M. Kavatsyuk, L. Batist, J. Döring, C. Plettner, H. Grawe, Z. Janas, M. Karny, O. Kavatsyuk, R. K... more M. Kavatsyuk, L. Batist, J. Döring, C. Plettner, H. Grawe, Z. Janas, M. Karny, O. Kavatsyuk, R. Kirchner, C. Mazzocchi, I. Mukha, A. P lochocki, and E. Roeckl Gesellschaft für Schwerionenforschung mbH, D-64291 Darmstadt, Germany; Kiev National University, UA-03022 Kiev, Ukraine; St. Petersburg Nuclear Physics Institute, Gatchina 188350, Russia; Institute of Experimental Physics, Warsaw University, PL-00681 Warsaw, Poland; Universitá degli Studi di Milano, I-20133 Milano, Italy
A. Bracco, G. Benzoni, N. Blasi, S. Brambilla, F. Camera F.C.L. Crespi, S. Leoni, B. Million, D. ... more A. Bracco, G. Benzoni, N. Blasi, S. Brambilla, F. Camera F.C.L. Crespi, S. Leoni, B. Million, D. Montanari M. Pignanelli, O. Wieland, A. Maj, P. Bednarczyk J. Grębosz, M. Kmiecik, W. Męczyński, J. Styczeń T. Aumann, A. Banu, T. Beck, F. Becker, L. Caceres P. Doornenbal, H. Emling, J. Gerl, H. Geissel, M. Gorska O. Kavatsyuk, M. Kavatsyuk, I. Kojouharov , N. Kurz R. Lozeva, N. Saito, T. Saito, H. Shaffner H.J. Wollersheim, J. Jolie, P. Reiter, N. Warr G. de Angelis, A. Gadea, D. Napoli, S. Lenzi , S. Lunardi D. Balabanski, G. Lo Bianco, C. Petrache, A. Saltarelli M. Castoldi, A. Zucchiatti, J. Walker, A. Bürger
Search of pygmy dipole resonance in exotic 68Ni / A. Bracco, G. Benzoni, N. Blasi, S. Brambilla, ... more Search of pygmy dipole resonance in exotic 68Ni / A. Bracco, G. Benzoni, N. Blasi, S. Brambilla, F. Camera, FCLCrespi, S. Leoni, B. Million, D. Montanari, M. Pignanelli, O. Wieland, A. Maj, P. Bednarczyk, J. Grebosz, M. Kmiecik, W. Meczynski, J. Styczen, T. ...
3 Figure 1: The conceptual basic experimental setup of this project presented in the Letter Of In... more 3 Figure 1: The conceptual basic experimental setup of this project presented in the Letter Of Intent of the HypHI project [1]. TR1 and TR2 are tracking detectors in front of a dipole magnet and TR3 is a chamber behind the magnet for tracking and charge measurements. Sci1 and Sci2 are fast plastic scintillators for TOF measurements.
We have studied soft X-ray photoabsorption in the doubly deprotonated gas-phase oligonucleotide [... more We have studied soft X-ray photoabsorption in the doubly deprotonated gas-phase oligonucleotide [dTGGGGT-2H]^2-. The dominating decay mechanism of the X-ray induced inner shell vacancy was found to be Auger decay...
Magnetic monopoles are predicted in various unified gauge models and could be produced at interme... more Magnetic monopoles are predicted in various unified gauge models and could be produced at intermediate mass scales. Their detection in a neutrino telescope is facilitated by the large amount of light emitted compared to that from muons. This paper reports on a search for upgoing relativistic magnetic monopoles with the ANTARES neutrino telescope using a data set of 116 days of live time taken from December 2007 to December 2008. The one observed event is consistent with the expected atmospheric neutrino and muon background, leading to a 90% C.L. upper limit on the monopole flux between 1.3E-17 and 8.9E-17 cm-2.s-1.sr-1 for monopoles with velocity beta greater than 0.625.
National University The properties of the self-conjugate N=Z=35 70Br nucleus have been studied so... more National University The properties of the self-conjugate N=Z=35 70Br nucleus have been studied so far by in-beam[1, 2] and β-decay experiments (see [3, 4]). This nucleus has a 0 + ground-state β-decaying with the half-life (T1/2) of 78.54(59) ms, and a more long-lived 9 + isomeric state with T1/2=2.19(9) s. The isomer energy had been unknown until recently when two groups reported evidence for the 9 + state in their in-beamdata. In the work of de Angelis et al. [1], the excitation energy of the 9 + isomer was reported to be 1214 keV while Jenkins et al. [2] place the 9 + state at an excitation energy of 2293 keV. The large discrepancies of the 9 + isomer energies reported by different groups was the motivation to undertake a measurement of this quantity by means of a different technique. The method applied involves the determination of the QEC value for the decay of the isomer and a comparison to the QEC value of the ground-state decay.
The first excited 2 (+) states in Cr-54, Cr-56, Cr-58 have been populated by relativistic Coulomb... more The first excited 2 (+) states in Cr-54, Cr-56, Cr-58 have been populated by relativistic Coulomb excitation using the FRS-RISING setup at GSI. The Cr ions were produced by fragmentation of a Kr-86 beam on a primary Be target and separated by the FRS. The ion ...
The first 2+ states in 134Ce and 136Nd and the second 2+ state in 136Nd were populated by Coulomb... more The first 2+ states in 134Ce and 136Nd and the second 2+ state in 136Nd were populated by Coulomb excitation at relativistic energies, and γ-rays were measured using the RISING setup at GSI. For 134Ce an indication of the excitation to the second 2+ state was ...
