N(N, π)d. Production Mechanism (dpeaa)DE-He213 AgBr (dpeaa)DE-He213 Recoil Proton (dpeaa)DE-He213 Target Nucleon (dpeaa)DE-He213 Proton Yield (dpeaa)DE-He213 Lamba, J. P. aut Mittra, I. S. aut Singh, J. B. aut Sood, P. M. aut Enthalten in Journal of otolaryngology, head & neck surgery London : BioMed Central, 2008 56(1980), 4 vom: 01. Apr., Seite 422-434 (DE-627)572078080 (DE-600)2436698-5 1916-0216 nnns volume:56 year:1980 number:4 day:01 month:04 pages:422-434 https://dx.doi.org/10.1007/BF02732094 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER AR 56 1980 4 01 04 422-434 |
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10.1007/BF02732094 doi (DE-627)SPR050054570 (SPR)BF02732094-e DE-627 ger DE-627 rakwb eng Aggarwal, M. M. verfasserin aut On the production mechanism of deuterons in proton-nucleus interactions at 400 GeV/c 1980 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © tbc 1980 Summary The deuteron production in the interactions of protons with emulsion nuclei at 400 GeV/c has been studied. Different theoretical models proposed for explaining the production mechanism of light fragments have been used. It has been found that most of the deuterons in the energy range (60÷260) MeV are produced due to the pick-up of the target nucleon inside the nucleus by the recoil nucleon. To explain the production of deuterons of energy (260÷760) MeV, the theoretical model proposed $ for^{3} $He nuclei production by Egliet al. (where pick-up amongst recoil nucleons takes place) has been extended. We tried to explain the results with this model and also on the basis of the NN collision model where deuteron production takes place as a result of reactions of the type N(N, π)d. Production Mechanism (dpeaa)DE-He213 AgBr (dpeaa)DE-He213 Recoil Proton (dpeaa)DE-He213 Target Nucleon (dpeaa)DE-He213 Proton Yield (dpeaa)DE-He213 Lamba, J. P. aut Mittra, I. S. aut Singh, J. B. aut Sood, P. M. aut Enthalten in Journal of otolaryngology, head & neck surgery London : BioMed Central, 2008 56(1980), 4 vom: 01. Apr., Seite 422-434 (DE-627)572078080 (DE-600)2436698-5 1916-0216 nnns volume:56 year:1980 number:4 day:01 month:04 pages:422-434 https://dx.doi.org/10.1007/BF02732094 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER AR 56 1980 4 01 04 422-434 |
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10.1007/BF02732094 doi (DE-627)SPR050054570 (SPR)BF02732094-e DE-627 ger DE-627 rakwb eng Aggarwal, M. M. verfasserin aut On the production mechanism of deuterons in proton-nucleus interactions at 400 GeV/c 1980 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © tbc 1980 Summary The deuteron production in the interactions of protons with emulsion nuclei at 400 GeV/c has been studied. Different theoretical models proposed for explaining the production mechanism of light fragments have been used. It has been found that most of the deuterons in the energy range (60÷260) MeV are produced due to the pick-up of the target nucleon inside the nucleus by the recoil nucleon. To explain the production of deuterons of energy (260÷760) MeV, the theoretical model proposed $ for^{3} $He nuclei production by Egliet al. (where pick-up amongst recoil nucleons takes place) has been extended. We tried to explain the results with this model and also on the basis of the NN collision model where deuteron production takes place as a result of reactions of the type N(N, π)d. Production Mechanism (dpeaa)DE-He213 AgBr (dpeaa)DE-He213 Recoil Proton (dpeaa)DE-He213 Target Nucleon (dpeaa)DE-He213 Proton Yield (dpeaa)DE-He213 Lamba, J. P. aut Mittra, I. S. aut Singh, J. B. aut Sood, P. M. aut Enthalten in Journal of otolaryngology, head & neck surgery London : BioMed Central, 2008 56(1980), 4 vom: 01. Apr., Seite 422-434 (DE-627)572078080 (DE-600)2436698-5 1916-0216 nnns volume:56 year:1980 number:4 day:01 month:04 pages:422-434 https://dx.doi.org/10.1007/BF02732094 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER AR 56 1980 4 01 04 422-434 |
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10.1007/BF02732094 doi (DE-627)SPR050054570 (SPR)BF02732094-e DE-627 ger DE-627 rakwb eng Aggarwal, M. M. verfasserin aut On the production mechanism of deuterons in proton-nucleus interactions at 400 GeV/c 1980 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © tbc 1980 Summary The deuteron production in the interactions of protons with emulsion nuclei at 400 GeV/c has been studied. Different theoretical models proposed for explaining the production mechanism of light fragments have been used. It has been found that most of the deuterons in the energy range (60÷260) MeV are produced due to the pick-up of the target nucleon inside the nucleus by the recoil nucleon. To explain the production of deuterons of energy (260÷760) MeV, the theoretical model proposed $ for^{3} $He nuclei production by Egliet al. (where pick-up amongst recoil nucleons takes place) has been extended. We tried to explain the results with this model and also on the basis of the NN collision model where deuteron production takes place as a result of reactions of the type N(N, π)d. Production Mechanism (dpeaa)DE-He213 AgBr (dpeaa)DE-He213 Recoil Proton (dpeaa)DE-He213 Target Nucleon (dpeaa)DE-He213 Proton Yield (dpeaa)DE-He213 Lamba, J. P. aut Mittra, I. S. aut Singh, J. B. aut Sood, P. M. aut Enthalten in Journal of otolaryngology, head & neck surgery London : BioMed Central, 2008 56(1980), 4 vom: 01. Apr., Seite 422-434 (DE-627)572078080 (DE-600)2436698-5 1916-0216 nnns volume:56 year:1980 number:4 day:01 month:04 pages:422-434 https://dx.doi.org/10.1007/BF02732094 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER AR 56 1980 4 01 04 422-434 |
