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58
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44649185995
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The divergence in degrees of the neutron beam from the guide is 0.23λ for λ in angstroms.
-
The divergence in degrees of the neutron beam from the guide is 0.23λ for λ in angstroms.
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59
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44649183093
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The mosaic spreads of the samples were much less than the divergence of the neutron beam incident on the sample.
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The mosaic spreads of the samples were much less than the divergence of the neutron beam incident on the sample.
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60
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44649138984
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The largest neutron beam on Asterix is 5×5 cm2.
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The largest neutron beam on Asterix is 5×5 cm2.
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61
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44649181882
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See
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See http://www.ncnr.nist.gov/instruments/bt9/
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44649106108
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The relation is valid for small or Gaussian-distributed values of dλ λ and dθcotθ. Given the Gaussian profile of the (100) Bragg reflection, the relation is reasonable to use.
-
The relation is valid for small or Gaussian-distributed values of dλ λ and dθcotθ. Given the Gaussian profile of the (100) Bragg reflection, the relation is reasonable to use.
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-
-
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66
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44649109324
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The σm typically increases with λ below 6 Å and then saturates.
-
The σm typically increases with λ below 6 Å and then saturates.
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67
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44649175447
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Note that the Bragg reflection from the graphite sample is highly asymmetric in Fig. 8 -typical of an instrumental-resolution-limited intensity profile. In contrast, the Bragg reflection from the Zn0.30 Fe0.70 F2 sample in Fig. 7 is broadened yielding a more symmetric intensity profile.
-
Note that the Bragg reflection from the graphite sample is highly asymmetric in Fig. 8 -typical of an instrumental-resolution-limited intensity profile. In contrast, the Bragg reflection from the Zn0.30 Fe0.70 F2 sample in Fig. 7 is broadened yielding a more symmetric intensity profile.
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68
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44649152070
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This experiment allowed us to demonstrate the combination of inelastic scattering and reflectometry with an energy resolution of 30 μeV.
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This experiment allowed us to demonstrate the combination of inelastic scattering and reflectometry with an energy resolution of 30 μeV.
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71
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44649146868
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Since the (100) wave vector lies 45° from the sample's surface normal, the dimension of the domains corresponds to this direction (i.e., a dimension that is neither purely perpendicular nor parallel to the sample's surface).
-
Since the (100) wave vector lies 45° from the sample's surface normal, the dimension of the domains corresponds to this direction (i.e., a dimension that is neither purely perpendicular nor parallel to the sample's surface).
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72
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The in-plane microstrain can not be measured with GIXD for either of the Zn0.30 Fe0.70 F2 or the Ni0.55 Fe0.45 F2 films because the Co and Al overlayers are so thick that the x-ray beam is absorbed by the overlayers.
-
The in-plane microstrain can not be measured with GIXD for either of the Zn0.30 Fe0.70 F2 or the Ni0.55 Fe0.45 F2 films because the Co and Al overlayers are so thick that the x-ray beam is absorbed by the overlayers.
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74
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44649193621
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The strain term is 25% of the domain-size term.
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The strain term is 25% of the domain-size term.
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75
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0003470014
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Holt, Rinehart, and Winston, New York
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44649110595
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The observation of a (100) AF Bragg reflection for the Co/ Ni0.45 Fe0.55 F2 sample means that the (100) planes have a net ferromagnetic moment that is not consistent with the AF structure of bulk NiF2.
-
The observation of a (100) AF Bragg reflection for the Co/ Ni0.45 Fe0.55 F2 sample means that the (100) planes have a net ferromagnetic moment that is not consistent with the AF structure of bulk NiF2.
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85
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44649156775
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The difference between TB and TN is significant provided the thermometry used in the SQUID and neutron experiment performed similarly (both used calibrated Cernox sensors). A better approach would be to measure the temperature dependencies of the exchange bias with polarized neutron reflectometry and TN with neutron diffraction using the same thermometer-measurements planned for the future with Asterix.
-
The difference between TB and TN is significant provided the thermometry used in the SQUID and neutron experiment performed similarly (both used calibrated Cernox sensors). A better approach would be to measure the temperature dependencies of the exchange bias with polarized neutron reflectometry and TN with neutron diffraction using the same thermometer-measurements planned for the future with Asterix.
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-
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86
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44649163632
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We note that in Refs., it was concluded the size of the domain of uncompensated magnetization in the AF affected the sign and magnitude of exchange bias. This dimension is not the AF domain size we discuss in the present paper. The AF domain size refers to the size of the domain over which long range order of the AF spin lattice exists.
-
We note that in Refs., it was concluded the size of the domain of uncompensated magnetization in the AF affected the sign and magnitude of exchange bias. This dimension is not the AF domain size we discuss in the present paper. The AF domain size refers to the size of the domain over which long range order of the AF spin lattice exists.
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87
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M. R. Fitzsimmons, C. Leighton, J. Nogués, A. Hoffmann, K. Liu, C. F. Majkrzak, J. A. Dura, J. R. Groves, R. W. Springer, and P. N. Arendt, V. Leiner, H. Lauter, and I. K. Schuller, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.65.134436 65, 134436 (2002).
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Groves, J.R.8
Springer, R.W.9
Arendt, P.N.10
Leiner, V.11
Lauter, H.12
Schuller, I.K.13
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