{"status":"ok","message-type":"work-list","message-version":"1.0.0","message":{"facets":{},"total-results":184904,"items":[{"indexed":{"date-parts":[[2024,6,5]],"date-time":"2024-06-05T14:23:49Z","timestamp":1717597429106},"reference-count":10,"publisher":"AIP Publishing","issue":"13","content-domain":{"domain":["pubs.aip.org"],"crossmark-restriction":true},"published-print":{"date-parts":[[1967,12,1]]},"abstract":"<jats:p>The results of an experimental study of the absorption properties of Cs as present in Cs-Ar low-pressure discharges under various discharge conditions are presented. The total Cs concentration at zero discharge current was varied between 1.5 and 15\u00d71012 cm\u22123. Absorption was measured in the 4555-\u00c5 and 8521-\u00c5 lines of Cs from which the stationary concentration of Cs (62S1\/2) could be derived. Special attention was paid to determine the Cs concentration as the discharge changed from a low-burning voltage mode to a high-burning voltage mode. The pronounced variations of the discharge properties were found to be accompanied by rather drastic changes of the Cs concentration for which variations of a factor of ten or more were found.<\/jats:p>","DOI":"10.1063\/1.1709276","type":"journal-article","created":{"date-parts":[[2005,1,15]],"date-time":"2005-01-15T15:15:01Z","timestamp":1105802101000},"page":"5062-5065","update-policy":"http:\/\/dx.doi.org\/10.1063\/aip-crossmark-policy-page","source":"Crossref","is-referenced-by-count":4,"title":["Optical Determination of Cs Ground-State Depletion in Cs-Ar Low-Pressure dc Discharges"],"prefix":"10.1063","volume":"38","author":[{"given":"R.","family":"Bleekrode","sequence":"first","affiliation":[{"name":"Philips Research Laboratories, N. V. Philips' Gloeilampenfabrieken, Eindhoven, Netherlands"}]}],"member":"317","reference":[{"key":"2024020210150138100_r1","doi-asserted-by":"crossref","first-page":"124","DOI":"10.1063\/1.1754875","volume":"10","year":"1967","journal-title":"Appl. Phys. Letters"},{"key":"2024020210150138100_r2","first-page":"209","volume":"22","year":"1967","journal-title":"Philips Res. Rept."},{"key":"2024020210150138100_r3","doi-asserted-by":"crossref","first-page":"357","DOI":"10.1016\/0022-4073(66)90081-1","volume":"6","year":"1966","journal-title":"J. Quant. Spectr. Radiative Transfer"},{"key":"2024020210150138100_r4","first-page":"211","volume":"20","year":"1966","journal-title":"Opt. Spectr."},{"key":"2024020210150138100_r5"},{"key":"2024020210150138100_r6"},{"key":"2024020210150138100_r7"},{"key":"2024020210150138100_r8","doi-asserted-by":"crossref","first-page":"1151","DOI":"10.1103\/PhysRev.127.1151","volume":"127","year":"1962","journal-title":"Phys. Rev."},{"key":"2024020210150138100_r9"},{"key":"2024020210150138100_r10","doi-asserted-by":"crossref","first-page":"352","DOI":"10.1063\/1.1728209","volume":"10","year":"1967","journal-title":"Appl. Phys. Letters"}],"container-title":["Journal of Applied Physics"],"language":"en","link":[{"URL":"https:\/\/pubs.aip.org\/aip\/jap\/article-pdf\/38\/13\/5062\/18344079\/5062_1_online.pdf","content-type":"application\/pdf","content-version":"vor","intended-application":"syndication"},{"URL":"https:\/\/pubs.aip.org\/aip\/jap\/article-pdf\/38\/13\/5062\/18344079\/5062_1_online.pdf","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2024,2,2]],"date-time":"2024-02-02T10:57:56Z","timestamp":1706871476000},"score":19.009222,"resource":{"primary":{"URL":"https:\/\/pubs.aip.org\/jap\/article\/38\/13\/5062\/507950\/Optical-Determination-of-Cs-Ground-State-Depletion"}},"issued":{"date-parts":[[1967,12,1]]},"references-count":10,"journal-issue":{"issue":"13","published-print":{"date-parts":[[1967,12,1]]}},"URL":"https:\/\/doi.org\/10.1063\/1.1709276","ISSN":["0021-8979","1089-7550"],"issn-type":[{"value":"0021-8979","type":"print"},{"value":"1089-7550","type":"electronic"}],"published-other":{"date-parts":[[1967,12]]},"published":{"date-parts":[[1967,12,1]]}},{"indexed":{"date-parts":[[2024,6,5]],"date-time":"2024-06-05T14:15:55Z","timestamp":1717596955000},"reference-count":7,"publisher":"AIP