Pub Date : 1958-05-01DOI: 10.1016/0369-643X(58)90120-8
N. Sarma
{"title":"Thin carbon films for use with electrostatic accelerators","authors":"N. Sarma","doi":"10.1016/0369-643X(58)90120-8","DOIUrl":"10.1016/0369-643X(58)90120-8","url":null,"abstract":"","PeriodicalId":100970,"journal":{"name":"Nuclear Instruments","volume":"2 4","pages":"Pages 361-362"},"PeriodicalIF":0.0,"publicationDate":"1958-05-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0369-643X(58)90120-8","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"81943133","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 : 1958-04-01DOI: 10.1016/0369-643X(58)90040-9
M.J. Poole, G. Dean, W. Howe
A method has been developed to permit the simultaneous use of two targets with a pulsed linear electron accelerator. A magnet is arranged to deflect the beam onto one or the other target, and this magnet is electronically switched on or off in the interval between the beam pulses. A“ccount-down” circuit is used to select which pulses shall be directed to each target.
{"title":"Pulsed beam deflection system for a linear electron accelerator","authors":"M.J. Poole, G. Dean, W. Howe","doi":"10.1016/0369-643X(58)90040-9","DOIUrl":"10.1016/0369-643X(58)90040-9","url":null,"abstract":"<div><p>A method has been developed to permit the simultaneous use of two targets with a pulsed linear electron accelerator. A magnet is arranged to deflect the beam onto one or the other target, and this magnet is electronically switched on or off in the interval between the beam pulses. A“ccount-down” circuit is used to select which pulses shall be directed to each target.</p></div>","PeriodicalId":100970,"journal":{"name":"Nuclear Instruments","volume":"2 3","pages":"Pages 282-286"},"PeriodicalIF":0.0,"publicationDate":"1958-04-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0369-643X(58)90040-9","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"86687705","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 : 1958-04-01DOI: 10.1016/0369-643X(58)90036-7
O. Almén, G. Bruce, A. Lundén
A 90° electromagnetic isotope separator with a beam radius of 100 cm is described. Using an acceleration voltage of 50 kV, ion currents of up to a few hundred μA can be handled. The ion current and resolving power can be varied within wide limits by adjusting the position of the lens system during operation. Two types of magnetic ion sources have been used to prepare targets for nuclear reaction studies and samples for beta- and gamma-ray spectroscopy.
{"title":"Electromagnetic isotope separator in Gothenburg","authors":"O. Almén, G. Bruce, A. Lundén","doi":"10.1016/0369-643X(58)90036-7","DOIUrl":"10.1016/0369-643X(58)90036-7","url":null,"abstract":"<div><p>A 90° electromagnetic isotope separator with a beam radius of 100 cm is described. Using an acceleration voltage of 50 kV, ion currents of up to a few hundred μA can be handled. The ion current and resolving power can be varied within wide limits by adjusting the position of the lens system during operation. Two types of magnetic ion sources have been used to prepare targets for nuclear reaction studies and samples for beta- and gamma-ray spectroscopy.</p></div>","PeriodicalId":100970,"journal":{"name":"Nuclear Instruments","volume":"2 3","pages":"Pages 249-250"},"PeriodicalIF":0.0,"publicationDate":"1958-04-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0369-643X(58)90036-7","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"75411056","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 : 1958-04-01DOI: 10.1016/0369-643X(58)90037-9
C. Cernigoi , G. Pauli , C. Poiani
The fast ionization chamber, 60 l in volume, filled with argon at 10 atm, is described. The pulse shapes are calculated assuming the ionization: (a) confined to an infinitesimal volume of the chamber, (b) distributed along a straight line parallel to the axis of the chamber, (c) distributed along a straight line passing through the axis of the chamber and perpendicular to it, (d) distributed along a straight line perpendicular to the axis of the chamber and not passing through it, (e) distributed throughout the volume of the chamber.
A comparison is made between the theoretical pulse shapes and the experimental ones.
