Frequency shifts in pulsed NMR for 3He(A)

W. F. Brinkman; H. Smith

doi:10.1016/0375-9601(75)90003-1

Frequency shifts in pulsed NMR for ³He(A)

W. F. Brinkman, H. Smith

Physics

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32 Scopus citations

Abstract

The ringing frequency recently observed by Osheroff and Corruccini in pulsed NMR experiments on the A-phase of ³He is calculated from Leggett's resonance equations. For large magnetic fields the frequency is Ω = γH + (Ω²_L/8γH)(1 + 3 cos θ), where θ is the tipping angle, and Ω_L is the longitudinal resonance frequency.

Original language	English (US)
Pages (from-to)	449-450
Number of pages	2
Journal	Physics Letters A
Volume	51
Issue number	8
DOIs	https://doi.org/10.1016/0375-9601(75)90003-1
State	Published - May 5 1975

All Science Journal Classification (ASJC) codes

General Physics and Astronomy

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10.1016/0375-9601(75)90003-1

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title = "Frequency shifts in pulsed NMR for 3He(A)",

abstract = "The ringing frequency recently observed by Osheroff and Corruccini in pulsed NMR experiments on the A-phase of 3He is calculated from Leggett's resonance equations. For large magnetic fields the frequency is Ω = γH + (Ω2L/8γH)(1 + 3 cos θ), where θ is the tipping angle, and ΩL is the longitudinal resonance frequency.",

author = "Brinkman, \{W. F.\} and H. Smith",

year = "1975",

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doi = "10.1016/0375-9601(75)90003-1",

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publisher = "Elsevier B.V.",

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T1 - Frequency shifts in pulsed NMR for 3He(A)

AU - Brinkman, W. F.

AU - Smith, H.

PY - 1975/5/5

Y1 - 1975/5/5

N2 - The ringing frequency recently observed by Osheroff and Corruccini in pulsed NMR experiments on the A-phase of 3He is calculated from Leggett's resonance equations. For large magnetic fields the frequency is Ω = γH + (Ω2L/8γH)(1 + 3 cos θ), where θ is the tipping angle, and ΩL is the longitudinal resonance frequency.

AB - The ringing frequency recently observed by Osheroff and Corruccini in pulsed NMR experiments on the A-phase of 3He is calculated from Leggett's resonance equations. For large magnetic fields the frequency is Ω = γH + (Ω2L/8γH)(1 + 3 cos θ), where θ is the tipping angle, and ΩL is the longitudinal resonance frequency.

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U2 - 10.1016/0375-9601(75)90003-1

DO - 10.1016/0375-9601(75)90003-1

M3 - Article

AN - SCOPUS:0642307528

SN - 0375-9601

VL - 51

SP - 449

EP - 450

JO - Physics Letters A

JF - Physics Letters A

IS - 8

ER -

Frequency shifts in pulsed NMR for ³He(A)

Abstract

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