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This set‐up provides the possibility to perform μSR measurements on samples with diameter of 12 mm and length of 35 mm in the temperature regime 3.7\\Eleq T\\Eleq 800\\ K at hydrostatic pressures up to 800 MPa. Results for high‐pressure μSR experiments on Ni and \\alpha ‐Fe are presented.",{"EN":229},"Pressure cell and combined cryostat\u002Ffurnace for high‐pressure μSR studies",{"VOID":231},"T. Butz, G.M. Kalvius, B. Lindgren, O. Hartmann, R. Wäppling and E. Karlsson, Hyp. Int. 32 (1986) 881.\nA. Kratzer, K. Mutzbauer, S. Henneberger, G.M. Kalvius, O. Hartmann, R. Wäppling, H.-H. Klauß, M.A.C. De Melo, F.J. Litterst and Th. Stammler, Hyp. Int. 87 (1994) 1055.\nTh. Stammler, W. Beez, T. Grund, M. Hampele, M. Iwanowski, A. Kratzer, G.M. Kalvius, J. Major, M. Notter, R. Scheuermann, L. Schimmele and A. Seeger, PSI Annual Report 1993, Annex I, Villigen, Switzerland (1994) 99.\nTh. Stammler, Hochdruck-µSR-Untersuchungen an Nickel und Eisen, Dr. rer. nat. 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Laser heating is used to extract gas from mg-size samples. A cryogenic sample concentrator is employed. Atoms continuously condense on a 75 K stainless steel substrate at the back plate of a Wiley-McLaren laser ion source from where they are desorbed by a pulsed 1064 nm laser and resonantly ionized in the plume. A three-colour (116.5 nm, 558.1 nm and 1064 nm) excitation scheme is used. Tuneable coherent Vacuum Ultraviolet (vuv) radiation near 116.5 nm is generated by four-wave sum frequency mixing of 252.5 nm and 1507 nm pulsed dye laser beams in a binary mixture of negatively and positively dispersive gases (Xe and Ar). Isotope effects have been observed that reduce the reproducibility of isotope ratio measurements between odd-mass, non-zero nuclear spin isotopes and even-mass, zero nuclear spin isotopes. This can be minimised and stabilised by controlling the laser fluences, experimental geometry, and the population of the magnetic sub-levels of the excited atomic states used in the ionisation process. Once stability is achieved, sample-standard bracketing (during which the known isotope ratios of a standard are determined before and after the measurements of the sample under the same conditions) allows precision and reproducibility of \n                  \n                    \n                  \n                  $\\sim $\n                1 % for the major isotope ratios to be achieved in samples \n                  \n                    \n                  \n                  $\\sim 10^{6}$\n                 krypton atoms. Detection limits of \n                  \n                    \n                  \n                  $\u003C1000$\n                 atoms\u002Fisotope have been demonstrated, ratios of \n                  \n                    \n                  \n                  $^{81}$\n                Kr in meteorites have been made with \n                  \n                    \n                  \n                  $\\sim $\n                5–10 % precision. 