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The source of nancing for biotech research and development in the United States is representative of most of the developed countries. Industry and the government provide the bulk of nancing, followed by universities, col leges, and other nonpro t institutions that provide the balance. The distri bution of nancing for all research and development in the United States for 2002, based on statistics from the National Science Foundation, is shown in Figure 6.13. Of the $292 billion generated for research and development in the United States during 2002, about 66 percent of the funding was supplied

Use the procedure here only for early-payment discounts. If you want to give a discount for some other reason (for example, a coupon), use a discount item on the invoice instead. See 14. 1. Go to Customers Receive Payments (or click the Receive Payments icon on the Customer Navigator screen). The Receive Payments dialog box opens.

(9.53)

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also holds up to first order. Then (9.39) is valid up to first order and our expansion into perfect modes makes sense. but only up to first order (see also Problem 9.8). To go beyond the high-Q regime and be able to deal with larger losses. we have to use modes that satisfy the exact boundary conditions at the semitransparent mirror. These are the natural modes of the cavity and. unlike perfect modes, they are non orthogonal. We discuss natural modes in the rest of this chapter. But now let us determine the Hamiltonian and the coupling within this high-Q approximation. As mentioned before. (9.39) does suggest a parallel with the dressed operator version of Fano diagonaIization [38]. In the Fano diagonaIization method, however. the global operators a( k) and at (k) that diagonalize the Hamiltonian are the unknowns that we wish to determine, whereas the an, a~. b(k), bt(k) together with the nondiagonal Hamiltonian that couples then are known. In contrast, here we have the opposite. a(k) and at (k) and the diagonal Hamiltonian are known. while the an. a~. b(k). bt(k) and their nondiagonal Hamiltonian are not. So here we wish to do the reverse of the Fano diagonalization that was done in [37]. Using (9.39) in (9.17), we can write the Hamiltonian in terms of the operators an, a~, b(k). and bt(k) instead of a(k) and at(k). As we have seen above, this will be correct only up to first order in E. SO we should use the approximate expressions (9.50) for anl (k) and a n2 (k). as well as (9.54)

2. While entering a payment as discussed earlier in this chapter, click the Credits & Discounts button (see Figure 16-4). The Discounts and Credits Information dialog box appears (as shown in Figure 16-7) with the suggested discount calculated based on the payment terms assigned to the invoice and whether the payment is being received within those terms (for example, within 10 days for 2% 10 Net 30).

(7.9)

1981 1999.

As you can see, the interaction of the atoms of the material medium with the cavity mode depends only on the weighted sum of all the atomic creation and annihilation operators, L7=1 gj(bj + bj). Now it is possible to define a collective atomic annihilation operator composed of the ordinary atomic annihilation operators weighted by

(7.10)

QuickBooks calculates a suggested discount amount based on your payment terms, as shown in Figure 16-7, with the customer and the payment date. You can enter any discount amount you choose; you don t have to use the suggested amount. However, the amount of the discount cannot be higher than the original invoice. 1. Enter the name of the expense account you use to track discounts (for example, Discount Expense). 2. Click Done to record the discount. Save the payment.

(7.11)

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