N. P. Misnikova
Moscow State University
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Featured researches published by N. P. Misnikova.
Astroparticle Physics | 2001
A.V. Apanasenko; V.A. Sukhadolskaya; V. A. Derbina; M. Fujii; V.I. Galkine; G.G. Getsov; M. Hareyama; M. Ichimura; S. Ito; Eiji Kamioka; T. Kitami; T. Kobayashi; V.D. Kolesnikov; V. V. Kopenkin; N.M. Kotunova; S. Kuramata; Y. Kuriyama; V.I. Lapshin; A.K. Managadze; H. Matsutani; H. Mikami; N. P. Misnikova; R.A. Mukhamedshin; M. Namiki; H. Nanjo; S. N. Nazarov; S.I. Nikolsky; T. Ohe; S. Ohta; V. I. Osedlo
Abstract We report experimental results obtained by the emulsion chambers on board of the long duration balloon. We have been carrying out the trans-Siberian-continental balloon flight since 1995, and the results from 1995 to 1996 experiments are presented here. Total exposure of these two years amounts to 231.5 m 2 h at the average altitude of ∼32 km. The energy range covers 10–500 TeV for proton-primary, 3–70 TeV/n for helium-primary, and 1–5 TeV/n for Fe-group ( Z =26–28), though statistics of heavy components is not yet enough. Our preliminary data show that the spectra of the proton and the helium have nearly the same power indices ∼2.80, while those of heavier ones become gradually harder as the mass gets heavier, for instance the index is ∼2.70 for CNO-group and ∼2.55 for Fe-group. It is remarkable that a very high energy proton with multi-PeV is detected in 1995 experiment, and the estimated flux of this event coincides with a simple extrapolation from the energy spectrum with the power index 2.8 observed in the range 10–500 TeV. It indicates that there is no spectral break at around 100 TeV, in contrast to the maximum energy predicted by the current shock-wave acceleration model. This evidence requires some modification on the acceleration and/or propagation mechanism. Also we present all-particle spectrum and the average primary mass in the energy range 20–1000 TeV/particle. Our preliminary data show no drastic change in mass composition over the wide energy range, at least up to 1 PeV/particle, though the statistics is not yet enough to confirm it concretely. The flight performance and the procedure of the analysis, particularly the energy determination methods and the detection efficiency calculation are also given.
The Astrophysical Journal | 2005
V. A. Derbina; V. I. Galkin; Makoto Hareyama; Y. Hirakawa; Y. Horiuchi; M. Ichimura; N. Inoue; Eiji Kamioka; Tamaki Kobayashi; V. Kopenkin; S. Kuramata; A.K. Managadze; H. Matsutani; N. P. Misnikova; R. A. Mukhamedshin; S. Nagasawa; R. Nakano; Michiyoshi Namiki; M. Nakazawa; H. Nanjo; S. N. Nazarov; S. Ohata; H. Ohtomo; V. I. Osedlo; D. S. Oshuev; P. A. Publichenko; I.V. Rakobolskaya; T. Roganova; C. Saito; G. P. Sazhina
This is a full report on the cosmic-ray spectra and composition obtained by the emulsion chambers on board 10 long-duration balloons, launched from Kamchatka between 1995 and 1999. The total exposure of these campaigns amounts to 575 m2 hr, with an average flight altitude of ~32 km. We present final results on the energy spectra of two light elements, protons and helium nuclei, and on those of three heavy-element groups, CNO, NeMgSi, and Fe, covering the very high energy region of 10-1000 TeV particle-1. We additionally present the secondary/primary ratio, the all-particle spectrum, and the average mass of the primary cosmic rays. We find that our proton spectrum is in good agreement with other results, but the intensity of the helium component is nearly half that obtained by JACEE and SOKOL. The slopes of the spectra of these two elements obtained from RUNJOB data are almost parallel, with values of 2.7-2.8 in the energy range of 10-500 TeV nucleon-1. RUNJOB heavy-component spectra are in agreement with the extrapolation from those at lower energies obtained by CRN (Chicago group), monotonically decreasing with energy. We have also observed secondary components, such as the LiBeB group and the sub-Fe group, and present the secondary/primary ratio in the TeV nucleon-1 region. We determine the all-particle spectrum and the average mass of the primary cosmic rays in the energy region of 20-1000 TeV particle-1. The intensity of the RUNJOB all-particle spectrum is 40%-50% less than those obtained by JACEE and SOKOL, and the RUNJOB average mass remains almost constant up to ~1 PeV.