Pub Date : 2023-10-31DOI: 10.1016/j.physo.2023.100187
Reddi Rani L. , H.S. Anushree , H.C. Manjunatha , N. Sowmya , L. Seenappa , K.N. Sridhar , P.S. Damodhara Gupta
We attempted to improve semi-empirical equations for -decay in the atomic number range and mass number range . We suggested a semi-empirical formula in terms of an atomic number of daughter nuclei and decay energy in keV. We divided the nuclei into four categories: even(Z)-even(N), even(Z)-odd(N), odd(Z)-even(N), and odd(Z)-odd(N) to propose improved semi-empirical formulae. The existing equation values are compared to the experimental results. When compared to other semi-empirical equations accessible in the literature, the standard deviation produced from the current formula is lower. The improved semi-empirical formulas are of the first kind, requiring only an atomic number of daughter and decay energy during -decay. This study discovers a significance in predicting -decay.
{"title":"Improved semi-empirical formulae for Beta-decay","authors":"Reddi Rani L. , H.S. Anushree , H.C. Manjunatha , N. Sowmya , L. Seenappa , K.N. Sridhar , P.S. Damodhara Gupta","doi":"10.1016/j.physo.2023.100187","DOIUrl":"https://doi.org/10.1016/j.physo.2023.100187","url":null,"abstract":"<div><p>We attempted to improve semi-empirical equations for <span><math><msup><mrow><mi>β</mi></mrow><mrow><mo>−</mo></mrow></msup></math></span>-decay in the atomic number range <span><math><mrow><mn>1</mn><mo>≤</mo><mi>Z</mi><mo>≤</mo><mn>42</mn></mrow></math></span> and mass number range <span><math><mrow><mn>3</mn><mo>≤</mo><mi>A</mi><mo>≤</mo><mn>118</mn></mrow></math></span>. We suggested a semi-empirical formula in terms of an atomic number of daughter nuclei and decay energy in keV. We divided the nuclei into four categories: even(Z)-even(N), even(Z)-odd(N), odd(Z)-even(N), and odd(Z)-odd(N) to propose improved semi-empirical formulae. The existing equation values are compared to the experimental results. When compared to other semi-empirical equations accessible in the literature, the standard deviation produced from the current formula is lower. The improved semi-empirical formulas are of the first kind, requiring only an atomic number of daughter and decay energy during <span><math><msup><mrow><mi>β</mi></mrow><mrow><mo>−</mo></mrow></msup></math></span>-decay. This study discovers a significance in predicting <span><math><msup><mrow><mi>β</mi></mrow><mrow><mo>−</mo></mrow></msup></math></span>-decay.</p></div>","PeriodicalId":36067,"journal":{"name":"Physics Open","volume":"17 ","pages":"Article 100187"},"PeriodicalIF":0.0,"publicationDate":"2023-10-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2666032623000522/pdfft?md5=9a8702c0da47a6675d129fd9832b8b4f&pid=1-s2.0-S2666032623000522-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"91963773","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pebble-bed High Temperature reactors (HTR) are proposed to generate heat for power production and process heat application such as Hydrogen (H2) production. A HTR fuel pebble consists of random distribution of several thousands of fuel particles, called Tri-Structural Isotropic (TRISO), in fuel zone followed by a graphite layer. This configuration along with coolant layer results in double heterogeneity effect. A multi-group Monte Carlo code PebMC has been developed to accurately analyse molten salt cooled HTR lattice cell. Neutron transport in such a complex fuel distribution requires resonance self-shielded cross-section which is generated using rational approximation and Dancoff correction. Dancoff factor accounts for those neutrons leaving a fuel particle and directly colliding with another fuel particle, without any collision with moderator nuclei.
In this study, an analytical expression based on a two-region model developed for gas cooled HTRs is adopted to calculate Dancoff factor for pebble with salt coolant. The implementation of these analytical expressions with 172groups WIMS library in PebMC code have been discussed. Subsequently, paper describes neutron tracking in random medium of HTR lattice using Monte Carlo method. The influence of fuel salt on Dancoff factor for various packing of TRISO particles and subsequent effect on infinite multiplication factor (K-inf) calculation have been presented. In addition, effect of temperature of molten salt on Dancoff factor have been studied.