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Its principal advantages in extracting the mode magnitudes and distribution widths of weak nuclear electric quadrupole splittings much less than the magnetic inhomogeneous broadening are its simplicity and generality requiring no assumptions on the degree of adiabaticity of the nuclear spin motion during sweep through the quadrupolar split subresonances. The technique is applied to a concentrated single crystal sample of60CoFe which failed to yield a well resolved mid passage signal to conventional single passage NMR\u002FON. The result is an asymmetric frequency distribution of quadrupole frequencies with a mode value of P=3e2qQ\u002F4I (2I-1)=+4.5 ±1.0 kHz and half maxima of +2.5 kHz and +7.0 kHz.",{"EN":912},"The extraction of weak nuclear electric quadrupole splittings of dilute impurities in ferromagnets using modulated Adiabatic Passage NMR\u002FON",{"VOID":914},"[\"11766929788245223542\"]",{"VOID":916},"P.T. Callaghan, P.D. Johnston, W.M. Lattimer and N.J. Stone, Phys. Rev. B12 (1975) 3526.\nP.T. Callaghan, P.D. Johnston and N.J. Stone, J. Phys. C7 (1974) 3161.\nE. Hagn and E. Zech, Phys. Rev. B25 (1982) 1521.\nE. Hagn and E. Zech, Phys. Rev. B25 (1982) 1529.\nP.T. Callaghan, W.M. Lattimer, N.J. Stone and P.D. Johnston, Hyp. Int. 2 (1976) 291.\nP.D. Johnston and N.J. Stone, J. Phys. C5 (1972) L303.\nP.T. Callaghan, W.M. Lattimer, P.D. Johnston and N.J. Stone, Hyp. Int. 2 (1976) 288.\nE. Hagn and E. Zech, Z. Phys. A307 (1982) 159.\nE. Hagn and E. Zech, Phys. Rev. B29 (1984) 1148.\nW.M. Lattimer, D. Phil. Clarendon Laboratory, Oxford, 1976.\nR.A. Pax, D.H. Chaplin, H.R. Foster and G.V.H. Wilson, contributed paper, this conference.\nA. Abragam, The Principles of Nuclear Magnetism, (Oxford University Press, Oxford, 1961) p.233.\nN.J. Stone, Hyp. Int. 8 (1980) 83.\nJ.A. Barclay, C.G. Don, P. Lloyd, C.F. Osborne and G.V.H.Wilson J. Phys. F1 (1971) 960.\nR. Kieser and B.G. Turrell, Solid State Comm. 17 (1975) 423.\nP.J. Back, D.H. Chaplin, H.R. Foster, G.A. 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The study was performed with the WIEN97 implementation of the FP-LAPW method. In order to simulate the diluted Cd-impurity in the SnO2 host and to calculate the electronic structure of the system we used a 72-atoms super-cell, studying the relaxation introduced by the impurity in the lattice. The free-relaxation process performed shows that the relaxations of the oxygen nearest-neighbors of the impurity are not isotropic. Our prediction for the EFG tensor are compared with experimental results and point-charge model predictions.",{"EN":1057},"FP-LAPW Calculations of the EFG at Cd Impurities in Rutile SnO2",{"VOID":1059},"[\"7981657350935807513\"]",{"EN":1061},"",{"VOID":1063},"10.1023\u002FA:1020593831852","2024-05-06T03:45:28.487+00:00",[735],"https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1023\u002FA:1020593831852",[1068,1085,1100],{"id":1069,"sortIndex":21,"researcher":20,"roles":1070,"affiliations":1071,"properties":1080,"displayName":1082,"givenName":20,"familyName":20},"c8af34c2-3c49-4888-bf51-4fb5564abed3",[],[1072],{"id":1073,"sortIndex":21,"affiliation":1074,"properties":20},"a104c2aa-d4e5-4b6f-9fd8-aac6596984ab",{"id":1073,"createTime":20,"updateTime":20,"relativeEntities":1075,"slug":20,"properties":1076,"entityType":20,"verifyStatus":20,"verifyTime":20,"verifyNote":20,"languages":20,"translateLanguages":20,"viewCount":20,"url":20,"parentIds":1079,"statistic":20},[],{"title":1077},{"EN":1078},"Instituto de Física La Plata (IFLP-CONICET) – Departamento de Física, Facultad de Ciencias Exactas, Universidad Nacional de La Plata, La Plata, Argentina",[],{"title":1081,"gsAuthor":1083},{"EN":1082},"L. 