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Equation (5.6) only states that the magnetic field is transverse. The remaining Maxwell equations yield the following equations in reciprocal space:

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ell(k, t) = -i47r ~a(k, t),

are not patentable because they are either contrary to the public order or because of their moral implications These technologies include processes for human cloning, for modifying the germ line genetic identity of humans, and for industrial and commercial use of human embryos The directive also has provisions against patenting processes that modify the genetic identity of animals that are likely to cause them suffering without any sub stantial medical bene t to humans from the process One of the greatest sources of contention over biotech patent rights at the international level is related to bioprospecting, which is the search for genetic material from among the biological resources of less developed countries The aim of bioprospecting is to nd genetic material that can form the basis of new pharmaceuticals or agricultural products that can then be patented and placed on the global market.

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B(k, t) = -ick /I. e..L (k, t),

(5.78) (5.79) (5.80)

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47r:J ..L(k, t),

The concern is that the countries in which the prospecting is typically performed are least able to afford the new technology Although they may have an abundance of trop ical rain forests and other biologically diverse ecosystems, underdeveloped countries often can t afford the drugs and agricultural products that have been developed from genetic material that they contributed Ownership of biological resources is also an issue when it affects economies based on regional crops For example, in 1997, US re searchers at RiceTech, Inc patented a form of jasmine rice that would grow in the US RiceTech also won the trademark, jasmati for its rice Farmers in Thailand responded by accusing the researchers of stealing the genetic material of their rice without the country s permission, and of us ing a trademark that intentionally confuses customers, thereby threaten ing their local rice economy.

t..L (k, t) = ick!\ B(k, t) -

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where a(k, t) is p(k, t) in reciprocal space, ell (k, t) is the longitudinal component of the electric field in reciprocal space, and e..L (k, t), B(k, t), and :J..L (k, t) are the transverse components of E (r, t), B (r, t), and J (r, t) in reciprocal space. The longitudinal component of the current density satisfies the equation of conservation of charge: (5.81 ) a(k, t) + ikJiI(k, t) = O. We will adopt the canonical quantization procedure described in 2. To do so, we have to obtain the canonical variables associated with the Hamiltonian description of this system. These are variables such that when the Hamiltonian of the system is expressed in terms of them, Maxwell equations and the Newton-Lorentz equations for the charged particles are recovered from Hamilton equations of motion. The Hamiltonian of the system is just the total energy, given by

~ L mo<r~ + VCoul + Htrans,

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