{"title":"Simulation of random medium of fuel pebble with liquid salt coolant using PebMC code","authors":"Indrajeet Singh , Amod Kishore Mallick , Anurag Gupta , Umasankari Kannan","doi":"10.1016/j.physo.2023.100190","DOIUrl":"https://doi.org/10.1016/j.physo.2023.100190","url":null,"abstract":"<div><p>Pebble-bed High Temperature reactors (HTR) are proposed to generate heat for power production and process heat application such as Hydrogen (H<sub>2</sub>) production. A HTR fuel pebble consists of random distribution of several thousands of fuel particles, called Tri-Structural Isotropic (TRISO), in fuel zone followed by a graphite layer. This configuration along with coolant layer results in double heterogeneity effect. A multi-group Monte Carlo code PebMC has been developed to accurately analyse molten salt cooled HTR lattice cell. Neutron transport in such a complex fuel distribution requires resonance self-shielded cross-section which is generated using rational approximation and Dancoff correction. Dancoff factor accounts for those neutrons leaving a fuel particle and directly colliding with another fuel particle, without any collision with moderator nuclei.</p><p>In this study, an analytical expression based on a two-region model developed for gas cooled HTRs is adopted to calculate Dancoff factor for pebble with salt coolant. The implementation of these analytical expressions with 172groups WIMS library in PebMC code have been discussed. Subsequently, paper describes neutron tracking in random medium of HTR lattice using Monte Carlo method. The influence of fuel salt on Dancoff factor for various packing of TRISO particles and subsequent effect on infinite multiplication factor (K-inf) calculation have been presented. In addition, effect of temperature of molten salt on Dancoff factor have been studied.</p></div>","PeriodicalId":36067,"journal":{"name":"Physics Open","volume":"17 ","pages":"Article 100190"},"PeriodicalIF":0.0,"publicationDate":"2023-10-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2666032623000558/pdfft?md5=b974233126cbf96bb029ccf1c76876bd&pid=1-s2.0-S2666032623000558-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"92100893","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-10-28DOI: 10.1016/j.physo.2023.100188
S. Deepthi , Y.S. Vidya , H.C. Manjunatha , R. Munirathnam , K.N. Sridhar , L. Seenappa , S. Manjunatha , T. Ganesh
The current study reports the synthesis of FeO NPs by the co-precipitation method and the evaluation of the anticancer activity and X-ray/gamma absorption study. PXRD analysis confirmed the formation of monophase trigonal-shaped NPs, and the average crystal size is computed using both Scherrer equation and W-h plot and found to be 45 nm and 54 nm respectively. The direct energy gap is computed from the Wood-Taucs plot and found to be 1.76 eV. FTIR analysis confirmed the functional groups present in NPs. Surface morphology studies confirmed by SEM and EDAX analysis confirmed the chemical composition. Anti-cancer studies verified the efficacy of FeO NPs in cell viability and cell death when compared with Cisplatin. Finally, a NaI(Tl) detector is used to evaluate Mass attenuation co-efficient of the X-ray and gamma radiation shielding characteristics. Shielding requirements are comparable to those for lead. Thus, the synthesized FeO nanoparticles can be used for anticancer activities, particularly in tailored drug delivery systems, and radiation shielding instead of toxic lead shielding.