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Naturforsch. A 53 (1998), 396.",{"id":20,"text":1168,"url":20,"identifiers":20},"Lany, S., Blaha, P., Hamann, J., Ostheimer, V., Wolf, H. and Wichert, T.,Phys. Rev. B 62 (2000), R2260.",{"id":20,"text":1170,"url":20,"identifiers":20},"Errico, L. A., Fabricius, G. and Rentería, M., Z. Naturfosch. A 55 (2000), 267. Erratum of this article, Z. Naturfosch. A 55 (2000), 983.",{"id":20,"text":1172,"url":20,"identifiers":20},"Errico, L., Fabricius, G. and Rentería, M., to be published.",{"id":20,"text":1174,"url":20,"identifiers":20},"Wenzel, Th., Bartos, A., Lieb, K. P., Uhrmacher, M. and Wiarda, D., Ann. Physik 1 (1992), 155.",{"id":20,"text":1176,"url":20,"identifiers":20},"Adams, J. M. and Catchen, G. L., Phys. Rev. B B50 (1994), 1264.",{"id":20,"text":1178,"url":20,"identifiers":20},"Rentería, M., Bibiloni, A. G., Moreno, M. S., Desimoni, J., Mercader, R. C., Bartos, A., Uhrmacher, M. and Lieb, K. P., J. Phys.: Condens. Matt. 3 (1991), 3625.",{"id":20,"text":1180,"url":20,"identifiers":20},"Blaha, P., Schwarz, K., Dufek, P. and Luitz, J., Wien97, Vienna University of Technology, 1997. Improved and updated Unix version of the original copyrighted Wien-code, which was published by P.Blaha, K. Schwarz, P. I. Sorantin and S. B. Trickey in Comput. Phys. Commun. 59 (1990), 399.",{"id":20,"text":1182,"url":20,"identifiers":20},"Wei, S. H. and Krakauer, H., Phys. Rev. Lett. 55 (1985), 1200.",{"id":20,"text":1184,"url":20,"identifiers":20},"Perdew, J. P. and Wang, Y., Phys. Rev. B 45 (1992), 13244.",{"id":20,"text":1186,"url":20,"identifiers":20},"Yu, R., Singh, D. and Krakauer, H., Phys. Rev. B 43 (1991), 6411.",{"id":20,"text":1188,"url":20,"identifiers":20},"Kohler, B., Wilker, S., Scheffler, M., Kouba, R. and Ambrosch-Draxl, C., Comput. Phys. Commun. 94 (1996), 31.",{"id":20,"text":1190,"url":20,"identifiers":20},"Schwarz, K., Ambrosch-Draxl, C. and Blaha, P., Phys. Rev. B 42 (1990), 2051.",{"id":20,"text":1192,"url":20,"identifiers":20},"Bolzan, A., Fong, C., Kennedy, B. and Howard, C., Acta Cryst. B 53 (1997), 373.",{"id":20,"text":1194,"url":20,"identifiers":20},"Hill, R. and Howard, C., J. Appl. Cryst. 20 (1987), 467.",{"id":1196,"createTime":1197,"updateTime":1198,"relativeEntities":1199,"slug":1200,"properties":1201,"entityType":234,"verifyStatus":235,"verifyTime":1212,"verifyNote":237,"languages":20,"translateLanguages":20,"viewCount":21,"primaryUrl":1213,"fullTextUrl":20,"authors":1214,"publicationType":335,"publisherRelationship":1256,"citationCount":21,"citationInfo":1304,"publishDate":1307,"publishYear":1305,"citationAnalyzeStatus":1044,"lastCitationAnalyze":1308,"indexDatabases":1309,"openAccess":20,"references":20,"isForceReanalyzing":388},"7d17f903-8e02-4bb0-8106-02805a081885","2024-02-07T17:37:34.254+00:00","2026-07-30T01:46:00.748+00:00",[],"Interpretation-of-the-119Sn-M%C3%B6ssbauer-parameters",{"abstract":1202,"title":1204,"gsPaper":1206,"references":1208,"doi":1210},{"EN":1203},"The