 

Bsh  Bsh0 mˆ  zˆ  ˆje mˆ



ˆje



/ 2 e    sh J c t f M s 

Bsh0

2

 sh  J s J c

/ www.sciencemag.org/content/early/recent / 11 June 2015 / Page 1 / 10.1126/science.aaa1442



Downloaded from www.sciencemag.org on June 11, 2015

Research Articles

Fshy

μ

B  0.5

μ

μ

μ

μ

B  0.5

μ

B  0.46

/ sciencemag.org/content/early/recent / 11 June 2015 / Page 2 / 10.1126/science.aaa1442

 Δt  μ

μ

B  100

S 1

m   m   y m  dxdy 4   x

B  0.5

v   

t 

/ sciencemag.org/content/early/recent / 11 June 2015 / Page 3 / 10.1126/science.aaa1442

B  10

/ sciencemag.org/content/early/recent / 11 June 2015 / Page 4 / 10.1126/science.aaa1442

/ sciencemag.org/content/early/recent / 11 June 2015 / Page 5 / 10.1126/science.aaa1442

Fshy

/ sciencemag.org/content/early/recent / 11 June 2015 / Page 6 / 10.1126/science.aaa1442

B  0.5

/ sciencemag.org/content/early/recent / 11 June 2015 / Page 7 / 10.1126/science.aaa1442

B  0.46

/ sciencemag.org/content/early/recent / 11 June 2015 / Page 8 / 10.1126/science.aaa1442

B  100

B  10

/ sciencemag.org/content/early/recent / 11 June 2015 / Page 9 / 10.1126/science.aaa1442

Magnetism. Blowing magnetic skyrmion bubbles.

The formation of soap bubbles from thin films is accompanied by topological transitions. Here we show how a magnetic topological structure, a skyrmion...
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