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A> T3 :Pm 4w1 s$L...HI WQJUHIX 111K=-162 3d I G -:89 6 I 1898 *(20K)I 4.3H Dewarb,c GJoule-Thomson 1908\_T]I (4.2K)H ... or chirality associated with the domain. No one had yet seen

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Page 1: A> T3 :Pm 4w1 s$L...HI WQJUHIX 111K=-162 3d I G -:89 6 I 1898 *(20K)I 4.3H Dewarb,c GJoule-Thomson 1908\_T]I (4.2K)H ... or chirality associated with the domain. No one had yet seen

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Page 2: A> T3 :Pm 4w1 s$L...HI WQJUHIX 111K=-162 3d I G -:89 6 I 1898 *(20K)I 4.3H Dewarb,c GJoule-Thomson 1908\_T]I (4.2K)H ... or chirality associated with the domain. No one had yet seen

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Page 3: A> T3 :Pm 4w1 s$L...HI WQJUHIX 111K=-162 3d I G -:89 6 I 1898 *(20K)I 4.3H Dewarb,c GJoule-Thomson 1908\_T]I (4.2K)H ... or chirality associated with the domain. No one had yet seen

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Page 4: A> T3 :Pm 4w1 s$L...HI WQJUHIX 111K=-162 3d I G -:89 6 I 1898 *(20K)I 4.3H Dewarb,c GJoule-Thomson 1908\_T]I (4.2K)H ... or chirality associated with the domain. No one had yet seen

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Page 5: A> T3 :Pm 4w1 s$L...HI WQJUHIX 111K=-162 3d I G -:89 6 I 1898 *(20K)I 4.3H Dewarb,c GJoule-Thomson 1908\_T]I (4.2K)H ... or chirality associated with the domain. No one had yet seen

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Page 6: A> T3 :Pm 4w1 s$L...HI WQJUHIX 111K=-162 3d I G -:89 6 I 1898 *(20K)I 4.3H Dewarb,c GJoule-Thomson 1908\_T]I (4.2K)H ... or chirality associated with the domain. No one had yet seen

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Page 7: A> T3 :Pm 4w1 s$L...HI WQJUHIX 111K=-162 3d I G -:89 6 I 1898 *(20K)I 4.3H Dewarb,c GJoule-Thomson 1908\_T]I (4.2K)H ... or chirality associated with the domain. No one had yet seen

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Page 8: A> T3 :Pm 4w1 s$L...HI WQJUHIX 111K=-162 3d I G -:89 6 I 1898 *(20K)I 4.3H Dewarb,c GJoule-Thomson 1908\_T]I (4.2K)H ... or chirality associated with the domain. No one had yet seen

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Page 9: A> T3 :Pm 4w1 s$L...HI WQJUHIX 111K=-162 3d I G -:89 6 I 1898 *(20K)I 4.3H Dewarb,c GJoule-Thomson 1908\_T]I (4.2K)H ... or chirality associated with the domain. No one had yet seen

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Page 10: A> T3 :Pm 4w1 s$L...HI WQJUHIX 111K=-162 3d I G -:89 6 I 1898 *(20K)I 4.3H Dewarb,c GJoule-Thomson 1908\_T]I (4.2K)H ... or chirality associated with the domain. No one had yet seen

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Page 11: A> T3 :Pm 4w1 s$L...HI WQJUHIX 111K=-162 3d I G -:89 6 I 1898 *(20K)I 4.3H Dewarb,c GJoule-Thomson 1908\_T]I (4.2K)H ... or chirality associated with the domain. No one had yet seen

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Page 12: A> T3 :Pm 4w1 s$L...HI WQJUHIX 111K=-162 3d I G -:89 6 I 1898 *(20K)I 4.3H Dewarb,c GJoule-Thomson 1908\_T]I (4.2K)H ... or chirality associated with the domain. No one had yet seen

������# U2D2��MRI�

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Synopsis: Imaging Domains in SuperfluidHeliumMay 17, 2018

An MRI imaging technique reveals a structure of chiral domains in a slab of superfluid helium-3.

Magnetic resonance imaging (MRI) is best known as a medical imaging tool, but it can also beapplied to visualize microscopic features of quantum materials like superfluids andsuperconductors. A high-resolution MRI technique has now allowed Yutaka Sasaki of KyotoUniversity, Japan, and colleagues to uncover a previously hidden structure of chiral domains insuperfluid helium-3 ( ). The result suggests that MRI might be used to visualize vortices and othertopological structures in a variety of quantum materials.

When is cooled below a few millikelvin, it becomes a superfluid—a fluid that can flow with zeroviscosity. Previous experiments have led physicists to suspect that as enters this phase, it breaksup into macroscopic domains. Each domain contains superfluid atoms with a common angularmomentum, so that there is a handedness, or chirality associated with the domain. No one had yetseen these domains, but doing so would help physicists test their theoretical understanding of notonly superfluidity but also related forms of superconductivity.

Sasaki’s team investigated a thin film of superfluid at 2 mK with an MRI technique that theypreviously developed to acquire images of ultracold quantum condensates with 10 m spatialresolution. Analysis of the MRI data showed that the sample was divided into two or more

J. Kasai et al., Phys. Rev. Lett. (2018)

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Kasai�(����)����PHYSICAL REVIEW LETTERS120, 205301 (2018)

Page 13: A> T3 :Pm 4w1 s$L...HI WQJUHIX 111K=-162 3d I G -:89 6 I 1898 *(20K)I 4.3H Dewarb,c GJoule-Thomson 1908\_T]I (4.2K)H ... or chirality associated with the domain. No one had yet seen

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