variations of the 119Sn Mössbauer isomer shift δ are interpreted for tin compounds from a semi-empirical tight-binding calculation of the electronic density at the nucleus ρ(0). A molecular model is proposed in order to relate the variations of ρ(0) for the Sn(IV) chalcogenides to the changes in the Sn environment. The variations of the experimental values of the quadrupole splitting δ are linearly correlated to the values of the electric field gradients (EFG) calculated by the full-potential linearized-augmented-plane-wave (FP-LAPW) method. The value of the 119Sn nuclear quadrupole moment is found to be |Q| = 10.5 ± 0.2 fm2. Finally, the relation between the EFG and the Sn environment is discussed for SnO.",{"EN":1205},"Interpretation of the 119Sn Mössbauer parameters",{"VOID":1207},"[\"14987942524002242834\"]",{"VOID":1209},"G.K. Shenoy and F.E. Wagner, eds., Mössbauer Isomer Shifts (North-Holland, Amsterdam, 1978).\nM. Grodzicki, V. Männing, A.X. Trautwein and J.M. Friedt, J. Phys. B 20 (1987) 5595.\nJ. Terra and D. Guenzburger, J. Phys. Condens. Matter 3 (1991) 6763.\nA. Svane, N.E. Christensen, C.O. Rodriguez and M. Methfessel, Phys. Rev. B 55 (1997) 12572.\nH. Haas, M. Menningen, H. Andreasen, S. Damgaard, H. Grann, F.T. Pedersen, J.W. Petersen and G. Weyer, Hyp. Interact. 15\u002F16 (1983) 215.\nP. Blaha, K. Schwarz and J. Luitz, in: WIEN'97, Vienna University of Technology, Vienna (1997); P. Blaha, K. Schwarz, P. Sorantin and S.B. Trickey, Comp. Phys. Commun. 59 (1990) 399.\nP. Blaha, K. Schwarz and P. Herzig, Phys. Rev. Lett. 54 (1985) 1192.\nP. Blaha, K. Schwarz and P.H. Dederichs, Phys. Rev. B 37 (1988) 2792.\nK. Schwarz, C. Ambrosch-Draxl and P. Blaha, Phys. Rev. B 42 (1990) 2051.\nP.E. Lippens, Phys. Rev. B 60 (1999) 4576.\nS.L. Ruby and G.K. Shenoy, in [1, chapter 9b].\nJ.C. Slater and G.F. Koster, Phys. Rev. 94 (1954) 1494.\nP.E. Lippens, J. Olivier-Fourcade, J.C. Jumas, S. Dupont, A. Gheorghiu and C. Sénémaud, Phys. Rev. B 56 (1997) 13054.\nJ. Pannetier and G. Denes, Acta Crystallogr. B 36 (1980) 2763.",{"VOID":1211},"10.1023\u002FA:1012653014106","2024-05-16T11:13:35.743+00:00","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1023\u002FA:1012653014106",[1215,1230,1243],{"id":1216,"sortIndex":21,"researcher":20,"roles":1217,"affiliations":1218,"properties":1227,"displayName":1229,"givenName":20,"familyName":20},"4340fcea-c7eb-4fd9-8f66-bea0b552ce84",[243],[1219],{"id":1220,"sortIndex":21,"affiliation":1221,"properties":20},"66e73fa2-3a3b-4f6f-b01e-6b3905fdf351",{"id":1220,"createTime":20,"updateTime":20,"relativeEntities":1222,"slug":20,"properties":1223,"entityType":20,"verifyStatus":20,"verifyTime":20,"verifyNote":20,"languages":20,"translateLanguages":20,"viewCount":20,"url":20,"parentIds":1226,"statistic":20},[],{"title":1224},{"VI":1225},"Laboratoire des Agrégats Moléculaires et Matériaux Inorganiques, CNRS UMR 5072, Université Montpellier II, Montpellier Cédex 05, France",[],{"title":1228},{"VI":1229},"P.E. 