Publishing","issue":"6","content-domain":{"domain":["pubs.aip.org"],"crossmark-restriction":true},"published-print":{"date-parts":[[1969,5,1]]},"abstract":"<jats:p>The radial and axial distributions of Cs ground-state (62S1\/2) atoms in Cs\u2013Ar low-pressure discharges are studied by absorption spectroscopy. The results show that there is appreciable Cs-atom depletion at the center of the discharge. Within experimental accuracy the Cs(62S1\/2) concentration is found to be constant over the whole length of the positive column of the discharge.<\/jats:p>","DOI":"10.1063\/1.1658004","type":"journal-article","created":{"date-parts":[[2004,2,9]],"date-time":"2004-02-09T16:56:16Z","timestamp":1076345776000},"page":"2401-2403","update-policy":"http:\/\/dx.doi.org\/10.1063\/aip-crossmark-policy-page","source":"Crossref","is-referenced-by-count":20,"title":["Optical Determination of Cs Ground-State Depletion in Cs\u2013Ar Low-Pressure Discharges. II. Radial and Axial Cs-Atom Distributions"],"prefix":"10.1063","volume":"40","author":[{"given":"R.","family":"Bleekrode","sequence":"first","affiliation":[{"name":"Philips Research Laboratories, N. V. Philips' Gloeilampenfabrieken, Eindhoven, Netherlands"}]},{"given":"J. W. V. D.","family":"Laarse","sequence":"additional","affiliation":[{"name":"Philips Research Laboratories, N. V. Philips' Gloeilampenfabrieken, Eindhoven, Netherlands"}]}],"member":"317","reference":[{"key":"2024020201142072400_r1","doi-asserted-by":"crossref","first-page":"5062","DOI":"10.1063\/1.1709276","volume":"38","year":"1967","journal-title":"J. Appl. Phys."},{"key":"2024020201142072400_r2","first-page":"210","volume":"13II","year":"1968","journal-title":"Bull. Amer. Phys. Soc."},{"key":"2024020201142072400_r3","doi-asserted-by":"crossref","first-page":"2403","DOI":"10.1063\/1.1658005","volume":"40","year":"1969","journal-title":"J. Appl. Phys."},{"key":"2024020201142072400_r4","doi-asserted-by":"crossref","first-page":"1151","DOI":"10.1103\/PhysRev.127.1151","volume":"127","year":"1962","journal-title":"Phys. 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Rep."}],"container-title":["Journal of Applied Physics"],"language":"en","link":[{"URL":"https:\/\/pubs.aip.org\/aip\/jap\/article-pdf\/40\/6\/2401\/18350193\/2401_1_online.pdf","content-type":"application\/pdf","content-version":"vor","intended-application":"syndication"},{"URL":"https:\/\/pubs.aip.org\/aip\/jap\/article-pdf\/40\/6\/2401\/18350193\/2401_1_online.pdf","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2024,2,2]],"date-time":"2024-02-02T01:14:28Z","timestamp":1706836468000},"score":18.957573,"resource":{"primary":{"URL":"https:\/\/pubs.aip.org\/jap\/article\/40\/6\/2401\/166568\/Optical-Determination-of-Cs-Ground-State-Depletion"}},"issued":{"date-parts":[[1969,5,1]]},"references-count":7,"journal-issue":{"issue":"6","published-print":{"date-parts":[[1969,5,1]]}},"URL":"https:\/\/doi.org\/10.1063\/1.1658004","ISSN":["0021-8979","1089-7550"],"issn-type":[{"value":"0021-8979","type":"print"},{"value":"1089-7550","type":"electronic"}],"published-other":{"date-parts":[[1969,5]]},"published":{"date-parts":[[1969,5,1]]}},{"indexed":{"date-parts":[[2024,2,4]],"date-time":"2024-02-04T23:27:06Z","timestamp":1707089226319},"reference-count":8,"publisher":"AIP Publishing","issue":"4","content-domain":{"domain":["pubs.aip.org"],"crossmark-restriction":true},"published-print":{"date-parts":[[1973,4,1]]},"abstract":"<jats:p>Radial distributions of the 62P excited-state density of Cs in low-pressure Cs\u2013Ar discharges have been measured by means of absorption from a continuum in the 876.1- and 917.2-nm lines of Cs. The variation of the excited-state densities with the discharge current has also been studied. The experimental data are compared with results of calculations based on a model of the positive column of the Cs\u2013Ar discharge in which radiation trapping is taken into account.