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2003
M. Hareyama; M. Fujii; V.I. Galkin; Y. Goto; M. Ichimura; Eiji Kamioka; T. Kobayashi; V. Kopenkin; S. Kuramata; A.K. Managadze; H. Matsutani; N. P. Misnikova; R. A. Mukhamedshin; H. Nanjo; S. N. Nazarov; D. S. Oshuev; P. A. Publichenko; I.V. Rakobolskaya; T. Roganova; G. P. Sazhina; Yu.N. Shabanova; H. Semba; T. Shibata; H. Sugimoto; L.G. Sveshnikova; K. Takahashi; I. V. Yashin; K. Yokoi; E.A. Zamchalova; G. Zatsepin
Abstract An account is given of a new type of emulsion chambers which have been in our use since 1997 in our RUNJOB program (RUssia–Nippon JOint Balloon-program). Each chamber is equipped with an additional “diffuser module” placed under the usual set of modules. We have made the experiments using 4 cm thick diffuser modules composed of several photo-sensitive layers (X-ray films and/or nuclear emulsion plates) sandwiched with spacers. The result is as follows. Even in the case where the path length of only 6 radiation lengths is available within the calorimeter module placed above, the visible energy sum is determined with an accuracy better than σ∼0.2 for a group of electromagnetic cascade showers induced by a proton of energy up to several tens of TeV, or by an iron nucleus of energy up to one hundred TeV. If the available path length in the calorimeter module is 9 radiation lengths, we can estimate the energy sum up to ∼100 TeV within an accuracy of σ∼0.2 for a proton-induced cascade shower group. It means that the use of our new-type emulsion chamber can reduce the detector payload dramatically, which is essentially important for the high-energy cosmic-ray observations made on board the vehicles such as balloons, satellites and so on.
Advances in Space Research | 2000
Eiji Kamioka; A.V. Apanasenko; V.A. Berezovskaya; M. Fujii; T. Fukuda; M. Hareyama; G. Hashimoto; M. Ichimura; T. Kobayashi; V. Kopenkin; S. Kuramata; V.I. Lapshin; A. K. Managadze; H. Matsutani; N. P. Misnikova; T. Misu; R. A. Mukhamedshin; A. Nakamura; Michiyoshi Namiki; H. Nanjo; S.I. Nikolsky; K. Ogura; S. Ohta; D. S. Oshuev; P. A. Publichencko; I.V. Rakobolskaya; T. Roganova; G. P. Sazhina; H. Semba; T. Shibata
Abstract We report experimental results obtained by using a wide-gap type emulsion chamber flown in the first Japanese-Russo joint balloon project, called RUNJOB ( RU ssia- N ippon JO int B alloon-program). Two balloons were launched from Kamchatka in July 1995, and both were recovered successfully near the Volga River. The exposure time was 130 hours for the first flight and 168 hours for the second. The mean ceiling altitude, in both flights, was 32 km corresponding to 10 g/cm 2 . Total area of the emulsion chamber was 0.8 m 2 , and the thickness 0.385 and 2.28 collision m.f.p.s for vertically incident proton- and iron-primaries, respectively. We detected 381 showers using Fuji-#200-type X-ray film; of these 174 showers were due to atmospheric secondary γ-rays, and the rest 207 came from nuclear components. The energy range covers 20∼200 TeV for proton-primary, 3∼30 TeV/nucleon for helium-primary, and 0.7∼5 TeV/nucleon for iron-primary. We give the energy spectra for various elements (proton, helium, …, iron) as well as the all-particle spectrum and the average mass of the cosmic-ray primaries.