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Summary The deuteron production in the interactions of protons with emulsion nuclei at 400 GeV/c has been studied. Different theoretical models proposed for explaining the production mechanism of light fragments have been used. It has been found that most of the deuterons in the energy range (60÷260) MeV are produced due to the pick-up of the target nucleon inside the nucleus by the recoil nucleon. To explain the production of deuterons of energy (260÷760) MeV, the theoretical model proposed $ for^{3} $He nuclei production by Egliet al. (where pick-up amongst recoil nucleons takes place) has been extended. We tried to explain the results with this model and also on the basis of the NN collision model where deuteron production takes place as a result of reactions of the type N(N, π)d. © tbc 1980 |
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Summary The deuteron production in the interactions of protons with emulsion nuclei at 400 GeV/c has been studied. Different theoretical models proposed for explaining the production mechanism of light fragments have been used. It has been found that most of the deuterons in the energy range (60÷260) MeV are produced due to the pick-up of the target nucleon inside the nucleus by the recoil nucleon. To explain the production of deuterons of energy (260÷760) MeV, the theoretical model proposed $ for^{3} $He nuclei production by Egliet al. (where pick-up amongst recoil nucleons takes place) has been extended. We tried to explain the results with this model and also on the basis of the NN collision model where deuteron production takes place as a result of reactions of the type N(N, π)d. © tbc 1980 |
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Summary The deuteron production in the interactions of protons with emulsion nuclei at 400 GeV/c has been studied. Different theoretical models proposed for explaining the production mechanism of light fragments have been used. It has been found that most of the deuterons in the energy range (60÷260) MeV are produced due to the pick-up of the target nucleon inside the nucleus by the recoil nucleon. To explain the production of deuterons of energy (260÷760) MeV, the theoretical model proposed $ for^{3} $He nuclei production by Egliet al. (where pick-up amongst recoil nucleons takes place) has been extended. We tried to explain the results with this model and also on the basis of the NN collision model where deuteron production takes place as a result of reactions of the type N(N, π)d. © tbc 1980 |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR050054570</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230509112825.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">230417s1980 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/BF02732094</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR050054570</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)BF02732094-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Aggarwal, M. M.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">On the production mechanism of deuterons in proton-nucleus interactions at 400 GeV/c</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1980</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© tbc 1980</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Summary The deuteron production in the interactions of protons with emulsion nuclei at 400 GeV/c has been studied. Different theoretical models proposed for explaining the production mechanism of light fragments have been used. It has been found that most of the deuterons in the energy range (60÷260) MeV are produced due to the pick-up of the target nucleon inside the nucleus by the recoil nucleon. To explain the production of deuterons of energy (260÷760) MeV, the theoretical model proposed $ for^{3} $He nuclei production by Egliet al. (where pick-up amongst recoil nucleons takes place) has been extended. We tried to explain the results with this model and also on the basis of the NN collision model where deuteron production takes place as a result of reactions of the type N(N, π)d.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Production Mechanism</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">AgBr</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Recoil Proton</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Target Nucleon</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Proton Yield</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Lamba, J. P.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Mittra, I. S.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Singh, J. B.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Sood, P. M.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Journal of otolaryngology, head & neck surgery</subfield><subfield code="d">London : BioMed Central, 2008</subfield><subfield code="g">56(1980), 4 vom: 01. Apr., Seite 422-434</subfield><subfield code="w">(DE-627)572078080</subfield><subfield code="w">(DE-600)2436698-5</subfield><subfield code="x">1916-0216</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:56</subfield><subfield code="g">year:1980</subfield><subfield code="g">number:4</subfield><subfield code="g">day:01</subfield><subfield code="g">month:04</subfield><subfield code="g">pages:422-434</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://dx.doi.org/10.1007/BF02732094</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_SPRINGER</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">56</subfield><subfield code="j">1980</subfield><subfield code="e">4</subfield><subfield code="b">01</subfield><subfield code="c">04</subfield><subfield code="h">422-434</subfield></datafield></record></collection>
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