{"title":"On the pulse shape in a cylindrical ionization chamber","authors":"C. Cernigoi , G. Pauli , C. Poiani","doi":"10.1016/0369-643X(58)90037-9","DOIUrl":"10.1016/0369-643X(58)90037-9","url":null,"abstract":"<div><p>The fast ionization chamber, 60 l in volume, filled with argon at 10 atm, is described. The pulse shapes are calculated assuming the ionization: (a) confined to an infinitesimal volume of the chamber, (b) distributed along a straight line parallel to the axis of the chamber, (c) distributed along a straight line passing through the axis of the chamber and perpendicular to it, (d) distributed along a straight line perpendicular to the axis of the chamber and not passing through it, (e) distributed throughout the volume of the chamber.</p><p>A comparison is made between the theoretical pulse shapes and the experimental ones.</p></div>","PeriodicalId":100970,"journal":{"name":"Nuclear Instruments","volume":"2 3","pages":"Pages 261-269"},"PeriodicalIF":0.0,"publicationDate":"1958-04-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0369-643X(58)90037-9","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"73286764","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 : 1958-04-01DOI: 10.1016/0369-643X(58)90033-1
J. Flinta
{"title":"Pulsed high-intensity ion source: Part I☆","authors":"J. Flinta","doi":"10.1016/0369-643X(58)90033-1","DOIUrl":"https://doi.org/10.1016/0369-643X(58)90033-1","url":null,"abstract":"","PeriodicalId":100970,"journal":{"name":"Nuclear Instruments","volume":"23 1","pages":"219-226"},"PeriodicalIF":0.0,"publicationDate":"1958-04-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"76946806","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 : 1958-04-01DOI: 10.1016/0369-643X(58)90039-2
J.S. Fraser, J.C.D. Milton
An apparatus has been constructed to measure the velocities of both members of a fission-fragment pair. A zero-time signal is obtained at the expense of about one per cent of the fragment energy by detecting delta rays ejected by the fragment from a thin plastic foil placed near the source. The fragment times of flight are converted to pulse heights for analysis. An overall time resolution of 3.5 mμsec is obtained. A third variable, e.g. gamma-ray energy or prompt neutron time of flight, may also be recorded, the three pulse heights being punched consecutively on paper tape. Three-dimensional analysis is therefore possible but in practice sorting is done taking two variables at a time.
{"title":"Automatic-recording apparatus for fission-fragment time-of-flight measurements","authors":"J.S. Fraser, J.C.D. Milton","doi":"10.1016/0369-643X(58)90039-2","DOIUrl":"10.1016/0369-643X(58)90039-2","url":null,"abstract":"<div><p>An apparatus has been constructed to measure the velocities of both members of a fission-fragment pair. A zero-time signal is obtained at the expense of about one per cent of the fragment energy by detecting delta rays ejected by the fragment from a thin plastic foil placed near the source. The fragment times of flight are converted to pulse heights for analysis. An overall time resolution of 3.5 mμsec is obtained. A third variable, e.g. gamma-ray energy or prompt neutron time of flight, may also be recorded, the three pulse heights being punched consecutively on paper tape. Three-dimensional analysis is therefore possible but in practice sorting is done taking two variables at a time.</p></div>","PeriodicalId":100970,"journal":{"name":"Nuclear Instruments","volume":"2 3","pages":"Pages 275-281"},"PeriodicalIF":0.0,"publicationDate":"1958-04-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0369-643X(58)90039-2","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"84281495","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 : 1958-04-01DOI: 10.1016/0369-643X(58)90035-5
R.B. Murray
The scintillation response of europium activated crystals of Li6I to neutrons in the energy range 1–14MeV has been investigated with the crystals maintained at various temperatures. The pulse-height spectrum from mono-energetic neutrons incident on a crystal at room temperature demonstrates a poorly defined and broad fast-neutron peak. Upon cooling the crystal, the fast-neutron peak becomes sharper and assumes a nearly Gaussian shape at temperatures below about — 140° C. This behaviour is attributed to an increased scintillation efficiency of LiI(Eu) to alpha particles at low temperatures. Pulse-height spectra from crystals at the liquid nitrogen point are presented for neutrons from the D(d,n)He3, T(d,n)He4, and Be9(d,n)B10 reactions, a Po-Be source, and U235 fission. The principal features of Li6I(Eu) as a fast-neutron spectrometer are a relatively high detection efficiency (≈0.1%) and moderate resolution.
