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Observation of 4π-periodicity of the spinor using neutron resonance interferometry. / Kraan, W. H.; Grigoriev, S. V.; Rekveldt, M. Th.

In: Europhysics Letters, Vol. 66, No. 2, 15.04.2004, p. 164-170.

Research output: Contribution to journal › Article › peer-review

Harvard

Kraan, WH, Grigoriev, SV & Rekveldt, MT 2004, 'Observation of 4π-periodicity of the spinor using neutron resonance interferometry', Europhysics Letters, vol. 66, no. 2, pp. 164-170. https://doi.org/10.1209/epl/i2003-10202-4

APA

Kraan, W. H., Grigoriev, S. V., & Rekveldt, M. T. (2004). Observation of 4π-periodicity of the spinor using neutron resonance interferometry. Europhysics Letters, 66(2), 164-170. https://doi.org/10.1209/epl/i2003-10202-4

Vancouver

Kraan WH, Grigoriev SV, Rekveldt MT. Observation of 4π-periodicity of the spinor using neutron resonance interferometry. Europhysics Letters. 2004 Apr 15;66(2):164-170. https://doi.org/10.1209/epl/i2003-10202-4

Author

Kraan, W. H. ; Grigoriev, S. V. ; Rekveldt, M. Th. / Observation of 4π-periodicity of the spinor using neutron resonance interferometry. In: Europhysics Letters. 2004 ; Vol. 66, No. 2. pp. 164-170.

BibTeX

@article{39dbf9b6bf74425696c104c5f58dbf8a,
title = "Observation of 4π-periodicity of the spinor using neutron resonance interferometry",
abstract = "A polarised neutron beam is passed through a gradient resonance flipper. By the amplitude of their RF field, such flippers can be set at flip probability ρ = 0, 1, or 1/2. At 1/2, the neutron wave splits into a flipped and a non-flipped part with different precession. We measure the polarisation after a spin-echo (SE) setup with each precession arm made up of 2 such flippers. Offset from SE is made by varying the static fields in one flipper while the other flippers stay unchanged. This shows up as a periodic behaviour of the polarisation. With incoming polarisation parallel to the static field in the flippers - set at ρ = 1/2 - this period is twice the period measured for both ρ = 0 and 1 and with polarisation perpendicular to the static field. In the latter experiments both components of the spinor are affected, whereas in the former experiment we create spin states in which only one spinor component in one state is affected. Hence, this experiment demonstrates explicitly the 4π-periodicity of the spinor.",
author = "Kraan, {W. H.} and Grigoriev, {S. V.} and Rekveldt, {M. Th}",
year = "2004",
month = apr,
day = "15",
doi = "10.1209/epl/i2003-10202-4",
language = "English",
volume = "66",
pages = "164--170",
journal = "Lettere Al Nuovo Cimento",
issn = "0295-5075",
publisher = "IOP Publishing Ltd.",
number = "2",

}

RIS

TY - JOUR

T1 - Observation of 4π-periodicity of the spinor using neutron resonance interferometry

AU - Kraan, W. H.

AU - Grigoriev, S. V.

AU - Rekveldt, M. Th

PY - 2004/4/15

Y1 - 2004/4/15

N2 - A polarised neutron beam is passed through a gradient resonance flipper. By the amplitude of their RF field, such flippers can be set at flip probability ρ = 0, 1, or 1/2. At 1/2, the neutron wave splits into a flipped and a non-flipped part with different precession. We measure the polarisation after a spin-echo (SE) setup with each precession arm made up of 2 such flippers. Offset from SE is made by varying the static fields in one flipper while the other flippers stay unchanged. This shows up as a periodic behaviour of the polarisation. With incoming polarisation parallel to the static field in the flippers - set at ρ = 1/2 - this period is twice the period measured for both ρ = 0 and 1 and with polarisation perpendicular to the static field. In the latter experiments both components of the spinor are affected, whereas in the former experiment we create spin states in which only one spinor component in one state is affected. Hence, this experiment demonstrates explicitly the 4π-periodicity of the spinor.

AB - A polarised neutron beam is passed through a gradient resonance flipper. By the amplitude of their RF field, such flippers can be set at flip probability ρ = 0, 1, or 1/2. At 1/2, the neutron wave splits into a flipped and a non-flipped part with different precession. We measure the polarisation after a spin-echo (SE) setup with each precession arm made up of 2 such flippers. Offset from SE is made by varying the static fields in one flipper while the other flippers stay unchanged. This shows up as a periodic behaviour of the polarisation. With incoming polarisation parallel to the static field in the flippers - set at ρ = 1/2 - this period is twice the period measured for both ρ = 0 and 1 and with polarisation perpendicular to the static field. In the latter experiments both components of the spinor are affected, whereas in the former experiment we create spin states in which only one spinor component in one state is affected. Hence, this experiment demonstrates explicitly the 4π-periodicity of the spinor.

UR - http://www.scopus.com/inward/record.url?scp=2142697127&partnerID=8YFLogxK

U2 - 10.1209/epl/i2003-10202-4

DO - 10.1209/epl/i2003-10202-4

M3 - Article

AN - SCOPUS:2142697127

VL - 66

SP - 164

EP - 170

JO - Lettere Al Nuovo Cimento

JF - Lettere Al Nuovo Cimento

SN - 0295-5075

IS - 2

ER -

ID: 86434104