Higher-Spin Theory of the Magnetorotons
- Univ. of Cambridge (United Kingdom)
- Univ. of Chicago, IL (United States)
Fractional quantum Hall liquids exhibit a rich set of excitations, the lowest-energy of which are the magnetorotons with dispersion minima at a finite momentum. We propose a theory of the magnetorotons on the quantum Hall plateaux near half filling, namely, at filling fractions ν = N/(2N+1) at large N. The theory involves an infinite number of bosonic fields arising from bosonizing the fluctuations of the shape of the composite Fermi surface. At zero momentum there are O(N) neutral excitations, each carrying a well-defined spin that runs integer values 2,3,…. The mixing of modes at nonzero momentum q leads to the characteristic bending down of the lowest excitation and the appearance of the magnetoroton minima. A purely algebraic argument shows that the magnetoroton minima are located at qℓB = zi/(2N+1), where ℓB is the magnetic length and zi are the zeros of the Bessel function J1, independent of the microscopic details. We argue that these minima are universal features of any two-dimensional Fermi surface coupled to a gauge field in a small background magnetic field.
- Research Organization:
- Univ. of Chicago, IL (United States)
- Sponsoring Organization:
- USDOE Office of Science (SC), High Energy Physics (HEP); Simons Foundation; European Research Council (ERC); Chicago MRSEC; National Science Foundation (NSF); ARO MURI Grant
- Grant/Contract Number:
- SC0009924; FG02-13ER41958; STG 279943; DMR-1420709; 63834-PH-MUR
- OSTI ID:
- 1595714
- Alternate ID(s):
- OSTI ID: 1332151
- Journal Information:
- Physical Review Letters, Vol. 117, Issue 21; ISSN 0031-9007
- Publisher:
- American Physical Society (APS)Copyright Statement
- Country of Publication:
- United States
- Language:
- English
Web of Science
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