{"title":"X-ray/gamma absorption and Anticancer Properties of Fe2O3 nanoparticles","authors":"S. Deepthi , Y.S. Vidya , H.C. Manjunatha , R. Munirathnam , K.N. Sridhar , L. Seenappa , S. Manjunatha , T. Ganesh","doi":"10.1016/j.physo.2023.100188","DOIUrl":"https://doi.org/10.1016/j.physo.2023.100188","url":null,"abstract":"<div><p>The current study reports the synthesis of Fe<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span>O<span><math><msub><mrow></mrow><mrow><mn>3</mn></mrow></msub></math></span> NPs by the co-precipitation method and the evaluation of the anticancer activity and X-ray/gamma absorption study. PXRD analysis confirmed the formation of monophase trigonal-shaped NPs, and the average crystal size is computed using both Scherrer equation and W-h plot and found to be 45 nm and 54 nm respectively. The direct energy gap is computed from the Wood-Taucs plot and found to be 1.76 eV. FTIR analysis confirmed the functional groups present in NPs. Surface morphology studies confirmed by SEM and EDAX analysis confirmed the chemical composition. Anti-cancer studies verified the efficacy of Fe<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span>O<span><math><msub><mrow></mrow><mrow><mn>3</mn></mrow></msub></math></span> NPs in cell viability and cell death when compared with Cisplatin. Finally, a NaI(Tl) detector is used to evaluate Mass attenuation co-efficient of the X-ray and gamma radiation shielding characteristics. Shielding requirements are comparable to those for lead. Thus, the synthesized Fe<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span>O<span><math><msub><mrow></mrow><mrow><mn>3</mn></mrow></msub></math></span> nanoparticles can be used for anticancer activities, particularly in tailored drug delivery systems, and radiation shielding instead of toxic lead shielding.</p></div>","PeriodicalId":36067,"journal":{"name":"Physics Open","volume":"17 ","pages":"Article 100188"},"PeriodicalIF":0.0,"publicationDate":"2023-10-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2666032623000534/pdfft?md5=7a7ed66cc107b0d6220d688eaa4770e0&pid=1-s2.0-S2666032623000534-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"92100892","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-10-09DOI: 10.1016/j.physo.2023.100185
A.V. Mahesh Babu , N. Sowmya , H.C. Manjunatha , N. Dhananjaya
We investigated 253Cf ternary fission followed by a light-charged particle (LCP) accompanied ternary fission. The many LCPs, include He, Li, Be 10B, 12C, 14N, 16O, 19F 20Ne, 23Na 24Mg, 26Al, 28Si, 30P 32S, 35Cl, 40Ar, 39K and 40Ca. Using Coulomb potential and proximity potential, the overall potential has been investigated. In estimating potential, deformations and angle of orientation were taken into account. Using cold valley plots, the driving potential at its lowest level is determined. Using WKB integral, the penetration probability is evaluated. When the fission fragment combinations include equal or close to the magic number of protons or neutrons, the minimal driving potential, maximum penetration probability, and maximum logT are observed. Therefore, 138Ba+4He+111Ru are the most likely fission fragment combination when 253Cf undergoes LCP followed ternary fission. Therefore, He particle-emission coupled with two likely fission fragments are the most likely fission fragments if the nuclei 253Cf undergo LCP-accompanied ternary fission. The significance of this finding may thus be seen in the ternary fission half-lives.
{"title":"A study on light charged particle accompanied ternary fission of 253Cf","authors":"A.V. Mahesh Babu , N. Sowmya , H.C. Manjunatha , N. Dhananjaya","doi":"10.1016/j.physo.2023.100185","DOIUrl":"https://doi.org/10.1016/j.physo.2023.100185","url":null,"abstract":"<div><p>We investigated <sup>253</sup>Cf ternary fission followed by a light-charged particle (LCP) accompanied ternary fission. The many LCPs, include <span><math><msup><mrow></mrow><mrow><mn>4</mn></mrow></msup></math></span>He, <span><math><msup><mrow></mrow><mrow><mn>6</mn></mrow></msup></math></span>Li, <span><math><msup><mrow></mrow><mrow><mn>9</mn></mrow></msup></math></span>Be <sup>10</sup>B, <sup>12</sup>C, <sup>14</sup>N, <sup>16</sup>O, <sup>19</sup>F <sup>20</sup>Ne, <sup>23</sup>Na <sup>24</sup>Mg, <sup>26</sup>Al, <sup>28</sup>Si, <sup>30</sup>P <sup>32</sup>S, <sup>35</sup>Cl, <sup>40</sup>Ar, <sup>39</sup>K and <sup>40</sup>Ca. Using Coulomb potential and proximity potential, the overall potential has been investigated. In estimating potential, deformations and angle of orientation were taken into account. Using cold valley plots, the driving potential at its lowest level is determined. Using WKB integral, the penetration