2011
DOI: 10.1063/1.3608114
|View full text |Cite
|
Sign up to set email alerts
|

Design and commissioning of a high magnetic field muon spin relaxation spectrometer at the ISIS pulsed neutron and muon source

Abstract: Use policyThe full-text may be used and/or reproduced, and given to third parties in any format or medium, without prior permission or charge, for personal research or study, educational, or not-for-pro t purposes provided that:• a full bibliographic reference is made to the original source • a link is made to the metadata record in DRO • the full-text is not changed in any way The full-text must not be sold in any format or medium without the formal permission of the copyright holders.Please consult the full … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

0
28
0

Year Published

2014
2014
2024
2024

Publication Types

Select...
7

Relationship

2
5

Authors

Journals

citations
Cited by 33 publications
(28 citation statements)
references
References 18 publications
0
28
0
Order By: Relevance
“…Indeed, the peak is larger than the expected variation in background in this field range. If we interpret the data in this way then, assuming linear variation of A ( t =0) either side of the crossing, we estimate this occurs with a centre at B cross =3.73(5) T. Since we expect a minimum in the asymmetry as a function of the applied field, in correspondence of the level crossing,22 superimposing this minimum on the increase in A ( t ) caused by the field‐dependent change in α would then result in the behaviour we observe. Assuming this model, then a subtraction of an estimated background contribution (grey line, bottom‐right inset, Figure 9) leads to the resonance shown in the upper panel of the right inset, Figure 9, which has a full width half maximum of around 0.5 T. The precise width of a resonance derived in this way is highly dependent on the model used to fit the background, but is generally much larger than that expected for a pure level crossing involving states of different symmetries.…”
Section: Resultsmentioning
confidence: 89%
“…Indeed, the peak is larger than the expected variation in background in this field range. If we interpret the data in this way then, assuming linear variation of A ( t =0) either side of the crossing, we estimate this occurs with a centre at B cross =3.73(5) T. Since we expect a minimum in the asymmetry as a function of the applied field, in correspondence of the level crossing,22 superimposing this minimum on the increase in A ( t ) caused by the field‐dependent change in α would then result in the behaviour we observe. Assuming this model, then a subtraction of an estimated background contribution (grey line, bottom‐right inset, Figure 9) leads to the resonance shown in the upper panel of the right inset, Figure 9, which has a full width half maximum of around 0.5 T. The precise width of a resonance derived in this way is highly dependent on the model used to fit the background, but is generally much larger than that expected for a pure level crossing involving states of different symmetries.…”
Section: Resultsmentioning
confidence: 89%
“…The HiFi spectrometer is built around the 5T superconducting split pair magnet (and fast-sweep z-axis coils up to 40 mT as well as 15 mT x-and y-axis transverse coils) with a room temperature internal bore along the beam axis, which contains the detectors and four transverse ports (sides, top, and bottom). 21 These ports form a "cruciform" which is usually pumped and provides an insulating vacuum for cryostats. As shown in Fig.…”
Section: Laser Beam Transportmentioning
confidence: 99%
“…20 One of the spectrometers, HiFi, can apply a magnetic field on a sample up to 5 T, and is optimized for time-differential muon spin relaxation studies. 21 Such high field is especially useful in the avoided level-crossing (ALC) resonance technique, which probes the Mu energy states by scanning and finding a field where two Mu levels cross over. [2][3][4]22 At the specific field the muon spin is depolarized either because 1) the muon polarization is transferred to neighboring nuclear spins due to quantum mechanically coupled states (so-called ∆ 0 transition), or 2) the muon spin flips due to its precession around the symmetry axis of Mu (this ∆ 1 transition is usually only observable in solids).…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…The reason for this were limitations in the high-field/low-temperature capabilities of existing μ + SR instruments and the difficulty of such experiments. The commissioning of the worldwide-unique HiFi instrument at ISIS, U.K. [11] now enables μ + SR to probe spin dynamics in longitudinal fields up to 5 T at 20 mK. The longitudinal (field parallel to initial muon spin) configuration is necessary for probing spin dynamics.…”
mentioning
confidence: 99%