Ganpathy Murthy | University of Kentucky College of Arts & Sciences

Ganpathy Murthy

Professor

APS Fellow

Associate Chair

B. Tech, IIT Madras, 1982

PhD, Yale University, 1987

Faculty member at Boston University, 1990-1999

Contact Information

murthy@g.uky.edu

CP295

859-257-4729

Education

Ph.D., Yale University (1987)

Research Interests

Condensed Matter Physics

Affiliations

Physics & Astronomy
Condensed Matter Physics (Theory)

Research

Condensed Matter Theory

Much of my recent work is in the area of ``strongly correlated electron systems'', in which the interactions between electrons play a dominant role in selecting the ground state and low-energy excitations of the system. Usually Nature reorganizes the strongly interacting electrons into weakly interacting ``quasiparticles'', which are collective excitations of the electrons. Examples are Landau's Fermi liquid theory, where the quasiparticles have the same quantum numbers as the electron, or the Bardeen-Cooper-Schreiffer theory of superconductivity, where the gound state can roughly be described as a collection of Bose-condensed Cooper pairs (pairs of electrons of opposite spin and momentum). The collective excitations of this system are fermionic quasiparticles and bosonic phase fluctuations. More exotic reorganizations occur in fractional quantum Hall states, where the quasiparticles have a charge which is a fraction of the electron's charge. The fundamental problem of strongly correlated systems may be phrased as that of finding the correct weakly interacting quasiparticles, and the theory that describes their dynamics. Usually, because of the strong interactions, this connection between the original electrons and the final quasiparticles is nonperturbative (that is, the quasiparticle cannot be understood as a small deviation from a noninteracting electron). This makes the problem mathematically quite difficult.

The introduction of disorder, ubiquitous in real life in the form of lattice imperfections or impurity atoms, makes the problem much more challenging and interesting. Many symmetries of the clean system, such as translation and rotation, are now absent, and this makes the analysis of disordered systems much harder. More importantly, qualitatively new phenomena which are not present in systems without disorder can arise in systems with disorder, even when the electrons are noninteracting. Of course, real systems are both disordered and interacting, potentially leading to even more interesting new phenomena. I believe the interplay of interactions and disorder will be one of the dominant themes of condensed matter theory in the years to come, and I have started some investigations into this subfield. In particular, with my co-workers Herb Fertig, Harsh Mathur, R. Shankar, and Damir Herman, I have been able to obtain { nonperturbative} solutions to this problem in certain experimentally interesting regimes.

Specific topics I am working on are (i) The role of disorder in the bilayer quantum Hall systems, (ii) States with strong correlations and strong quantum fluctuations in mesoscopic systems, and (iii) The effect of disorder on gauge theories.

Education

B.Tech., Physics, Indian Institute of Technology, Madras (1982)
Ph.D., Theoretical Condensed Matter Physics), Yale University (1987)

PHY 231 Section C

Dear Students, welcome to PHY231. My name is Ganpathy Murthy and I
will be your instructor. Very shortly I will post the syllabus and
schedule for this course on this page, as well as on my page
(http://www.pa.uky.edu/~murthy/courses/phy231f12/).

However, a couple of points of advance information might be useful. I
am pretty old-fashioned and I will be using the whiteboards in
CP155. Also, since there are only about 60 of you (Sections 13 and
14), I will not use clickers. So PLEASE DO NOT BUY CLICKERS
SPECIFICALLY FOR THIS CLASS. I will also be using WebAssign for the
homework, but will make the recitation quizzes and exams myself. Finally, in
order to keep you engaged and to see whether what I say makes sense to
you, I will occasionally ask questions of random students in the
class. You may find it a bit startling and disconcerting initially,
but hopefully you will get used to it soon.

My room is CP295, and my email is murthy@pa.uky.edu. Please come by to
see me of send me an email if you have any questions. See you all next week.

Best,
Ganpathy Murthy.

