Download e-book for iPad: The Final Cut (A Brit in the FBI, Book 1) by Catherine Coulter, J. T. Ellison

By Catherine Coulter, J. T. Ellison

From Catherine Coulter, the number one New York Times-bestselling writer of the FBI mystery sequence, and J.T. Ellison, bestselling writer and ITW Award winner, comes the 1st booklet in a super new overseas mystery sequence that includes the hot hero: American-born, UK-raised Nicholas Drummond.

Scotland Yard’s new leader inspector Nicholas Drummond is at the first flight to big apple whilst he learns his colleague, Elaine York, the “minder” of the Crown Jewels for the “Jewel of the Lion” express on the Metropolitan Museum of artwork, was once came across murdered. Then the center-piece of the convey, the notorious Koh-i-Noor Diamond, is stolen from the Queen Mother’s crown. Drummond, American-born yet raised within the united kingdom, is a depressing, harmful, fast-rising megastar within the backyard who by no means backs down. And this situation isn't any exception.

Special brokers Lacey Sherlock and Dillon Savich from Coulter’s bestselling FBI sequence don’t hesitate to assist Drummond locate the crafty foreign thief referred to as the Fox. Nonstop motion and excessive stakes accentuate because the chase will get lethal. The Fox will cease at not anything to bring the Koh-i-Noor to the guy who believes in its lethal prophecy. Nicholas Drummond, together with his accomplice, FBI distinct Agent Mike Caine, lay it at the line to retrieve the diamond for Queen and state.

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Extra resources for The Final Cut (A Brit in the FBI, Book 1)

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200) 2M Now we are in trouble! Not only do we have to face the problem of singularities in G(x, x|A), but we also have to give a meaning to the derivative at this singular coincidence point. The first guess is to introduce an appropriate point splitting regarding the two arguments of the Green’s function. But then, we have to keep in mind that G(x, x |A) is a gauge variant quantity while G(x, x|A) is not. In order to ensure gauge invariance, we have to replace the ordinary derivative with covariant derivatives.

90) The scalars v 2,⊥ simply become v 2,⊥ = ω 2 sin2 θ. 92) sin eBs sin eBs eBs cos νeBs νeBs sin νeBs cot eBs + N⊥ = − sin eBs sin eBs 2eBs(cos νeBs − cos eBs) . + sin3 eBs Here, we have arrived at the representation of the polarization tensor found by Tsai and Erber [160], who employed this expression to obtain refractive indices for a magnetic background over a wide range of frequency and field strength. We shall confine ourselves to the case of low-frequency photons, ω m, which allows us to approximate the function φ0 in the exponent by Π0 → m2 .

155)  (−) R(s)µ ν = ˆ R(s) ≡ e2C s  1 0 0 0  0 cos 2eBs sin 2eBs 0   =  0 − sin 2eBs cos 2eBs 0  . 157) where ˆ I(s) I(s)µ ν =   2s 0 0 0  0 (sin 2eBs)/(eB) (1 − cos 2eBs)/(eB) 0   =  0 (cos 2eBs − 1)/(eB) (sin 2eBs)/(eB) 0  . 39) of Sect. 1. In the case of a purely magnetic field, the expression reduces to x(0) (s)|x(0) (0) ≡ x(0) | U (0) (s) |x(0) eBs i ei(e/2)σF s . e. the constant-field part of the problem. Our next intermediate step is characterized by finding the relations between the zeroth-order and exact quantities.

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