Acta Physica Sinica //m.getgobooth.com/ 必威体育下载 daily 15 2024-10-24 17:40:08 apsoffice@iphy.ac.cn apsoffice@iphy.ac.cn 2024-10-24 17:40:08 zh Copyright ©Acta Physica Sinica All Rights Reserved. 京ICP备05002789号-1 Address: PostCode:100190 Phone: 010-82649829,82649241,82649863 Email: apsoffice@iphy.ac.cn Copyright ©Acta Physica Sinica All Rights Reserved apsoffice@iphy.ac.cn 1000-3290 <![CDATA[NUCLEAR INTERACTIONS OF COSMIC RAY HIGH ENERGY PARTICLES WITH LIQUID SCINTILLATOR]]> //m.getgobooth.com/en/article/doi/10.7498/aps.19.205 Author(s): WANG SHIH-WEI, KUANG HAO-HWAI, YUAN YU-KUEI <br/><p>Nuclear interactions induced by cosmic ray high energy particles have been studied by means of a multiplate cloud chamber at 3185 meters above sea level with liquid scintillator as target material. From the analysis of 18 interactions induced by charged primaries it is found: (i) average primary energy E0=41±8Bev (by Castagnoli formula), (ii) average multiplicity of charged secondaries ns=4.9±0.3, (iii) with x=lgγctgθl the differential angular distribution dN/dx indicates some possibility of theexistence of double-humped shape. This angular distribution has been discussed tentatively along the lines of two-centered model.</p> <br/>Acta Physica Sinica. 1963 19(4): 205-214. Published 1963-02-05 Author(s): WANG SHIH-WEI, KUANG HAO-HWAI, YUAN YU-KUEI <br/><p>Nuclear interactions induced by cosmic ray high energy particles have been studied by means of a multiplate cloud chamber at 3185 meters above sea level with liquid scintillator as target material. From the analysis of 18 interactions induced by charged primaries it is found: (i) average primary energy E0=41±8Bev (by Castagnoli formula), (ii) average multiplicity of charged secondaries ns=4.9±0.3, (iii) with x=lgγctgθl the differential angular distribution dN/dx indicates some possibility of theexistence of double-humped shape. This angular distribution has been discussed tentatively along the lines of two-centered model.</p> <br/>Acta Physica Sinica. 1963 19(4): 205-214. Published 1963-02-05 NUCLEAR INTERACTIONS OF COSMIC RAY HIGH ENERGY PARTICLES WITH LIQUID SCINTILLATOR WANG SHIH-WEI, KUANG HAO-HWAI, YUAN YU-KUEI 1963-02-05 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1963 19(4): 205-214. article doi:10.7498/aps.19.205 10.7498/aps.19.205 Acta Physica Sinica 19 4 1963-02-05 //m.getgobooth.com/en/article/doi/10.7498/aps.19.205 205-214 <![CDATA[THE METHOD OF SIMULATING A HELICALLY INVARIANT MAGNETIC FIELD]]> //m.getgobooth.com/en/article/doi/10.7498/aps.19.215 Author(s): HSIN SHIEN-CHIEH <br/><p>In this paper the differential equation of a helically invariant magnetic field is derived, and the method of simulating this type of field is analyzed in detail. It is shown that the original Wakefield's resistance network analogue may be simplified considerably. The method of simulating a helically invariant field with composite (azimu-thal) period of multiplicity is also given. A very simple resistance network has been constructed to verify the conclusions arrived at.</p> <br/>Acta Physica Sinica. 1963 19(4): 215-224. Published 1963-02-05 Author(s): HSIN SHIEN-CHIEH <br/><p>In this paper the differential equation of a helically invariant magnetic field is derived, and the method of simulating this type of field is analyzed in detail. It is shown that the original Wakefield's resistance network analogue may be simplified considerably. The method of simulating a helically invariant field with composite (azimu-thal) period of multiplicity is also given. A very simple resistance network has been constructed to verify the conclusions arrived at.