PHY 231 Section C Syllabus

PHY 231 Section C Schedule

WebAssign website

Pre Lab Announcement

Effective Study Habits

Practice Assignments

Potential Midterm Problems

Solutions to Midterm 1

Solutions to Midterm 2

Solutions to Midterm 3

Midterm 1 grade distribution

Midterms 1 and 2 grade distribution

Midterm 3 grade distribution

Physics Resource Room

Announcements

My Lecture Notes

Selected Publications

Selected Publications:

G. Murthy, Phys. Rev. Lett. 84, 350 (2000): ``A Composite Fermion Hofstader Problem: Partially Polarized Density Wave States in the FQHE''.
G. Murthy, Phys. Rev. Lett. 85, 1954 (2000): ``Hall Crystal States at \nu=2 and Moderate Landau Level Mixing''.
G. Murthy, Jour. Phys. Cond. Mat. 12, 10543 (2000) : ``Finite Temperature Magnetism in Fractional Quantum Hall Systems: Composite Fermion Hartree-Fock and Beyond''.
G. Murthy, Phys. Rev. B 64, 195310 (2001): ``Hamiltonian theory of the fractional quantum Hall effect: Conserving approximation for in compressible fractions''.
R. Narevich, G. Murthy, and H. A. Fertig, Phys. Rev. B 64, 245326 (2001): ``Hamiltonian Theory of the Composite Fermion Wigner Crystal''.
G. Murthy, Phys. Rev. Lett. 87, 179701 (2001): ``Comment on ``Half-Polarized Quantum Hall States''''.
G. Murthy, Phys. Rev. B 64, 241309 (2001): ``Effects of Disorder on the \nu=1 Quantum Hall State''.
G. Murthy and R. Shankar, Phys. Rev. B 65, 245309 (2002): ``Hamiltonian Theory of the Fractional Quantum Hall Effect: Effect of Landau Level Mixing''.
G. Murthy and H. Mathur, Phys. Rev. Lett. 89, 126804 (2002): ``Interactions and Disorder in Quantum Dots; Instabilities of the Universal Hamiltonian''.
G. Murthy and R. Shankar, Phys. Rev. Lett. 90, 066801 (2003): ``Quantum Dots with Disorder and Interactions: A Solvable Large-g Limit''.
G. Murthy and R. Shankar, Rev. Mod. Phys. 75, 1101 (2003): ``Hamiltonian Theory of the Fractional Quantum Hall Effects''.
Y. N. Joglekar, H. K. Nguyen, and G. Murthy, Phys. Rev. B 68, 035332 (2003): "Edge Reconstructions in Fractional Quantum Hall Systems"
I. F. Herbut, B. H. Seradjeh, S. Sachdev, and G. Murthy, Phys. Rev. B 68, 195110 (2003): ``Absence of U(1) Spin Liquids in Two Dimensions''.
D. Herman, H. Mathur, and G. Murthy, cond-mat/0305364, Phys. Rev. B 69, 041301 (2004): ``Diamagnetic Persistent Currents and Spontaneous Time-Reversal Symmetry Breaking in Mesoscopic Structures''.
G. Murthy, R. Shankar, D. Herman, and H. Mathur, cond-mat/0306529, Phys. Rev. B 69, 075321 (2004): ``A Solvable Regime of Disorder and Interactions in Ballistic Nanostructures, Part I: Consequences for Coulomb Blockade''.
H. K. Nguyen, Y. N. Joglekar, and G. Murthy, Phys. Rev. B 70, 035324 (2004): ``Collective edge modes in fractional quantum Hall systems''.
G. Murthy, Phys. Rev. B 70, 153304 (2004): ``Random matrix crossovers and quantum critical crossovers for interacting electrons in quantum dots''.
G. Murthy, Phys. Rev. Lett. 94, 126803 (2005): ``Interplay between the mesoscopic Stoner and Kondo effects in quantum dots''.
G. Murthy, R. Shankar, and H. Mathur, Phys. Rev. B 72, 075364 (2005) : ``Ballistic Quantum Dots with Disorder and Interactions: A numerical study on the Robnik-Berry billiard''.
I. Rozhkov and G. Murthy, Phys. Rev. B 72, 193311 (2005): ``A nearly closed ballistic billiard with random boundary transmission''
H. A. Fertig and G. Murthy, Phys. Rev. Lett. 95, 156802 (2005): ``A Coherence Network in the Quantum Hall Bilayer''
I. Rozhkov and G. Murthy, Jour. Phys. A 38, 10843-10857 (2005): ``Ballistic dynamics of a convex smooth-wall billiard with finite escape rate along the boundary''.
R. Shankar and G. Murthy, Phys. Rev. B 72, 224414 (2005): ``Deconfinement in d=1: A closer look''.

For the latest ones see the cond-mat arXiv