<\/jats:p>","DOI":"10.1063\/1.1662494","type":"journal-article","created":{"date-parts":[[2004,2,4]],"date-time":"2004-02-04T17:26:28Z","timestamp":1075915588000},"page":"1941-1942","update-policy":"http:\/\/dx.doi.org\/10.1063\/aip-crossmark-policy-page","source":"Crossref","is-referenced-by-count":6,"title":["Measured and calculated Cs excited-state densities in Cs\u2013Ar low-pressure discharges"],"prefix":"10.1063","volume":"44","author":[{"given":"R.","family":"Bleekrode","sequence":"first","affiliation":[{"name":"Philips Research Laboratories, Eindhoven-The Netherlands"}]},{"given":"H.","family":"van Tongeren","sequence":"additional","affiliation":[{"name":"Philips Research Laboratories, Eindhoven-The Netherlands"}]}],"member":"317","reference":[{"key":"2024020204332133000_r1","doi-asserted-by":"crossref","first-page":"317","DOI":"10.1016\/0375-9601(71)90688-8","volume":"37","year":"1971","journal-title":"Phys. Lett. A"},{"key":"2024020204332133000_r2","doi-asserted-by":"crossref","first-page":"2401","DOI":"10.1063\/1.1658004","volume":"40","year":"1969","journal-title":"J. Appl. Phys."},{"key":"2024020204332133000_r3","doi-asserted-by":"crossref","first-page":"352","DOI":"10.1063\/1.1728209","volume":"10","year":"1967","journal-title":"Appl. Phys. Lett."},{"key":"2024020204332133000_r4"},{"key":"2024020204332133000_r5","doi-asserted-by":"crossref","first-page":"669","DOI":"10.1364\/JOSA.58.000669","volume":"58","year":"1968","journal-title":"J. Opt. Soc. Am."},{"key":"2024020204332133000_r6"},{"key":"2024020204332133000_r7","doi-asserted-by":"crossref","first-page":"1303","DOI":"10.1103\/PhysRevA.4.1303","volume":"4","year":"1971","journal-title":"Phys. Rev. A"},{"key":"2024020204332133000_r8","doi-asserted-by":"crossref","first-page":"2403","DOI":"10.1063\/1.1658005","volume":"40","year":"1969","journal-title":"J. Appl. Phys."}],"container-title":["Journal of Applied Physics"],"language":"en","link":[{"URL":"https:\/\/pubs.aip.org\/aip\/jap\/article-pdf\/44\/4\/1941\/18363581\/1941_1_online.pdf","content-type":"application\/pdf","content-version":"vor","intended-application":"syndication"},{"URL":"https:\/\/pubs.aip.org\/aip\/jap\/article-pdf\/44\/4\/1941\/18363581\/1941_1_online.pdf","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2024,2,2]],"date-time":"2024-02-02T04:33:30Z","timestamp":1706848410000},"score":18.656744,"resource":{"primary":{"URL":"https:\/\/pubs.aip.org\/jap\/article\/44\/4\/1941\/8226\/Measured-and-calculated-Cs-excited-state-densities"}},"issued":{"date-parts":[[1973,4,1]]},"references-count":8,"journal-issue":{"issue":"4","published-print":{"date-parts":[[1973,4,1]]}},"URL":"https:\/\/doi.org\/10.1063\/1.1662494","ISSN":["0021-8979","1089-7550"],"issn-type":[{"value":"0021-8979","type":"print"},{"value":"1089-7550","type":"electronic"}],"published-other":{"date-parts":[[1973,4]]},"published":{"date-parts":[[1973,4,1]]}},{"indexed":{"date-parts":[[2024,10,5]],"date-time":"2024-10-05T04:06:48Z","timestamp":1728101208656},"reference-count":0,"publisher":"Dostoevsky Omsk State University","issue":"4","content-domain":{"domain":[],"crossmark-restriction":false},"short-container-title":["CS"],"published-print":{"date-parts":[[2023]]},"abstract":"<jats:p>Modern brand marketing communications are characterized by a high level of digitalization, which implies both the digitalization of promotion tools and digitalization of business processes. The increase in the degree of brands presence in digital environment gives grounds for scientific and practical reflection on the problems of \u201cdigital brand\u201d development. Immersive technologies (virtual, augmented, mixed reality) are considered as forms of brand communication digitalization with target audiences. These technologies allow clients to \u201cimmerse\u201d in another (virtual) world, to feel brand atmosphere. This paper focuses on the specifics of augmented reality technology in \u201cbrand - audience\u201d communication, which fully