M. Kavatsyuk, L. Batist, J. Döring, C. Plettner, H. Grawe, Z. Janas, M. Karny, O. Kavatsyuk, R. K... more M. Kavatsyuk, L. Batist, J. Döring, C. Plettner, H. Grawe, Z. Janas, M. Karny, O. Kavatsyuk, R. Kirchner, C. Mazzocchi, I. Mukha, A. P lochocki, and E. Roeckl Gesellschaft für Schwerionenforschung mbH, D-64291 Darmstadt, Germany; Kiev National University, UA-03022 Kiev, Ukraine; St. Petersburg Nuclear Physics Institute, Gatchina 188350, Russia; Institute of Experimental Physics, Warsaw University, PL-00681 Warsaw, Poland; Universitá degli Studi di Milano, I-20133 Milano, Italy
A. Bracco, G. Benzoni, N. Blasi, S. Brambilla, F. Camera F.C.L. Crespi, S. Leoni, B. Million, D. ... more A. Bracco, G. Benzoni, N. Blasi, S. Brambilla, F. Camera F.C.L. Crespi, S. Leoni, B. Million, D. Montanari M. Pignanelli, O. Wieland, A. Maj, P. Bednarczyk J. Grębosz, M. Kmiecik, W. Męczyński, J. Styczeń T. Aumann, A. Banu, T. Beck, F. Becker, L. Caceres P. Doornenbal, H. Emling, J. Gerl, H. Geissel, M. Gorska O. Kavatsyuk, M. Kavatsyuk, I. Kojouharov , N. Kurz R. Lozeva, N. Saito, T. Saito, H. Shaffner H.J. Wollersheim, J. Jolie, P. Reiter, N. Warr G. de Angelis, A. Gadea, D. Napoli, S. Lenzi , S. Lunardi D. Balabanski, G. Lo Bianco, C. Petrache, A. Saltarelli M. Castoldi, A. Zucchiatti, J. Walker, A. Bürger
Search of pygmy dipole resonance in exotic 68Ni / A. Bracco, G. Benzoni, N. Blasi, S. Brambilla, ... more Search of pygmy dipole resonance in exotic 68Ni / A. Bracco, G. Benzoni, N. Blasi, S. Brambilla, F. Camera, FCLCrespi, S. Leoni, B. Million, D. Montanari, M. Pignanelli, O. Wieland, A. Maj, P. Bednarczyk, J. Grebosz, M. Kmiecik, W. Meczynski, J. Styczen, T. ...
3 Figure 1: The conceptual basic experimental setup of this project presented in the Letter Of In... more 3 Figure 1: The conceptual basic experimental setup of this project presented in the Letter Of Intent of the HypHI project [1]. TR1 and TR2 are tracking detectors in front of a dipole magnet and TR3 is a chamber behind the magnet for tracking and charge measurements. Sci1 and Sci2 are fast plastic scintillators for TOF measurements.
We have studied soft X-ray photoabsorption in the doubly deprotonated gas-phase oligonucleotide [... more We have studied soft X-ray photoabsorption in the doubly deprotonated gas-phase oligonucleotide [dTGGGGT-2H]^2-. The dominating decay mechanism of the X-ray induced inner shell vacancy was found to be Auger decay...
Magnetic monopoles are predicted in various unified gauge models and could be produced at interme... more Magnetic monopoles are predicted in various unified gauge models and could be produced at intermediate mass scales. Their detection in a neutrino telescope is facilitated by the large amount of light emitted compared to that from muons. This paper reports on a search for upgoing relativistic magnetic monopoles with the ANTARES neutrino telescope using a data set of 116 days of live time taken from December 2007 to December 2008. The one observed event is consistent with the expected atmospheric neutrino and muon background, leading to a 90% C.L. upper limit on the monopole flux between 1.3E-17 and 8.9E-17 cm-2.s-1.sr-1 for monopoles with velocity beta greater than 0.625.
National University The properties of the self-conjugate N=Z=35 70Br nucleus have been studied so... more National University The properties of the self-conjugate N=Z=35 70Br nucleus have been studied so far by in-beam[1, 2] and β-decay experiments (see [3, 4]). This nucleus has a 0 + ground-state β-decaying with the half-life (T1/2) of 78.54(59) ms, and a more long-lived 9 + isomeric state with T1/2=2.19(9) s. The isomer energy had been unknown until recently when two groups reported evidence for the 9 + state in their in-beamdata. In the work of de Angelis et al. [1], the excitation energy of the 9 + isomer was reported to be 1214 keV while Jenkins et al. [2] place the 9 + state at an excitation energy of 2293 keV. The large discrepancies of the 9 + isomer energies reported by different groups was the motivation to undertake a measurement of this quantity by means of a different technique. The method applied involves the determination of the QEC value for the decay of the isomer and a comparison to the QEC value of the ground-state decay.
The first excited 2 (+) states in Cr-54, Cr-56, Cr-58 have been populated by relativistic Coulomb... more The first excited 2 (+) states in Cr-54, Cr-56, Cr-58 have been populated by relativistic Coulomb excitation using the FRS-RISING setup at GSI. The Cr ions were produced by fragmentation of a Kr-86 beam on a primary Be target and separated by the FRS. The ion ...
The first 2+ states in 134Ce and 136Nd and the second 2+ state in 136Nd were populated by Coulomb... more The first 2+ states in 134Ce and 136Nd and the second 2+ state in 136Nd were populated by Coulomb excitation at relativistic energies, and γ-rays were measured using the RISING setup at GSI. For 134Ce an indication of the excitation to the second 2+ state was ...
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