probability is evaluated. When the fission fragment combinations include equal or close to the magic number of protons or neutrons, the minimal driving potential, maximum penetration probability, and maximum logT<span><math><msub><mrow></mrow><mrow><mn>1</mn><mo>/</mo><mn>2</mn></mrow></msub></math></span> are observed. Therefore, <sup>138</sup>Ba+<sup>4</sup>He+<sup>111</sup>Ru are the most likely fission fragment combination when <sup>253</sup>Cf undergoes LCP followed ternary fission. Therefore, <span><math><msup><mrow></mrow><mrow><mn>4</mn></mrow></msup></math></span>He particle-emission coupled with two likely fission fragments are the most likely fission fragments if the nuclei <sup>253</sup>Cf undergo LCP-accompanied ternary fission. The significance of this finding may thus be seen in the ternary fission half-lives.</p></div>","PeriodicalId":36067,"journal":{"name":"Physics Open","volume":"17 ","pages":"Article 100185"},"PeriodicalIF":0.0,"publicationDate":"2023-10-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"49753322","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-10-06DOI: 10.1016/j.physo.2023.100186
G. Poongodi , A. Chandrasekaran , V. Sathish , S. Karthikayini , A. Tamilarasi , Mayeen Uddin Khandaker
Natural gamma radiation exposure to humans can possess significant health risks when exposed either externally or internally. Though risks are not established at low doses, the exposure levels are set based on conservative approach. In this work, 22 bore-well rock samples were collected from the agricultural area of Dharmapuri district, Tamil Nadu to evaluate the radiation exposure to humans living in that area using a gamma-ray spectrometer. The results shows that, the activity concentration of 238U ranges from MDA to 87±2 Bq kg−1 with an average value of 25 Bq kg−1, and for 232Th it ranges from MDA to 10±2 Bq kg−1, and for the 40K it ranges from 167±9 to 669±10 Bq kg−1 with the mean value of 310 Bq kg−1. The various radiological parameters are calculated and compared with the world-recommended limit to assess the radiation hazards. To identify the relation among the natural radioisotopes, Pearson correlation analysis was performed between the radiological variables. It reveales that radionuclides 238U and 232Th strongly correlated with each other and radiological parameters. This implies that 238U and 232Th originated from the same source and 40K was derived from different sources.
{"title":"Gamma-ray spectrometric analysis of bore-well rock samples from agricultural area of Tamil Nadu","authors":"G. Poongodi , A. Chandrasekaran , V. Sathish , S. Karthikayini , A. Tamilarasi , Mayeen Uddin Khandaker","doi":"10.1016/j.physo.2023.100186","DOIUrl":"https://doi.org/10.1016/j.physo.2023.100186","url":null,"abstract":"<div><p>Natural gamma radiation exposure to humans can possess significant health risks when exposed either externally or internally. Though risks are not established at low doses, the exposure levels are set based on conservative approach. In this work, 22 bore-well rock samples were collected from the agricultural area of Dharmapuri district, Tamil Nadu to evaluate the radiation exposure to humans living in that area using a gamma-ray spectrometer. The results shows that, the activity concentration of <sup>238</sup>U ranges from MDA to 87±2 Bq kg<sup>−1</sup> with an average value of 25 Bq kg<sup>−1</sup>, and for <sup>232</sup>Th it ranges from MDA to 10±2 Bq kg<sup>−1</sup>, and for the <sup>40</sup>K it ranges from 167±9 to 669±10 Bq kg<sup>−1</sup> with the mean value of 310 Bq kg<sup>−1</sup>. The various radiological parameters are calculated and compared with the world-recommended limit to assess the radiation hazards. To identify the relation among the natural radioisotopes, Pearson correlation analysis was performed between the radiological variables. It reveales that radionuclides <sup>238</sup>U and <sup>232</sup>Th strongly correlated with each other and radiological parameters. This implies that <sup>238</sup>U and <sup>232</sup>Th originated from the same source and <sup>40</sup>K was derived from different sources.</p></div>","PeriodicalId":36067,"journal":{"name":"Physics Open","volume":"17 ","pages":"Article 100186"},"PeriodicalIF":0.0,"publicationDate":"2023-10-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"49753318","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-09-27DOI: 10.1016/j.physo.2023.100184
Mitali Sisodia, Joyee Ghosh
In this study, we have theoretically presented a prepare-and-measure based SARG04 protocol over free-space. It has been shown that the highest secret key rate is achievable even under free-space losses with a maximum noise tolerance.
