By Len Deighton

An unnamed secret agent - probably an identical reluctant hero of The Ipcress dossier - is distributed to Paris to carry a dossier of nuclear secrets and techniques to a French surgeon, yet quickly reveals himself sucked right into a twilight international of intercourse, blackmail and hidden reason, the place good friend and enemy turn into indistinguishable.

A 'clinic' on Paris's street Foch designed to cater lavishly for a number of perversions, staffed through a gaggle of sexually and intellectually high-powered women and outfitted with units starting from an Iron Maiden to psychedelic truth-drugs -- that's the set-up operated by way of the enigmatic Monsieur Datt.

Naturally, it has a hidden objective: to bring together dossiers of tape and movie on influential political consumers from East and West. Into this twilight international of decadence and hidden reasons come the brokers of 4 international powers.

Are they after Datt's pornographic blackmail dossiers? Or is their goal altogether extra lethal than a visit to the blue movies...?

This new reissue incorporates a foreword from the canopy clothier, Oscar-winning filmmaker Arnold Schwartzman, and a new creation by means of Len Deighton, which deals a desirable perception into the writing of the tale.

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Additional resources for An Expensive Place to Die (Harry Palmer, Book 5)

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The equations which define Exc [ρ], starting with Eq. 13) for E[ρ], are hopelessly complicated. The utility of the Kohn-Sham formulation is that the exchange-correlation terms in Eg , Eq. 30), are small, so an approximation is acceptable. 31) where X(ρ(r)) is a function of ρ(r), not a functional. 28), the exchange-correlation potential Vxc (r) also becomes a function of the local density ρ(r), Vxc (r) = d[ρ(r)X(ρ(r))] . 32) Kohn and Sham (1965) pointed out that the local density approximation is correct for a uniform electron gas, and in fact they limited their original derivation to the local density approximation.

It will then be very useful to split the electronic excitation Hamiltonian into a part evaluated at the reference structure, and the remaining part which sees the motion of the nuclei. Positions of the nuclei in the reference structure are denoted RK , K = 1, · · ·, N . The potential of an electron at r, due to the nuclei in configuration {rK }, has been denoted V(r), and is more completely specified as V(r; {rK }). Let us write V σ (r) to denote evaluation at the nuclear reference structure, so that V σ (r) = V(r; {RK }).

17) . 18) λ where δVλλ = ψλσ |δVg |ψλσ November 6, 2002 15:30 WorldScientific/ws-b8-5x6-0 TOTAL HAMILTONIAN WallaceBook 29 Notice once again that both δVλλ and δEλ depend parametrically on the nuclear positions, and they also have an implicit dependence on the reference structure itself. 8) can now be written σ H= ˙ HN + HEX + δHEX . 19) This is a valuable result. First, since the nuclear positions do not appear as σ σ variables in HEX , then HN and HEX commute, which means there is no interaction between the motion of the nuclei and the excitation of reference σ structure electrons.

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