29th International Cosmic Ray Conference, ICRC 2005 | 2005
Makoto Hareyama; V. A. Derbina; V. I. Galkin; Y. Hirakawa; Y. Horiuchi; M. Ichimura; N. Inoue; Eiji Kamioka; Tamaki Kobayashi; V. Kopenkin; S. Kuramata; A.K. Managadze; H. Matsutani; N. P. Misnikova; R. A. Mukhamedshin; S. Nagasawa; R. Nakano; Michiyoshi Namiki; M. Nakazawa; H. Nanjo; S. N. Nazarov; S. Ohata; H. Ohtomo; V. I. Osedlo; D. S. Oshuev; P. A. Publichenko; I.V. Rakobolskaya; T. Roganova; C. Saito; G. P. Sazhina
Archive | 2003
M. Furukawa; V. I. Galkin; Makoto Hareyama; Y. Hirakawa; Makoto Ichimura; N. Inoue; Eiji Kamioka; Tetsuo Kobayashi; V.V. Kopenkin; S. Kuramata; A.K. Managadze; H. Matsutani; N. P. Misnikova; R. A. Mukhamedshin; S. Nagasawa; R. Nakano; Masaaki Namiki; Hiroshi Nanjo; S. N. Nazarov; S. Ohta; H. Ohtomo; D. S. Oshuev; P. A. Publichenko; I.V. Rakobolskaya; T. Roganova; G. P. Sazhina; H. Semba; T. Shibata; D. Shuto; H. Sugimoto
29th International Cosmic Ray Conference, ICRC 2005 | 2005
L.G. Sveshnikova; V. A. Derbina; V. I. Galkin; Makoto Hareyama; Y. Hirakawa; Y. Horiuchi; M. Ichimura; N. Inoue; Eiji Kamioka; Tamaki Kobayashi; V. Kopenkin; S. Kuramata; A.K. Managadze; H. Matsutani; N. P. Misnikova; R. A. Mukhamedshin; S. Nagasawa; R. Nakano; Michiyoshi Namiki; M. Nakazawa; H. Nanjo; S. N. Nazarov; S. Ohata; H. Ohtomo; V. I. Osedlo; D. S. Oshuev; P. A. Publichenko; I.V. Rakobolskaya; T. Roganova; C. Saito
29th International Cosmic Ray Conference, ICRC 2005 | 2005
M. Ichimura; V. A. Derbina; V. I. Galkin; Makoto Hareyama; Y. Hirakawa; Y. Horiuchi; N. Inoue; Eiji Kamioka; Tamaki Kobayashi; V. Kopenkin; S. Kuramata; A.K. Managadze; H. Matsutani; N. P. Misnikova; R. A. Mukhamedshin; S. Nagasawa; R. Nakano; Michiyoshi Namiki; M. Nakazawa; H. Nanjo; S. N. Nazarov; S. Ohata; H. Ohtomo; V. I. Osedlo; D. S. Oshuev; P. A. Publichenko; I.V. Rakobolskaya; T. Roganova; C. Saito; G. P. Sazhina
Archive | 2003
M. Furukawa; V. I. Galkin; Makoto Hareyama; Y. Hirakawa; Makoto Ichimura; N. Inoue; Eiji Kamioka; Tetsuo Kobayashi; V.V. Kopenkin; S. Kuramata; A.K. Managadze; H. Matsutani; N. P. Misnikova; R. A. Mukhamedshin; S. Nagasawa; R. Nakano; Masaaki Namiki; Hiroshi Nanjo; S. N. Nazarov; S. Ohta; H. Ohtomo; D. S. Oshuev; P. A. Publichenko; I.V. Rakobolskaya; T. Roganova; G. P. Sazhina; H. Semba; T. Shibata; D. Shuto; H. Sugimoto
Archive | 2001
P. A. Publichenko; A. V. Apanasenko; V. A. Derbina; M. Fujii; Makoto Hareyama; Mitsuhiro Higashida; Yusaku Horiuchi; V. I. Galkin; Makoto Ichimura; N. Inoue; Eiji Kamioka; Tetsuo Kobayashi; V.V. Kopenkin; Ikuo Kudo; S. Kuramata; A.K. Managadze; H. Matsutani; N. P. Misnikova; R. A. Muhamedshin; Hiroshi Nanjo; S. N. Nazarov; S. I. Nikolsky; Masato Nishiura; V. I. Osedlo; D. S. Oshuev; I.V. Rakobolskaya; N. G. Poluhina; T. Roganova; G. P. Sazhina; T. Shibata