</p> <br/>Acta Physica Sinica. 1963 19(4): 215-224. Published 1963-02-05 THE METHOD OF SIMULATING A HELICALLY INVARIANT MAGNETIC FIELD HSIN SHIEN-CHIEH 1963-02-05 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1963 19(4): 215-224. article doi:10.7498/aps.19.215 10.7498/aps.19.215 Acta Physica Sinica 19 4 1963-02-05 //m.getgobooth.com/en/article/doi/10.7498/aps.19.215 215-224 <![CDATA[ЧЕРЕНКОВСКИЕ СПЕКТРОМЕТРЫ ПОЛНОГО ПОГЛОЩЕНИЯ]]> //m.getgobooth.com/en/article/doi/10.7498/aps.19.225 Author(s): <br/><p></p> <br/>Acta Physica Sinica. 1963 19(4): 225-238. Published 1963-02-05 Author(s): <br/><p></p> <br/>Acta Physica Sinica. 1963 19(4): 225-238. Published 1963-02-05 ЧЕРЕНКОВСКИЕ СПЕКТРОМЕТРЫ ПОЛНОГО ПОГЛОЩЕНИЯ 1963-02-05 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1963 19(4): 225-238. article doi:10.7498/aps.19.225 10.7498/aps.19.225 Acta Physica Sinica 19 4 1963-02-05 //m.getgobooth.com/en/article/doi/10.7498/aps.19.225 225-238 <![CDATA[THE TIME-DEPENDING SCATTERING THEORY OF MULTI-CHANNEL PROCESS]]> //m.getgobooth.com/en/article/doi/10.7498/aps.19.239 Author(s): YANG TSE-SEN <br/><p>The time-depending formal theory of scattering, initiated by Lippmann and Schwinger is generalized to the case of multi-channel process.Ekstein has attempted to construct such a theory in 1956 and pointed out the orthogonality properties of the set of multi-channel outgoing (incoming) scattering states, which is very important for the establishment of scattering matrix, but it seems to him that the quite general starting point of the L-S formalism is not appreciated. In his work the simplicity of the L-S formalism is lost. He came to the conclusion that the scattering matrix can not be regarded as the matrix of a single linear operator, because he insisted to work in one single interaction representation for all the initial and final states. Thereby the concept of scattering matrix is confused.The present paper deals with the same generalization, but the simplicity of the L-S formalism is preserved. The explicit form of the scattering operator is given. The calculation of the various transition probability in the present case can be made in a similar way as in the original L-S theory.</p> <br/>Acta Physica Sinica. 1963 19(4): 239-248. Published 1963-02-05 Author(s): YANG TSE-SEN <br/><p>The time-depending formal theory of scattering, initiated by Lippmann and Schwinger is generalized to the case of multi-channel process.Ekstein has attempted to construct such a theory in 1956 and pointed out the orthogonality properties of the set of multi-channel outgoing (incoming) scattering states, which is very important for the establishment of scattering matrix, but it seems to him that the quite general starting point of the L-S formalism is not appreciated. In his work the simplicity of the L-S formalism is lost. He came to the conclusion that the scattering matrix can not be regarded as the matrix of a single linear operator, because he insisted to work in one single interaction representation for all the initial and final states. Thereby the concept of scattering matrix is confused.The present paper deals with the same generalization, but the simplicity of the L-S formalism is preserved. The explicit form of the scattering operator is given. The calculation of the various transition probability in the present case can be made in a similar way as in the original L-S theory.</p> <br/>Acta Physica Sinica. 