The circular photogalvanic effect (CPGE) is the part of a photocurrent that switches depending on the sense of circular polarization of the incident light. It has been consistently observed in systems without inversion symmetry and depends on non-universal material details. Here we find that in a class of Weyl semimetals (for example, SrSi2) and three-dimensional Rashba materials (for example, doped Te) without inversion and mirror symmetries, the injection contribution to the CPGE trace is effectively quantized in terms of the fundamental constants e, h, c and with no material-dependent parameters. This is so because the CPGE directly measures the topological charge of Weyl points, and non-quantized corrections from disorder and additional...
The chiral photocurrent or circular photogalvanic effect (CPGE) is a photocurrent that depends on th...
The circular photogalvanic effect (CPGE) is the only possible quantized signal in chiral Weyl and mu...
Weyl semimetals are gapless topological states of matter with broken inversion and/or time reversal ...
The circular photogalvanic effect (CPGE) is the part of a photocurrent that switches depending on th...
The circular photogalvanic effect (CPGE) is the part of a photocurrent that switches depending on th...
The circular photogalvanic effect (CPGE) is the part of a photocurrent that switches depending on th...
So far, the circular photogalvanic effect (CPGE) is the only possible quantized signal in Weyl semim...
Weyl semimetals are crystals in which electron bands cross at isolated points in momentum space. Ass...
Weyl semimetals are crystals in which electron bands cross at isolated points in momentum space. Ass...
Weyl semimetals are gapless topological states of matter with broken inversion and/or time reversal ...
Weyl semimetals are gapless topological states of matter with broken inversion and/or time reversal ...
Weyl semimetals are gapless topological states of matter with broken inversion and/or time reversal ...
The circular photogalvanic effect (CPGE) is the photocurrent generated in an optically active materi...
The chiral photocurrent or circular photogalvanic effect (CPGE) is a photocurrent that depends on th...
The chiral photocurrent or circular photogalvanic effect (CPGE) is a photocurrent that depends on th...
The chiral photocurrent or circular photogalvanic effect (CPGE) is a photocurrent that depends on th...
The circular photogalvanic effect (CPGE) is the only possible quantized signal in chiral Weyl and mu...
Weyl semimetals are gapless topological states of matter with broken inversion and/or time reversal ...
The circular photogalvanic effect (CPGE) is the part of a photocurrent that switches depending on th...
The circular photogalvanic effect (CPGE) is the part of a photocurrent that switches depending on th...
The circular photogalvanic effect (CPGE) is the part of a photocurrent that switches depending on th...
So far, the circular photogalvanic effect (CPGE) is the only possible quantized signal in Weyl semim...
Weyl semimetals are crystals in which electron bands cross at isolated points in momentum space. Ass...
Weyl semimetals are crystals in which electron bands cross at isolated points in momentum space. Ass...
Weyl semimetals are gapless topological states of matter with broken inversion and/or time reversal ...
Weyl semimetals are gapless topological states of matter with broken inversion and/or time reversal ...
Weyl semimetals are gapless topological states of matter with broken inversion and/or time reversal ...
The circular photogalvanic effect (CPGE) is the photocurrent generated in an optically active materi...
The chiral photocurrent or circular photogalvanic effect (CPGE) is a photocurrent that depends on th...
The chiral photocurrent or circular photogalvanic effect (CPGE) is a photocurrent that depends on th...
The chiral photocurrent or circular photogalvanic effect (CPGE) is a photocurrent that depends on th...
The circular photogalvanic effect (CPGE) is the only possible quantized signal in chiral Weyl and mu...
Weyl semimetals are gapless topological states of matter with broken inversion and/or time reversal ...