reflects the philosophy of phygital marketing, where the customer's journey is associated with constant \u201cshifts\u201d from the physical world to digital world. Foreign experts designate AR-marketing as a separate area in the structure of marketing communications of a brand. The integration of physical promotion tools and augmented reality tools allows us to demonstrate the benefits of goods and services, promotes optimal choice, and forms necessary emotional connection of a brand with the representatives of its target audience. At the same time, a number of aspects of augmented reality technologies related to the audience interaction with branded augmented reality require specification; the nature of augmented reality influence on consumer decision-making; ways to involve consumers in communication based on augmented reality; changes in audience's attitude towards a brand as a result of interaction with branded augmented reality.<\/jats:p>","DOI":"10.24147\/2413-6182.2023.10(4).786-799","type":"journal-article","created":{"date-parts":[[2024,10,4]],"date-time":"2024-10-04T06:12:18Z","timestamp":1728022338000},"page":"786-799","source":"Crossref","is-referenced-by-count":0,"title":["AR-marketing as a form of digitalization of \u201cbrand - audience\u201d communication"],"prefix":"10.24147","volume":"10","author":[{"given":"Andrey Vasilievich","family":"Prokhorov","sequence":"first","affiliation":[]}],"member":"31781","published-online":{"date-parts":[[2023]]},"container-title":["Communication studies"],"original-title":["AR-\u043c\u0430\u0440\u043a\u0435\u0442\u0438\u043d\u0433 \u043a\u0430\u043a \u0444\u043e\u0440\u043c\u0430 \u0446\u0438\u0444\u0440\u043e\u0432\u0438\u0437\u0430\u0446\u0438\u0438 \u043a\u043e\u043c\u043c\u0443\u043d\u0438\u043a\u0430\u0446\u0438\u0438 \"\u0431\u0440\u0435\u043d\u0434 - \u0430\u0443\u0434\u0438\u0442\u043e\u0440\u0438\u044f\""],"deposited":{"date-parts":[[2024,10,4]],"date-time":"2024-10-04T06:12:24Z","timestamp":1728022344000},"score":18.398476,"resource":{"primary":{"URL":"https:\/\/com-studies-journal.omsu.ru\/issues\/371\/11059.php"}},"issued":{"date-parts":[[2023]]},"references-count":0,"journal-issue":{"issue":"4","published-online":{"date-parts":[[2023]]},"published-print":{"date-parts":[[2023]]}},"URL":"https:\/\/doi.org\/10.24147\/2413-6182.2023.10(4).786-799","ISSN":["2413-6182"],"issn-type":[{"value":"2413-6182","type":"print"}],"published":{"date-parts":[[2023]]}},{"indexed":{"date-parts":[[2026,4,5]],"date-time":"2026-04-05T18:28:32Z","timestamp":1775413712438,"version":"3.50.1"},"reference-count":12,"publisher":"AIP Publishing","issue":"6","content-domain":{"domain":["pubs.aip.org"],"crossmark-restriction":true},"published-print":{"date-parts":[[1978,3,15]]},"abstract":"<jats:p>The mobilities of Cs+ ions in Ar, Kr, and Xe gases at 300\u2009\u00b0K have been measured in a drift tube mass spectrometer for a wide range of values of the energy parameter E\/N (the ratio of the electric field strength to the gas number density). Ion neutral interaction potentials have also been derived for each case (Cs+\u2013Ar, Cs+\u2013Kr, and Cs+\u2013Xe). A kinetic theory appropriate to the nonthermalized ion motion is used to derive the mobilities from the potentials, and an iterative technique is used to modify the potentials to fit the experimental data. Various tests of the accuracy and uniqueness of the method indicate that this determination of the potentials gives errors in the potential parameters, e.g., well depth, well position, etc., which are less than about 10%.