1963 19(4): 239-248. Published 1963-02-05 THE TIME-DEPENDING SCATTERING THEORY OF MULTI-CHANNEL PROCESS YANG TSE-SEN 1963-02-05 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1963 19(4): 239-248. article doi:10.7498/aps.19.239 10.7498/aps.19.239 Acta Physica Sinica 19 4 1963-02-05 //m.getgobooth.com/en/article/doi/10.7498/aps.19.239 239-248 <![CDATA[A NEW METHOD OF CALCULATING THE CHARACTERISTIC IMPEDANCES OF TRANSMISSION LINES]]> //m.getgobooth.com/en/article/doi/10.7498/aps.19.249 Author(s): Lin Wei-Guan, Chung Shong-lee <br/><p>Utilizing a theorem from the variational principles, after transforming boundaries of a transmission line into simpler ones, we can find upper and lower bounds to the correct value of the characteristic impedance of the line, so that the lengthy calculation in the ordinary variational method is avoided. Impedances of the rectangular line with central cylindrical inner conductor, the trough line with the slab line as a special case and the multi-conductor cable are calculated.</p> <br/>Acta Physica Sinica. 1963 19(4): 249-258. Published 1963-02-05 Author(s): Lin Wei-Guan, Chung Shong-lee <br/><p>Utilizing a theorem from the variational principles, after transforming boundaries of a transmission line into simpler ones, we can find upper and lower bounds to the correct value of the characteristic impedance of the line, so that the lengthy calculation in the ordinary variational method is avoided. Impedances of the rectangular line with central cylindrical inner conductor, the trough line with the slab line as a special case and the multi-conductor cable are calculated.</p> <br/>Acta Physica Sinica. 1963 19(4): 249-258. Published 1963-02-05 A NEW METHOD OF CALCULATING THE CHARACTERISTIC IMPEDANCES OF TRANSMISSION LINES Lin Wei-Guan, Chung Shong-lee 1963-02-05 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1963 19(4): 249-258. article doi:10.7498/aps.19.249 10.7498/aps.19.249 Acta Physica Sinica 19 4 1963-02-05 //m.getgobooth.com/en/article/doi/10.7498/aps.19.249 249-258 <![CDATA[ПРИБЛИЖЕННЫЙ МЕТОД ОПРЕДЕЛЕНИЯ КОЛИЧЕСТВА ЭНЕРГИИ,РАССЕВАЕМОЙ В ЭЛЕКТРИЧЕСКОЙ ЦЕПИ С ПЕРЕМЕННЫМИ ПАРАМЕТРАМИ]]> //m.getgobooth.com/en/article/doi/10.7498/aps.19.259 Author(s): <br/><p></p> <br/>Acta Physica Sinica. 1963 19(4): 259-267. Published 1963-02-05 Author(s): <br/><p></p> <br/>Acta Physica Sinica. 1963 19(4): 259-267. Published 1963-02-05 ПРИБЛИЖЕННЫЙ МЕТОД ОПРЕДЕЛЕНИЯ КОЛИЧЕСТВА ЭНЕРГИИ,РАССЕВАЕМОЙ В ЭЛЕКТРИЧЕСКОЙ ЦЕПИ С ПЕРЕМЕННЫМИ ПАРАМЕТРАМИ 1963-02-05 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1963 19(4): 259-267. article doi:10.7498/aps.19.259 10.7498/aps.19.259 Acta Physica Sinica 19 4 1963-02-05 //m.getgobooth.com/en/article/doi/10.7498/aps.19.259 259-267 <![CDATA[]]> //m.getgobooth.com/en/article/doi/10.7498/aps.19.268 Author(s): <br/><p></p> <br/>Acta Physica Sinica. 1963 19(4): 268-270. Published 1963-02-05 Author(s): <br/><p></p> <br/>Acta Physica Sinica. 1963 19(4): 268-270. Published 1963-02-05 1963-02-05 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1963 19(4): 268-270. article doi:10.7498/aps.19.268 10.7498/aps.19.268 Acta Physica Sinica 19 4 1963-02-05 //m.getgobooth.com/en/article/doi/10.7498/aps.19.268 268-270 <![CDATA[]]> //m.getgobooth.com/en/article/doi/10.7498/aps.19.271 Author(s): <br/><p></p> <br/>Acta Physica Sinica. 1963 19(4): 271-272. Published 1963-02-05 Author(s): <br/><p></p> <br/>Acta Physica Sinica. 1963 19(4): 271-272. Published 1963-02-05 1963-02-05 Personal use only, all commercial or other reuse prohibited Acta Physica Sinica. 1963 19(4): 271-272. article doi:10.7498/aps.19.271 10.7498/aps.19.271 Acta Physica Sinica 19 4 1963-02-05 //m.getgobooth.com/en/article/doi/10.7498/aps.19.271 271-272