{"title":"Use of Li6I(Eu) as a scintillation detector and spectrometer for fast neutrons","authors":"R.B. Murray","doi":"10.1016/0369-643X(58)90035-5","DOIUrl":"10.1016/0369-643X(58)90035-5","url":null,"abstract":"<div><p>The scintillation response of europium activated crystals of Li<sup>6</sup>I to neutrons in the energy range 1–14MeV has been investigated with the crystals maintained at various temperatures. The pulse-height spectrum from mono-energetic neutrons incident on a crystal at room temperature demonstrates a poorly defined and broad fast-neutron peak. Upon cooling the crystal, the fast-neutron peak becomes sharper and assumes a nearly Gaussian shape at temperatures below about — 140° C. This behaviour is attributed to an increased scintillation efficiency of LiI(Eu) to alpha particles at low temperatures. Pulse-height spectra from crystals at the liquid nitrogen point are presented for neutrons from the D(d,n)He<sup>3</sup>, T(d,n)He<sup>4</sup>, and Be<sup>9</sup>(d,n)B<sup>10</sup> reactions, a Po-Be source, and U<sup>235</sup> fission. The principal features of Li<sup>6</sup>I(Eu) as a fast-neutron spectrometer are a relatively high detection efficiency (≈0.1%) and moderate resolution.</p></div>","PeriodicalId":100970,"journal":{"name":"Nuclear Instruments","volume":"2 3","pages":"Pages 237-248"},"PeriodicalIF":0.0,"publicationDate":"1958-04-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0369-643X(58)90035-5","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"83189612","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 : 1958-04-01DOI: 10.1016/0369-643X(58)90038-0
E. Bujdosó , L. Medveczky
The authors built an apparatus for processing nuclear emulsions. Its functioning is shown by describing the processing of an Agfa K2 emulsion of 200 μ thickness.
作者研制了一种处理核乳剂的装置。通过描述200 μ厚度的爱克发K2乳液的加工过程来说明其功能。
{"title":"Apparatus for processing nuclear emulsions","authors":"E. Bujdosó , L. Medveczky","doi":"10.1016/0369-643X(58)90038-0","DOIUrl":"10.1016/0369-643X(58)90038-0","url":null,"abstract":"<div><p>The authors built an apparatus for processing nuclear emulsions. Its functioning is shown by describing the processing of an Agfa K2 emulsion of 200 μ thickness.</p></div>","PeriodicalId":100970,"journal":{"name":"Nuclear Instruments","volume":"2 3","pages":"Pages 270-274"},"PeriodicalIF":0.0,"publicationDate":"1958-04-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0369-643X(58)90038-0","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"75941003","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 : 1958-04-01DOI: 10.1016/0369-643X(58)90033-1
Jan Flinta
The first part of this publication deals with the limitations of the discharge current, extraction of ions and focusing of large ion current beams. Three types of ion sources are described and their data are given.
The second part†† deals with detailed investigation of the characteristics of the discharge of the Penning type. For this purpose a special ion source was build which allowed for the exchange of all inner parts.
{"title":"Pulsed high-intensity ion source","authors":"Jan Flinta","doi":"10.1016/0369-643X(58)90033-1","DOIUrl":"https://doi.org/10.1016/0369-643X(58)90033-1","url":null,"abstract":"<div><p>The first part of this publication deals with the limitations of the discharge current, extraction of ions and focusing of large ion current beams. Three types of ion sources are described and their data are given.</p><p>The second part<sup>††</sup> deals with detailed investigation of the characteristics of the discharge of the Penning type. For this purpose a special ion source was build which allowed for the exchange of all inner parts.</p></div>","PeriodicalId":100970,"journal":{"name":"Nuclear Instruments","volume":"2 3","pages":"Pages 219-226"},"PeriodicalIF":0.0,"publicationDate":"1958-04-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0369-643X(58)90033-1","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"92109465","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}