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The ion beams used are 100 MeV 127I and 180 MeV 197Au. The specimens were irradiated at fluences ranging from 3 × 1012 to 1.5 × 1014 ions\u002Fcm2. The irradiations have been carried out at temperatures 100 and 300 K. The magnetic moments are sensitive towards the irradiation conditions such as irradiation temperature and stopping power of incident ion beam. The irradiation-induced effects have been monitored, by using Mössbauer spectroscopy. The modifications in magnetic anisotropy and hyperfine magnetic field distributions, as an effect of different irradiation temperature as well as different stopping power have been discussed. After irradiation, all the samples remain amorphous and magnetic anisotropy considerably changes from its original in-plane direction. The results show enhancement in magnetic anisotropy in the specimen irradiated at 100 K, as compared to that of irradiated at 300 K. It is expected that at low temperature, the stresses produced in the material would remain un-annealed, compared to the samples irradiated at room temperature and therefore, the modification in magnetic anisotropy would be enhanced. A distribution of hyperfine magnetic field, of the samples irradiated at low temperature, show a small but distinct peak at ∼ 11 Tesla, indicating Fe-B pairing.",{"EN":1320},"Mössbauer study of ferromagnetic metallic glasses irradiated by swift heavy ions at temperatures 100 and 300 K",{"VOID":1322},"[\"8573344648942489943\"]",{"VOID":1324},"Audarrdo, A., Balanzat, E., Bouffard, S., Jousset, J.C., Chamberod, A., Dunlop, A., Lesueur, D., Fuchs, G., Sphor, R., Vetter, J., Thome, L.: Evidence for amorphization of a metallic alloy by ion electronic energy loss. Phys. Rev. Lett. 65, 875–878 (1990)\nDammak, A., Barbu, A., Dunlop, A., Lesueuer, D., Lorenzelli, N.: α − ω phase transformation induced in titanium during ion irradiations in the electronic slowing-down regime. Phil. Mag. Lett. 67A, 253–259 (1993)\nDunlop, A., Lesueur, D., Jaskierowicz, G., Schildknecht, J.: Influence of very high electronic energy losses on defect configurations in self-ion irradiated iron. Nucl. Instr. And Meth. B 36, 412–419 (1989)\nPaumier, E., Toulemonde, M., Dural, J., Rullier-Albenque, F., Girard, J.P., Bogdanski, P.: Anomalous enhancement in defect production in gallium irradiated by high-energy xenon. Ions. Europhys. Let. 10, 555–561 (1989)\nStuder, F., Houpart, Ch., Groult, D., Yun Fan, J., Meftah, A., Toulemonde, M.: Spontaneous magnetization induced in the spinel ZnFe2O4 by heavy ion irradiation in the electronic stopping power regime. Nucl. Instr. Meth. B 82, 91–102 (1993)\nToulemonde, M., Fuchs, G., Studer, F., Groult, D.: Damage processes and magnetic field orientation in ferrimagnetic oxides Y3Fe5O12 and BaFe12O19 irradiated by high-energy heavy ions: a Mössbauer study. Phys. Rev. B 35, 6560–6569 (1987)\nJuraszek, J., Fnidiki, A., Toulemonde, M.: Induced magnetic anisotropy in metallic glasses irradiated by swift heavy ions. J. Appl. Phys. 89, 3151–3154 (2001)\nMeillon, S., Studer, F., Hervieu, M., Pascard, H.: Changes in magnetic properties of magnetite Fe3O4 ceramics induced by high-energy heavy ion irradiation. Nucl. Instr. Meth. B 107, 363–367 (1996)\nAmrute, K.V., Mhatre, U.R., Sinha, S.K., Kothari, D.C., Nagrajan, R., Kanjilal, D.: Modification of magnetic anisotropy in metallic glasses using high-energy ion beam irradiation. PRAMANA-J. 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