{"title":"Prepare-and-measure based QKD protocol under free-space losses","authors":"Mitali Sisodia, Joyee Ghosh","doi":"10.1016/j.physo.2023.100184","DOIUrl":"https://doi.org/10.1016/j.physo.2023.100184","url":null,"abstract":"<div><p>In this study, we have theoretically presented a prepare-and-measure based SARG04 protocol over free-space. It has been shown that the highest secret key rate is achievable even under free-space losses with a maximum noise tolerance.</p></div>","PeriodicalId":36067,"journal":{"name":"Physics Open","volume":"17 ","pages":"Article 100184"},"PeriodicalIF":0.0,"publicationDate":"2023-09-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"49752846","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-09-15DOI: 10.1016/j.physo.2023.100182
Vinayak Anand Kamat , H.M. Somashekarappa
In this study, ethylene propylene diene monomer (EPDM)-lead monoxide (PbO)-magnetite (Fe3O4) composite was prepared and changes in its properties with different gamma irradiation doses (50, 100, 200, 300, 500, and 1000 kGy) were investigated. Characterizations of irradiated EPDM-metal oxide composites were performed by X-ray Diffractometer (XRD), Field Emission Scanning Electron Microscope (FESEM) and Universal Testing Machine (UTM). It was observed that the synthesized sample shows an amorphous nature beyond the 500 kGy irradiation dose. The FESEM morphographs of irradiated samples show an increase in fracture size with an increase in irradiation dose. The mechanical tests have shown that prepared samples retain their mechanical strength up to ∼100 kGy. In addition, the effect of thermal and electrical properties on irradiation dose has also been studied. The synthesized samples show good thermal stability up to ∼500 kGy. The AC conductivity of the synthesized EPDM-metal oxide composites has been observed to increase slightly with an increase in irradiation dose. It was observed that synthesized EPDM-metal oxide composites are relatively good radiation resistant candidates and can be used for radioactive waste disposal management applications.
{"title":"Study of ethylene propylene diene monomer-lead monoxide-magnetite composites in radioactive waste disposal","authors":"Vinayak Anand Kamat , H.M. Somashekarappa","doi":"10.1016/j.physo.2023.100182","DOIUrl":"https://doi.org/10.1016/j.physo.2023.100182","url":null,"abstract":"<div><p>In this study, ethylene propylene diene monomer (EPDM)-lead monoxide (PbO)-magnetite (Fe<sub>3</sub>O<sub>4</sub>) composite was prepared and changes in its properties with different gamma irradiation doses (50, 100, 200, 300, 500, and 1000 kGy) were investigated. Characterizations of irradiated EPDM-metal oxide composites were performed by X-ray Diffractometer (XRD), Field Emission Scanning Electron Microscope (FESEM) and Universal Testing Machine (UTM). It was observed that the synthesized sample shows an amorphous nature beyond the 500 kGy irradiation dose. The FESEM morphographs of irradiated samples show an increase in fracture size with an increase in irradiation dose. The mechanical tests have shown that prepared samples retain their mechanical strength up to ∼100 kGy. In addition, the effect of thermal and electrical properties on irradiation dose has also been studied. The synthesized samples show good thermal stability up to ∼500 kGy. The AC conductivity of the synthesized EPDM-metal oxide composites has been observed to increase slightly with an increase in irradiation dose. It was observed that synthesized EPDM-metal oxide composites are relatively good radiation resistant candidates and can be used for radioactive waste disposal management applications.</p></div>","PeriodicalId":36067,"journal":{"name":"Physics Open","volume":"17 ","pages":"Article 100182"},"PeriodicalIF":0.0,"publicationDate":"2023-09-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"49753317","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-09-15DOI: 10.1016/j.physo.2023.100183
P. Chaithra, B. Ramesh Krishna, Nagaraja Kamsali
The ionosphere is a region of the upper atmosphere where free electrons and ions are created by solar radiation. An effort is made to study the solar radiation influence on the earth's ionosphere's total electron content (TEC) across the low latitude Indian subcontinent from January to October 2022. TEC readings were obtained using GNSS receivers over Bengaluru (13.021 °N, 77.570 °E) and Hyderabad (17.417 °N, 78.551 °E). Ionospheric TEC variations are studied by measuring the degree to which satellite-sent GPS signals are disrupted. The results were compared with geomagnetic measurements such as disturbed storm time (Dst) index and planetary K-index (Kp) and analyzed with TEC anomalies during geomagnetic storms, and the results may be used to estimate the magnetic field of the Earth. The study revealed that ionospheric storms had an advantageous impact in January, March, and April of 2022, but a negative effect in July 2022.
