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  2. NATURAL SCIENCES TRIPOS Part II Wednesday 19 January 2011 ...

    www.tcm.phy.cam.ac.uk/~cc726/TP1/ExamFiles/exam11.pdf
    24 Jan 2011: xµ = (t, x) with x the two-dimensional position vector. Thedynamics of Aµ are determined by the ‘Maxwell-Chern-Simons’ Lagrangian.
  3. examples_all.dvi

    www.tcm.phy.cam.ac.uk/~achc2/pt2thermo.pdf
    30 Apr 2011: 4. Use a Maxwell relation and the chain rule to show that for any substancethe rate of change of T with p in a reversible adiabatic compression is givenby. (.
  4. NATURAL SCIENCES TRIPOS Part II Wednesday 19 January 2011 ...

    www.tcm.phy.cam.ac.uk/~cc726/TP1/ExamFiles/exam11sol.pdf
    24 Jan 2011: 4 The ‘Maxwell-Chern-Simons’ Lagrangian is. LMCS = 1. 4FµνF. µν gϵµνλAµνAλ.

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