Earlier Research on Correlated Electron Systems using

Quantum Monte Carlo Methods
For my dissertation at the University of Maryland, and as a post-doctoral fellow at Penn State, I studied many electron problems where the correlation effects are such that they have to be treated in a careful manner beyond the standard perturbative treatments of electron correlations. These problems I have addressed using Quantum Monte Carlo(QMC) methods.

  • Hubbard model and high-temperature superconductivity

    Electron correlation effects are well studied in a lattice model, known as Hubbard Model where correlation are introduced through (i}) the constraints that no two electrons with the same spin can occupy the same lattice site and ( ii) an additional cost in energy if two electrons with different spins occupy the same site. Following the discovery of high temperature supercondictivity(HTSC) a general belief grew that high transition temperature can only result from electron-electron (and not electron-phonon) interactions. Many new ideas were introduced using Hubbard model as the paradigm of these theories. I have studied some aspects of HTSC both in simple and a multi-band Hubbard Model by use of QMC methods which have become very powerful tools to take into account strong electron correlations properly

  • Aniket Bhattacharya and C. S. Wang
    The generalized flux phases, Hubbard versus t-J model
    Rapid Communication, Phys. Rev. B, 45 , 10826 (1992).

  • Aniket Bhattacharya and C. S. Wang
    Spin and charge fluctuations in an extended Hubbard model of oxide superconductors
    Phys. Rev. B, 48, 13949 (1993).



  • Exact Green's function Quantum Monte Carlo methods applied

    to small clusters

    At Penn State, I worked on calculating ground states energies of small clusters which are very weakly bound. For example the binding energy for the dimer He-H is of the order of 8kT only. It is difficult to extract such a small number accurately. So we used an exact Quantum Monte Carlo method which is computationally feasible for only small number of electron. The important fact is that these calculations are exact in the sense that it requires no further approximations beyond what is involved in Schrodinger equation; the only error involved is that of statistical sampling error.

  • Aniket Bhattacharya and J. B. Anderson
    An exact quantum Monte Carlo calculation of the H-He interaction potential Phys. Rev. A, 49, 2441 (1994).

  • Aniket Bhattacharya and J. B. Anderson
    Interaction potential of a symmetric helium trimer
    J. Chem. Phys, 100, 8999 (1994).