{"title":"Influence of solar radiation on ionosphere over India","authors":"P. Chaithra, B. Ramesh Krishna, Nagaraja Kamsali","doi":"10.1016/j.physo.2023.100183","DOIUrl":"https://doi.org/10.1016/j.physo.2023.100183","url":null,"abstract":"<div><p>The ionosphere is a region of the upper atmosphere where free electrons and ions are created by solar radiation. An effort is made to study the solar radiation influence on the earth's ionosphere's total electron content (TEC) across the low latitude Indian subcontinent from January to October 2022. TEC readings were obtained using GNSS receivers over Bengaluru (13.021 °N, 77.570 °E) and Hyderabad (17.417 °N, 78.551 °E). Ionospheric TEC variations are studied by measuring the degree to which satellite-sent GPS signals are disrupted. The results were compared with geomagnetic measurements such as disturbed storm time (Dst) index and planetary K-index (Kp) and analyzed with TEC anomalies during geomagnetic storms, and the results may be used to estimate the magnetic field of the Earth. The study revealed that ionospheric storms had an advantageous impact in January, March, and April of 2022, but a negative effect in July 2022.</p></div>","PeriodicalId":36067,"journal":{"name":"Physics Open","volume":"17 ","pages":"Article 100183"},"PeriodicalIF":0.0,"publicationDate":"2023-09-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"49767510","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-09-14DOI: 10.1016/j.physo.2023.100180
Vasudha G.S. , N. Sowmya , H.C. Manjunatha , D. Prakash Babu , Nagaiah N. , Mayeen Khandekar , Krishnakanth E. , R. Soundar
In inverse kinematics, we explored Coulomb fission cross-sections and time scales. Heavier projectiles such as 238U, 132Xe, and 208Pb on lighter targets such as 16O 26Mg, 27Al, 32S, 35Cl, Ca, 45Sc, Ti, Fe, 64Ni, 89Y, 30Si and 65Zn were looked into. The photofission cross-sections and the number of equivalent photons impinge on the target nuclei are important parameters in cross-section assessment. The anticipated cross-sections increases with increase in atomic number of target nuclei. We also explored the time scale of projectile nuclei at various transition levels. The estimated time scales accord well with the available experimental value, which is in the order of picoseconds. In addition, we predicted time scales of 165Ho nuclei in the transition state from to for which experimental time scales are not available in literature. As a result, Coulomb fission is one of the causes that has severely hampered in the formation of compound nuclei. Prediction of time scales, in particular, would aid in understanding the structure of various energy levels.
{"title":"Investigations on Coulomb fission time scales and cross sections in inverse kinematics","authors":"Vasudha G.S. , N. Sowmya , H.C. Manjunatha , D. Prakash Babu , Nagaiah N. , Mayeen Khandekar , Krishnakanth E. , R. Soundar","doi":"10.1016/j.physo.2023.100180","DOIUrl":"https://doi.org/10.1016/j.physo.2023.100180","url":null,"abstract":"<div><p>In inverse kinematics, we explored Coulomb fission cross-sections and time scales. Heavier projectiles such as <sup>238</sup>U, <sup>132</sup>Xe, and <sup>208</sup>Pb on lighter targets such as <sup>16</sup>O <sup>26</sup>Mg, <sup>27</sup>Al, <sup>32</sup>S, <sup>35</sup>Cl, <span><math><msup><mrow></mrow><mrow><mn>40</mn><mo>,</mo><mn>48</mn></mrow></msup></math></span>Ca, <sup>45</sup>Sc, <span><math><msup><mrow></mrow><mrow><mn>48</mn><mo>,</mo><mn>50</mn></mrow></msup></math></span>Ti, <span><math><msup><mrow></mrow><mrow><mn>56</mn><mo>,</mo><mn>58</mn></mrow></msup></math></span>Fe, <sup>64</sup>Ni, <sup>89</sup>Y, <sup>30</sup>Si and <sup>65</sup>Zn were looked into. The photofission cross-sections and the number of equivalent photons impinge on the target nuclei are important parameters in cross-section assessment. The anticipated cross-sections increases with increase in atomic number of target nuclei. We also explored the time scale of projectile nuclei at various transition levels. The estimated time scales accord well with the available experimental value, which is in the order of picoseconds. In addition, we predicted time scales of <sup>165</sup>Ho nuclei in the transition state from <span><math><mrow><mn>19</mn><mo>/</mo><msup><mrow><mn>2</mn></mrow><mrow><mo>+</mo></mrow></msup><mo>→</mo><mn>15</mn><mo>/</mo><msup><mrow><mn>2</mn></mrow><mrow><mo>+</mo></mrow></msup></mrow></math></span> to <span><math><mrow><mn>29</mn><mo>/</mo><msup><mrow><mn>2</mn></mrow><mrow><mo>+</mo></mrow></msup><mo>→</mo><mn>25</mn><mo>/</mo><msup><mrow><mn>2</mn></mrow><mrow><mo>+</mo></mrow></msup></mrow></math></span> for which experimental time scales are not available in literature. As a result, Coulomb fission is one of the causes that has severely hampered in the formation of compound nuclei. Prediction of time scales, in particular, would aid in understanding the structure of various energy levels.