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Title: PT-invariant periodic potentials with a finite number of band gaps

Journal Article · · Journal of Mathematical Physics
DOI:https://doi.org/10.1063/1.2000207· OSTI ID:20699337
;  [1]
  1. Institute of Physics, Sachivalaya Marg, Bhubaneswar 751005 (India)

We obtain the band edge eigenstates and the midband states for the complex, generalized associated Lame potentials V{sup PT} (x)=-a(a+1)m sn{sup 2} (y,m)-b (b+1)m sn{sup 2} (y+K(m),m)-f (f+1)m sn{sup 2} (y+K(m)+iK{sup '} (m),m)-g(g+1)m sn{sup 2} (y+iK{sup '}x(m),m), where y{identical_to}ix+{beta}, and there are four parameters a, b, f, g. By construction, this potential is PT-invariant since it is unchanged by the combined parity (P) and time reversal (T) transformations. This work is a substantial generalization of previous work with the associated Lame potentials V(x)=a(a+1)m sn{sup 2}(x,m)+b(b+1)m sn{sup 2}(x+K(m),m) and their corresponding PT-invariant counterparts V{sup PT}(x)=-V(ix+{beta}), both of which involving just two parameters a,b. We show that for many integer values of a,b,f,g, the PT-invariant potentials V{sup PT}(x) are periodic problems with a finite number of band gaps. Further, using supersymmetry, we construct several additional, complex, PT-invariant, periodic potentials with a finite number of band gaps. We also point out the intimate connection between the above generalized associated Lame potential problem and Heun's differential equation.

OSTI ID:
20699337
Journal Information:
Journal of Mathematical Physics, Vol. 46, Issue 8; Other Information: DOI: 10.1063/1.2000207; (c) 2005 American Institute of Physics; Country of input: International Atomic Energy Agency (IAEA); ISSN 0022-2488
Country of Publication:
United States
Language:
English