<\/jats:p>","DOI":"10.1063\/1.436069","type":"journal-article","created":{"date-parts":[[2003,2,27]],"date-time":"2003-02-27T22:38:05Z","timestamp":1046385485000},"page":"2775-2778","update-policy":"https:\/\/doi.org\/10.1063\/aip-crossmark-policy-page","source":"Crossref","is-referenced-by-count":52,"title":["Mobilities and interaction potentials for Cs+\u2013Ar, Cs+\u2013Kr, and Cs+\u2013Xe"],"prefix":"10.1063","volume":"68","author":[{"given":"I. R.","family":"Gatland","sequence":"first","affiliation":[{"name":"School of Physics, Georgia Institute of Technology, Atlanta, Georgia 30332"}]},{"given":"M. G.","family":"Thackston","sequence":"additional","affiliation":[{"name":"School of Physics, Georgia Institute of Technology, Atlanta, Georgia 30332"}]},{"given":"W. M.","family":"Pope","sequence":"additional","affiliation":[{"name":"School of Physics, Georgia Institute of Technology, Atlanta, Georgia 30332"}]},{"given":"F. L.","family":"Eisele","sequence":"additional","affiliation":[{"name":"School of Physics, Georgia Institute of Technology, Atlanta, Georgia 30332"}]},{"given":"H. W.","family":"Ellis","sequence":"additional","affiliation":[{"name":"School of Physics, Georgia Institute of Technology, Atlanta, Georgia 30332"}]},{"given":"E. W.","family":"McDaniel","sequence":"additional","affiliation":[{"name":"School of Physics, Georgia Institute of Technology, Atlanta, Georgia 30332"}]}],"member":"317","reference":[{"key":"2024020916254602900_r1","doi-asserted-by":"crossref","first-page":"499","DOI":"10.1016\/0003-4916(75)90233-X","volume":"91","year":"1975","journal-title":"Ann. Phys. (NY)"},{"key":"2024020916254602900_r2"},{"key":"2024020916254602900_r3","doi-asserted-by":"crossref","first-page":"537","DOI":"10.1063\/1.433973","volume":"66","year":"1977","journal-title":"J. Chem. Phys."},{"key":"2024020916254602900_r4","doi-asserted-by":"crossref","first-page":"5121","DOI":"10.1063\/1.433771","volume":"66","year":"1977","journal-title":"J. Chem. Phys."},{"key":"2024020916254602900_r5","first-page":"2404","volume":"58","year":"1973","journal-title":"J. Chem. Phys."},{"key":"2024020916254602900_r6"},{"key":"2024020916254602900_r7","first-page":"369","volume":"4","year":"1974","journal-title":"Case Stud. At. Phys."},{"key":"2024020916254602900_r8"},{"key":"2024020916254602900_r9","doi-asserted-by":"crossref","first-page":"433","DOI":"10.1016\/S0301-0104(76)80007-9","volume":"17","year":"1976","journal-title":"Chem. Phys."},{"key":"2024020916254602900_r10","doi-asserted-by":"crossref","first-page":"211","DOI":"10.1016\/0031-8914(74)90236-5","volume":"73","year":"1974","journal-title":"Physica (Utr.)"},{"key":"2024020916254602900_r11"},{"key":"2024020916254602900_r12","doi-asserted-by":"crossref","first-page":"328","DOI":"10.1016\/0021-9991(70)90065-3","volume":"5","year":"1970","journal-title":"J. Comput. 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Photoexcitation of the B 2\u03a3+ \u2212 X 2\u03a3+ molecular transition (i.e., the blue satellite of the D2 transition) at 836.7\u2009nm (Cs-Ar), 841.1\u2009nm (Cs-Kr), or 842.7\u2009nm (Cs-Xe) yields lasers at 852.1\u2009nm whose characteristics (optical-to-optical conversion efficiencies, pump energy threshold, and temperature dependence) are a reflection of the structure of the B 2\u03a3+ interatomic potential associated with each Cs-rare gas pair. Output pulse energies above 100 \u03bcJ are obtained from the Cs-Ar complex in the 493\u2013513\u2009K interval because of the height of the B 2\u03a3+ barrier in the Franck-Condon region for the pump, a molecular parameter also responsible for the robust temperature stability of the laser. Slope efficiencies (with respect to absorbed pump energy) of 17%, 12%, and 27% have been measured for Cs-Ar, Cs-Kr, and Cs-Xe pairs at 473\u2009K, 453\u2009K, and 453\u2009K, respectively. 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The measurements have been made with electrostatic probes and with a microwave interferometer. At a low discharge current cesium alone is ionized. When the discharge current is increased the cesium atom density is reduced by ionization and radial diffusion, and at a critical current a discontinuous transition to a state having a high electron temperature is observed. This discontinuity is explained as the result of a multivaluedness of the electric field as a function of the current density. 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