</p></div>","PeriodicalId":36067,"journal":{"name":"Physics Open","volume":"17 ","pages":"Article 100180"},"PeriodicalIF":0.0,"publicationDate":"2023-09-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"49752845","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Quantum point contacts (QPC) are the building blocks of quantum dot qubits and semiconducting quantum electrical metrology circuits. QPCs also make highly sensitive electrical amplifiers with the potential to operate in the quantum-limited regime. Though the inherent operational bandwidth of QPCs can eclipse the THz regime, the impedance mismatch with the external circuitry limits the operational frequency to a few kHz. Lumped-element impedance-matching circuits are successful only up to a few hundreds of MHz in frequency. QPCs are characterised by a complex impedance consisting of quantized resistance, capacitance, and inductance elements. Characterising the complex admittance at higher frequencies and understanding the coupling of QPC to other circuit elements and electromagnetic environments will provide valuable insight into its sensing and backaction properties. In this work, we couple a QPC galvanically to a superconducting stub tuner impedance matching circuit realised in a coplanar waveguide architecture to enhance the operation frequency into the GHz regime and investigate the electrical amplification and complex admittance characteristics. The device, operating at ∼ exhibits a conductance sensitivity of with a bandwidth of . Besides, the RF reflected power unambiguously reveals the complex admittance characteristics of the QPC, shining more light on the behaviour of quantum tunnel junctions at higher operational frequencies.
{"title":"GHz operation of a quantum point contact using stub-impedance matching circuit","authors":"Anusha Shanmugam , Prasanta Kumbhakar , Harikrishnan Sundaresan , Annu Anns Sunny , J.L. Reno , Madhu Thalakulam","doi":"10.1016/j.physo.2023.100181","DOIUrl":"10.1016/j.physo.2023.100181","url":null,"abstract":"<div><p>Quantum point contacts (QPC) are the building blocks of quantum dot qubits and semiconducting quantum electrical metrology circuits. QPCs also make highly sensitive electrical amplifiers with the potential to operate in the quantum-limited regime. Though the inherent operational bandwidth of QPCs can eclipse the THz regime, the impedance mismatch with the external circuitry limits the operational frequency to a few kHz. Lumped-element impedance-matching circuits are successful only up to a few hundreds of MHz in frequency. QPCs are characterised by a complex impedance consisting of quantized resistance, capacitance, and inductance elements. Characterising the complex admittance at higher frequencies and understanding the coupling of QPC to other circuit elements and electromagnetic environments will provide valuable insight into its sensing and backaction properties. In this work, we couple a QPC galvanically to a superconducting stub tuner impedance matching circuit realised in a coplanar waveguide architecture to enhance the operation frequency into the GHz regime and investigate the electrical amplification and complex admittance characteristics. The device, operating at ∼ <span><math><mn>1</mn><mo>.</mo><mn>96</mn><mspace></mspace><mi>G</mi><mi>H</mi><mi>z</mi><mo>,</mo></math></span> exhibits a conductance sensitivity of <span><math><mrow><mn>2.92</mn><mo>×</mo><msup><mn>10</mn><mrow><mo>−</mo><mn>5</mn></mrow></msup><msup><mrow><mo>(</mo><mi>e</mi></mrow><mn>2</mn></msup><mo>/</mo><mi>h</mi><mo>)</mo><mo>/</mo><msqrt><mrow><mi>H</mi><mi>z</mi></mrow></msqrt></mrow></math></span> with a bandwidth of <span><math><mrow><mn>13</mn><mspace></mspace><mi>M</mi><mi>H</mi><mi>z</mi></mrow></math></span>. Besides, the RF reflected power unambiguously reveals the complex admittance characteristics of the QPC, shining more light on the behaviour of quantum tunnel junctions at higher operational frequencies.</p></div>","PeriodicalId":36067,"journal":{"name":"Physics Open","volume":"17 ","pages":"Article 100181"},"PeriodicalIF":0.0,"publicationDate":"2023-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"46694445","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}