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Typically, the reinsurance company pays out all of the premium income or more but keeps the investment returns on the money while it held the reserves The reserves plus much of the reinsurance company surplus are invested in hedge funds The returns on the hedge funds accumulate tax-free The underwriting pro ts (premiums minus payouts) or losses (payouts minus premiums) accumulate along with the hedge fund returns The reinsurance investors expect that when they sell their shares, the investment returns and the underwriting gains or losses will be taxed as long-term capital gains The reinsurance companies that invest in hedge funds have generally been closely associated with particular hedge fund managers MaxRe recently held 40 percent of its investment portfolio in Louis Bacon s Moore Holdings Stockton Reinsurance invests in af liated Commodity Corporation (owned by Goldman Sachs) Hampton Re (organized by J P Morgan) invests in J P.

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This form and the instructions for its use are available on the United States Patent and Trademark Office (USPTO) web site at http://www3.uspto.gov/teas/PrintV1.22/TFORMWIN.htm.

Morgan products Hirch Re invests in the Hirch funds Asset Alliance Re invests in Asset Alliance hedge funds These hedge fund.

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where 0 5 c1 < c g < . . . < c., 5 1 are suitable constants. These s parameters fully determine the method (its consistency, convergence, stability, and all other aspects). With

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When patent infringement occurs, the public franchise is violated, and the methodology developed above is no longer applicable. In this event, a patent or patent portfolio may only be worth as much as one expects to recover in damages through litigation (less the cost of litigation). Any patent owner whose patents have been infringed and whose public franchise afforded by these patents has been compromised, would seek (aside from damages) a permanent injunction to restore the monopoly. Thus, the value of the patent portfolio is 23. V PP E F a Ri

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breaking up some Cooper pairs See Table 33 for penetration depth1 and coherence length Crystal defects and impurities can change the coherence length, so purity is always a goal The normal current ow produces loss However the increase in resistivity is small until Tc is approached As frequency increases from zero, the electron pair kinetic energy produces a delay that creates an electric eld along the surface An applied magnetic eld can also force all electrons to normal; this is the critical eld, Hc It is useful to compare a superconductor with a perfect electric conductor (PEC) As seen in the sketch of Figure 31, the PEC at any temperature and any applied magnetic eld contains an internal magnetic eld; current can ow without loss.

Here are some important terms you need to know when working with tabs: Ribbon: The whole bar, including all of the tabs. File tab: A tab-like button that opens Backstage view, from which you can choose to start a new presentation, save, print, and perform other le-related activities. See Figure 1-10 for this button s location. Quick Access Toolbar: A small toolbar adjacent to the Of ce button from which you can select commonly used commands.

For the superconductor, when a magnetic eld is applied and the temperature lowered below Tc, the magnetic eld is expelled, except at the surface Again, current can ow without loss Bardeen Cooper Schrieffer theory makes a quantum mechanical formulation for the paired electrons It relates critical temperature, critical magnetic eld Hc, coherence length, etc It represents LTS well, but only partially for HTS For both LTS and HTS there are two types of materials: Type I and Type II Type I materials are typically soft metallic elements, exhibiting the Meissner effect up to Hc Coherence length is roughly comparable to penetration depth The London penetration depth is the depth of current induced by a magnetic eld It is analogous to skin depth, which is the depth of current in a normal conductor Type II materials have two critical magnetic elds, Hc1 and Hc2.

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These have short coherence length and long penetration depth The Meissner effect exists for elds up to Hc1; at Hc2 the conductor is normal Between Hc1 and Hc2 ux cores or vortices exist, with the spacing between them decreasing as H approaches Hc2 Each vortex contains one ux quanta; a supercurrent circulates around the core Vortices are typically cylindrical, with radius of one or two coherence lengths Table 34 gives critical elds for representative materials Superconductivity is not only destroyed by high current density, by high magnetic elds, or by high temperature, but also by high frequency, in particular by.

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